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Mt = k$ Di(12) 4. Torsion <strong>moment</strong> <strong>at</strong> a Slippage <strong>of</strong> <strong>the</strong> Wheel <strong>set</strong>1D i = i-i i0di0~ 0 =dt(13)~ 0in <strong>the</strong> complex domain i0=(14)sdi~~ = in <strong>the</strong> complex domain i =(15)dtswhere k – <strong>torsion</strong> constant <strong>of</strong> driving shaft (4) – Fig. 2. The<strong>torsion</strong> constant <strong>of</strong> <strong>the</strong> leaves part <strong>of</strong> <strong>the</strong> driving shaft (i.e. part <strong>of</strong><strong>the</strong> driving shaft from <strong>the</strong> jagged reductor to <strong>the</strong> near monoblock<strong>wheel</strong>) is k 1 55310 6 Nmrad 1 . Torsion constant <strong>of</strong> <strong>the</strong> longerpart <strong>of</strong> <strong>the</strong> driving shaft (i.e. part <strong>of</strong> <strong>the</strong> driving shaft from <strong>the</strong>jagged reductor to <strong>the</strong> fur<strong>the</strong>r monoblock <strong>wheel</strong>) is k 2 9.810 6 Nmrad 1 [3]; θ 0 – banking <strong>of</strong> driving shaft (4) induced by<strong>the</strong> <strong>wheel</strong>-rail system.3. Resonance Frequency <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>Asi =0kiJ m D 2e0 + $ d n o $ s + k2transfer function W M is:2(16)Based on <strong>the</strong> former equ<strong>at</strong>ions, we made a program in MAT-LAB-SIMULINK to simul<strong>at</strong>e <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>at</strong> <strong>the</strong> <strong>wheel</strong><strong>set</strong>. We received a chronological variety <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong><strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft according to Fig. 4 when westarted from this <strong>simul<strong>at</strong>ion</strong> program. We assumed th<strong>at</strong> a slippage<strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong> appeared because <strong>of</strong> a nuisance value <strong>of</strong> <strong>the</strong> tractioncoefficient <strong>at</strong>D/ F ot2= = 1 (The traction coefficient <strong>at</strong>Mthis environment is defined by <strong>the</strong> following term: F 2 n $ QM0n27924.8849n 1 = = 023 . ).D 121 .$ Q a $ 2000002 2We also assumed th<strong>at</strong> <strong>the</strong> rot<strong>at</strong>ing <strong>moment</strong> <strong>of</strong> <strong>the</strong> shaft <strong>of</strong> <strong>the</strong>traction electromotor for wavy direct current is determined by:33 2 161Mt ^ h = $ k0$ Isrd1+ cos 2~ t+ cos 4~tn=3233 33(21)= M ^1+ a cos 2~ t+a cos 4~thsrMFv)0n1 2v a (where M sr – in between value <strong>of</strong> <strong>the</strong> torque <strong>of</strong> <strong>the</strong> shaft <strong>of</strong> <strong>the</strong> tractionelectromotor for wavy direct current; a 1 16/33 – factoramplitude <strong>of</strong> a frequency 2f 2 50 100 Hz; a 2 1/33 – factoramplitude <strong>of</strong> a frequency 4f 4 50 200 Hz.Mt1Wt= =MkJ k J m D 2f m $ + es2 0 + $ d n op $h $ i 222k D J m2e0 + $ d n o $ si 2$JJ J m D 2Km $ e0 + $ d n oK2KkJ k J m D$ s2KK m $ + e2 0 + $ d n oh $ i 2L2NOO+ 1OOOP(17)The dominant poles <strong>of</strong> <strong>the</strong> transfer function W M define <strong>the</strong>resonance frequency <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. The resonance frequency <strong>of</strong><strong>the</strong> <strong>wheel</strong> <strong>set</strong> is determined by <strong>the</strong> next equ<strong>at</strong>ion:~ =kJ k J m D2m $ + e2 0 + $ d n oh $ i 2J J m D2m $ e0 + $ d n o2(18)Based on <strong>the</strong> equ<strong>at</strong>ion (18), resonance frequencies <strong>of</strong> <strong>the</strong>leaves and longer <strong>of</strong> <strong>the</strong> driving shaft (4) – Fig. 2 – are:~ 1 = 526.87 sradrad~ 2 = 70.14 sec(19)(20)Fig. 4 Compar<strong>at</strong>ive value <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longerpart <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong> a 1 16/33 <strong>of</strong> a frequency during2f 2 50 100 Hz <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>COMMUNICATIONS 3/2008 ●7


Based on Fig. 4, we can conclude th<strong>at</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong><strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft quite quickly rises during <strong>the</strong>slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. This <strong>moment</strong> achieved <strong>the</strong> value <strong>of</strong>M t1 /M 0n 23 (M t1 6.42 MNm) in a quite short period <strong>of</strong> t 0.3 s. Consequently, <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> during <strong>the</strong> slippage <strong>of</strong><strong>the</strong> <strong>wheel</strong> <strong>set</strong> will permanently impair <strong>the</strong> longer part <strong>of</strong> <strong>the</strong>driving shaft.If we curtail <strong>the</strong> value <strong>of</strong> <strong>the</strong> factor amplitude <strong>of</strong> a frequency2f 2 50 100 Hz from a 1 16/33 to a 1 0.1, <strong>the</strong> dependenceM t1 /M 0n f(t) during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong> will beaccording to Fig. 5. (The factor amplitude a 1 may dwindle if weenlarge inductance <strong>of</strong> central silencer).Fig. 6 Compar<strong>at</strong>ive value <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longerpart <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong> a 1 3 <strong>of</strong> a frequency2f 2 25 50 Hz during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>eject <strong>the</strong> cascade switch and simplify <strong>the</strong> traction transformer. Thissubstitute may also enable <strong>the</strong> applic<strong>at</strong>ion <strong>of</strong> recuper<strong>at</strong>ive brake.Consequently, we believe th<strong>at</strong> <strong>the</strong> modern symmetrical thyristorrectifier may elimin<strong>at</strong>e <strong>the</strong> impairing <strong>of</strong> <strong>the</strong> longer part <strong>of</strong> <strong>the</strong>driving shaft during <strong>the</strong> slippage. With this rectifier <strong>the</strong> existingantislippage shield <strong>of</strong> <strong>the</strong> ZS 441, ZS 461 and ZS 444 electrolocomotiveswill be enough speedy though now it is not.5. ConclusionFig. 5 Compar<strong>at</strong>ive value <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longerpart <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong> a 1 0.1 <strong>of</strong> a frequency2f 2 50 100 Hz during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>Based on Fig 5, we can conclude th<strong>at</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>at</strong>a 1 16/33 is five times smaller than <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> a 1 0.1<strong>at</strong> during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> driving <strong>wheel</strong> <strong>set</strong>. The peak value <strong>of</strong><strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong>a 1 0.1 is <strong>at</strong>tained in t 0.25 s. Besides, our program for <strong>simul<strong>at</strong>ion</strong>showed th<strong>at</strong> <strong>the</strong> peak value <strong>of</strong> this <strong>moment</strong> fur<strong>the</strong>r dwindledwhile we were fur<strong>the</strong>r dwindling <strong>the</strong> factor amplitude <strong>of</strong>a circular frequency 2f 2 50 100 Hz.If we commute <strong>the</strong> diode or asymmetrical thyristor rectifierwith <strong>the</strong> symmetrical thyristor rectifier, we’ll receive a passablevalue <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> with <strong>the</strong> frequency 2f 2 25 50 Hz.The dependence M t1 /M 0n f(t) during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong><strong>set</strong> with <strong>the</strong> frequency 2f 2 25 50 Hz and a 1 3 is shownin Fig. 6.Based on Fig. 6, we can conclude th<strong>at</strong> <strong>the</strong> substitution <strong>of</strong> <strong>the</strong>diode rectifier or <strong>the</strong> asymmetrical with modern symmetrical thyristorrectifier rel<strong>at</strong>es to a passable value <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong>during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. Besides, this substitution willThe <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft risesquite quickly during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. This <strong>moment</strong>was achieving <strong>the</strong> value <strong>of</strong> M t1 /M 0n 23 (M t1 6.42 MNm) inquite a short period <strong>of</strong> t 0.3 s. Consequently, <strong>torsion</strong> <strong>moment</strong>during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong> will permanently impair <strong>the</strong>longer part <strong>of</strong> <strong>the</strong> driving shaft.The <strong>torsion</strong> <strong>moment</strong> <strong>of</strong> <strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong>a 1 16/33 is five times smaller than <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> <strong>at</strong> a 1 0.1during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. The peak value <strong>of</strong> <strong>the</strong> <strong>torsion</strong><strong>moment</strong> <strong>of</strong> <strong>the</strong> longer part <strong>of</strong> <strong>the</strong> driving shaft <strong>at</strong> a 1 0.1 is<strong>at</strong>tained in t 0.25 s. Besides, our program for <strong>simul<strong>at</strong>ion</strong> showedth<strong>at</strong> <strong>the</strong> peak value <strong>of</strong> this <strong>moment</strong> fur<strong>the</strong>r dwindled while we werefur<strong>the</strong>r dwindling <strong>the</strong> factor amplitude <strong>of</strong> a frequency 2f 2 50 100 Hz.The substitution <strong>of</strong> <strong>the</strong> diode rectifier or <strong>the</strong> asymmetricalwith modern symmetrical thyristor rectifier rel<strong>at</strong>es to a passablevalue <strong>of</strong> <strong>the</strong> <strong>torsion</strong> <strong>moment</strong> with <strong>the</strong> frequency 2 f 2 25 50 Hz during <strong>the</strong> slippage <strong>of</strong> <strong>the</strong> <strong>wheel</strong> <strong>set</strong>. Besides, this substitutionwill eject <strong>the</strong> cascade switch and simplify <strong>the</strong> traction transformer.This substitution may also enable <strong>the</strong> applic<strong>at</strong>ion <strong>of</strong>recuper<strong>at</strong>ive brake. Consequently, we believe th<strong>at</strong> <strong>the</strong> modernsymmetrical thyristor rectifier may elimin<strong>at</strong>e <strong>the</strong> impairing <strong>of</strong> <strong>the</strong>longer part <strong>of</strong> <strong>the</strong> driving shaft during <strong>the</strong> slippage.8● COMMUNICATIONS 3/2008


References[1] JOVANOVIC, R.: Tension st<strong>at</strong>us <strong>of</strong> locomotive shaft in exploit<strong>at</strong>ion situ<strong>at</strong>ion, PhD dissert<strong>at</strong>ion, Mechanical Engineering Faculty, Belgrade,1978.[2] JOVANOVIC, R: Causes, appearances and odds elimin<strong>at</strong>ing some splits and mishaps <strong>of</strong> <strong>the</strong> oper<strong>at</strong>ive shaft (axle) <strong>of</strong> <strong>the</strong> rail <strong>vehicle</strong>s“,Research project MIN, Institution „Edvard Kardelj“, Nis, 1987.[3] JANJANIN, S.: Identific<strong>at</strong>ion <strong>of</strong> some reasons for <strong>torsion</strong>al <strong>moment</strong> <strong>of</strong> <strong>the</strong> oper<strong>at</strong>ive system <strong>of</strong> 441 locomotive with <strong>the</strong> analogue computer,The Community <strong>of</strong> Yugoslav Railways, Study, Zagreb, 1974.[4] GAVRILOVIC, S. B.: Motivity <strong>moment</strong> <strong>of</strong> <strong>the</strong> traction electromotor <strong>of</strong> <strong>the</strong> thyristoring JZ 444 series locomotives, Proc. <strong>of</strong> 5 th Intern.Scientific Conference on Production Engineering, pp. 553–558, ISBN 99589262-0-2, Bihac, BIH, 2005.COMMUNICATIONS 3/2008 ●9


Fig.1 3D model <strong>of</strong> <strong>vehicle</strong> (MSC.ADAMS/Rail [10])finite element method <strong>the</strong>ory. Because <strong>of</strong> special model parameters<strong>set</strong>ting (in accordance with <strong>the</strong> ADAMS system), it behaves like<strong>the</strong> system <strong>of</strong> no-mass frames. We can proclaim th<strong>at</strong> from <strong>the</strong> point<strong>of</strong> view <strong>of</strong> commercial programme packages fe<strong>at</strong>ures, <strong>the</strong> DELTAprogramme with its working fe<strong>at</strong>ures is closer to <strong>the</strong> FEM (ANSYS– <strong>the</strong> Transient analysis part) system than to MBS (ADAMS)system. It is possible to take into account <strong>the</strong> flexibility <strong>of</strong> modelledbodies when <strong>the</strong> real stiffness and cross-sections parametersare known and <strong>set</strong> as input parameters for a comput<strong>at</strong>ion. Theprogramme was built in <strong>the</strong> environment <strong>of</strong> <strong>the</strong> programme languageDELPHI for an oper<strong>at</strong>ion in <strong>the</strong> environment <strong>of</strong> <strong>the</strong> MSWindows XP oper<strong>at</strong>ional system. It was designed on <strong>the</strong> base <strong>of</strong> anopened component system. The programme DELTA allows performingst<strong>at</strong>ic and dynamic mechanical systems analyses. An input<strong>of</strong> d<strong>at</strong>a <strong>of</strong> a <strong>vehicle</strong> mechanical system is carried out with <strong>the</strong> help<strong>of</strong> node points and elements: a linear spring, nonlinear spring,a beam, a linear damper, nonlinear damper and mass point.Boundary and starting conditions:– prescribed displacements, velocities and acceler<strong>at</strong>ions <strong>of</strong> nodes;– prescribed revolutions, angular velocities and angular acceler<strong>at</strong>ions<strong>of</strong> nodes;– prescribed forces and torques acting in nodal points;– prescribed acceler<strong>at</strong>ions acting on a <strong>vehicle</strong>.Methods for dynamics solution:– <strong>the</strong> eigenfrequencies and eigenvectors assessment with <strong>the</strong> help<strong>of</strong> Jacobi’s rot<strong>at</strong>ion method;– a response analysis evoked by harmonic excit<strong>at</strong>ion;– a direct solution <strong>of</strong> a model oscill<strong>at</strong>ion in <strong>the</strong> time domain with<strong>the</strong> following methods: <strong>the</strong> differential method, <strong>the</strong> HHT- method,<strong>the</strong> method <strong>of</strong> linear acceler<strong>at</strong>ions, <strong>the</strong> Newmark method, <strong>the</strong>Wilson- method and <strong>the</strong> Crank-Nicolson method.Equ<strong>at</strong>ions solution methods (solver) are Frontal elimin<strong>at</strong>ionand L-U decomposition.The otput is graphical and textual. The eigenfrequencies andeigenvectors assessment was performed with <strong>the</strong> Jacobi’s rot<strong>at</strong>ionmethod. A response analysis from harmonic excit<strong>at</strong>ion and a directsolution <strong>of</strong> model oscill<strong>at</strong>ion were performed in <strong>the</strong> time domain.Fig.2 The DELTA programme main screenwhen <strong>the</strong> menu are openedThe Newmark modified method was used for <strong>the</strong> direct solutionin <strong>the</strong> time domain. This method is known as <strong>the</strong> ”HHTmethod“.The method was modified for <strong>the</strong> solution <strong>of</strong> dynamicsystems with nonlinear members. The usage <strong>of</strong> this method hasbeen recently very relevant in <strong>the</strong> field <strong>of</strong> technical comput<strong>at</strong>ionsperformance. The main advantage is in <strong>the</strong> decrease <strong>of</strong> time whichis necessary for computing. The linear algebraic equ<strong>at</strong>ions systemwas computed with <strong>the</strong> help <strong>of</strong> <strong>the</strong> Frontal elimin<strong>at</strong>ion method.This method is suitable for big systems <strong>of</strong> linear equ<strong>at</strong>ion solution,known in connection with numerical analyses based on <strong>the</strong> Finiteelement method <strong>the</strong>ory. The comput<strong>at</strong>ional model was built up from80 nodal points and 132 elements. The model has 456 degrees <strong>of</strong>freedom, <strong>the</strong> comput<strong>at</strong>ional front width is 66. All <strong>the</strong> amount <strong>of</strong>track sections is 257, which represents <strong>the</strong> 1285 seconds <strong>of</strong> <strong>vehicle</strong>running.COMMUNICATIONS 3/2008 ●11


Fig. 3 Geometrical parameters <strong>of</strong> chosen dynamic model <strong>of</strong> <strong>vehicle</strong> in accordance with [10]Fig.4 The whole <strong>vehicle</strong> model (DELTA)The dominant oscill<strong>at</strong>ion shapes specific<strong>at</strong>ion Tab. 1Fig.5 The rear bogie with depicted consctruction elements,2. bogie (DELTA)The list <strong>of</strong> some important eigenfrequencies is processed in<strong>the</strong> following table. The eigenvectors due to <strong>the</strong>se frequencies represent<strong>at</strong>ionis in <strong>the</strong> following figures as well.O<strong>the</strong>r eigenfrequencies and to <strong>the</strong>m pertaining eigenvectorsare not important from <strong>the</strong> point <strong>of</strong> this analysis. The reason isth<strong>at</strong> <strong>the</strong>y represent deform<strong>at</strong>ions <strong>of</strong> ”rigid“ structures <strong>of</strong> <strong>the</strong> model(bogies frames or a <strong>vehicle</strong> body). The frequencies are out <strong>of</strong>analysis limits in <strong>the</strong> time domain where s, which corresponds to<strong>the</strong> 200 Hz frequency.ConsecutivenumberEigen anglevelocityOmega[1/rad]Eigenfrequencyf [Hz]5. Verific<strong>at</strong>ion <strong>of</strong> nonlinear modelDominant form<strong>of</strong> eigenvector1. 3.8846 0.618 Lower swaying2. 4.1525 0.661 Longitudinal oscill<strong>at</strong>ion3. 5.602 0.892 Yawing4. 5.8127 0.925 Upper swaying5. 6.2382 0.993 Bouncing6. 7.345 1.169 Pitching7. 28.5857 4.55 Swaying <strong>of</strong> individual bogiesin opposed directions8. 28.7195 4.571 Swaying <strong>of</strong> individual bogiesin a concurrent way9. 29.3639 4.673 Pitching <strong>of</strong> individual bogiesin opposed directions10. 29.4082 4.68 Pitching <strong>of</strong> individual bogiesin a concurrent wayThe <strong>vehicle</strong> in a real oper<strong>at</strong>ion has its special parameters. Ingeneral it is characterised by its own properties. For a reliable <strong>vehicle</strong>12 ● COMMUNICATIONS 3/2008


Fig. 6 1. eigenvector when <strong>the</strong> eigenfrequency is 0.618HzFig. 9 4. eigenvector when <strong>the</strong> eigenfrequency is 0.925HzFig. 7 2. eigenvector when <strong>the</strong> eigenfrequency is 0.661HzFig. 8 3. eigenvector when <strong>the</strong> eigenfrequency is 0.892HzFig. 10 5. eigenvector when <strong>the</strong> eigenfrequency is 0.993HzFig. 11 6. eigenvector when <strong>the</strong> eigenfrequency is 1.169HzFig. 12 9. eigenvector when <strong>the</strong> eigenfrequency is 4.673Hz – pitching<strong>of</strong> individual bogies in opposed directionsCOMMUNICATIONS 3/2008 ●13


Fig. 13 10. eigenvector when <strong>the</strong> eigenfrequency is 4.68Hz – pitching<strong>of</strong> individual bogies in a concurrent wayFig. 14 12. eigenvector when <strong>the</strong> eigenfrequency is i 5.465Hz – bouncing<strong>of</strong> individual bogies in opposed directionsproperties assessment and behaviour judgement we are to verify<strong>the</strong> trustworthiness <strong>of</strong> its comput<strong>at</strong>ional model.1. The comput<strong>at</strong>ion with linear members in <strong>the</strong> time and frequencydomains – provides a rough outline.2. Non-liner members do not have fe<strong>at</strong>ures <strong>of</strong> members (in anypoint <strong>of</strong> <strong>the</strong> characteristics) when a deform<strong>at</strong>ion is increasingor a deform<strong>at</strong>ion velocity is increasing. It may happen th<strong>at</strong> <strong>the</strong>internal force is decreasing or is maintained on an initial internalforce value level.3. Energetic balance:In our case we will perform <strong>the</strong> model verific<strong>at</strong>ion with <strong>the</strong> help<strong>of</strong> a comparison <strong>of</strong> <strong>the</strong>oretic characteristics <strong>of</strong> flexible bindingsmembers with <strong>the</strong> corresponding values <strong>of</strong> forces obtained fromcomput<strong>at</strong>ions.We put <strong>the</strong> spring <strong>of</strong> high stiffness in a serial way into <strong>the</strong>model. The spring in <strong>the</strong> place <strong>of</strong> a nonlinear member evalu<strong>at</strong>es<strong>the</strong> current value <strong>of</strong> an internal force due to velocity, or change <strong>of</strong>position <strong>of</strong> <strong>the</strong> nonlinear member boundary points. In an idealcase <strong>the</strong> depicted result is <strong>the</strong> same as <strong>the</strong> <strong>the</strong>oretically requestedcharacteristic curve.ΠqKFRTDP = P_ q+ dqi - P_ qi = dq $ ^F- Rh+1 T2+ dq $ Kt$ dq= dP+d P21 T2DP 0 d P = dq $ Kt$ dq2– is <strong>the</strong> energy– is <strong>the</strong> vector <strong>of</strong> generalised movements– is <strong>the</strong> tangential stiffness m<strong>at</strong>rix– is <strong>the</strong> vector <strong>of</strong> internal forces– is <strong>the</strong> vector <strong>of</strong> external loads(1)We analysed <strong>the</strong> dynamic properties <strong>of</strong> a “common model”<strong>vehicle</strong> with overtaken parameters [10]. We were looking for <strong>the</strong>acceler<strong>at</strong>ion evalu<strong>at</strong>ion on <strong>the</strong> <strong>vehicle</strong> with <strong>the</strong> purpose <strong>of</strong> definedkinem<strong>at</strong>ic excit<strong>at</strong>ion and when <strong>the</strong> acceler<strong>at</strong>ion acts due to <strong>the</strong>track geometry. No classic rail/<strong>wheel</strong> contact model was used for<strong>the</strong> analysis in spite <strong>of</strong> <strong>the</strong> fact th<strong>at</strong> <strong>the</strong> authors are interested invarious types <strong>of</strong> contact model evalu<strong>at</strong>ion.6. Modelling <strong>of</strong> excit<strong>at</strong>ion6.1. Acquired track parameters from measurementFor all <strong>the</strong> vectors is validdq is DP 2 04. The parameters <strong>of</strong> stability choice <strong>of</strong> <strong>the</strong> HHT methodan amplitude decreasing r<strong>at</strong>io c " ^0 ' 1/3 h=015 . (3)1 11 2a = ^ + ch; d = + c ; a = c;a # a (4)42f m f5. A <strong>vehicle</strong> model – an examin<strong>at</strong>ion whe<strong>the</strong>r a comput<strong>at</strong>ionalmodel with its parameters and excit<strong>at</strong>ion parameters correspondsto <strong>the</strong> reality and whe<strong>the</strong>r <strong>the</strong> results <strong>of</strong> comput<strong>at</strong>ionsare valid.(2)The input parameters for <strong>the</strong> excit<strong>at</strong>ion <strong>of</strong> a <strong>vehicle</strong> mechanicalsystem are: given (measured) geometric layout devi<strong>at</strong>ions Y L ,Y P , Z L , Z P , <strong>vehicle</strong> velocity V, cant U, track curv<strong>at</strong>ure K, track s,time t, w(x) is a track gauge th<strong>at</strong> is evalu<strong>at</strong>ed according to <strong>the</strong> followingrel<strong>at</strong>ion:w = 1435 + Y ^L xh-Y ^P xh• A <strong>vehicle</strong> is influenced by <strong>the</strong>se acceler<strong>at</strong>ions:dvax = ,dt(6)ay = aD$ cos a , (7)(5)14 ● COMMUNICATIONS 3/2008


aZ = aD$ sin a , (8) ness <strong>of</strong> rails and <strong>the</strong> difference in <strong>moment</strong>aneous rolling circlesdiameters.where• Right <strong>wheel</strong>sa v K, arctg U 2 V2 $ r $ xD =- $ a = , v =(9) uzP = Z ^ xh P + DRP _ yi, y = u0 $ sindn1500 36 .L(11)where6.2. Kinem<strong>at</strong>ic excit<strong>at</strong>ion <strong>of</strong> <strong>vehicle</strong> in <strong>the</strong> y-axisdirectionu oLx– is <strong>the</strong> amplitude <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,– is <strong>the</strong> wavelength <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,– is <strong>the</strong> line performed by <strong>the</strong> <strong>wheel</strong><strong>set</strong>The kinem<strong>at</strong>ic excit<strong>at</strong>ion <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> in <strong>the</strong> y-axis directionwas performed due to <strong>the</strong> difference <strong>of</strong> <strong>moment</strong>aneous rolling DRP_ y, wi=DR_y,wiif y 0radii circles function and wave movement <strong>of</strong> <strong>wheel</strong><strong>set</strong> with <strong>the</strong>amplitude <strong>of</strong> 3 mm and wavelength L 8.647 m. The wavelengthresults from <strong>the</strong> equivalent conicity function for <strong>the</strong> given contactcouple pr<strong>of</strong>iles and <strong>the</strong> amplitude <strong>of</strong> 3 mm.The kinem<strong>at</strong>ic excit<strong>at</strong>ion <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> system in <strong>the</strong> z-axisdirection is caused by a <strong>vehicle</strong> running across <strong>the</strong> measured uneven-2 $ r $ x Y ^xhL + Y ^xhPuy= u0 $ sindn +L2, (10)where:u o – is <strong>the</strong> aplitude <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,L – is <strong>the</strong> wavelength <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,x – is <strong>the</strong> line performed by <strong>the</strong> <strong>wheel</strong><strong>set</strong>6.3. Kinem<strong>at</strong>ic excit<strong>at</strong>ion in <strong>the</strong> z-axis directionFig.17 The function for common couple <strong>of</strong> <strong>the</strong>oretical pr<strong>of</strong>iles(a <strong>wheel</strong> S1002 and a rail UIC60 with <strong>the</strong> inclin<strong>at</strong>ion <strong>of</strong> 1:40, forvarious gauge values)Fig.15 Contact points <strong>of</strong> S1002/UIC60 pr<strong>of</strong>iles couple, for <strong>the</strong> gauge <strong>of</strong> 1435 mmFig.16 The wavelenght <strong>of</strong> periodical movement <strong>of</strong> a <strong>wheel</strong><strong>set</strong> with <strong>the</strong> amplitude <strong>of</strong> 3 mmCOMMUNICATIONS 3/2008 ●15


and D R _ y,wi=0 if y 0 (12) Dampers characteristics [10] Tab. 2Pwhere <strong>the</strong> ΔR(y, w) is <strong>the</strong> function <strong>of</strong> differency <strong>of</strong> <strong>moment</strong>aneous<strong>wheel</strong><strong>set</strong> <strong>wheel</strong>s rolling circles, computed from <strong>the</strong> geometricalcontact <strong>of</strong> <strong>wheel</strong> and rail pr<strong>of</strong>iles, w(x) is a track gauge th<strong>at</strong> is evalu<strong>at</strong>edaccording to <strong>the</strong> rel<strong>at</strong>ion (5).• Left <strong>wheel</strong>s2 $ r $ xusL = Z ^ xh L + DRL _ yi, y = u0 $ sindnLwhereu o – is <strong>the</strong> amplitude <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,L – is <strong>the</strong> wavelength <strong>of</strong> periodical <strong>wheel</strong><strong>set</strong> movement,x – is <strong>the</strong> line performed by <strong>the</strong> <strong>wheel</strong><strong>set</strong>DR _ y, wi=DR_y,wiLif y 0(13)and D R _ y,wi=0 if y 0 (14)where <strong>the</strong> ΔR(y, w) is <strong>the</strong> function <strong>of</strong> difference <strong>of</strong> <strong>moment</strong>aneous<strong>wheel</strong><strong>set</strong> <strong>wheel</strong>s rolling circles computed from <strong>the</strong> geometricalcontact <strong>of</strong> <strong>wheel</strong> and rail pr<strong>of</strong>iles, w(x) is a track gauge th<strong>at</strong> is evalu<strong>at</strong>edaccording to <strong>the</strong> rel<strong>at</strong>ion (5).7. Model verific<strong>at</strong>ionLThe model was verified with <strong>the</strong> help <strong>of</strong> <strong>the</strong> computed andgiven characteristic curves comparison. The depencence curvesbetween <strong>the</strong> forces and strain <strong>of</strong> springs, or between <strong>the</strong> forces andvelocities in <strong>the</strong> dampers were ”measured“ in <strong>the</strong> nonlinear members<strong>of</strong> <strong>the</strong> flexible bindings. The parameters <strong>of</strong> <strong>the</strong> given characteristiccurves were obtained from <strong>the</strong> liter<strong>at</strong>ure [10]:• a damper <strong>of</strong> primary suspension (MSC.ADAMS) PVD,• a damper <strong>of</strong> <strong>wheel</strong><strong>set</strong> turning (MSC.ADAMS) SYD,• a damper <strong>of</strong> secondary suspension (MSC.ADAMS) SVD,• a transversal damper (MSC.ADAMS) SLD,• a flexible bump stop (MSC.ADAMS) BS.PVD SVD SYD SLDV F V F V F V F[ms 1 ] [N] [ms 1 ] [N] [ms 1 ] [N] [ms 1 ] [N]1 -1.0 -1000 -1.0 -7100 -1.0 -3.97E4 -1.0 -85002 -0.28 -400 -0.26 -3000 -0.14 -1.1E4 -0.305 -40003 -0.16 -300 -8.0E-2 -2000 -0.11 -1.0E4 -0.15 -30004 -9.0E-2 -200 -4.0E-2 -1775 -5.5E-2 -8000 -7.0E-2 -20005 -4.0E-2 -100 -1.5E-2 -1000 -4.0E-2 -7000 -3.0E-2 -10006 0.0 0 0.0 0 0.0 0.0 0.0 0.07 4.0E-2 100 1.5E-2 1000 4.0E-2 7000 3.0E-2 10008 9.0E-2 200 4.0E-2 2000 5.5E-2 8000 7.0E-2 20009 0.16 300 8.0E-2 2000 0.11 1.E4 0.15 300010 0.28 400 0.26 3000 0.14 1.1E4 0.305 400011 1.0 1000 1.0 7100 1.0 3.97E4 1.0 8500A bump stop characteristic [10] Tab. 3FBSThe assessment principle: <strong>the</strong> forces in nonlinear memberswere computed as <strong>the</strong> internal forces in <strong>the</strong> serial connected linearsprings with high stiffness.FDeform<strong>at</strong>ionDeform<strong>at</strong>ionDeform<strong>at</strong>ion[m] [N] [m] [N] [m] [N]1 0 0 4 1.5E2 3730 7 3.0E2 1.717E42 5.0E-3 600 5 2.0E2 6870 8 3.5E2 2.92E43 1.0E-2 1760 6 2.5E2 1.158E4 9 4.0E2 2.3E5FThe prescribed flexible member characteristics are representedby <strong>the</strong> curves in <strong>the</strong> graphs. The linear dependence represents <strong>the</strong>basic stiffness, or better <strong>the</strong> basic stiffness constant.8. Comfort indexes for a model with nonlinear membersFig.18 The bogie scheme with flexible bindingsThe comput<strong>at</strong>ional model with nonlinear members topologyshown in <strong>the</strong> Fig. 21 consists <strong>of</strong> 80 nodal points and 132 elements.The nodes 67, 77, 73, 80 and 70 cre<strong>at</strong>e <strong>the</strong> left side <strong>of</strong> <strong>the</strong> <strong>vehicle</strong>frame, <strong>the</strong> nodes 65, 22, 71, 78 and 88 cre<strong>at</strong>e <strong>the</strong> right side <strong>of</strong><strong>vehicle</strong> frame. The <strong>vehicle</strong> model moves in <strong>the</strong> direction from <strong>the</strong>left to <strong>the</strong> right side. The Tab. 4 represents <strong>the</strong> list <strong>of</strong> computedcomfort indexes. These indexes were evalu<strong>at</strong>ed under <strong>the</strong> abovementioned conditions. In Fig. 23 and Fig. 24 <strong>the</strong>re are graphicalinterpret<strong>at</strong>ions <strong>of</strong> indexes valid for <strong>the</strong> depicted nodes.16 ● COMMUNICATIONS 3/2008


Fig. 19 Forces evalu<strong>at</strong>ion in <strong>the</strong> damper <strong>of</strong> primary suspension(DELTA)Fig. 20 Forces evalu<strong>at</strong>ion in <strong>the</strong> longitudinal damper (DELTA)Fig. 21 The node points numbering in <strong>the</strong> places <strong>of</strong> indexes evalu<strong>at</strong>ionPassanger comfort indexes for <strong>the</strong> model Tab. 4with nonlinear membersNodeIndexfloorIndexstandingpositionNodeIndexfloorIndexstandingposition1 65 2.319 2.205 9 73 1.555 1.6922 66 2.069 2.18 10 78 1.895 2.0383 67 2.279 2.207 11 79 1.734 2.0124 22 1.707 1.763 12 80 1.872 2.045 54 1.522 1.709 13 68 2.674 2.746 77 1.692 1.737 14 69 2.49 2.7167 71 1.531 1.691 15 70 2.662 2.7428 72 1.367 1.6629. ConclusionA <strong>vehicle</strong>s dynamics properties analysis is a very wide field.We can process this issue form various points <strong>of</strong> view. We put our<strong>at</strong>tention in <strong>the</strong> acceler<strong>at</strong>ions calcul<strong>at</strong>ion. These acceler<strong>at</strong>ions inputinto <strong>the</strong> rel<strong>at</strong>ions for passenger ride comfort assessment. The acceler<strong>at</strong>ionsare commonly measured in <strong>the</strong> given places <strong>of</strong> a <strong>vehicle</strong>body when <strong>the</strong> <strong>vehicle</strong> is running. They are filtered, weighted inaccordance with <strong>the</strong> European standards ENV 12999:1999 orprENV 12999:2006 before processing for <strong>the</strong> comfort indexesevalu<strong>at</strong>ion [1, 12]. The acceler<strong>at</strong>ions in question can be obtainedwith <strong>the</strong> help <strong>of</strong> a <strong>simul<strong>at</strong>ion</strong> comput<strong>at</strong>ion [5] as well. The method<strong>of</strong> m<strong>at</strong>hem<strong>at</strong>ical model comput<strong>at</strong>ion, <strong>vehicle</strong> parameters andboundary conditions are <strong>of</strong> gre<strong>at</strong> importance for results (acceler<strong>at</strong>ions)trustworthiness. In <strong>the</strong> paper we described one proposalor idea <strong>of</strong> possible verific<strong>at</strong>ion <strong>of</strong> a comput<strong>at</strong>ional nonlinear modelbased on a strictly given mechanical system excit<strong>at</strong>ion which comesout from real track d<strong>at</strong>a. The final acceler<strong>at</strong>ions as <strong>the</strong> <strong>vehicle</strong>model response from excit<strong>at</strong>ion were used as input parameters for<strong>the</strong> common comfort index evalu<strong>at</strong>ion due to <strong>the</strong> above mentionedEuropean standard.COMMUNICATIONS 3/2008 ●17


Fig. 22 Comfort for passengers for a floor evalu<strong>at</strong>ion,when <strong>the</strong> <strong>vehicle</strong> model has nonlinear membersFig. 23 Comfort for passengers for a standing position evalu<strong>at</strong>ion,when <strong>the</strong> <strong>vehicle</strong> model has nonlinear membersAcknowledgementThe work was supported by <strong>the</strong> Scientific Grant Agency <strong>of</strong><strong>the</strong> Ministry <strong>of</strong> Educ<strong>at</strong>ion <strong>of</strong> <strong>the</strong> Slovak Republic and <strong>the</strong> SlovakAcademy <strong>of</strong> Sciences in <strong>the</strong> project No. 1/3169/06 “PropertiesResearch <strong>of</strong> Rail Vehicles in Movement with Emphasis on <strong>the</strong>Solution <strong>of</strong> a Wheel and Rail Contact <strong>at</strong> <strong>the</strong> Wheel<strong>set</strong> Rolling in <strong>the</strong>Rail via Computer Simul<strong>at</strong>ion“ and in <strong>the</strong> project No. 1/4119/07:”Investig<strong>at</strong>ion <strong>of</strong> a dynamical properties <strong>of</strong> a <strong>vehicle</strong>“.References[1] ENV 12299: 1999E Railway Applic<strong>at</strong>ions – Ride Comfort for Passengers – Measurement and Evalu<strong>at</strong>ion, European Prestandard, February1999.[2] GERLICI, J., LACK, T.: Methods for Vehicle Vibr<strong>at</strong>ion Analysis in Time Domain, Prace naukowe Politechniki Warszawskiej, Z. 63,Transport, 2007, pp. 71–81. Publishing House <strong>of</strong> <strong>the</strong> Warsaw University <strong>of</strong> Technology, ISSN 1230-9265, Warszawa 2007.[3] GERLICI, J., LACK, T.: Survey <strong>of</strong> Ride Comfort for Passengers (in Slovak), Acta Mechanica Slovaca, Kosice 4-B/2006, pp.155–162, Optimiz<strong>at</strong>ion <strong>of</strong> Mechanical Systems, vol. 10, ISSN 1335-2393, Kosice, 2006.[4] GERLICI, J., LACK, T., ONDROVA, Z.: Evalu<strong>at</strong>ion <strong>of</strong> Comfort for Passengers <strong>of</strong> Railway Vehicles. Communic<strong>at</strong>ions – ScientificLetters <strong>of</strong> <strong>the</strong> University <strong>of</strong> Zilina, 4/2007, pp. 44–49, ISSN 1335-4205, EDIS – Publishing house <strong>of</strong> University <strong>of</strong> Zilina, 2007.[5] LACK, T.: The Dynamic Properties Analysis <strong>of</strong> Vehicles from <strong>the</strong> Point <strong>of</strong> View <strong>of</strong> Ride Comfort (in Slovak), Habilit<strong>at</strong>ion Work, pp.176, Faculty <strong>of</strong> Mechanical Engineering University <strong>of</strong> Zilina, 2007.[6] LACK, T., GERLICI, J.: Vehicles Dynamical Properties Analysis from <strong>the</strong> Point <strong>of</strong> View <strong>of</strong> Comfort for Passengers, Archives <strong>of</strong> Transport,1-2/2007, pp. 91–110, ISSN 8066-9546, Warszawa 2007.[7] LACK, T., GERLICI, J.: The Programme System DELTA Exploit<strong>at</strong>ion for Numerical Analysis Performances (in Slovak), Proc. <strong>of</strong> 18thIntern<strong>at</strong>ional Conference “Current Problems in Rail Vehicles – PRORAIL 2007” – Part II., pp. 11 22, EDIS, ISBN 978-80-89276-07-3, Zilina, 2007.[8] LACK, T., GERLICI, J., HLAVNA, V.: Evalu<strong>at</strong>ion <strong>of</strong> Ride Comfort for Passengers, pp. 9–13, Horizonty dopravy, ISSN 1210-0978,5/2006, Special Edition, Transport Research Institute, Zilina 2006.[9] LACK, T., GERLICI, J., HLAVNA, V.: The Vehicle Comfort, Case study, Maintenance and Reliability 2006, ISSN 1507-2711,4(32)/2006, pp. 89–91, Polskie Naukowo-Techniczne Towarysztwo Eksplo<strong>at</strong>acyjne Warszawa, 2006.[10] MSC.ADAMS/Rail: A Model <strong>of</strong> ERRI Coach Wagon for Programme System Verific<strong>at</strong>ion.[11] POLACH, O.: Rail Vehicles Analysis, Transport Means – Comput<strong>at</strong>ional Methods, Textbook, University <strong>of</strong> Zilina, ISBN 80-8070-476-7, EDIS–Publishing house <strong>of</strong> University <strong>of</strong> Zilina, 2005.[12] prENV 12299: 2006 Bahanwendungen – Fahrkomfort für Fahrgäste – Messung und Auswertung, 2006.18 ● COMMUNICATIONS 3/2008


Jaromir Siroky *SYSTEMATIC TIME TABLES – MODELLING OF TRAINS’ PATHSBY USING GENETIC ALGORITHMSOne <strong>of</strong> construction possibilities <strong>of</strong> a time table is <strong>the</strong> implement<strong>at</strong>ion <strong>of</strong> system<strong>at</strong>ic timetabling. In system<strong>at</strong>ic timetabling, <strong>the</strong> trains’ p<strong>at</strong>hsare ordered regularly (thus system<strong>at</strong>ically). In cargo transport <strong>the</strong>re exist a range <strong>of</strong> possibilities <strong>of</strong> using an “integr<strong>at</strong>ed tact timetable”, whichensures time and space sequences among individual services, forwarders or o<strong>the</strong>r kinds <strong>of</strong> transport. A net-system <strong>of</strong> service is used in intermodaltransport trains, which ensures a net-wide service <strong>of</strong> each intermodal terminal in <strong>the</strong> network. The Hub and Spoke system (H&S) isused <strong>the</strong> most. The intermodal train model <strong>of</strong> route loc<strong>at</strong>ion in a chosen network is presented in this article. The methods <strong>of</strong> genetic algorithmwere used for finding <strong>the</strong> result. The modelling <strong>of</strong> trains’ p<strong>at</strong>hs lies in <strong>the</strong> minimiz<strong>at</strong>ion <strong>of</strong> intermodal unit transhipment times in intermodaltransport ranges.1. IntroductionA prerequisite for effective functioning <strong>of</strong> <strong>the</strong> intermodal systemin Europe is a system <strong>of</strong> shuttle or multiple-section trains regularlyoper<strong>at</strong>ing among intermodal terminals or ports oriented on technologiessuch as Night Jump (Nachtdprung in German) or Just inTime (with guaranteed term <strong>of</strong> delivery), as described by Lindner[19] and Panda [22].An important part <strong>of</strong> an intermodal train’s travelling time is<strong>the</strong> reloading time in node terminals. Th<strong>at</strong> is why routes <strong>of</strong> tho<strong>set</strong>rains must be coordin<strong>at</strong>ed on a track and in a terminal. Th<strong>at</strong> isalso a dominant <strong>the</strong>me <strong>of</strong> this paper. Emphasis on a system<strong>at</strong>icapproach is <strong>the</strong> key to <strong>the</strong> solution. This solution will use findingswhich are described in Caprara [3], Nielsen [20], Sevele [23] orSchmitt [24]. Results <strong>of</strong> our paper will contribute to better timeand space sequence <strong>of</strong> intermodal trains in node terminals. Ourapproach will increase <strong>the</strong> quality <strong>of</strong> railroad cargo transport.2. System<strong>at</strong>ic time tablesSystem<strong>at</strong>ic timetabling is one <strong>of</strong> <strong>the</strong> possibilities for a timetableconstruction. Its principle is in a periodically repe<strong>at</strong>ed structure <strong>of</strong>passenger and goods trains so th<strong>at</strong> during <strong>the</strong> day <strong>the</strong> same groups<strong>of</strong> trains are repe<strong>at</strong>ed. According to distance among those groupswe have a lag timetable or pulse timetable.In railroad transport we have a household word – lag timetable.Its characteristic is a constant time period among trains. Therefore,we can find one-hour, two-hour, three-hour or eventuallyfour-hour pulses, as described by Bar [1] and Ferchland [7].On a higher quality level <strong>the</strong>re exists an integr<strong>at</strong>ed lag timetable(fur<strong>the</strong>r only ILT). It system<strong>at</strong>ically coordin<strong>at</strong>es lag timetablesamong more train p<strong>at</strong>hs or o<strong>the</strong>r means <strong>of</strong> transport. More basicinform<strong>at</strong>ion about ILT can be found in Diermeier [6].Bar [1] and Hesse [12] suggest <strong>the</strong> most important requirementsfor ILT:● Offer <strong>of</strong> lag transport during every day <strong>of</strong> <strong>the</strong> week,● Offering each train p<strong>at</strong>h in a basic pulse (passenger trains oneor two hours, intermodal trains – 4, 6, 12 or 24 hours),● Ensuring train services for passengers from 5am to 10pm, combinedwith intermodal transport in continuous oper<strong>at</strong>ion,● Ensure good connection in node st<strong>at</strong>ions among system<strong>at</strong>ic trainsand o<strong>the</strong>r types <strong>of</strong> trains,● Increase standard <strong>of</strong> quality for passengers and customers incargo transport,● Ensure maximum accuracy <strong>of</strong> trains (following <strong>the</strong> time table).Ano<strong>the</strong>r important aspect <strong>of</strong> lag timetabling is axis <strong>of</strong> symmetry.It is an instant <strong>of</strong> time when trains on <strong>the</strong> same train routeare crossing (on <strong>the</strong> single track line) or meeting (on double trackline). Hesse [12] found th<strong>at</strong> an important requirement for ILT is<strong>the</strong> same symmetry time for all train routes. If we observe th<strong>at</strong>principle it leads to a mirrored timetable. So th<strong>at</strong> for each train indirection A–B we have a train in direction B–A with <strong>the</strong> same lagtime, similar reloading time and block speed. In standard practice<strong>the</strong> so-called zero symmetry is <strong>of</strong>ten used. It means th<strong>at</strong> one symmetrytime is right <strong>at</strong> <strong>the</strong> beginning <strong>of</strong> an hour. For example, ifone train arrives to <strong>the</strong> st<strong>at</strong>ion in <strong>the</strong> 54 th minute (60 6), <strong>the</strong>n<strong>the</strong> train on <strong>the</strong> same route in <strong>the</strong> opposite direction will arrive in6 th minute (60 6).* Jaromir SirokyDepartment <strong>of</strong> Transport Technology and Control, Jan Perner Transport Faculty, University <strong>of</strong> Pardubice, Czech Republic,E-mail: jaromir.siroky@upce.czCOMMUNICATIONS 3/2008 ●19


3. Intermodal trainsIntermodal trains are taken as a system <strong>of</strong> fast train connections<strong>of</strong> intermodal transport (hereinafter as IMT) which ensuresconnection among individual IMT terminals in desired quality andsufficient volume <strong>of</strong> transported goods. Systems <strong>of</strong> through trainsand mixed trains are used for <strong>the</strong> train connection among IMT terminals.From <strong>the</strong> <strong>railway</strong> carrier’s point <strong>of</strong> view <strong>the</strong> whole cargo(transport unit) is transported ei<strong>the</strong>r as an individual <strong>set</strong> <strong>of</strong> coachesor as a group <strong>of</strong> <strong>set</strong>s <strong>of</strong> coaches or as <strong>the</strong> shuttle train. The biggestshare <strong>of</strong> IMT cargos is transported in <strong>the</strong> shuttle trains which allbelong to <strong>the</strong> “Nex” train c<strong>at</strong>egory.Heinrici [11] found th<strong>at</strong> <strong>the</strong> systems <strong>of</strong> train connections <strong>of</strong>IMT transport units can be oper<strong>at</strong>ed on an individual line or ona specified line network. In <strong>the</strong> former case we speak <strong>of</strong> so-called“line system” and in <strong>the</strong> l<strong>at</strong>ter case we speak <strong>of</strong> <strong>the</strong> so-called“network system”.The network system <strong>of</strong> train connections is characterized asa network service <strong>of</strong> individual terminals on a specified trafficnetwork. This means th<strong>at</strong> <strong>the</strong>re is a gap in <strong>the</strong> service <strong>of</strong> individualIMT terminals using line systems which are included in <strong>the</strong> trafficnetwork. A system <strong>of</strong> shuttle trains connecting <strong>the</strong> individual IMTterminals is usually used in <strong>the</strong> network system. This networksystem is in <strong>the</strong> IMT area represented by <strong>the</strong> “Hub-and-Spoke”system, as described by Novak [21].this technology is used mainly abroad. For example, in Germany(IMT oper<strong>at</strong>or Kombiverkehr) this system is represented as <strong>the</strong>“goods IC-concept”. It is a very similar system to <strong>the</strong> one used bypassenger trains IC, ICE and EC c<strong>at</strong>egories, as described byHeinrici [11].A practical applic<strong>at</strong>ion <strong>of</strong> this technology has been found notonly abroad but also in <strong>the</strong> Czech Republic. Especially in transport<strong>at</strong>ionamong seaports (Rotterdam, Bremerhaven, Hamburg)and some inland terminals (Praha-Uhrineves, Melník, Lovosice)th<strong>at</strong> have <strong>the</strong> position <strong>of</strong> node terminals. In <strong>the</strong>se lines <strong>the</strong> freighttraffic volumes are high and <strong>the</strong> trains are usually <strong>set</strong> out twice perday (24 hours). In o<strong>the</strong>r sequential directions (o<strong>the</strong>r terminals in<strong>the</strong> CR or adjacent countries) <strong>the</strong> freight traffic volumes are muchlower and <strong>the</strong> train <strong>set</strong>-out frequency is much lower (2 to 5 trainsper week).4. Train routes model for intermodal trainsThe task <strong>of</strong> any transport problem solved by a m<strong>at</strong>hem<strong>at</strong>icmodel is finding its <strong>at</strong>tributes, analysing all its st<strong>at</strong>es and verifyingits scheduled parameters. This is subjected to right definition anddimensioning <strong>of</strong> system items, efficient regul<strong>at</strong>ion and organiz<strong>at</strong>ion<strong>of</strong> <strong>the</strong> system.4.1 General solutionIn <strong>the</strong> node terminal two groups <strong>of</strong> shipments are assembledfor one train. Cerna [4] and Janacek [13] suggest th<strong>at</strong> in <strong>the</strong> firstgroup are shipments which enter <strong>the</strong> system in th<strong>at</strong> node. Thesecond group are shipments which came into th<strong>at</strong> node by train.If <strong>the</strong>re is a node u in time t ij (arrival time <strong>of</strong> train j on line i) , <strong>the</strong>shipment will be brought by train sij on train p<strong>at</strong>h L i , will bereloaded for time l (time <strong>of</strong> reload from line i to lane r) to positionon train p<strong>at</strong>h L r and will wait for <strong>the</strong> nearest train s rg <strong>of</strong> th<strong>at</strong>train p<strong>at</strong>h with <strong>the</strong> depart <strong>at</strong> time t rg (departure time <strong>of</strong> train g online r):trg $ tij + tirl[min] (1)Providing th<strong>at</strong> <strong>the</strong> train s ij departs from a starting st<strong>at</strong>ion <strong>at</strong>time t o ij and th<strong>at</strong> <strong>the</strong> travelling time to node u is d u ij <strong>the</strong>n <strong>the</strong> arrivaltime to t ij can be formularized by 2 and 3:t ijo= t + dijuij[min] (2)Fig. 1 Logistic technology „Hub-and-Spoke“and for <strong>the</strong> train s rg :t rgo= t + drgurg[min] (3)The “Hub-and-Spoke” technology can be combined with <strong>the</strong>line principle using <strong>the</strong> technology <strong>of</strong> multiple-section trains. Theschem<strong>at</strong>ic represent<strong>at</strong>ion <strong>of</strong> this technology is in Fig. 1. Novak[21] and Vrenken [26] found th<strong>at</strong> <strong>the</strong> network structure based onBlackout time during waiting for reload can be formularizedby 4:o o u ut = t - t + d -d -tlczrgijrgijir[min] (4)20 ● COMMUNICATIONS 3/2008


If we are unable to influence <strong>the</strong> last three timing logic elementsth<strong>at</strong> means th<strong>at</strong> <strong>the</strong> travelling times <strong>of</strong> each train are dij u anddrg u and reloading time is l. Then we can lower <strong>the</strong> blackout timeby increasing <strong>the</strong> value <strong>of</strong> tij o to:ox ot = t + xijor by lowering t o rg value to:ox ot = t + x ; _ x 0irg[min] (5)Now we can extend <strong>the</strong> formula (1) to:ou out + x + d -t -x -d -tl0rgijrgrg[min] (6)Besides <strong>the</strong> boundary conditions like (7) <strong>the</strong>re is also ano<strong>the</strong>rone which ensures time loc<strong>at</strong>ions <strong>of</strong> trains s ij . It may vary in fixedbounds (a ij , b ij ):a # t + x # bij ij ij ijSimilarly for trains s rg :a # t + x # brg rg rg rgRoutes L i and L r pass through <strong>the</strong> node u and two lines <strong>of</strong>those routes s ij and s rg are coordin<strong>at</strong>ed if <strong>the</strong>re exist two numbersx ij and x rg , which fulfil conditions (8) and (9). So we can makea directed graph G (S, H), where (s ij , s rg ) ∈ H if node u existswe are able to coordin<strong>at</strong>e those lines (S – <strong>set</strong> <strong>of</strong> routes, H – coordin<strong>at</strong>edgraph <strong>of</strong> transport network). The edges determine h ∈ Hwhich pairs <strong>of</strong> nodes can be coordin<strong>at</strong>ed but not all <strong>of</strong> <strong>the</strong> pairsfrom <strong>the</strong> <strong>set</strong> H can be coordin<strong>at</strong>ed simultaneously by a differentvalue <strong>of</strong> x ij . Therefore, a coordin<strong>at</strong>ed subgraph G(S, H) mustbe found where for all i 1, … n, j 1, … m i exist values x ij fulfilling<strong>the</strong> condition (7).For <strong>the</strong> coordin<strong>at</strong>ed subgraph G <strong>the</strong>re exist usually more possibilitiesfor <strong>the</strong> x ij value, which comply with each pair <strong>of</strong> nodes(x ij , x rg ) ∈ H conditions (7) and (8). The selection <strong>of</strong> final valuewill depend on <strong>the</strong> consignment volume f ir , which will be reloadedin a node from L i to L r . Here we establish a term optimal solutionfor coordin<strong>at</strong>ed pairs <strong>of</strong> trains. It is determined by <strong>the</strong> subgraphG:X = # x ij -; = 1,… ; = 1,…(7)(8)(9), (10)for i, j which comply with condition (8), for all (x ij , x rg ) ∈ H andcondition (7) and which minimize <strong>the</strong> value <strong>of</strong> <strong>the</strong> objective functionur :/ou ouur= f _ t + x + d -t -x -d -tliir_ sij,srgiijrg rg 1rgrgijrgijrg(11)If we expect th<strong>at</strong> <strong>the</strong> values t o , d u , t are constant according to<strong>the</strong> optimiz<strong>at</strong>ion task <strong>the</strong> value <strong>of</strong> objective function ur is minimizedafter fulfilling above mentioned conditions:ijijir $ijijir/ur= f _ x -xiir rg ij_ sij,srgi! Hl(12)The resultant form <strong>of</strong> objective function depends on subtraction<strong>of</strong> values x ij and x rg which are additional times to arrival <strong>of</strong>a train on a train route t ij or departure <strong>of</strong> a train on a train routet rg . So if we want to <strong>set</strong> up <strong>the</strong> objective function for <strong>the</strong> train routemodel we have to come out from <strong>the</strong> formula (12) as described byCaprara [3] and Cerna [4].4.2 Formul<strong>at</strong>ion <strong>of</strong> a m<strong>at</strong>hem<strong>at</strong>ical modelRailroad timetable <strong>set</strong> up is an intensive and long process. Thereason is in a limited use <strong>of</strong> a computer applic<strong>at</strong>ion. It is mainly aninteractive process between human experiences and autom<strong>at</strong>edgener<strong>at</strong>ion <strong>of</strong> timetable tools. Kryze [18] and Nielsen [20] suggestth<strong>at</strong> <strong>the</strong> whole travelling time for a consignment in intermodaltransport contains <strong>the</strong>se components:● Travelling times between terminals,● Time spent <strong>at</strong> stops on <strong>the</strong> train route,● Waiting time (result <strong>of</strong> insufficient capacity <strong>of</strong> oper<strong>at</strong>ion equipment),● Synchroniz<strong>at</strong>ion time (time needed to reload consignmentsbetween two trains).Shortening <strong>of</strong> first three times (travelling time, time spendand waiting time) is subjected to investments (<strong>of</strong> infrastructure).On <strong>the</strong> contrary, synchroniz<strong>at</strong>ion time is determined by timetableso th<strong>at</strong> we are able to shorten <strong>the</strong> synchroniz<strong>at</strong>ion time only bychange <strong>of</strong> organiz<strong>at</strong>ional <strong>set</strong>-up (non-investment character). Thereforeit would be better to work on optimiz<strong>at</strong>ion leading to minimiz<strong>at</strong>ion<strong>of</strong> synchroniz<strong>at</strong>ion time, as described by Dirmeier [6].In railroad cargo transport <strong>the</strong>re exist two types <strong>of</strong> synchroniz<strong>at</strong>ion:1. Waiting <strong>of</strong> train due to unloading <strong>of</strong> goods.During this first type <strong>of</strong> synchroniz<strong>at</strong>ion <strong>the</strong>re is an extendedtravelling time for goods due to unloading, and <strong>the</strong>refore <strong>the</strong>reis no advantage from synchronized times.2. Waiting <strong>of</strong> goods for connecting trainIn <strong>the</strong> second form is extended travelling time <strong>of</strong> goods whichneeds synchroniz<strong>at</strong>ion.Reloading process (form<strong>at</strong>ion <strong>of</strong> synchroniz<strong>at</strong>ion time principle)<strong>of</strong> transport units between two trains is in Fig. 2. From th<strong>at</strong>figure it follows th<strong>at</strong> <strong>the</strong> waiting time has several significant spells.Those spells are due to shipping and traffic reasons. The mostimportant part is synchroniz<strong>at</strong>ion time which depends on a minimalreloading time. Waiting time is a result <strong>of</strong> insufficient capacity <strong>of</strong>railroad infrastructure or insufficient locomotives. This time maynot apply to each train. The size <strong>of</strong> th<strong>at</strong> time is variable for differentgroups <strong>of</strong> trains. On <strong>the</strong> o<strong>the</strong>r hand, stopping time and timefor disp<strong>at</strong>ch <strong>of</strong> a train must be kept to a minimum for each train.In Fig. 2, we can see a striking difference between <strong>the</strong> waiting time<strong>of</strong> “not-reloaded” consignments in <strong>the</strong> first or second train and <strong>the</strong>waiting <strong>of</strong> reloaded consignments between those trains. Th<strong>at</strong> canbe applied also for more than two trains in a st<strong>at</strong>ion.COMMUNICATIONS 3/2008 ●21


Fig. 2 Consignment reloading processSpeaking <strong>of</strong> transform<strong>at</strong>ion into a m<strong>at</strong>hem<strong>at</strong>ic model <strong>the</strong>authors found two different approaches: Krista [16, 17] formul<strong>at</strong>edthis problem as a linear programming (for small transport networks)and solves it by simplex algorithm, Kolonko [15] solved itvia genetic algorithms (for large transport networks). The linearprogramming calcul<strong>at</strong>ion is very slow – it takes several hours. Incase <strong>of</strong> additional conditions, <strong>the</strong> time <strong>of</strong> calcul<strong>at</strong>ion increases.Th<strong>at</strong>’s why author used <strong>the</strong> genetic algorithm, which is useable forlarge transport networks.This method is in a couple <strong>of</strong> aspects different from <strong>the</strong>“classic” optimiz<strong>at</strong>ion methods. Goldberg [9] found th<strong>at</strong> it usesa random sample and th<strong>at</strong> is why th<strong>at</strong> method is non-deterministic.This means it can give us a different result for each optimiz<strong>at</strong>ion.During <strong>the</strong> optimiz<strong>at</strong>ion this method holds “popul<strong>at</strong>ion <strong>of</strong>candid<strong>at</strong>es for best bet”. Only one member <strong>of</strong> th<strong>at</strong> popul<strong>at</strong>ion is<strong>the</strong> best bet; <strong>the</strong> o<strong>the</strong>rs are sample points where <strong>the</strong> best bet canbe found l<strong>at</strong>er. Th<strong>at</strong> helps avoiding local optimums. Inspired byn<strong>at</strong>ural evolution this method makes periodically random mut<strong>at</strong>ions<strong>of</strong> one or more members from “popul<strong>at</strong>ion <strong>of</strong> candid<strong>at</strong>es forbest bet”. Th<strong>at</strong> process gives us new candid<strong>at</strong>es. Best members <strong>of</strong><strong>the</strong> popul<strong>at</strong>ion survive and <strong>the</strong> weak ones are elimin<strong>at</strong>ed. The disadvantage<strong>of</strong> th<strong>at</strong> method is th<strong>at</strong> we cannot recognize th<strong>at</strong> <strong>the</strong>solution is optimal; <strong>the</strong>refore we don’t know a fixed rule for <strong>the</strong>end <strong>of</strong> optimiz<strong>at</strong>ion, as described by Debels [5].Both methods have some common fe<strong>at</strong>ures:1. The objective function is defined according to optimiz<strong>at</strong>ioncriterions. It is derived from <strong>the</strong> requirement for “as short aspossible” travelling time <strong>at</strong> all stages (minimal network travellingtime). Because <strong>the</strong> only one variable in this value is <strong>the</strong>waiting time for connecting intermodal train in a terminal; <strong>the</strong>value can be limited to <strong>the</strong> sum <strong>of</strong> waiting times in all terminals.For ensuring favourable sequences for each consignment<strong>the</strong>ir volumes must be taken into account because <strong>the</strong> wholetravelling time is affected by volumes <strong>of</strong> reloaded consignments.The objective function is <strong>the</strong>n defined as a minimumfrom <strong>the</strong> sum <strong>of</strong> products <strong>of</strong> synchroniz<strong>at</strong>ion time for reloading<strong>of</strong> consignments to a connecting train Ti synch and volume <strong>of</strong>reloaded consignments fi.min urn/ i synch fi# Tisynchl -i= 1= min T )(12)2. Besides travelling time, stay in terminal or reloading time modelscan also take into account o<strong>the</strong>r constraint condition likeimpossible occup<strong>at</strong>ion <strong>of</strong> a single line stage by two oppositedirected trains or oper<strong>at</strong>ing intervals.Within common fe<strong>at</strong>ures <strong>the</strong>re exist some important differences:1. The solution via a simplex method needs a objective functionand constraint conditions in a linear form but <strong>the</strong> basic problemisn’t linear. A character <strong>of</strong> lag timetable means th<strong>at</strong> reloadinglinkage (eventually constraint conditions) may not be <strong>set</strong> upbetween two train routes during one period and leads to <strong>the</strong>use <strong>of</strong> <strong>the</strong> nonlinear function which returns a division reminderafter integer division. Jentsch [18] found th<strong>at</strong> lineariz<strong>at</strong>ioncalls for an integer parameter (pulse multiplier) tm and pulseinterval T which enable pulse movement T p . Then we have:T p t m * T (13)Such multipliers take <strong>the</strong> value from 10 to 10. For eachreloading terminal (constraint condition) a self pulse multipliermust be <strong>set</strong> up which is an integer parameter.22 ● COMMUNICATIONS 3/2008


2. The simplex algorithm finds a definite optimal solution. On<strong>the</strong> contrary, a genetic algorithm finds a different solution foreach calcul<strong>at</strong>ion. Th<strong>at</strong>’s why a genetic algorithm must be useda number <strong>of</strong> times (<strong>the</strong> more calcul<strong>at</strong>ions <strong>the</strong> higher possibilityto find <strong>the</strong> optimal solution). In <strong>the</strong> next step we analyze<strong>the</strong> best values from <strong>the</strong> genetic algorithm according to o<strong>the</strong>rcriterions because all <strong>the</strong> terms <strong>of</strong> a real system cannot beadded into <strong>the</strong> objective function. Here we can find th<strong>at</strong> <strong>the</strong>best value from <strong>the</strong> genetic algorithm will be unsuitable fora real system and <strong>the</strong> most suitable will be a slightly worsevalue.If we want to solve <strong>the</strong> train route problem we have to definemodel inputs (sort and range <strong>of</strong> values). We used <strong>the</strong> followinginput parameters:● Railroad network – graph (vertices and edges) <strong>of</strong> a real railroadnetwork; vertices are intermodal terminals, edges are tracks(Fig. 3),● Travelling times between vertices,● Train routes – present proposed routes <strong>of</strong> each train accordingto a train oper<strong>at</strong>ion technology,● Stopping time – minimal stopping time <strong>of</strong> a train in node,● Sort <strong>of</strong> pulse – each route has a self pulse between 6 and 24hours,● Reloading time – time needed for reload <strong>of</strong> transport unitsamong trains,● Terminal outputs – volume <strong>of</strong> units reloaded in each node.Fig. 3 Cut <strong>of</strong> Railroad networkFor a <strong>the</strong>oretic model proposal a network from Fig. 3 waschosen. Sixteen nodes (intermodal terminals) and 51 reloadinglinks were added. Distances, travelling times between nodes andpulses were proposed. The pulses are 6, 12 or 24 hours. Thosevalues come up to real pulses for intermodal transports. Reloadingtimes were also valued (from 6 to 10 hours). This time is enoughfor unloading and loading <strong>of</strong> transport units. In Fig. 3 <strong>the</strong>re arealso r<strong>at</strong>ings <strong>of</strong> each reloading link (importance <strong>of</strong> each node).This quantity is stipul<strong>at</strong>ed as a link r<strong>at</strong>ing among each route. Thevalue <strong>of</strong> r<strong>at</strong>ing is a tenth <strong>of</strong> reloaded transport units in TEU(Twenty-foot Equivalent Unit). It means th<strong>at</strong> if we reload 10 TEU,<strong>the</strong> r<strong>at</strong>ing value is 1.Fig. 4 Reloading times and reloading link’s r<strong>at</strong>ings – exampleA very important advantage <strong>of</strong> this model is its variability.This is important especially during individual comput<strong>at</strong>ions andcan without any problems react to some input changes. This <strong>of</strong>fersus <strong>the</strong> possibility to acquire more variable solutions, as describedby Bienstock [2].4.3 The solution resultsThe input d<strong>at</strong>a <strong>of</strong> <strong>the</strong> model were transformed using <strong>the</strong>Premium Solver Pl<strong>at</strong>form Version 7.0 s<strong>of</strong>tware, Frontline Systemsfor Micros<strong>of</strong>t Excel 2007. Based on this product which uses <strong>the</strong>method <strong>of</strong> genetic algorithms, <strong>the</strong> model solution was run inMicros<strong>of</strong>t Excel 2007. For <strong>the</strong> needs <strong>of</strong> finding <strong>the</strong> optimal solutionthis comput<strong>at</strong>ion was run 200 times. The genetic algorithmfinds solutions th<strong>at</strong> cannot be immedi<strong>at</strong>ely classified as optimalones, as described by Debels [5] and Goldberg [9]. Gondro [8]suggests th<strong>at</strong> searching for <strong>the</strong> solution is random and <strong>the</strong>re areusually different results in each comput<strong>at</strong>ion. The optimiz<strong>at</strong>ionwas also carried out several times (<strong>the</strong> more times <strong>the</strong> more probability<strong>of</strong> finding <strong>the</strong> optimal solution). It also seems to be appropri<strong>at</strong>eto choose a few best results and evalu<strong>at</strong>e <strong>the</strong>m followingo<strong>the</strong>r criteria. Because we cannot cover all <strong>the</strong> inputs existing in<strong>the</strong> real world in our objective function it is possible th<strong>at</strong> <strong>the</strong> solutionwith its minimal value can be unsuitable in real life and, on <strong>the</strong>contrary, <strong>the</strong> best usable solution can be a solution with a slightlyworse value <strong>of</strong> <strong>the</strong> objective function. Schmitt [24] and Tuzar[25] found th<strong>at</strong> <strong>the</strong> finding <strong>of</strong> several suboptimal solutions can<strong>the</strong>refore be successfully used.The solution <strong>of</strong> this model can be interpreted ei<strong>the</strong>r in a tableor in a graphic form. The results in a graphic form are expressedas a schem<strong>at</strong>ic represent<strong>at</strong>ion <strong>of</strong> computed results <strong>of</strong> departuresand arrivals <strong>of</strong> <strong>the</strong> trains into nodes in a network graph where <strong>the</strong>vertices are different nodes marked A to P and <strong>the</strong> edges representindividual train connections. Each node was drawn in all <strong>the</strong> relevantconnections with direction and time positions <strong>of</strong> all departuresand arrivals. These time positions are in hours. A value isCOMMUNICATIONS 3/2008 ●23


<strong>at</strong>tached to individual tracks shown by <strong>the</strong> number within eachsmall frame. Theses values say wh<strong>at</strong> pulse was used on th<strong>at</strong> track.A section <strong>of</strong> this graph can be seen in Fig. 5.Fig. 5 Cut <strong>of</strong> graphic expression <strong>of</strong> final model solutionResults <strong>of</strong> 20 best solutions (10 % <strong>of</strong> <strong>the</strong> total count <strong>of</strong> foundsolutions) are shown in Fig. 6. All <strong>the</strong>se solutions have <strong>the</strong> value<strong>of</strong> <strong>the</strong> objective function (sum <strong>of</strong> product <strong>of</strong> waiting times duringreload and weight <strong>of</strong> reloading links representing amount <strong>of</strong> transhippedtransport units) from 110 to 195. From <strong>the</strong> table it isclear th<strong>at</strong> if we choose a simple sum <strong>of</strong> synchroniz<strong>at</strong>ion times <strong>the</strong>Σ T syncΣ T sync *RaitingvalueStandingsStandingsΣ T syncΣ T sync *Raitingvalue1. 39 110 11. 59 1592. 33 115 12. 52 1623. 37 116 13. 53 1634. 38 120 14. 64 1685. 29 125 15. 71 1756. 41 128 16. 70 1847. 51 132 17. 67 1858. 48 136 18. 66 1899. 53 141 19. 78 19110. 60 158 20. 72 195Fig. 6 Resultant value <strong>of</strong> objective function for 20 best resultsbest solution will be no. 5. On <strong>the</strong> contrary <strong>the</strong> solution no. 1 –<strong>the</strong> best one according to <strong>the</strong> objective function – will be in 5 thspot. It is necessary to say th<strong>at</strong> <strong>the</strong> weights <strong>of</strong> <strong>the</strong> transhippedtransport units th<strong>at</strong> significantly influence <strong>the</strong> results are only <strong>the</strong>oreticallyestim<strong>at</strong>ed. Therefore it is valid to investig<strong>at</strong>e also o<strong>the</strong>rsolutions.It has to be said th<strong>at</strong> this designed <strong>the</strong>oretical model is directedto <strong>the</strong> phase <strong>of</strong> <strong>the</strong> prepar<strong>at</strong>ion <strong>of</strong> possible timetables <strong>of</strong> IMTtrains. Therefore, <strong>the</strong> comput<strong>at</strong>ions are based on a premise th<strong>at</strong><strong>the</strong> timetables are adhered to and <strong>the</strong>re are no reserves for elimin<strong>at</strong>ion<strong>of</strong> possible delays.5. ConclusionThe presented method <strong>of</strong> optimiz<strong>at</strong>ion <strong>of</strong> train time positionsminimizes <strong>the</strong> transport<strong>at</strong>ion time in a given system <strong>of</strong> IMT cargotransport through minimiz<strong>at</strong>ion <strong>of</strong> time spent waiting on <strong>the</strong> sequentialtrain in <strong>the</strong> terminal. This method can be used in o<strong>the</strong>r trafficsystems especially in public passenger traffic, i.e. in regional <strong>railway</strong>traffic, bus traffic or in <strong>the</strong> multi-traffic systems.The presented m<strong>at</strong>hem<strong>at</strong>ical model cannot practically solve<strong>the</strong> <strong>set</strong>-up <strong>of</strong> pulse timetable with all constraint conditions becauseeach constraint condition makes <strong>the</strong> solution more complic<strong>at</strong>edand decreases <strong>the</strong> probability for an optimal solution. The mostimportant constraint conditions must be incorpor<strong>at</strong>ed into <strong>the</strong>model.A big advantage <strong>of</strong> <strong>the</strong> proposed model is <strong>the</strong> possibility forarbitrary change <strong>of</strong> inputs. Th<strong>at</strong> makes <strong>the</strong> solution more variable.It is necessary to realize th<strong>at</strong> <strong>the</strong> change <strong>of</strong> a route time or change<strong>of</strong> a line interval (or any o<strong>the</strong>r input) can result in a significantchange <strong>of</strong> <strong>the</strong> total solution for time positions <strong>of</strong> o<strong>the</strong>r lines.Because <strong>of</strong> this, <strong>the</strong> main criterion <strong>of</strong> countries which advoc<strong>at</strong>ea working pulse timetable is to spend a gre<strong>at</strong> deal <strong>of</strong> investment indeveloping a timetable.The presented results are part <strong>of</strong> <strong>the</strong> task MSM 0021627505“Theory <strong>of</strong> transport systems”.References[1] BAR, M.: Fahrplan/Taktfahrplan, Vorlesungsbegleitendes Studienm<strong>at</strong>erial, 1998, Dresden.[2] BIENSTOCK, D., RASKINA, O., SANIEE, I., WANG, Q.: Combined Network Design and Multiperiod Pricing: Modeling, SolutionTechniques, and Comput<strong>at</strong>ion, Oper<strong>at</strong>ions Research, 2/2006, pp. 261–276, ISSN 0030-364X.[3] CAPRARA, A., MONACI, M., TOTH, P., GUIDA, P., L.: A Lagrangian Heuristic Algorithm for a Real-World Train TimetablingProblem, Proc. <strong>of</strong> <strong>the</strong> 1st Intern<strong>at</strong>ional Seminar on Railway Oper<strong>at</strong>ions Modelling and Analysis, pp. 10–29, Delft, 2005, ISBN 90-9019596-3.[4] CERNA, A., CERNY, J.: Theory <strong>of</strong> management and decision in transport systems (in Czech), Institut Jana Pernera, o.p.s. 2004,1. vydani, pp. 159, ISBN 80-86530-15-9.[5] DEBELS, D., VANHOUCKE, M.: A Decomposition-Based Genetic Algorithm for <strong>the</strong> Resource-Constrained Project-Scheduling Problem,Oper<strong>at</strong>ions Research, 3/2007, pp. 457-469, ISSN 0030-364X.[6] DIRMEIER, W.: Die Durchführung des Taktfahrplans in Eisenbahn-Knotenpunkten, Thesis, Technische Hochschule Darmstadt,July 1997.24 ● COMMUNICATIONS 3/2008


[7] FERCHLAND, CH.: Taktverkehr, Proc. <strong>of</strong> ZEL´ 97, pp. 85–90, Zilina, 1997, ISBN 80-7135-050-8.[8] GONDRO C, KINGHORN B.P.: A simple genetic algorithm for multiple sequence alignment, Genetics and Molecular Research 6,pp. 964–982, 2007.[9] GOLDBERG, D. E.: Genetic Algorithms in Search, Optimiz<strong>at</strong>ion, and Machine Learning, Addison-Wesley Publishing Company, pp.412, 2006.[10] HALLOWELL, S. F., HARKER, P. T.: Predicting on-time performance in scheduled railroad oper<strong>at</strong>ions: methodology and applic<strong>at</strong>ionto train scheduling, Transport<strong>at</strong>ion research an Intern<strong>at</strong>ional journal Part A, Vol. 4, pp.279–295, 1998.[11] HEINRICI, T.: Guterzuge im InterCity-Takt, Deutsche Verkehrs-Zeitung, Nr. 148, pp. 10, Hamburg, December 2006, ISSN 0342-166X.[12] HESSE, W., GUCKERT, M., HESLE, R.: OptiTakt – A tool for developing and evalu<strong>at</strong>ing periodic timetables, Proc. <strong>of</strong> 1st Intern<strong>at</strong>ionalSeminar on Railway Oper<strong>at</strong>ions Modelling and Analysis, pp. 55–72, Delft, 2005, ISBN 90-9019596-3.[13] JANACEK, J.: Optimiz<strong>at</strong>ion on Transport Networks (in Czech), Zilinská univerzita, 2006, pp. 248, ISBN 80-8070-586-0.[14] JENTSCH, E., GROPLER, O.: Stochastische Zugfahrt<strong>simul<strong>at</strong>ion</strong> – Zusammenhange und Anwendungsmoglichkeiten, Proc. Taktfahrplanund Kapazit<strong>at</strong>, pp. 154–171, Utrecht 1995, ISSN 0948-8154.[15] KOLONKO, M., NACHTIGALL, K., VOGET, S.: Optimierung von integralen Taktfahrplanen mit genetischen Algorithmen, CeBit96, Universit<strong>at</strong> Hildesheim, 1996, ISSN 0941-3014.[16] KRISTA, M.: Fahrplanoptimierung durch Minimierung der Synchronzeiten, Signal+Draht 1-2, pp. 34–38, Hamburg, June 1999,ISSN 0037-4997.[17] KRISTA, M.: Verfahren zur Fahrplanoptimierung dargestellt am Beispiel der Synchronzeiten, Schriftenreihe des Instituts für Eisenbahnwesenund Verkehrssicherung, TU Braunschweig, Braunschweig 1996, ISSN 0721-7137.[18] KRYZE, P.: Timetable and Transmissivity (in Czech), Thesis, Univerzita Pardubice, Dopravni fakulta Jana Pernera, Pardubice, September2005.[19] LINDNER, H.-R., REDERN, H. W.: Guterzuge im Taktfahrplan – Moglichkeiten und Grenzen, Die Bundesbahn, Vol. 10, pp.867–874, 1989.[20] NIELSEN. M. N., HOVE, B., CLAUSEN, J.: Constructing periodic timetables using MIP – a case study from DSB S-train, Intern.Journal <strong>of</strong> Oper<strong>at</strong>ional Research, 3/2006, pp. 213–227, 2006, ISSN 1745-7653.[21] NOVAK, J.: Combined Transport (in Czech), Institut Jana Pernera, o.p.s., pp.123–136, Pardubice August 2006, ISBN 80-86530-32-9.[22] PANDA, S.: Optimal JIT safety stock and buffer inventory for minimal repair and regular preventive maintenance, Intern. Journal <strong>of</strong>Oper<strong>at</strong>ional Research, 4/2007, pp. 440–451, ISSN 1745-7653.[23] SEVELE, S., SCHNEIDER, E.: Disp<strong>at</strong>ching <strong>of</strong> train oper<strong>at</strong>ions using genetic algorithms, Proc. <strong>of</strong> <strong>the</strong> 1 st Intern<strong>at</strong>ional Seminar onRailway Oper<strong>at</strong>ions Modelling and Analysis, pp.112–123, Delft, June 2005, ISBN 90-9019596-3.[24] SCHMITT, L. M.: Theory <strong>of</strong> Genetic Algorithms II: models for genetic oper<strong>at</strong>ors over <strong>the</strong> string-tensor represent<strong>at</strong>ion <strong>of</strong> popul<strong>at</strong>ions andconvergence to global optima for arbitrary fitness function under scaling, Theoretical Computer Science (310), pp. 181–231, 2004,ISSN 0304-3975.[25] TUZAR, A.: Transport Theories (in Czech), Lecture notes, Univerzita Pardubice, Dopravni fakulta Jana Pernera, Pardubice,October 1996, ISBN 80-7194-039-9.[26] VRENKEN, H., MACHARIS, C., WOLTERS, P.: Intermodal Transport in Europe, European Intermodal Associ<strong>at</strong>ion EIA, pp.61–92, Brussels, October 2005, ISBN 9090199136.COMMUNICATIONS 3/2008 ●25


Juraj Gerlici – Tomas Lack *MODIFIED HHT METHOD USAGE FOR VEHICLEVIBRATION ANALYSIS IN TIME DOMAINThe paper deals with <strong>the</strong> analysis <strong>of</strong> <strong>vehicle</strong> vibr<strong>at</strong>ions in <strong>the</strong> time domain. The main aim is to modify <strong>the</strong> HHT-method for <strong>the</strong> solution<strong>of</strong> mechanical systems with nonlinear members. The modific<strong>at</strong>ion enables <strong>the</strong> comput<strong>at</strong>ion with <strong>the</strong> constant system comput<strong>at</strong>ional m<strong>at</strong>rix.This causes th<strong>at</strong> <strong>the</strong> triangul<strong>at</strong>ion is to be performed once only and <strong>the</strong> nonlinear members affect only <strong>the</strong> right side <strong>of</strong> <strong>the</strong> algebraic equ<strong>at</strong>ionssystem. This can dram<strong>at</strong>ically decrease <strong>the</strong> time consumption <strong>of</strong> <strong>the</strong> comput<strong>at</strong>ion. We used <strong>the</strong> method modified in this way for <strong>the</strong>dynamic analysis <strong>of</strong> <strong>the</strong> model with <strong>the</strong> parameters <strong>of</strong> <strong>the</strong> specimen “ERRI – <strong>vehicle</strong>” th<strong>at</strong> was kinem<strong>at</strong>ically excited.Key words: vibr<strong>at</strong>ion analysis, time domain, modified HHT-method1. IntroductionThe analysis <strong>of</strong> mechanical systems (for example mechanicalsystems <strong>of</strong> <strong>vehicle</strong>s) vibr<strong>at</strong>ion is permanently very topical. The<strong>vehicle</strong> dynamic properties are determined with <strong>the</strong> help <strong>of</strong> thisanalysis during a new <strong>vehicle</strong> design, or a renewal <strong>of</strong> an older existing<strong>vehicle</strong>. The Eigen frequencies are characteristic <strong>of</strong> a <strong>vehicle</strong>construction. A <strong>vehicle</strong> mechanical system is excited with varioustypes <strong>of</strong> loads in <strong>the</strong> oper<strong>at</strong>ion and this is <strong>the</strong> reason why its individualparts oscill<strong>at</strong>e. The aim <strong>of</strong> a dynamical analysis is not onlyto judge <strong>the</strong> influence <strong>of</strong> an excit<strong>at</strong>ion on <strong>the</strong> mechanical systembut also, on <strong>the</strong> base <strong>of</strong> th<strong>at</strong> analysis, to propose and to performconstruction changes <strong>of</strong> a <strong>vehicle</strong> for <strong>the</strong> detected neg<strong>at</strong>ive st<strong>at</strong>eelimin<strong>at</strong>ion or improvement.3. Methods for vibr<strong>at</strong>ion analysis in <strong>the</strong> time domainThe direct numerical integr<strong>at</strong>ion <strong>of</strong> <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motion iswidely used for <strong>the</strong> linear systems solutions where <strong>the</strong> individualprocess character monitoring is important. The principal idea <strong>of</strong>a numerical integr<strong>at</strong>ion lies in <strong>the</strong> fact th<strong>at</strong> we will fulfil <strong>the</strong> equ<strong>at</strong>ion<strong>of</strong> motion in <strong>the</strong> finite t 0 , t 1 , …, t m <strong>moment</strong>s. The distance <strong>of</strong>individual <strong>moment</strong>s is Δt k t k 1 t k , where k 0, 1, …, m1,is labeled a length <strong>of</strong> integr<strong>at</strong>ion step. Starting conditions are aninseparable part <strong>of</strong> an equ<strong>at</strong>ion <strong>of</strong> motion. We consider <strong>the</strong> startto be <strong>the</strong> time t 0. Then it holds:q^h=0 q0qo^h=qo. (1)0 02. Vehicle vibr<strong>at</strong>ion analysisThe aim <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> vibr<strong>at</strong>ion analysis may be <strong>the</strong> <strong>vehicle</strong>behaviour prediction before a performance <strong>of</strong> experimental testsfor a <strong>vehicle</strong> approving into <strong>the</strong> oper<strong>at</strong>ion and saving <strong>the</strong> time andfinancial expenses th<strong>at</strong> may arise according to <strong>the</strong> tests repetition,in <strong>the</strong> case when previous tests had failed. The vibr<strong>at</strong>ion analysiswith <strong>the</strong> help <strong>of</strong> comput<strong>at</strong>ions allows <strong>simul<strong>at</strong>ion</strong> <strong>of</strong> extreme loadingsth<strong>at</strong> evoke critical st<strong>at</strong>es without m<strong>at</strong>erial losses, neg<strong>at</strong>iveinfluence <strong>of</strong> a <strong>vehicle</strong> on <strong>the</strong> track, environment and so on. Thesecomput<strong>at</strong>ions are in practice <strong>of</strong>ten executed with commercial accessibleprogramme packages. They provide results <strong>of</strong> analysis on <strong>the</strong>base <strong>of</strong> chosen <strong>vehicle</strong> parameters, track parameters and loads.The programmes utilise various methods which are <strong>the</strong>ir internalcomponents. It has not become usual th<strong>at</strong> a common user canaffect <strong>the</strong>m.We distinguish <strong>the</strong> three types <strong>of</strong> direct integr<strong>at</strong>ion numericalmethods:– explicit,– implicit,– predictor – corrector.We consider <strong>the</strong> first two types to be <strong>the</strong> fundamental ones.The Predictor – corrector method is in fact a <strong>simul<strong>at</strong>ion</strong> <strong>of</strong> <strong>the</strong>implicit method and is suitable for nonlinear systems solutions.The Integr<strong>at</strong>ion method may be explicit or implicit in dependenceon <strong>the</strong> <strong>moment</strong> in which it uses <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> movement.We compute <strong>the</strong> qt+ Dt, qot+ Dt,qpt+Dtvectors from <strong>the</strong> equ<strong>at</strong>ion<strong>of</strong> motion with <strong>the</strong> help <strong>of</strong> an explicit method on <strong>the</strong> base <strong>of</strong> <strong>the</strong>q, qq o,p moving characteristics course shape presupposition in <strong>the</strong>interval and <strong>the</strong>ir knowledge in <strong>the</strong> time <strong>moment</strong> t.* Juraj Gerlici, Tomas LackFaculty <strong>of</strong> Mechanical Engineering, University <strong>of</strong> Zilina, Slovakia, E-mail: juraj.gerlici@fstroj.uniza.sk.26 ● COMMUNICATIONS 3/2008


The implicit methods, vice versa, use <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motionin <strong>the</strong> time t Δt. They are suitable, first <strong>of</strong> all, for <strong>the</strong> solution<strong>of</strong> <strong>the</strong> linear equ<strong>at</strong>ion <strong>of</strong> motion with a consistent mass m<strong>at</strong>rix.The stability is a characteristic fe<strong>at</strong>ure <strong>of</strong> numerical methods fora direct integr<strong>at</strong>ion <strong>of</strong> an equ<strong>at</strong>ion <strong>of</strong> motion. The stability meansth<strong>at</strong> <strong>the</strong> solutions must not go through limits for <strong>the</strong> arbitrarystarting conditions. If this condition <strong>of</strong> an arbitrary r<strong>at</strong>io <strong>of</strong> Δt/T nis fulfiled, we describe <strong>the</strong> method as unconditionally stable andif it is fulfiled for an individual critical r<strong>at</strong>io Δt/T n only, we talkabout an conditionally stable method. In <strong>the</strong> following text we willapply some methods th<strong>at</strong> may be used for <strong>the</strong> mechanical systemvibr<strong>at</strong>ion analysis in <strong>the</strong> time domain. They are: <strong>the</strong> Differencemethod, <strong>the</strong> Linear acceler<strong>at</strong>ion method, <strong>the</strong> Wilson θ – method,<strong>the</strong> Newmark method [3], and <strong>the</strong> HHT-method [3, 6].Its advantage is <strong>the</strong> possibility to use it for a nonlinear taskssolution as well.3.2 The method <strong>of</strong> linear acceler<strong>at</strong>ionThis method is based on <strong>the</strong> presupposition <strong>of</strong> a linear acceler<strong>at</strong>ioncourse during each <strong>of</strong> integr<strong>at</strong>ion steps, as shown in Fig.1.3.1 The differential methodFor <strong>the</strong> numerical integr<strong>at</strong>ion <strong>of</strong> <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motion wesubstitute <strong>the</strong> time invariant variable for differenties. The simpliestdifferential substitutions <strong>of</strong> <strong>the</strong> acceler<strong>at</strong>ions vector qp and <strong>the</strong>velocities vector qo in <strong>the</strong> time t are:1qo = $ _ qt + D t-qt -Dti, (2)2 $ Dt1qp = , (3)t$ _ q 2 $ q q2 t+ Dt- t+t-DtiDth<strong>at</strong> we apply to <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motion in <strong>the</strong> time tM$ qp+ B$ qo+ K$q = F . (4)t t t tAfter insertion and modific<strong>at</strong>ion we obtain:1 1 2d $ M + $ Bn$ q F K M q2 t+Dt = t-d- $ n$t-2Dt2 $ DtDt(5)1 1-d$ M - $ Bn$ qtt.2+ DDt2 $ DtThe differential method is <strong>the</strong> type <strong>of</strong> an explicit method. Themethod has all <strong>the</strong> advantages <strong>of</strong> explicit methods, if <strong>the</strong> dampingm<strong>at</strong>rix is B 0 or B α ⋅ M. The most effective usage is in <strong>the</strong>case <strong>of</strong> a diagonal mass m<strong>at</strong>rix, id est for solutions <strong>of</strong> systems withconcentr<strong>at</strong>ed massess. The method is only conditionally stable, inthis case <strong>the</strong> lenght <strong>of</strong> integr<strong>at</strong>ion step Δt has to meet <strong>the</strong> followingdemand:T nDt# , (6)rwhere T n is <strong>the</strong> smallest period <strong>of</strong> <strong>the</strong> vibr<strong>at</strong>ion. The rel<strong>at</strong>ively veryshort length <strong>of</strong> integr<strong>at</strong>ion step is needed in order to ensure th<strong>at</strong><strong>the</strong> difference method gives <strong>the</strong> correct solution. Ano<strong>the</strong>r disadvantageis <strong>the</strong> fact, th<strong>at</strong> we need to use <strong>the</strong> special procedure in<strong>the</strong> first step.2Dtq- Dt = q0- Dt$ qo0+$ qp02(7)Fig. 1 An acceler<strong>at</strong>ion courseWe label <strong>the</strong> variable th<strong>at</strong> changes in <strong>the</strong> interval with<strong>the</strong> mark τ, we express <strong>the</strong> rel<strong>at</strong>ion for acceler<strong>at</strong>ion with:xqt p^+ xh= qp t q qt+ _ pt +D t-ptiD(8)We obtain <strong>the</strong> rel<strong>at</strong>ions for qt o ^ + xh and qt ^ + xhvia <strong>the</strong>double integr<strong>at</strong>ion:2xqt o^+ xh= x$qp + _t q p q q2+D - pi+ o$ Dt t t. (9)2 3x xqt ^ + xh= $ qp 2 6 t q q q qt+ _ pt+Dt- pti+ x $ ot+t$ DIn <strong>the</strong> end <strong>the</strong> integr<strong>at</strong>ion step for x = Dt we will get:Dt Dt qot+ Dt = Dt$qpt+ _ q pt+ Dt- q pti+ q ot = q ot+ _ q pt+Dt+q pti2 22 2Dt Dtqt+ Dt = q pt+ _ qpt+Dt- qpti+ Dt$qot+ qt=2 62Dt= qt+ Dt$ qot+ _ qpt+Dt+2 $ qpti6(10)From <strong>the</strong>se rel<strong>at</strong>ions we obtain <strong>the</strong> rel<strong>at</strong>ions for qp t+Dta qot+Dt6qpt+ Dt = _ q t q q 2 q2 t+Dt-D$ ot- ti- $ ptDt3q qt q t q q t q Dt ot+ Dt = ot+ _ t+Dt-D$ ot- ti- D $ pt+ q pt=D233 Dt = $ qt+Dt-2$ qot- $ qt-q p(11)tDtDt2COMMUNICATIONS 3/2008 ●27


After <strong>the</strong> insertion <strong>of</strong> <strong>the</strong> previous rel<strong>at</strong>ions into <strong>the</strong> equ<strong>at</strong>ion<strong>of</strong> motion in <strong>the</strong> time t Δt and after modific<strong>at</strong>ion <strong>the</strong> equ<strong>at</strong>ionobtains <strong>the</strong> form:6t M 3d +t B + K n $ q2t+Dt=D D6 6= F M q(12)t t q qt+ Dt+ d t+ ot+ 2ptn+2 2D D3Bt q q Dt + d t+ 2 ot+q ptnD2The method <strong>of</strong> <strong>the</strong> linear acceler<strong>at</strong>ion does not request anystarting procedure because displacements, velocities and acceler<strong>at</strong>ionsin <strong>the</strong> time t Δt are expressed in <strong>the</strong> dependence on <strong>the</strong>same quantities in <strong>the</strong> time t.3.3 The Wilson θ-methodSimilar to <strong>the</strong> Newmark method, <strong>the</strong> Wilson method is implicitas well. Its original version, <strong>the</strong> method <strong>of</strong> linear acceler<strong>at</strong>ion, is infact <strong>the</strong> Newmark method, where δ 1/2 and α 1/6. The method<strong>of</strong> linear acceler<strong>at</strong>ion is a special case <strong>of</strong> <strong>the</strong> Wilson θ-method,where θ 2. The linear change <strong>of</strong> acceler<strong>at</strong>ion in <strong>the</strong> interval is <strong>the</strong> basic presupposition, as is shown in Fig. 2. In <strong>the</strong>arbitrary point <strong>of</strong> <strong>the</strong> interval <strong>the</strong> following holds:2 2 2 2i $ Dt i $ Dtqt+ iDt = qt+ i $ Dt$qot+ q pt+ _ qpt+iDt- qpti=2 62 2i $ Dt= qt+ i $ Dt$qot+ _ qpt+iDt+2 $ qpti6These rel<strong>at</strong>ions lead to <strong>the</strong> expressions for qp t+iDta qot+iDt6qpt+ iDt = _ qt t-i$ Dt$ qt-qt -2$ q2 2 + iDo i pti $ Dt3qo qt q t q qt+ iDt = ot+ _ t+iDt-i$ D $ ot- ti-i $ D(16)i $ Dt3- i $ Dt$qp q2t q 2 qt+ $ pt = t+iDt- $ ot-i $ D3t q i $ Dt- t-$ qpti $ D 2We insert <strong>the</strong> previous rel<strong>at</strong>ions into <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motionin <strong>the</strong> time τ θ ⋅ Δt and after <strong>the</strong> modific<strong>at</strong>ion <strong>the</strong> equ<strong>at</strong>ion gets<strong>the</strong> form:6t M 3d +t B + K n $ q F2 2t+ iDt = t+iDt+i $ D i $ D6 6+ Md$ qt+ $ qot+ 2 $ qptn+(17)2 2i $ Dti $ Dt3i $ Dt+ Be$ qt+ 2 $ qot+$ qptoi $ Dt2The stability and <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong> method depends on <strong>the</strong>coefficient θ choice. For <strong>the</strong> method stability it is necessary to beθ 1.37.3.4 The Newmark methodThis method is an implicit method. It comes out from <strong>the</strong>method <strong>of</strong> <strong>the</strong> average constant acceler<strong>at</strong>ion. The principal ret<strong>at</strong>ions<strong>of</strong> <strong>the</strong> Newmark method give <strong>the</strong> rel<strong>at</strong>ionship between <strong>the</strong>displacement, <strong>the</strong> velocity and <strong>the</strong> acceler<strong>at</strong>ion in <strong>the</strong> t and t Δt.They are:Fig. 2 An acceler<strong>at</strong>ion dependence on <strong>the</strong> timexqt p^+ xh= qp (13)t q qt+ _ pt+iDt-ptii $ DVia a double integr<strong>at</strong>ion we obtain <strong>the</strong> rel<strong>at</strong>ions for qt o ^ + xhand qt ^ + xh:2xqt o^+ xh= qo qt q qt+ xpt+ _ pt+iDt-pti2 $ i $ D(14)2 3x xqt ^ + xh= q q q2 6 t q qt+ xot+ pt+ _ pt+iDt-pti$ i $ DAt <strong>the</strong> end <strong>of</strong> an integr<strong>at</strong>ion step for τ θ ⋅ Δt we have:i $ Dt qot+ iDt = qt+ i $ Dt$qpt+ _ q pt+iDt- q pti=2i $ Dt = qot+ _ q pt+iDt-q pti(15)2pq t+Dqo = qo + Dt$ 7d$qp + ^1-dhqpAt+ Dt t t+Dt tdqt q dq do1t qt+ Dt = t+Dt-e- o ot- t-a $ D b a $ Dd-Dtd-1nqpt2 $ a(18)12qt+ Dt = qt+ Dt$ qot+ = a$ qpt+Dt+ d -anqptG$ Dt(19)2From <strong>the</strong> previous rel<strong>at</strong>ions we obtain <strong>the</strong> expressions fort and qot+Dt11qpt+ Dt = _ qt t-Dt$qt-qt - -1qt(20)2 + Do i d npa $ Dt2 $ a(21)Inserting <strong>the</strong> previous rel<strong>at</strong>ions into <strong>the</strong> equ<strong>at</strong>ion <strong>of</strong> motion in<strong>the</strong> time t Δt and after <strong>the</strong> modific<strong>at</strong>ion, <strong>the</strong> equ<strong>at</strong>ion has <strong>the</strong>form:28 ● COMMUNICATIONS 3/2008


where:3.5 HHT method(22)The HHT method [6] comes directly out from <strong>the</strong> Newmarkmethod, where we cre<strong>at</strong>e for qp n+1 and qon+1 <strong>the</strong> rel<strong>at</strong>ions <strong>of</strong>:where1da $ Dt2d$ M + $ B+ Knqt+ Dt = Ft+Dt+a $ DtdB1t q dq t d+ =qt+ c - 1mot+ D $ d - nptG+a $ D a2 $ a1M1t q 1t q 1+ =2q2 t+ ot+ d - nptGa $ D a $ D $ a1 1d = , a = . (23)2 4qp= a _ q -qi-a $ qo-a $ qn+ 1 0 n+1 n 2 n 3 n(24)qo = a_q -qi-a $ qo -a $ qp. (25)n+ 1 1 n+1 n 4 n 5 nThe principal equ<strong>at</strong>ion isMqp + _ 1 - a iCqo + a Cqo+n+ 1f n+1 f n+ _ 1 - a iKq + a Kq = F^utf n+ 1 f n n+1u tn+1 = tn+ _ 1 -afiDt(26)We put <strong>the</strong> rel<strong>at</strong>ions (24) and (25) into <strong>the</strong> (26) and we get:A8a $ M+ a $ B+ _ - a i$ KB$ q = F -0 1 1 f n+ 1 n+1- a $ K$ q + M$ 7a $ q + a $ qo+ a $ qpA +f n 0 n 2 n 3 n+ B$ 7a $ q + a $ qo+ a $ qpA1 n 4 n 5 nwhereAF = _ 1 - a i$ F + a $ F is an applied loadn+ 1 f n+1 f n(27)1 a 1 1maamf $ da0 = - aa12 2 = - _4 = - i-a $ Dta $ Dta_ 1 af$ d 1 ama1= - ia3= - - 1(28)a $ Dt2 $ ada5= _ 1 -afi$ d -1n$ Dt2 $ aThe basic <strong>set</strong>ting is1 112a = $ ^ + chd = + c af= c am= 0 (29)42γ – is <strong>the</strong> coefficient <strong>of</strong> an amplitude damping; it may reach1<strong>the</strong> value c = 0 " .3hIt is possible to change <strong>the</strong> <strong>set</strong>ting according to <strong>the</strong> conditions.1 1 11d $ a $ $ d d = - am+af am # af# (30)2 2 22If we use <strong>the</strong>se altern<strong>at</strong>ives, we determine two o<strong>the</strong>r methodsfor <strong>the</strong> parameters determin<strong>at</strong>ion. We can choose <strong>the</strong> given coefficient<strong>of</strong> an amplitude damping γ for four integr<strong>at</strong>ion parametersin <strong>the</strong> following way [8].1 12 1a = $ ^ + chd = + c af= 0 am=-c, (31)42or we can use <strong>the</strong> procedure via Chung and Hulbert [3]:1 c 1 3$ca f = - am= - . (32)224. Modified HHT for <strong>the</strong> solution <strong>of</strong> systemswith nonlinear members [4]whereA8a $ M+ a $ B+ _ - a i$ KB$ q = F -a$ K$0 1 1 f n+ 1 n+1K+B$ q + F + F + + M7a $ q + a $ q o + a $ q p A +nn+1 n+1 0 n 2 n 3 n+ Ba 7 $ q+ a$ qo+ a$qpA1 n 4 n 5 nF A n1 is an applied loadingAF = _ 1 - a i$ F + a $ Fn+ 1 f n+1 f nF Kn1 is <strong>the</strong> additional force <strong>of</strong> nonlinear springsK+ K+K+F = F _ qi $ _ 1 + a i -F _ q i $ an+1 n n f n-1 n-1F Bn1 is <strong>the</strong> additional force <strong>of</strong> <strong>the</strong> nonlinear dampersB+ B+B+F = F _ qoi $ _ 1 - a i + F _ qoi $ an+1 n n f n-1 n-1,(33)(34)(35)(36)All <strong>the</strong> comput<strong>at</strong>ions in <strong>the</strong> time domain were performed by<strong>the</strong> HHT method which was modified for nonlinear members with<strong>the</strong> following parameters γ 0.15, α m 0.15 and Δ t 0.005 sec.comput<strong>at</strong>ion.The FkK and FkB for a nonlinear spring and a nonlineardamper determin<strong>at</strong>ion respectivelyFor a nonlinear spring <strong>the</strong> following holds:kK TT-kk = $ < F $ T - k kfd k dFK +TT $ $k = > ^ h -$ T-_fd ^ h -k$diHfff(37)(38)COMMUNICATIONS 3/2008 ●29


where:k – is <strong>the</strong> basic spring stiffness,T – is <strong>the</strong> transform<strong>at</strong>ion m<strong>at</strong>rix for <strong>the</strong> transform<strong>at</strong>ion froma local into a global coordin<strong>at</strong>e system,K k – is <strong>the</strong> element stiffness m<strong>at</strong>rix,d – is <strong>the</strong> strain <strong>of</strong> a spring in <strong>the</strong> local coordin<strong>at</strong>e system <strong>of</strong><strong>the</strong> spring,f(d) – is <strong>the</strong> prescribed functional dependence <strong>of</strong> an internalforce and strain in a spring,– is <strong>the</strong> additional force from a nonlinear spring.F Kkdeform<strong>at</strong>ion “measured” in nonlinear members <strong>of</strong> comput<strong>at</strong>ionalmodel flexible bindings and given teoretical characteristics. Thesenonlinear courses may in fact describe <strong>the</strong> properties <strong>of</strong> dampersand springs. The example <strong>of</strong> a bogie model th<strong>at</strong> would be equipedwith flexible bindings and dampers with nonlinear characteristicsis depicted in Fig. 3.For a nonlinear damper <strong>the</strong> following holds:bB TT-bk = $ < F $ T - b b(39)fv b vFB +TT $ $k = > ^ h -$ T(40)-_fv ^ h -b$viHwhere:b – is <strong>the</strong> basic damping constant <strong>of</strong> a damper,T – is <strong>the</strong> transform<strong>at</strong>ion m<strong>at</strong>rix for a transform<strong>at</strong>ion froma local into a global coordin<strong>at</strong>e system,B k – is <strong>the</strong> m<strong>at</strong>rix <strong>of</strong> an element damping,v – is <strong>the</strong> mutual velocity <strong>of</strong> node points <strong>of</strong> a damper in <strong>the</strong>local coordin<strong>at</strong>e system <strong>of</strong> a damper,f(v) – is <strong>the</strong> prescribed functional dependence <strong>of</strong> an internalforce in a damper and a mutual velocity <strong>of</strong> node points <strong>of</strong>F Bka damper in <strong>the</strong> local coordin<strong>at</strong>e system <strong>of</strong> a damper,– is <strong>the</strong> additional force from a nonlinear damper.5. Test <strong>of</strong> modified HHT-methodFor this method valid<strong>at</strong>ion we used <strong>the</strong> comparison <strong>of</strong> computerevalu<strong>at</strong>ed dependence courses <strong>of</strong> forces and velocities, orThe principle: <strong>the</strong> forces in nonlinear members were computedas <strong>the</strong> internal forces in <strong>the</strong> serial connected linear springs withhigh stiffness. The prescribed flexible member characteristics arerepresented by curves in <strong>the</strong> graphs. The linear dependency represents<strong>the</strong> basic stiffness, or better, <strong>the</strong> basic stiffness constant.6. ConclusionFig. 3 An example <strong>of</strong> a bogie model (MSC.ADAMS)Simul<strong>at</strong>ion comput<strong>at</strong>ions mainly supported by comput<strong>at</strong>ionaltechnique are used for <strong>the</strong> <strong>vehicle</strong> vibr<strong>at</strong>ion analysis. The proceduresand methods are used for <strong>the</strong> forced oscill<strong>at</strong>ion <strong>of</strong> a mechanicalFig. 4 A secondary suspension damper (left: given parameters, right: a comparison)30 ● COMMUNICATIONS 3/2008


Fig. 5 A prescribed characteristicsFig. 6 An internal force versus a deform<strong>at</strong>ionFig. 7 Schem<strong>at</strong>ic depiction <strong>of</strong> “measurement” principle <strong>of</strong> internal forces in a flexible bindingsystem solution. The <strong>vehicle</strong> model was cre<strong>at</strong>ed for this purpose[4]. A kinem<strong>at</strong>ic excit<strong>at</strong>ion and acceler<strong>at</strong>ions act on <strong>the</strong> model.We can search a response from a harmonic excit<strong>at</strong>ion via <strong>the</strong> solutionin a complex or real form, or we can analyse <strong>the</strong> <strong>vehicle</strong> vibr<strong>at</strong>ionin <strong>the</strong> time domain. It is useful to use <strong>the</strong> HHT method [7]as a special variant <strong>of</strong> <strong>the</strong> Newmark method. The main aim was tomodify <strong>the</strong> HHT-method for <strong>the</strong> solution <strong>of</strong> mechanical systemswith nonlinear members. The modific<strong>at</strong>ion enables <strong>the</strong> comput<strong>at</strong>ionwith <strong>the</strong> constant system comput<strong>at</strong>ional m<strong>at</strong>rix. This causesth<strong>at</strong> <strong>the</strong> triangul<strong>at</strong>ion is to be performed once only and <strong>the</strong> nonlinearmembers affect only <strong>the</strong> right side <strong>of</strong> <strong>the</strong> algebraic equ<strong>at</strong>ionssystem. This can dram<strong>at</strong>ically decrease time consumption <strong>of</strong> <strong>the</strong>comput<strong>at</strong>ion. We used <strong>the</strong> method modified in this way for <strong>the</strong>dynamical analysis <strong>of</strong> <strong>the</strong> model with <strong>the</strong> parameters <strong>of</strong> <strong>the</strong> specimen“ERRI – <strong>vehicle</strong>” th<strong>at</strong> was kinem<strong>at</strong>ically excited. The procedureswere performed with <strong>the</strong> DELTA programme [5].7. AcknowledgementThe work was supported by <strong>the</strong> Scientific Grant Agency <strong>of</strong><strong>the</strong> Ministry <strong>of</strong> Educ<strong>at</strong>ion <strong>of</strong> <strong>the</strong> Slovak Republic and <strong>the</strong> SlovakAcademy <strong>of</strong> Sciences in <strong>the</strong> project No. 1/3169/06 “PropertiesResearch <strong>of</strong> Rail Vehicles in Movement with Emphasis on <strong>the</strong>Solution <strong>of</strong> a Wheel and Rail Contact <strong>at</strong> <strong>the</strong> Wheel<strong>set</strong> Rolling in <strong>the</strong>Rail via Computer Simul<strong>at</strong>ion” and in <strong>the</strong> project No. 1/4119/07:“Investig<strong>at</strong>ion <strong>of</strong> a dynamic properties <strong>of</strong> a <strong>vehicle</strong>”.References[1] GERLICI, J., LACK, T.: An Analysis <strong>of</strong> Bumpers and Springs Parameters Influence on <strong>the</strong> Ride Comfort (in Slovak), Dynamics <strong>of</strong>Rigid and Deformable Bodies, Proc. <strong>of</strong> V. intern<strong>at</strong>ional conference, ISBN 978-80-7044-914-1, pp. 39–48, Univerzita J. E. Purkynev Usti nad Labem, 2007.COMMUNICATIONS 3/2008 ●31


[2] GERLICI, J., LACK, T.: Methods for Vehicle Vibr<strong>at</strong>ion Analysis in Time Domain, Prace naukowe Politechniki Warszawskiej, Z. 63,Transport, 2007, pp. 71–81, Publishing House <strong>of</strong> <strong>the</strong> Warsaw University <strong>of</strong> Technology, ISSN 1230-9265, Warszawa, 2007.[3] CHUNG, J., HULBERT, G. M.: A Time Integr<strong>at</strong>ion Algorithm for Structural Dynamics with Improved Numerical Dissip<strong>at</strong>ion: The Generalized-αMethod, Journal <strong>of</strong> Applied Mechanics, ISSN: 0021-8936, Vol. 60, p. 371 (1993).[4] LACK, T.: The Dynamic Properties Analysis <strong>of</strong> Vehicles from <strong>the</strong> Point <strong>of</strong> View <strong>of</strong> Ride Comfort (in Slovak), Habilit<strong>at</strong>ion Work, pp.176, Faculty <strong>of</strong> Mechanical Engineering University <strong>of</strong> Zilina, 2007.[5] LACK, T., GERLICI, J.: The Programme System DELTA Exploit<strong>at</strong>ion for Numerical Analysis Performances (in Slovak), Proc. <strong>of</strong> 18 thIntern<strong>at</strong>ional Conference “Current Problems in Rail Vehicles – PRORAIL 2007” – Part II, pp. 11–22, EDIS, ISBN 978-80-89276-07-3, Zilina, 2007.[6] LACK, T., GERLICI, J.: Vehicles Dynamic Properties Analysis from <strong>the</strong> Point <strong>of</strong> View <strong>of</strong> Comfort for Passengers, Archives <strong>of</strong> Transport,issue 1-2/2007, pp. 91–110, ISSN 8066-9546, Warszawa, 2007.[7] NEGRUT, D., RAMPALLI, R., SAJDAK, T.: On <strong>the</strong> Implement<strong>at</strong>ion <strong>of</strong> <strong>the</strong> method in MSC.ADAMS, p. 12, 2004, Technical supportfor MSC.SOFTWARE users, published on <strong>the</strong> Internet.[8] WOOD, W. L., BOSSAK, M., ZIENKIEWICZ, O. C.: An Alpha Modific<strong>at</strong>ion <strong>of</strong> Newmark Method, Intern<strong>at</strong>ional Journal <strong>of</strong> NumericalMethod in Engineering, ISSN 0020-7683, vol. 15, p. 1562, 198132 ● COMMUNICATIONS 3/2008


Peter Faith *PASSENGER ROAD TRANSPORT TRENDS IN THESLOVAK REPUBLICThe article deals with <strong>the</strong> present trends in <strong>the</strong> passenger road transport in <strong>the</strong> Slovak Republic. It provides <strong>the</strong> characteristic <strong>of</strong> indic<strong>at</strong>ors<strong>of</strong> development phases <strong>of</strong> <strong>the</strong> passenger road transport trends. Existing increase <strong>of</strong> number <strong>of</strong> <strong>vehicle</strong>s and individual road transport performancesshall bring unfavourable impacts on environment on <strong>the</strong> one hand and on <strong>the</strong> o<strong>the</strong>r hand, it shall be <strong>the</strong> source <strong>of</strong> <strong>the</strong> st<strong>at</strong>e budgetincome.Permanent conflict between individual road transport and mass passenger transport makes all administr<strong>at</strong>ive authorities to follow impactson <strong>the</strong> life <strong>of</strong> inhabitants in agglomer<strong>at</strong>ions with assumed higher concentr<strong>at</strong>ion <strong>of</strong> inhabitants. Demand for passenger cars will be permanentand any decrease in <strong>the</strong> passenger road transport cannot be assumed. Therefore, it is necessary to show a permanent interest in this sphere<strong>of</strong> problems and deal with it on <strong>the</strong> highest possible level.1. IntroductionFollowing <strong>the</strong> Slovak Republic accession to <strong>the</strong> European structuresand gradual market economy development, markedly changeshave been accomplished including different social and popul<strong>at</strong>ionimpacts.At present, passenger road transport trends in our country arenecessary to be studied in light <strong>of</strong> different aspects. On <strong>the</strong> onehand, existing increase <strong>of</strong> number <strong>of</strong> <strong>vehicle</strong>s and individual roadtransport performances brings unfavourable impacts on environmentand on <strong>the</strong> o<strong>the</strong>r hand it represents an income to <strong>the</strong> st<strong>at</strong>ebudget from sale <strong>of</strong> fuels, <strong>vehicle</strong>s and o<strong>the</strong>r items rel<strong>at</strong>ed to <strong>the</strong>passenger road transport.A separ<strong>at</strong>e chapter includes building necessary transport areas,namely parking and lay-by areas, final building and maintaininggood conditions <strong>of</strong> all road c<strong>at</strong>egories.Most intensive passenger road transport development is evidentin areas with high density <strong>of</strong> popul<strong>at</strong>ion where it causes difficultiesin sustainable environment, i.e. it acts mainly as an unfavourablefactor.Permanent conflict between individual road transport and masspassenger transport makes all administr<strong>at</strong>ive bodies to followimpacts on <strong>the</strong> life <strong>of</strong> popul<strong>at</strong>ion in agglomer<strong>at</strong>ions with assumedhigher concentr<strong>at</strong>ion <strong>of</strong> inhabitants. It is necessary to determinean effective co-oper<strong>at</strong>ion r<strong>at</strong>e between individual road transportand mass passenger transport which is impossible in number <strong>of</strong>cases. Different measures, however, may be taken to influence efficientlymodal split, particularly in <strong>the</strong> event <strong>of</strong> travels for workpurposes, i. e. regularly repe<strong>at</strong>ed trips per day.All present impacts on passenger road transport developmentwhich included, for example, <strong>the</strong> energy crisis <strong>at</strong> <strong>the</strong> beginning <strong>of</strong>seventies, <strong>the</strong> increase <strong>of</strong> fuel prices or cars didn’t cause anymarkedly deceler<strong>at</strong>ion <strong>of</strong> development <strong>of</strong> <strong>the</strong> said mode <strong>of</strong> passengertransport. This trend may be observed not only in <strong>the</strong> developedcountries where <strong>the</strong> degree <strong>of</strong> passenger road transport amounts toaround 2.5 inhabitants per one passenger car but also in lessdeveloped countries with <strong>the</strong> degree <strong>of</strong> passenger road transportamounting to around 5.5 inhabitants per one passenger car.2. Present passenger road transport trends in SlovakiaIssues concerning development and reach <strong>of</strong> reasonable s<strong>at</strong>ur<strong>at</strong>ion<strong>of</strong> individual transport needs <strong>of</strong> <strong>the</strong> popul<strong>at</strong>ion rank amongtopical issues, in particular, in rel<strong>at</strong>ion to a living standard, <strong>the</strong> way<strong>of</strong> living and environment. Rel<strong>at</strong>ion to a passenger car and to <strong>the</strong>passenger road transport trends in general represents an importantfactor. Opinions concerning passenger car have been different andreflect political and economic situ<strong>at</strong>ion <strong>of</strong> <strong>the</strong> society.Slovakia during its independence period has failed to reach<strong>the</strong> degree <strong>of</strong> passenger road transport <strong>of</strong> majority <strong>of</strong> Europeancountries and it even lacks behind <strong>the</strong> Visegrad Four Countries orsome Baltic Countries. At present, <strong>the</strong> degree <strong>of</strong> passenger roadtransport in Slovakia has amounted to about 4 inhabitants per onepassenger car which in <strong>the</strong> Czech Republic has amounted to 2.4inhabitants, in Hungary to 3.5 and in Poland to 3.1 inhabitantsper one passenger car [2].* Peter FaithDepartment <strong>of</strong> Road Transport, Faculty <strong>of</strong> Oper<strong>at</strong>ion and Economic <strong>of</strong> Transport and Communic<strong>at</strong>ions, University <strong>of</strong> Zilina, SlovakiaE-mail: Peter.Faith@fpedas.uniza.skCOMMUNICATIONS 3/2008 ●33


Resulting from experience <strong>the</strong> degree <strong>of</strong> passenger road transport<strong>of</strong> about 5 inhabitants per one passenger car starts to causefirst problems within <strong>the</strong> society, which means <strong>the</strong> road safety,parking problems, etc. With <strong>the</strong> degree <strong>of</strong> passenger road transport<strong>of</strong> 2.5 inhabitants per one passenger car very serious problemsoccur in <strong>the</strong> urban traffic and <strong>the</strong> weekend peak hour traffic whencar congestions are formed <strong>at</strong> entries to bigger towns.Present passenger road transport trends in Slovakia may becharacterised as gradually developing (Table 1). During <strong>the</strong> periodfrom 1970 to 1980 number <strong>of</strong> passenger cars increased 3.4 times,from 1980 to 1990 1.6 times, from 1990 to 2000 1.5 times. Eventhough <strong>the</strong> comparison <strong>of</strong> present individual passenger road transporttrends indic<strong>at</strong>es th<strong>at</strong> certain car boom level already has occurredin Slovakia it may be expected th<strong>at</strong> a cyclic development with differentlevel <strong>of</strong> increases will continue in <strong>the</strong> future.Vehicle Number Trends in Slovakia Table 1YEARPassengercarsSource: The SR Presidency <strong>of</strong> <strong>the</strong> Traffic PolicePassenger roadtransport degree/inhabitans/car/Number<strong>of</strong> passengercars/1000inhabit.1965 53870 81.53 12.271970 158690 28.61 34.951975 339427 14.03 71.251980 535952 9.32 107.271985 687067 7.54 135.811990 875550 6.07 165.951995 1015794 5.28 189.242000 1274244 4.24 235.862005 1304705 4.13 242.102006 1333749 4.04 247.28Passenger road transport trends should be understood fromtwo views; an external – social and an internal – an individual (afamily). There is a narrow connection between exogenous andendogenous factors <strong>of</strong> <strong>the</strong> economic development. To carry outan exhausting analysis <strong>of</strong> this economic changes and decisionsinteraction means a very demanding task. In specific<strong>at</strong>ion <strong>of</strong> individualpassenger road transport development trends it is <strong>the</strong>reforenecessary to result from existing experience and knowledge <strong>of</strong>countries which already have faced <strong>the</strong> similar problem. An assumedindividual car transport development in Slovakia is presented in<strong>the</strong> altern<strong>at</strong>ive development scenarios by 2030.With regard to <strong>the</strong> Slovak economy orient<strong>at</strong>ion to <strong>the</strong> marketeconomy an issue concerning <strong>the</strong> social establishment differencesis insignificant and purely economic issues and issues concerning<strong>the</strong> way <strong>of</strong> living are foreground.In connection with this it is necessary to mention <strong>the</strong> basicfact th<strong>at</strong> Slovakia will be one <strong>of</strong> <strong>the</strong> countries with <strong>the</strong> highestportion <strong>of</strong> manufactured passenger cars per one inhabitant peryear in <strong>the</strong> world.This fact should also be taken in consider<strong>at</strong>ion in approach to<strong>the</strong> economic evalu<strong>at</strong>ion <strong>of</strong> individual road transport developmentwhich can be divided into several phases [1]:● In Phase 1, leading economists considered <strong>the</strong> road transporttrends toge<strong>the</strong>r with building own manufacturing basis one <strong>of</strong><strong>the</strong> main important factors which should speed-up economicdevelopment in <strong>the</strong> country; this period falls into <strong>the</strong> post-wareconomic restor<strong>at</strong>ion period. Phase 1 also covers <strong>the</strong> presentperiod when after gaining an economic independence <strong>the</strong> passengercar manufacture development in Slovakia assumed a newdimension when two world automobile factories have added up<strong>the</strong> existing automobile factory;● In Phase 2, a passenger car has been understood a mean <strong>of</strong>transport evalu<strong>at</strong>ed under commonly used criteria in evalu<strong>at</strong>ion<strong>of</strong> o<strong>the</strong>r public transport systems, i. e. an economic efficiencycriterion <strong>of</strong> <strong>the</strong> basic mean in <strong>the</strong> light <strong>of</strong> transport sector;● In Phase 3, an economic efficiency criterion has been transferredto <strong>the</strong> popul<strong>at</strong>ion personal consumption where a passenger caris understood a long-term consumed as<strong>set</strong> suitable for realis<strong>at</strong>ion<strong>of</strong> an increasing income <strong>of</strong> <strong>the</strong> popul<strong>at</strong>ion; its transport<strong>at</strong>ionfunction is secondary in number <strong>of</strong> cases;● Finally, <strong>at</strong> present, <strong>the</strong> convergence <strong>of</strong> aspects all preceding developmentphases have occurred and a passenger car is on <strong>the</strong> onehand considered a mean <strong>of</strong> production for a group <strong>of</strong> peopleand on <strong>the</strong> o<strong>the</strong>r hand, a mean <strong>of</strong> transport s<strong>at</strong>isfying best criteriafor passenger transport.In every development phase it is possible to accept an economicevalu<strong>at</strong>ion method where <strong>the</strong> amount <strong>of</strong> a gross n<strong>at</strong>ional product(GNP) plays an important role from <strong>the</strong> social aspect. Time pricedepending on an income amount is decisive in <strong>the</strong> light <strong>of</strong> an individual,i.e., time saving expressed in monetary units achieved thanksto a passenger car use. The fact th<strong>at</strong> <strong>the</strong> GNP amount depends toa certain level on number <strong>of</strong> passenger cars per inhabitant hasalready been proved in <strong>the</strong> preceding development phase analyses.Upon gross n<strong>at</strong>ional product increase per inhabitant in <strong>the</strong>country <strong>the</strong> number <strong>of</strong> passenger cars has increased while <strong>the</strong> timefactor plays an important role and decrease <strong>of</strong> necessary GNPlevel per one car occurs with time in <strong>the</strong> country. It means th<strong>at</strong>countries with lower GNP level are able to alloc<strong>at</strong>e a lower amountto passenger road transport than more developed countries witha higher GNP level. Foreign experience indic<strong>at</strong>es th<strong>at</strong> passengerroad transport grows faster in <strong>the</strong> countries in which a higher GNPinter-year increase has been recorded than in <strong>the</strong> countries whichreach a high GNP level/inhabitant in <strong>the</strong> long term and approach<strong>the</strong> s<strong>at</strong>ur<strong>at</strong>ion level <strong>of</strong> number <strong>of</strong> passenger cars per number <strong>of</strong>inhabitants. To compare <strong>the</strong> situ<strong>at</strong>ion in <strong>the</strong> CR and Slovakia in2005, <strong>the</strong>re was 1000 EUR GNP/inhabitant sufficient for approxim<strong>at</strong>ely44 passenger cars/1000 inhabitants in <strong>the</strong> CR and thisvalue corresponds to 35 passenger cars/1000 inhabitants in Slovakia.Yet more interesting is a comparison between some EUcountries for 2002 presented in <strong>the</strong> following Fig. 1 [2].34 ● COMMUNICATIONS 3/2008


Despite an unsteady SR economic development when <strong>the</strong> GNPdevelopment has recorded a higher level in comparison with o<strong>the</strong>rEuropean countries it is possible to assume th<strong>at</strong> <strong>the</strong> next individualpassenger road transport development will be very dynamic. Thepreceding economic situ<strong>at</strong>ion was r<strong>at</strong>her complic<strong>at</strong>ed and nontransparentto forecast <strong>the</strong> passenger road transport trends and itwas impossible to consider it sustainable and make definite conclusions.We may assume th<strong>at</strong> <strong>the</strong> present economic growth willfur<strong>the</strong>r continue in <strong>the</strong> next years thus increasing <strong>the</strong> r<strong>at</strong>e <strong>of</strong> passengercars/inhabitants in passenger road transport development.LuxemburgItalyPortugalGermanyEU-15SpainFranceBelgiumSwedenUnited KingdomNe<strong>the</strong>rlandFinlandCzech republicGreeceIrelandDenmarkPolandHungarySlovakiaSource: The Eurost<strong>at</strong>Fig. 1 Rel<strong>at</strong>ion between GNP in EUR per one inhabitant and number <strong>of</strong> passenger cars per 1000 inhabitants in selected European countriesCOMMUNICATIONS 3/2008 ●35


Upon this streng<strong>the</strong>ning <strong>of</strong> pretensions to a passenger car Slovakiawill be able to reach soon some European countries.From economic factors studies it is possible to derive bo<strong>the</strong>xogenous and endogenous factor impact on <strong>the</strong> passenger roadtransport development. Endogenous factors include a family income,an average wage amount, a time price, and a way <strong>of</strong> living. Theliving standard which may be considered a summary explic<strong>at</strong>ion<strong>of</strong> endogenous factors has been considerably differenti<strong>at</strong>ed.A principal insufficiency rests upon <strong>the</strong> fact th<strong>at</strong> differenti<strong>at</strong>ionhas failed to proceed in accordance with <strong>the</strong> r<strong>at</strong>e <strong>of</strong> labourand business results. The living standard has increased only withsome preferred pr<strong>of</strong>essions, while <strong>the</strong> living standard <strong>of</strong> majority<strong>of</strong> <strong>the</strong> popul<strong>at</strong>ion has considerably decreased. The aforesaid factshave influenced <strong>the</strong> level <strong>of</strong> passenger cars in Slovakia.There are still more frequent “expensive” foreign cars on ourroads on <strong>the</strong> one hand and on <strong>the</strong> o<strong>the</strong>r hand families with lowincome try to maintain in oper<strong>at</strong>ion older cars which frequentlydo not comply with requirements for <strong>vehicle</strong> technical conditions.Resulting from this economic analysis in <strong>the</strong> light <strong>of</strong> <strong>the</strong> high– optimistic scenario it is possible to expect <strong>the</strong> amount <strong>of</strong> 420passenger cars per 1000 inhabitants, i.e. 1.4 inhabitants per 1 passengercar in 2030 [1].3. Passenger Road Transport TrendsIn <strong>the</strong> past, passenger road transport trends in Slovakia werecharacterised by different r<strong>at</strong>es <strong>of</strong> growth <strong>of</strong> number <strong>of</strong> passengercars [3]:● 1965 – 1970 in average by 66.7 %,● 1971 – 1975 in average by 43.0 %,● 1976 – 1980 in average by 28.4 %,● 1981 – 1985 in average by 17.5 %,● 1986 – 1990 in average by 16.2 %,● 1991 – 1995 in average by 10.8 %,● 1996 – 2000 in average by 13.3 %,● 2001 – 2005 in average by 13.5 %.As in December 31, 2006 <strong>the</strong> total number <strong>of</strong> passenger carsin oper<strong>at</strong>ion reached 1 333 305 units and <strong>the</strong> total number <strong>of</strong>motor <strong>vehicle</strong>s reached 1 710 645 units [3].In <strong>the</strong> light <strong>of</strong> <strong>the</strong> <strong>at</strong>tained passenger road transport degree <strong>of</strong>4.05 inhabitants per 1 passenger car, i.e. 247.28 passenger cars per1000 inhabitants, Slovakia ranks among <strong>the</strong> European countrieswith <strong>the</strong> lowest passenger road transport development degree.Source: The SR Presidency <strong>of</strong> <strong>the</strong> Traffic PoliceFig. 2 Trends <strong>of</strong> number <strong>of</strong> passenger car per 1000 inhabitants in Slovakia (1965-2006)36 ● COMMUNICATIONS 3/2008


The degree <strong>of</strong> passenger road transport development in Slovakia,however, did not develop equally in all areas <strong>of</strong> <strong>the</strong> countrywhich was caused by number <strong>of</strong> reasons being not studied thoroughlyyet.As regards <strong>the</strong> passenger car degree, some regions as <strong>the</strong>Trencin region, <strong>the</strong> Presov and <strong>the</strong> Zilina regions reach only half<strong>of</strong> <strong>the</strong> Br<strong>at</strong>islava level. It is impossible to determine exactly causes<strong>of</strong> differences in <strong>the</strong> passenger car degree in individual SR regions.A survey and a more detail analysis should be performed. From<strong>the</strong> given Fig. 3 higher passenger car degree per inhabitants isshown in <strong>the</strong> Br<strong>at</strong>islava region, which is caused by a high degree <strong>of</strong>cars in <strong>the</strong> town where it <strong>at</strong>tains 429.97 passenger cars per 1000inhabitants [1].Source: The SR Presidency <strong>of</strong> <strong>the</strong> Traffic PoliceFig. 4 Trends in increase <strong>of</strong> number <strong>of</strong> passenger cars and inhabitantspresent, <strong>the</strong>re are 48 passenger car makes <strong>of</strong> different types andmodels marketed in our market.Older cars which were ei<strong>the</strong>r bought in <strong>the</strong> used-car dealershipsand from sellers or imported from abroad should be also calcul<strong>at</strong>edin <strong>the</strong> passenger car increase.Annually, <strong>the</strong>re are 57 000 new cars sold in average <strong>at</strong> ourmarket. However, <strong>the</strong>re were 74 903 cars sold in total <strong>at</strong> our marketin 1996 which was caused by cancell<strong>at</strong>ion <strong>of</strong> import duty on passengercars with cylinder capacity by 1400 cm 3 .Source: The SR Presidency <strong>of</strong> <strong>the</strong> Traffic PoliceFig. 3 Differences <strong>of</strong> passenger car degree per inhabitants according toindividual regions (year 2006)In 2004 an oblig<strong>at</strong>ory replacement <strong>of</strong> car registr<strong>at</strong>ion pl<strong>at</strong>eswas introduced which caused higher number <strong>of</strong> older cars beingremoved from <strong>the</strong> Transport Inspector<strong>at</strong>e Records and significantdecrease occurred in <strong>the</strong> real increase <strong>of</strong> passenger cars.5. Passenger car sales by car makes4. Passenger car sales and increasesTrends <strong>of</strong> <strong>the</strong> specific passenger car increase registered by <strong>the</strong>transport police in Slovakia have been favourable. An annualaverage increase has represented 35 000 units <strong>of</strong> passenger cars bynow. It is interesting to compare an increase <strong>of</strong> number <strong>of</strong> inhabitantswith number <strong>of</strong> passenger car increase for <strong>the</strong> analysedperiod from 1966 to 2006. When <strong>the</strong> proportion <strong>of</strong> number <strong>of</strong>inhabitants increase to <strong>the</strong> number <strong>of</strong> passenger car increase wasmore than 1 by 1985, <strong>the</strong>re was a turnover after 1985 when anannual increase <strong>of</strong> number <strong>of</strong> passenger cars exceeded <strong>the</strong> number<strong>of</strong> inhabitants increase (Fig. 4) [5, 4].After 1989 principal changes occurred in <strong>the</strong> passenger carmarket. The supply – demand r<strong>at</strong>io turned after 1989 and all <strong>the</strong>world car makes have been gradually introduced in our market. AtAn annual passenger car increase (<strong>the</strong> difference between <strong>the</strong>newly registered cars and those removed from <strong>the</strong> Transport Inspector<strong>at</strong>eRecords) represents around 40 000 units.For <strong>the</strong> period from 1965 to 2006 <strong>the</strong> first position was constantlyheld by Skoda car whose average annual sales representedapproxim<strong>at</strong>ely 15 000 units, <strong>at</strong> present Fabia and Octavia typesprevail. In recent years, Volkswagen, Renault, Peugeot, Opel andCitroen are o<strong>the</strong>r most frequently sold car makes. Certain shifts bycar makes occurred <strong>at</strong> <strong>the</strong> passenger car market over <strong>the</strong> past twoyears. It can be said th<strong>at</strong> <strong>the</strong> Slovak market is typically oriented <strong>at</strong>cheaper cars which must, however, meet basic usable properties,and its orient<strong>at</strong>ion is also aimed <strong>at</strong> car makes whose productionstarted in Slovakia in 2006, i.e. Peugeot and Kia. While Peugeotbelonged to <strong>the</strong> well sold cars also before 2006, Kia has <strong>at</strong>tainedvery quickly an important position in <strong>the</strong> market; by 2006 number<strong>of</strong> sold Kia cars was low, some 500 units per year, after 2006 itCOMMUNICATIONS 3/2008 ●37


<strong>at</strong>tained <strong>the</strong> 6th position <strong>of</strong> <strong>the</strong> best sold cars and in 2007 it sold3743 cars which means tripled sales <strong>of</strong> cars in 2006 [5].6. Passenger car lifetimeAn average passenger car lifetime may be assumed for 20 – 25years in <strong>the</strong> SR. More than 44 000 passenger cars are older than30 years. The highest number <strong>of</strong> passenger cars is within <strong>the</strong> range<strong>of</strong> 5 – 10 years <strong>of</strong> age which represents approxim<strong>at</strong>ely 356 000units (Fig. 5) [3].At present, an average age <strong>of</strong> <strong>the</strong> passenger car fleet is about13 years. The above lifetime significantly exceeds values <strong>at</strong>tainedin <strong>the</strong> developed countries which results from two following factors:● The rel<strong>at</strong>ion between <strong>the</strong> total price <strong>of</strong> a new car and income <strong>of</strong>inhabitants;● Amount <strong>of</strong> fuel price and spare part price for a passenger car.measures taken in <strong>the</strong> tax or charge payments.Macroeconomic indic<strong>at</strong>ors and <strong>the</strong> society sustainable developmentinfluence passenger road transport trends from externalpoint <strong>of</strong> view and <strong>the</strong> way <strong>of</strong> living <strong>of</strong> inhabitants and <strong>the</strong>ir livingstandard influence it from an internal point <strong>of</strong> view. There isa narrow connection between exogenous and endogenous factors<strong>of</strong> <strong>the</strong> economic development. To perform an exhausting analysis<strong>of</strong> an interaction between <strong>the</strong> economic changes and decisionswhich influence passenger road transport is a very demanding task.In our conditions, this task is even more complic<strong>at</strong>ed for <strong>the</strong> presentstage <strong>of</strong> <strong>the</strong> economic development and for <strong>the</strong> next stable developmentand line-up with more developed European countries.The passenger road transport forecast should result from <strong>the</strong>present experience and knowledge <strong>of</strong> <strong>the</strong> countries <strong>at</strong>taining highdegree <strong>of</strong> number <strong>of</strong> passenger cars per inhabitants.It may be assumed th<strong>at</strong> opinions concerning <strong>the</strong> passenger carownership do not change, on <strong>the</strong> contrary, <strong>the</strong>re is a permanentinterest in a passenger car and its use will become an inevitablepart <strong>of</strong> <strong>the</strong> everyday life <strong>of</strong> people for different purposes.A passenger car meets a wide range <strong>of</strong> quality criteria laid ondifferent purposes <strong>of</strong> trips. It is characterised by a high level <strong>of</strong>readiness for transport, high speed door-to-door transport<strong>at</strong>ionservices, it is evalu<strong>at</strong>ed as a very comfortable means <strong>of</strong> transportand travelling by a passenger car ensures a maximum degree <strong>of</strong>privacy. In addition, many passenger car owners consider cars <strong>the</strong>irhobby.Source: The SR Presidency <strong>of</strong> <strong>the</strong> Traffic Police and own calcul<strong>at</strong>ionsFig. 5 Year structure passenger cars in <strong>the</strong> Slovak Republic(st<strong>at</strong>e <strong>at</strong> 31.12.2006)Tax decrease <strong>of</strong> new <strong>vehicle</strong>s and fuels and increase <strong>of</strong> sparepart tax could lead to <strong>the</strong> decrease <strong>of</strong> an average lifetime to approxim<strong>at</strong>ely15 – 18 years and to <strong>the</strong> substantial increase <strong>of</strong> efficiency<strong>of</strong> oper<strong>at</strong>ion <strong>of</strong> <strong>the</strong> entire passenger car fleet.A long car life oper<strong>at</strong>ion or its maintenance in <strong>the</strong> SR hasbeen reflected in different fields, for example in:● fuel consumption increase and <strong>the</strong>ir assortment preserv<strong>at</strong>ion;● necessity to produce, import and store spare parts for excessively/toolong time (for 10 years),● increase <strong>of</strong> m<strong>at</strong>erial use for oper<strong>at</strong>ion to ensure <strong>the</strong> oper<strong>at</strong>ion –fleet capabilities,● deterior<strong>at</strong>ion <strong>of</strong> unfavourable impacts <strong>of</strong> <strong>the</strong> passenger roadtransport on environment etc.7. ConclusionIndividual passenger road transport trends in <strong>the</strong> SlovakRepublic will continue to move forward and in <strong>the</strong> light <strong>of</strong> <strong>the</strong>present experience it will be nei<strong>the</strong>r stopped by such events asenergy crisis, increase <strong>of</strong> car and fuel prices in <strong>the</strong> past, nor by <strong>the</strong>A passenger car compared with means <strong>of</strong> mass passenger transportstill successfully competes in <strong>the</strong> high speed long distancetransfer. A passenger car use gradually becomes a problem in urbanareas with high density <strong>of</strong> popul<strong>at</strong>ion from both <strong>the</strong> environmentaland time loss point <strong>of</strong> view where mass urban transport shouldtake over a part <strong>of</strong> passengers, especially in trips for work purposes.From results <strong>of</strong> performed surveys resulted th<strong>at</strong> a passenger car isused more frequently for trips to <strong>the</strong> work than means <strong>of</strong> masspassenger transport.Assuming th<strong>at</strong> <strong>the</strong> share <strong>of</strong> leisure time <strong>of</strong> inhabitants willincrease it is possible to expect an increased interest in <strong>the</strong> passengercar use in trips for sport, recre<strong>at</strong>ional and holiday purposes.From <strong>the</strong> point <strong>of</strong> view <strong>of</strong> <strong>the</strong> st<strong>at</strong>e <strong>the</strong> passenger road transportrepresents an effective source <strong>of</strong> income to <strong>the</strong> st<strong>at</strong>e budgetinto which flow important portions which partially return for <strong>the</strong>road infrastructure development. High quality and large capacityroad infrastructure is inevitable to preserve <strong>the</strong> safe and continuousroad traffic. Its level reflects <strong>the</strong> passenger road transport degreein <strong>the</strong> countryThe passenger road transport from <strong>the</strong> social point <strong>of</strong> viewshould be also considered <strong>the</strong> factor stimul<strong>at</strong>ing activities in <strong>the</strong>region and cre<strong>at</strong>ion <strong>of</strong> new work opportunities, <strong>the</strong> educ<strong>at</strong>ion levelincrease as well as <strong>the</strong> orient<strong>at</strong>ion in achieving new knowledge inmodern technology.38 ● COMMUNICATIONS 3/2008


Modal split between <strong>the</strong> individual passenger transport and <strong>the</strong>public mass transport should be influenced by quality improvement<strong>of</strong> services provided mainly by urban mass transport. The individualpassenger transport may reasonably substitute <strong>the</strong> public masstransport under certain conditions.Finally, it should be mentioned th<strong>at</strong> opinions concerning passenger road transport trend dynamics and its growth limits in ourcountry may differ. However, in general, <strong>the</strong> number <strong>of</strong> passenger cars will no doubt increase in <strong>the</strong> next few decades.References[1] Research project: Development <strong>of</strong> <strong>the</strong> Individual Motoring in <strong>the</strong> Slovak Republic to 2020 (in Slovak), TRI Zilina, 1997[2] http://epp.eurost.ec.europa.eu[3] The Registr<strong>at</strong>ion <strong>of</strong> Motor <strong>vehicle</strong>s (in Slovak), The SR Presidency <strong>of</strong> <strong>the</strong> Traffic Police[4] The St<strong>at</strong>istics Year Book (in Slovak), The St<strong>at</strong>istical Office <strong>of</strong> <strong>the</strong> Slovak Republic[5] The Sale Survey <strong>of</strong> <strong>the</strong> Passenger Cars (in Slovak), The Automotive Industry Associ<strong>at</strong>ion <strong>of</strong> <strong>the</strong> Slovak Republic.COMMUNICATIONS 3/2008 ●39


Jozef Jandacka – Stefan Papucik – Vladimir Dekys – Richard Melicher *AN ANALYSIS OF AIR FLOW AT VARIOUS SPACING OF FANSON A PHYSICAL MODEL OF A ROAD TUNNELIn this article, <strong>the</strong> influence <strong>of</strong> a jet fan spacing in a longitudinal air conditioning system in a road tunnel on a physical model <strong>of</strong> <strong>the</strong>tunnel is analyzed. The analysis <strong>of</strong> air transport on a physical model with a length <strong>of</strong> 30 metres was accomplished for various combin<strong>at</strong>ions<strong>of</strong> <strong>the</strong> connection <strong>of</strong> 8 jet fans (parallel connection <strong>of</strong> 8 fans, combined connection <strong>of</strong> 2 4 parallel fans, combined connection (<strong>of</strong>) 4 2parallel fans and serial connection <strong>of</strong> 8 fans). From <strong>the</strong> analysis <strong>of</strong> measurement on <strong>the</strong> physical model follows wh<strong>at</strong> a big influence <strong>the</strong> fanspacing has on <strong>the</strong> speed pr<strong>of</strong>ile, which to a gre<strong>at</strong> extent influences air transport in <strong>the</strong> tunnel. Our contribution deals with <strong>the</strong> interpret<strong>at</strong>ion<strong>of</strong> vibr<strong>at</strong>ion d<strong>at</strong>a from <strong>the</strong> point <strong>of</strong> view <strong>of</strong> vibr<strong>at</strong>ion sources identific<strong>at</strong>ion. These sources are searched and evalu<strong>at</strong>ed from <strong>the</strong> measured d<strong>at</strong>ausing a frequency and phase spectrum.1. IntroductionNowadays, transport in connection with <strong>the</strong> construction <strong>of</strong>transport infrastructure is moved much more <strong>of</strong>ten through undergroundtunnels, especially in mountainous regions and town agglomer<strong>at</strong>ions.This brings, though, a whole variety <strong>of</strong> problems withitself, which need to be solved reliably. This concerns <strong>the</strong> securing<strong>of</strong> <strong>the</strong> required volume flow r<strong>at</strong>e <strong>of</strong> fresh air for ventil<strong>at</strong>ion <strong>at</strong> anoptimum energy demand <strong>of</strong> vent system, a suitable way <strong>of</strong> ventingexhaust emissions with a minimiz<strong>at</strong>ion <strong>of</strong> environmental pollutionin <strong>the</strong> surrounding <strong>of</strong> <strong>the</strong> tunnel and a minimiz<strong>at</strong>ion <strong>of</strong> securityrisks <strong>at</strong> collisions in <strong>the</strong> tunnel especially.A very <strong>of</strong>ten used way <strong>of</strong> venting <strong>the</strong> road tunnels is, especiallyin shorter tunnels, a longitudinal ventil<strong>at</strong>ion, Fig.1, [1], [4].From <strong>the</strong> point <strong>of</strong> view <strong>of</strong> <strong>the</strong> jet fan oper<strong>at</strong>ion safety, vibr<strong>at</strong>ionsplay an important role. Because <strong>of</strong> this, increased <strong>at</strong>tentionhas to be paid to <strong>the</strong>m. The measurements <strong>of</strong> <strong>the</strong> vibr<strong>at</strong>ions haveto be checked <strong>at</strong> least every 6 months and in <strong>the</strong> initial oper<strong>at</strong>ioneven more <strong>of</strong>ten. The vibr<strong>at</strong>ion degree in <strong>the</strong> horizontal and verticaldirections has to be checked <strong>at</strong> <strong>the</strong> measuring points which weremarked out during <strong>the</strong> first measurement. If <strong>the</strong> vibr<strong>at</strong>ion valuesare extremely different, <strong>the</strong> reasons <strong>of</strong> <strong>the</strong>ir origin<strong>at</strong>ion have to befound (e.g. dust on <strong>the</strong> fan blades). In case <strong>of</strong> a vibr<strong>at</strong>ion increase,it is necessary to correct <strong>the</strong> balance <strong>of</strong> <strong>the</strong> fan. The increase <strong>of</strong>vibr<strong>at</strong>ions can cause <strong>the</strong> destruction <strong>of</strong> <strong>the</strong> fan and a guaranteedexpir<strong>at</strong>ion <strong>of</strong> conditions. At higher vibr<strong>at</strong>ions it is recommendedto check <strong>the</strong> fan more <strong>of</strong>ten than within 6 months. The vibr<strong>at</strong>ionsduring an oper<strong>at</strong>ion should not exceed <strong>the</strong> value <strong>of</strong> 2.8 mm/s [5].In this article, <strong>the</strong> influence <strong>of</strong> a jet fan spacing <strong>at</strong> a longitudinalventil<strong>at</strong>ing system in <strong>the</strong> road tunnel on a physical model <strong>of</strong> <strong>the</strong>tunnel is analysed. This article also introduces <strong>the</strong> way <strong>of</strong> vibr<strong>at</strong>ionmeasurement and <strong>the</strong> analysis <strong>of</strong> measured values [7], [8].Fig. 1 Longitudinal ventil<strong>at</strong>ion with jet fansNowadays, based on <strong>the</strong> knowledge and consequences <strong>of</strong> firesin <strong>the</strong> tunnels in Western Europe, <strong>the</strong> increased <strong>at</strong>tention is paidto venting and to <strong>the</strong> design <strong>of</strong> ventil<strong>at</strong>ing systems <strong>of</strong> road tunnels,which are an essential part <strong>of</strong> fire safety assurance in <strong>the</strong> tunnel.Calcul<strong>at</strong>ions are still applied <strong>at</strong> designing ventil<strong>at</strong>ing systems,which are based on <strong>the</strong> <strong>the</strong>ory <strong>of</strong> one-dimensional flow and onexperiments on already existing road tunnels. In many cases, toanalyse some problems <strong>of</strong> ventil<strong>at</strong>ion in labor<strong>at</strong>ory conditions onphysical models has shown to be very suitable [2], [3].2. Physical modelThe physical model was realized in <strong>the</strong> r<strong>at</strong>io 1:10 to <strong>the</strong> realroad tunnel. This model is shown in Fig. 2. Its framework wascre<strong>at</strong>ed with 15 stainless tubes with a diameter <strong>of</strong> 0.8 m and a length<strong>of</strong> 2 m. The total length <strong>of</strong> <strong>the</strong> physical model was 30 m. Polystyrenewas placed <strong>at</strong> <strong>the</strong> air entrance <strong>of</strong> <strong>the</strong> model to avoid turbulencesin <strong>the</strong> vicinity <strong>of</strong> <strong>the</strong> air entrance. The polystyrene wasplaced <strong>at</strong> <strong>the</strong> air exit <strong>of</strong> <strong>the</strong> model as well.The measured values were recorded (temper<strong>at</strong>ure, pressure andspeed) into <strong>the</strong> d<strong>at</strong>a logger. The temper<strong>at</strong>ures and pressure were* Jozef Jandacka 1 , Stefan Papucik 1 , Vladimir Dekys 2 , Richard Melicher 21 Department <strong>of</strong> Power Engineering, Faculty <strong>of</strong> Mechanical Engineering, University <strong>of</strong> Zilina, Slovakia2 Department <strong>of</strong> Applied Mechanics, Faculty <strong>of</strong> Mechanical Engineering, University <strong>of</strong> Zilina, Slovakia, E-mail: Jozef.Jandacka@fstroj.uniza.sk40 ● COMMUNICATIONS 3/2008


measured 60 cm from <strong>the</strong> edge <strong>at</strong> <strong>the</strong> entrance and <strong>the</strong> exit <strong>of</strong> <strong>the</strong>model to record <strong>the</strong> steady values <strong>of</strong> air flow. The speed was measuredwith a propeller-type flow meter <strong>at</strong> three places, Fig. 3. Themeasurement place A was situ<strong>at</strong>ed 30 cm from <strong>the</strong> model entrance,place B was 15 m from <strong>the</strong> model entrance and place C place was30 cm from <strong>the</strong> model exit. In each section, <strong>the</strong> speed was measured<strong>at</strong> 24 points in a horizontal section according to Fig. 3.The analysis <strong>of</strong> air transport on <strong>the</strong> physical model was accomplishedfor various spacing <strong>of</strong> <strong>the</strong> 8 fans. All <strong>the</strong> fans were <strong>of</strong> <strong>the</strong>same type: Turbo 100 produced by Dospel Company. The fandiameter in <strong>the</strong> model was 100 mm, and it supplied 160 m 3 .hod-1 <strong>of</strong> air <strong>at</strong> <strong>the</strong> oper<strong>at</strong>ing speed <strong>of</strong> 2500 min 1 . The following vari<strong>at</strong>ions<strong>of</strong> <strong>the</strong> fan positions were measured:a) Parallel connection <strong>of</strong> 8 fans, connected next to each o<strong>the</strong>r,<strong>at</strong> a distance <strong>of</strong> 1.5 m from <strong>the</strong> model entrance (Fig. 4).b) Combined connection <strong>of</strong> 2 4 parallel fans, <strong>at</strong> a distance <strong>of</strong>1.5 m from <strong>the</strong> model entrance and model exit (Fig. 5).c) Combined connection <strong>of</strong> 4 2 parallel fans, <strong>at</strong> a distance <strong>of</strong>1.5 m from <strong>the</strong> model entrance and model exit (1st pair <strong>of</strong>fans) and <strong>the</strong> 2nd pair <strong>of</strong> fans <strong>at</strong> a distance <strong>of</strong> 2 m from <strong>the</strong>1st pair (Fig. 6).d) Serial connection <strong>of</strong> 8 fans, where <strong>the</strong> 1st fan is placed 1.5 mfrom <strong>the</strong> model entrance and <strong>the</strong> next fans are placed 2 mfrom <strong>the</strong> previous fan (Fig. 7).Fig. 4 Parallel connection <strong>of</strong> 8 fans, variant aFig. 5 Combined connection <strong>of</strong> 2 4 parallel fans, variant bFig. 6 Combined connection <strong>of</strong> 4 2 parallel fans, variant cFig. 7 Serial connection <strong>of</strong> 8 fans, variant d3. Analysis <strong>of</strong> measured resultsFig. 2 The physical model <strong>of</strong> a road tunnelFig. 3 The scheme <strong>of</strong> measuring points for speed measuringIn graphs 1 to 4 are introduced measured and evalu<strong>at</strong>ed speedpr<strong>of</strong>iles <strong>of</strong> <strong>the</strong> physical model <strong>of</strong> <strong>the</strong> road tunnel <strong>at</strong> measuringplaces A, B, and C in a horizontal direction (see Fig. 3). From <strong>the</strong>presented graphs it can be seen th<strong>at</strong> <strong>the</strong> speed pr<strong>of</strong>ile <strong>at</strong> place A isapproxim<strong>at</strong>ely <strong>the</strong> same <strong>at</strong> all variants <strong>of</strong> fan spacing in <strong>the</strong> roadtunnel model, which implies th<strong>at</strong> various fan spacing has no cardinaleffect on <strong>the</strong> speed pr<strong>of</strong>ile <strong>at</strong> <strong>the</strong> air entrance to <strong>the</strong> physicalmodel <strong>of</strong> <strong>the</strong> tunnel. By <strong>the</strong> parallel connection <strong>of</strong> <strong>the</strong> 8 fans,graph 1, <strong>the</strong> processes <strong>of</strong> <strong>the</strong> speed pr<strong>of</strong>iles <strong>at</strong> <strong>the</strong> measuring placesB and C are approxim<strong>at</strong>ely <strong>the</strong> same. The reason for this can beseen in <strong>the</strong> stabilis<strong>at</strong>ion <strong>of</strong> air flow. In graph 2 , by <strong>the</strong> connection<strong>of</strong> 2 4 parallel fans, <strong>the</strong> speed pr<strong>of</strong>ile measured <strong>at</strong> place B is stabilized,but <strong>the</strong> speed pr<strong>of</strong>ile <strong>at</strong> place C has a decreasing trend in<strong>the</strong> direction <strong>of</strong> <strong>the</strong> lower part <strong>of</strong> <strong>the</strong> tunnel model. This effect canbe explained by <strong>the</strong> spacing <strong>of</strong> 4 parallel fans very close to <strong>the</strong>place <strong>of</strong> measuring. The fan sucks in air through its paddle <strong>wheel</strong>,which leads to <strong>the</strong> increase <strong>of</strong> air flow speed in <strong>the</strong> upper part <strong>of</strong><strong>the</strong> tunnel model. The air in <strong>the</strong> lower part <strong>of</strong> <strong>the</strong> tunnel model isflowing under <strong>the</strong> influence <strong>of</strong> air <strong>moment</strong>um, which is cre<strong>at</strong>ed by<strong>the</strong> jet fan. In <strong>the</strong> case <strong>of</strong> <strong>the</strong> connection <strong>of</strong> 4 2 parallel fans, <strong>the</strong>measured speed pr<strong>of</strong>ile <strong>at</strong> place C is steady; however, <strong>the</strong> speedpr<strong>of</strong>iles <strong>at</strong> place A and C change, which is again affected by <strong>the</strong>COMMUNICATIONS 3/2008 ●41


spacing <strong>of</strong> <strong>the</strong> fan from <strong>the</strong> measuring place. The air velocity fields<strong>at</strong> a serial fan connection are introduced in graph 4, where <strong>the</strong>influence <strong>of</strong> fan spacing on <strong>the</strong> measured place can be seen.From <strong>the</strong> measured air velocity fields were calcul<strong>at</strong>ed averagespeeds in <strong>the</strong> particular places <strong>of</strong> measuring. For each variant <strong>of</strong>fan combin<strong>at</strong>ion on <strong>the</strong> physical model and for each particularplace we got <strong>the</strong> following average values <strong>of</strong> speed (vstr):Variant a) measuring place A: v str 1.80 ms 1 , measuring placeB: v str 1.43 ms 1 , measuring place C: v str 1.44 ms 1 ,Variant b) measuring place A: v str 1.55 ms 1 , measuring placeB: v str 1.23 ms 1 , measuring place C: v str 1.64 ms 1 ,Variant c) measuring place A: v str 1.42 ms 1 , measuring placeB: v str 1.16 ms 1 , measuring place C: v str 1.10 ms 1 ,Variant d) measuring place A: v str 1.62 ms 1 , measuring placeB: v str 1.40 ms 1 , measuring place C: v str 1.36 ms 1 ,Graph 1 Measured speeds <strong>at</strong> parallel fan connectionGraph 2 Measured speeds <strong>at</strong> 2 4 parallel fan connectionGraph 3 Measured speeds <strong>at</strong> 4 2 parallel fan connection42 ● COMMUNICATIONS 3/2008


Graph 4 Measured speeds <strong>at</strong> serial fan connection4. Vibr<strong>at</strong>ion measurement <strong>of</strong> jet fansand <strong>the</strong>ir analysis.An important requirement placed on a jet fan is also its abilityto ensure <strong>the</strong> required immedi<strong>at</strong>e ventil<strong>at</strong>ion <strong>of</strong> <strong>the</strong> road tunnel.When this requirement is not s<strong>at</strong>isfied (because <strong>of</strong> <strong>the</strong> fan breakdown),<strong>the</strong> consequences can be f<strong>at</strong>al. The reliability and availabilityare <strong>the</strong>n essential properties <strong>of</strong> this object [5].The preventive maintenance can be seen as a rel<strong>at</strong>ively simpletool for increasing trouble-free oper<strong>at</strong>ion and availability, using <strong>the</strong>inform<strong>at</strong>ion about <strong>the</strong> object condition, for example, by <strong>the</strong> measurement<strong>of</strong> its vibr<strong>at</strong>ions.This maintenance str<strong>at</strong>egy is an acceptable solution till <strong>the</strong>total cost <strong>of</strong> maintenance is not very high for <strong>the</strong> oper<strong>at</strong>ing organiz<strong>at</strong>ionand <strong>the</strong>y do not need to predic<strong>at</strong>e a fault condition <strong>of</strong> <strong>the</strong>mechanism. However, <strong>the</strong> procedures <strong>of</strong> vibr<strong>at</strong>ion diagnostics areable to provide d<strong>at</strong>a for prediction as well as inform<strong>at</strong>ion for proactivemaintenance (on <strong>the</strong> base <strong>of</strong> which <strong>the</strong> reasons <strong>of</strong> failuresare detected). Because <strong>of</strong> this reason, it is essential to deal withvibr<strong>at</strong>ion diagnostics <strong>of</strong> fans. The sources <strong>of</strong> vibr<strong>at</strong>ion for fans canbe a rotor unbalance (it is indic<strong>at</strong>ed by a high vibr<strong>at</strong>ion <strong>at</strong> 1RPM(rot<strong>at</strong>ion per minute) in <strong>the</strong> frequency spectrum), misalignment(angularity or <strong>of</strong>f<strong>set</strong>) on <strong>the</strong> interconnection between <strong>the</strong> driverand <strong>the</strong> fan (with a high axial or radial vibr<strong>at</strong>ion in spectrum onboth 1RPM and 2RPM and 180° out-<strong>of</strong>-phase across <strong>the</strong> coupling),failure <strong>of</strong> bearings (detectable by significant peaks in spectrums<strong>at</strong> <strong>the</strong> bearing defect frequencies), or hydrodynamic processescaused by an unequal gap between <strong>the</strong> impeller and <strong>the</strong> st<strong>at</strong>or <strong>of</strong><strong>the</strong> fan (identifiable on <strong>the</strong> blade frequency <strong>of</strong> <strong>the</strong> machine) [6].An electro motor is a source <strong>of</strong> vibr<strong>at</strong>ion, too – st<strong>at</strong>or eccentricity,short-circuited insul<strong>at</strong>ion and loose iron (st<strong>at</strong>or problemsbecome evident from high vibr<strong>at</strong>ion <strong>at</strong> 2 line frequency in spectrum),eccentricity <strong>of</strong> rotor (with side-bands with interval <strong>of</strong> polefrequency), broken or cracked rotor bars or shorting rings (presence<strong>of</strong> rotor bar frequency), phase problems – loosening <strong>of</strong> connectors(side-bands with interval <strong>of</strong> 1/3 <strong>of</strong> <strong>the</strong> network frequency),etc. The properties <strong>of</strong> <strong>the</strong> framework are important, too, for exampleits mechanical looseness (multiples <strong>of</strong> <strong>the</strong> speed frequency inspectrum) or excit<strong>at</strong>ion <strong>of</strong> its n<strong>at</strong>ural frequency.In <strong>the</strong> case <strong>of</strong> fans with a gearbox to <strong>the</strong> source <strong>of</strong> vibr<strong>at</strong>ionsbelong also meshing spur gears with considerable amplitudes ongear frequencies, <strong>the</strong>ir multiples and with <strong>the</strong>ir side-bands in <strong>the</strong>spectrums.In Fig. 8 is depicted <strong>the</strong> frequency spectrum <strong>of</strong> oscill<strong>at</strong>ingspeed with one dominant amplitude on <strong>the</strong> speed frequency <strong>of</strong> <strong>the</strong>fan which is typical for sign<strong>at</strong>ure <strong>of</strong> <strong>the</strong> rotor unbalance <strong>of</strong> <strong>the</strong> fan.The Faculty <strong>of</strong> Mechanical Engineering <strong>of</strong> <strong>the</strong> University <strong>of</strong>Zilina deals also with <strong>the</strong>ses problems, and we are able to <strong>of</strong>fer ourpartners <strong>the</strong> solution <strong>of</strong> vibr<strong>at</strong>ion measurements on fans. It doesnot have to be only <strong>the</strong> safety system switching <strong>of</strong>f <strong>the</strong> fan afterreaching a certain level <strong>of</strong> vibr<strong>at</strong>ions, but also <strong>the</strong> on-line, respectivelyon-line monitoring and analysis <strong>of</strong> <strong>the</strong> measured d<strong>at</strong>a from<strong>the</strong> point <strong>of</strong> view <strong>of</strong> predictive and pro – active maintenance.Fig. 8 Spectrum <strong>of</strong> oscill<strong>at</strong>ing speed with one dominant peak <strong>at</strong> 38 Hz,(speed frequency), demonstr<strong>at</strong>ion <strong>of</strong> <strong>the</strong> rotor unbalance.COMMUNICATIONS 3/2008 ●43


5. ConclusionFrom <strong>the</strong> results presented above follows th<strong>at</strong> <strong>the</strong> serial connection<strong>of</strong> 8 fans is <strong>the</strong> best option. The reasons for this are highermedium speeds as well as uniformities <strong>of</strong> <strong>the</strong> flow pr<strong>of</strong>ile in <strong>the</strong>cross section <strong>of</strong> <strong>the</strong> tunnel. From <strong>the</strong> introduced analysis <strong>of</strong> measurementson a physical model follows wh<strong>at</strong> a big influence <strong>the</strong>fan spacing has on <strong>the</strong> speed pr<strong>of</strong>ile, which to a gre<strong>at</strong> extent influences<strong>the</strong> air transport in <strong>the</strong> tunnel. There is a real assumptionth<strong>at</strong> <strong>the</strong> spacing <strong>of</strong> fans on <strong>the</strong> course <strong>of</strong> <strong>the</strong> speed pr<strong>of</strong>iles hassimilar influences on <strong>the</strong> spacing <strong>of</strong> jet fans in real constructions<strong>of</strong> road tunnels.References[1] MALCHO, M.; JANDACKA, J.; PAPUCIK, S.; KAPJOR, A.; HORVATH, Z.: Effect Slewing Jet Fan on Effectiveness Transport Airin Road Tunnel with Longitudinal Ventil<strong>at</strong>ion, XXXVI. Setkani k<strong>at</strong>eder mechaniky tekutin a termomechaniky; Herbertov, 2007, p. 35;ISBN 80-86786-09-9.[2] HORVATH, Z., JANDACKA, J., MALCHO, M.: Extension <strong>of</strong> Fire in Tunel by Motor Vehicle Accident, Proc. <strong>of</strong> Intern. Conference:Experimental fluid mechanics 2006, Liberec, Czech Republic, p. 79, ISBN 80-7372-141-4.[3] JANDACKA, J., MALCHO, M., HORVATH, Z., KAPUSTA, J.: Longitudinal Ventil<strong>at</strong>ion Road Tunnel with Fire, Zbornik prednasokz 10. konferencie: Vetranie a klim<strong>at</strong>izacia 2006; Strbske Pleso, p. 87, (SSTP 0618), ISBN 80-89216-07-2.[4] JANDACKA, J., MALCHO, M., HORVATH, Z., KAPUSTA, J.: Simul<strong>at</strong>ion Fire on Road Tunnel in Various Time Bracing Ventil<strong>at</strong>ingSystem Tunnel, XV. Medzinarodna vedecka konferencia: Aplikacia experimentalnych a numerickych metod v mechaniketekutin, Strecno, 2006, p. 297, ISBN 80-8070-533-X.[5] DEKYS, V., SAPIETOVA, A., VASKO, M.: Condition Monitoring <strong>of</strong> Gearboxes (in Slovak), Acta Mechanica Slovaca, Optimalizaciamechanickych sustav a zariadeni, 4-A/2007, pp. 67–74.[6] SILVA, C. W.: Vibr<strong>at</strong>ion, Fundametals and Practice, CRC Press LLC, 2000.[7] MOBLEY, R. K.: Root Cause Failure Analysis, Newnes 1999.[8] BERRY, J. E.: Intensive Vibr<strong>at</strong>ion Diagnostics, SKF Condition Monitoring, Zaltbommel, 1985. Technical Associ<strong>at</strong>es <strong>of</strong> Charlotte,1985.44 ● COMMUNICATIONS 3/2008


REVIEWMiloslav Klinko – Juraj Grencik *TILTING BODY VEHICLES ON SLOVAK RAILWAYS – POTENTIALFOR USE AND PARAMETERS TO BE CONSIDEREDCompetition between various transport modes has been a characteristic fe<strong>at</strong>ure <strong>of</strong> <strong>the</strong> last decades not only in <strong>the</strong> world yet in Slovakia.Passenger rail transport proves to be most suitable for medium distances with high traffic intensity. In Slovakia this is valid first <strong>of</strong> all forBr<strong>at</strong>islava – Zilina – Kosice line. One solution for increasing travel speed and ride comfort is using <strong>the</strong> tilting body trains. In <strong>the</strong> paper <strong>the</strong>oreticalconsider<strong>at</strong>ions for use <strong>of</strong> tilting body <strong>vehicle</strong>s are presented. On <strong>the</strong> example <strong>of</strong> Zilina – Kosice <strong>railway</strong> line we show a potential forremarkable reduction <strong>of</strong> travel time which is <strong>the</strong> most expected benefit <strong>of</strong> <strong>the</strong> new train technology, But we present also parameters whichshould be considered when thinking about use <strong>of</strong> new technology.1. IntroductionCompetition between various transport modes has been a characteristicfe<strong>at</strong>ure <strong>of</strong> <strong>the</strong> last decades not only in <strong>the</strong> world yet inSlovakia. Road and air transport are continually growing while<strong>railway</strong>s seem to be declining. However, <strong>railway</strong> transport is alwaysproclaimed to be a more environmental friendly and more efficientthan <strong>the</strong> o<strong>the</strong>r ones, thus giving <strong>at</strong> least verbal support. But<strong>railway</strong> transport itself has to prove its benefits showing in realitywhich parameters are better comparing with o<strong>the</strong>r modes as wellelimin<strong>at</strong>e its weaknesses. Passenger rail transport proves to bemost suitable for medium distances with high traffic intensity. InSlovakia this is valid first <strong>of</strong> all for Br<strong>at</strong>islava – Zilina – Kosiceline, but o<strong>the</strong>r lines, especially connections to <strong>the</strong> Czech Republicare <strong>of</strong> interest as well.In sixties <strong>of</strong> <strong>the</strong> 20 th century most <strong>of</strong> leading <strong>railway</strong>s in <strong>the</strong>world realised th<strong>at</strong> if <strong>the</strong> <strong>railway</strong> traffic should withhold in competitionwith o<strong>the</strong>r traffic modes than passenger travel times shouldhave been reduced substantially.High-speed <strong>railway</strong> track can not be a universal solution forincreasing speed. In a country with high popul<strong>at</strong>ion or mountainousterrain, or where government is not much in favour <strong>of</strong> investmentsinto a new <strong>railway</strong> infrastructure, <strong>railway</strong> management haveto find ano<strong>the</strong>r way for ensuring <strong>the</strong> competitive travel speed.As an example <strong>of</strong> market pressure is th<strong>at</strong> in this situ<strong>at</strong>ion<strong>vehicle</strong> designers were challenged to solve somehow <strong>the</strong> constraintsgiven by conventional technology, geographical and financial conditions.In leading countries <strong>of</strong> Europe, North America and Japan<strong>the</strong>se problems were solved by development <strong>of</strong> a system usingtilting <strong>vehicle</strong> bodies th<strong>at</strong> enabled <strong>the</strong> train running in curves <strong>at</strong>a higher speed.2. Theoretical background <strong>of</strong> body tiltingand running in curveAccording to <strong>the</strong> second Newton’s law, a body continues inits movement until external force is acting on it. As a consequence<strong>of</strong> external force action, a body will change its movement velocityand degree <strong>of</strong> this change is called acceler<strong>at</strong>ion.Passenger trains normally have acceler<strong>at</strong>ion/ deceler<strong>at</strong>ion upto about 7 – 9 % gravity force (9 % g). This is given by adhesionacting between <strong>the</strong> <strong>wheel</strong> and rail.For acceptable acceler<strong>at</strong>ion with respect to passenger comfort<strong>the</strong> maximum <strong>of</strong> something less than 10 % g is considered.While instead <strong>of</strong> acceler<strong>at</strong>ion/deceler<strong>at</strong>ion on a straight tracka train is turning into curve, <strong>the</strong> Newton law is still valid. Passengerbodies tend to continue in a straight line while <strong>the</strong> effect <strong>of</strong>transversal forces acceler<strong>at</strong>es <strong>the</strong>m in a new direction.This “transversal acceler<strong>at</strong>ion” is more perceived by passengersthan deceler<strong>at</strong>ion or acceler<strong>at</strong>ion r<strong>at</strong>e. It occurs very frequentlyon a line with curves and its magnitude depends on <strong>the</strong> trackshape and train velocity.Same as acceler<strong>at</strong>ion, <strong>the</strong> transversal acceler<strong>at</strong>ion can beexpressed in % g. Normally <strong>the</strong> transversal acceler<strong>at</strong>ion maximumvalue is 7 % g, which roughly corresponds to <strong>the</strong> train brakingfrom speed <strong>of</strong> 160 km/h. In Switzerland, <strong>the</strong> country with <strong>railway</strong>* Miloslav Klinko 1 , Juraj Grencik 21 Department for Organiz<strong>at</strong>ion and Management, General-director<strong>at</strong>e ZSR, Br<strong>at</strong>islava, Slovakia, E-mail: Klinko.Miloslav@zsr.sk2 Department <strong>of</strong> Transport and Oper<strong>at</strong>ing Technics, Faculty <strong>of</strong> Mechanical Engineering, University <strong>of</strong> Zilina, SlovakiaCOMMUNICATIONS 3/2008 ●45


REVIEWlines with numerous curves <strong>the</strong> maximum 9 % g is permitted, inFrance 8.6 % g, exceptionally, when for example, one curve shouldremarkably affect <strong>the</strong> speed, 12 % g is accepted.Civil engineers can compens<strong>at</strong>e <strong>the</strong> action <strong>of</strong> transversal acceler<strong>at</strong>ionby superelev<strong>at</strong>ion <strong>of</strong> <strong>the</strong> outer rail – cant <strong>of</strong> track. Duringrunning in a curve <strong>the</strong> combin<strong>at</strong>ion (resultant) <strong>of</strong> transversal forceand body mass acts in a direction slanted in a certain angle rel<strong>at</strong>iveto <strong>the</strong> vertical. The balance appar<strong>at</strong>us in <strong>the</strong> human ear sensesthis angular tension as turning.The superelev<strong>at</strong>ion was traditionally measured in inches andfrom Stephenson’s era (on BR tracks with a standard rail gauge)one inch (25 mm) <strong>of</strong> superelev<strong>at</strong>ion corresponds to one degree <strong>of</strong>slant.On a <strong>railway</strong> line with a combined traffic, size <strong>of</strong> superelev<strong>at</strong>ionin a certain curve is always a compromise. Too many slowtrains on <strong>the</strong> lines cause an increased load on <strong>the</strong> internal rail andresulting increased wear <strong>of</strong> <strong>the</strong> <strong>wheel</strong>s and rails, for speed trains<strong>the</strong> superelev<strong>at</strong>ion is limited by passenger comfort.We should bear in mind th<strong>at</strong> certain transversal acceler<strong>at</strong>ionis acceptable and trains are allowed to run in curves <strong>at</strong> a higherspeed than corresponds to <strong>the</strong> balanced (compens<strong>at</strong>ed) acceler<strong>at</strong>ion.This uncompens<strong>at</strong>ed acceler<strong>at</strong>ion is known as cant deficiency.The maximum speed <strong>at</strong> which <strong>the</strong> train is allowed to run ina curve is given by cant deficiency plus maximum superelev<strong>at</strong>ion(cant) for freight transport. Danger <strong>of</strong> overturning caused bytransversal forces as a limiting factor need no be considered asthis would happen <strong>at</strong> more than 20 degrees <strong>of</strong> cant (depending ona <strong>vehicle</strong> design).Ano<strong>the</strong>r important factor is <strong>the</strong> r<strong>at</strong>e <strong>of</strong> change <strong>of</strong> <strong>the</strong> <strong>vehicle</strong>tilt as this has gre<strong>at</strong> effect on passenger comfort. Tilting effectscan be measured in degrees per second. Experimental evalu<strong>at</strong>ion<strong>of</strong> how passengers perceive <strong>the</strong> tilting showed th<strong>at</strong> <strong>at</strong> a r<strong>at</strong>e <strong>of</strong> 5–6degrees per second <strong>the</strong>y begin perceive <strong>the</strong> tilting.Very critical is <strong>the</strong> acting <strong>of</strong> tilt in opposite curves when traingoes from a maximum superelev<strong>at</strong>ion/tilt on one side to a maximumon <strong>the</strong> opposite side. The British experimental tilting train APTwas able to change from <strong>the</strong> tilt <strong>of</strong> 9 degrees and cant <strong>of</strong> 4.5 degreeon one side to <strong>the</strong> similar values on <strong>the</strong> opposite side within threeseconds, which was about 9 degrees per second. This has disturbingeffects even in a sitting position. When standing and <strong>the</strong> rot<strong>at</strong>ionaxle is in <strong>the</strong> level <strong>of</strong> knees, this can easily cause a person t<strong>of</strong>all down.Wh<strong>at</strong> is necessary is to somehow register tilting in advance.A simple and effective solution is placing <strong>the</strong> accelerometer on<strong>the</strong> first bogie <strong>of</strong> a train and to transmit <strong>the</strong> signals form <strong>the</strong>realong <strong>the</strong> train with a corresponding delay for individual <strong>vehicle</strong>sin <strong>the</strong> train. In this way each <strong>vehicle</strong> receives signal on tilt when itcomes to <strong>the</strong> beginning <strong>of</strong> a transient curve. This solution is knownas a preliminary registr<strong>at</strong>ion and has also an advantage th<strong>at</strong> itenables reducing a number <strong>of</strong> processors and thus increases alsoreliability <strong>of</strong> <strong>the</strong> whole system. But <strong>the</strong> first <strong>vehicle</strong> still suffersfrom delay.Fi<strong>at</strong> came probably with <strong>the</strong> best elabor<strong>at</strong>ed solution: besides<strong>the</strong> accelerometer <strong>the</strong> first bogie was equipped with a sensitivegyroscope and <strong>the</strong> appar<strong>at</strong>us for measurement <strong>of</strong> rail cant.This gyroscope can register already <strong>the</strong> beginning <strong>of</strong> cant ona transient section and transmits <strong>the</strong> signal to <strong>the</strong> tilting mechanism.It will start working earlier than <strong>the</strong> transversal acceler<strong>at</strong>ionreaches <strong>the</strong> value th<strong>at</strong> is registered by <strong>the</strong> accelerometer.For trains <strong>of</strong> series X – 2000 developed by a Swedish companyABB, <strong>the</strong> solution is partly different: an instantaneous slant angleis measured for each <strong>vehicle</strong>. When a <strong>vehicle</strong> enters a section witha transient curve, <strong>the</strong> tilt angle is continually increasing towards<strong>the</strong> next <strong>vehicle</strong>. The signal th<strong>at</strong> registers this difference <strong>of</strong> tilts isadded to <strong>the</strong> signal transmitted from <strong>the</strong> accelerometer from <strong>the</strong>first <strong>vehicle</strong>. This system improves tilt control and enables moreintensive action <strong>of</strong> <strong>the</strong> signal from <strong>the</strong> accelerometer. It is importantfor prevention <strong>of</strong> random transversal acceler<strong>at</strong>ions, e.g. ina straight track or on imperfect track conditions.In <strong>the</strong> era <strong>of</strong> <strong>the</strong> first series <strong>of</strong> APT-P and similar trains problems<strong>of</strong> passengers were connected with an extremely high compens<strong>at</strong>ion<strong>of</strong> transversal acceler<strong>at</strong>ion. Soon it became evident th<strong>at</strong>tilting is too perfect. A standing position or walking is possiblethanks to <strong>the</strong> processing <strong>of</strong> inform<strong>at</strong>ion in human brains. Duringsitting in a train with a perfect compens<strong>at</strong>ion <strong>of</strong> transversal acceler<strong>at</strong>ion,signals from <strong>the</strong> inner ear say th<strong>at</strong> <strong>the</strong> body is in erectedposition. When one looks out <strong>of</strong> <strong>the</strong> window, visual inform<strong>at</strong>iondoes not correspond to this inform<strong>at</strong>ion as <strong>the</strong> train is slanted by10 %. In th<strong>at</strong> <strong>moment</strong> <strong>the</strong> brain registers stability problems and insensitive individuals a phenomenon called nausea occurs, whichmay cause vomiting.BR denied th<strong>at</strong> this “nausea from tilt” would be any problem.But o<strong>the</strong>r <strong>railway</strong>s found quite a simple answer: instead <strong>of</strong> <strong>the</strong>perfect compens<strong>at</strong>ion <strong>the</strong>y introduced a tilting system compens<strong>at</strong>ingonly 70 % <strong>of</strong> cant deficit, so <strong>the</strong> remaining transversal acceler<strong>at</strong>ionacting on passengers induced a feeling th<strong>at</strong> <strong>the</strong>y are movingin curve. As a consequence, <strong>the</strong> maximum tilt angle can be reducedand standard <strong>of</strong> manufacturers stabilised <strong>at</strong> 8 % – with exception<strong>of</strong> Pendolino system, in which ETR train is adapted for a tilt <strong>of</strong> 10degrees plus 8 % g <strong>of</strong> an uncompens<strong>at</strong>ed transversal acceler<strong>at</strong>ion– and to 4.8 % cant deficiency.3. Calcul<strong>at</strong>ion <strong>of</strong> velocity <strong>of</strong> tilting body trainFor speed trains so called unbalanced acceler<strong>at</strong>ion a n is beingused, which corresponds to <strong>the</strong> cant deficiency70a g a . m.s 2n = $ ( n = 0457150046 ● COMMUNICATIONS 3/2008


REVIEWThe basic formula for calcul<strong>at</strong>ion <strong>of</strong> a maximum permittedvelocity <strong>the</strong> following formula is used:V =r$ _ pm+pnpi11.8(km.h 1 )wherer – curve radius (m)p m – maximum superelev<strong>at</strong>ion (mm)p np – cant deficiency (mm)A fur<strong>the</strong>r increase <strong>of</strong> speed without reducing <strong>the</strong> passengerride comfort (a n 0,457m.s 2 ) can be gained by tilting <strong>the</strong> carbody inwards toward <strong>the</strong> curve by a certain angle τ, which representsan additional superelev<strong>at</strong>ion p d .(mm)wheree – <strong>wheel</strong><strong>set</strong>/rail contact distance (mm)We get <strong>the</strong> permissible velocity with <strong>the</strong> use <strong>of</strong> a tilted bodyrV = $ _ p (km.h 1 m+ pnp+pdi)11.8This is not a complete solution because <strong>the</strong> increase <strong>of</strong> velocitybesides balancing <strong>the</strong> centrifugal force effecting passengers,brings an increase <strong>of</strong> <strong>vehicle</strong> effects on <strong>the</strong> track, too. The <strong>vehicle</strong>forces acting in a curve on <strong>the</strong> track, th<strong>at</strong> is safety against derailmentand track stability, become a dominant criterion.Foreign <strong>railway</strong>s use <strong>the</strong> Proud’hom’s formulae when <strong>the</strong>yprepare oper<strong>at</strong>ion <strong>of</strong> tilting body <strong>vehicle</strong>s. These formulae givelimit <strong>of</strong> <strong>the</strong> maximum transversal force between <strong>the</strong> <strong>wheel</strong> andrail, which results in an unbalanced centrifugal acceler<strong>at</strong>ion <strong>of</strong> <strong>the</strong><strong>vehicle</strong> a vn 1.65 1.8 m.s 2 and only exceptionally a vn 2.0 m.s 2 .A part <strong>of</strong> <strong>the</strong> transversal compens<strong>at</strong>ed acceler<strong>at</strong>ion a vk is elimin<strong>at</strong>edby <strong>the</strong> rail superelev<strong>at</strong>ion p m , so <strong>the</strong> resulting transversalacceler<strong>at</strong>ion can be increased by this value. The maximum permissiblespeed <strong>of</strong> <strong>the</strong> tilting body <strong>vehicle</strong> will <strong>the</strong>n be:(km/h)wherea c – total transversal acceler<strong>at</strong>ion (m.s 2 )a vk – transversal compens<strong>at</strong>ed acceler<strong>at</strong>ion(m.s 2 )a c a vn a vk (m.s 2 )a vn – uncompens<strong>at</strong>ed acceler<strong>at</strong>ion according to Proud´hom’sformulae (m.s 2 )erpd = e$ tgxV = v $ 36 . = 36 . $ a $ radm dm cvkpm= $ ge(m.s 2 )– <strong>wheel</strong><strong>set</strong>/rail contact distance (mm)– curve diameter (m)Fur<strong>the</strong>r on we need to determine how a big angle <strong>of</strong> <strong>the</strong> bodytilt is needed.a c a vk a n a d (m.s 2 )wherea n – unbalanced acceler<strong>at</strong>ion (m.s 2 )a d a c a vk a n (m.s 2 )a d – additionally compens<strong>at</strong>ed acceler<strong>at</strong>ion (m.s 2 )p d – additional superelev<strong>at</strong>ion (mm)From <strong>the</strong> following formula we get <strong>the</strong> required angle <strong>of</strong> a bodytilt:The obtained d<strong>at</strong>a from <strong>the</strong> <strong>simul<strong>at</strong>ion</strong> <strong>of</strong> a train run are certainlyonly <strong>the</strong>oretical, but <strong>the</strong>y can provide a starting point forcomparison <strong>of</strong> various types <strong>of</strong> train <strong>set</strong>s and testing <strong>the</strong>ir para-adpdpd= $ e tg x = & xge4. Computer <strong>simul<strong>at</strong>ion</strong> <strong>of</strong> a train runOne <strong>of</strong> <strong>the</strong> most important steps in <strong>the</strong> decision process on<strong>the</strong> use <strong>of</strong> tilting body <strong>vehicle</strong>s is also a <strong>the</strong>oretical calcul<strong>at</strong>ion <strong>of</strong>run parameters on <strong>the</strong> proposed <strong>railway</strong> line section.For this calcul<strong>at</strong>ion we used a program “Train dynamics”.Parameters <strong>of</strong> <strong>the</strong> selected <strong>railway</strong> line section have to be inputinto <strong>the</strong> program.A) Input d<strong>at</strong>a <strong>of</strong> <strong>the</strong> program comprise:1. Parameters <strong>of</strong> a selected <strong>railway</strong> line section2. Type <strong>of</strong> locomotive (or traction <strong>vehicle</strong>)3. Type <strong>of</strong> train4. Complementary d<strong>at</strong>a:– Braking deceler<strong>at</strong>ion– Traction force limit– Limit <strong>of</strong> push force5. Specific d<strong>at</strong>a:– Integr<strong>at</strong>ion step– Minimum coasting speed– Specific he<strong>at</strong>ing power– Coefficient <strong>of</strong> rel<strong>at</strong>ive decrease <strong>of</strong> speed during coasting– Distance step for d<strong>at</strong>a outputB) Results <strong>of</strong> a sample calcul<strong>at</strong>ionAfter correctly performed calcul<strong>at</strong>ion we can show <strong>the</strong> resultsin <strong>the</strong> form <strong>of</strong> a table or diagrams. In <strong>the</strong> table, besides traveltime, <strong>the</strong> total energy consumption in kWh or diesel in litrescan be presented. For electric locomotive <strong>the</strong> consumption isgiven without consumption <strong>of</strong> auxiliary drives and he<strong>at</strong>ing.These items can be considered ei<strong>the</strong>r by a coefficient or byadditional calcul<strong>at</strong>ion.(°)COMMUNICATIONS 3/2008 ●47


REVIEWmeters from <strong>the</strong> point <strong>of</strong> view <strong>of</strong> <strong>the</strong>ir suitability for <strong>the</strong> selected<strong>railway</strong> line section.As an example <strong>of</strong> <strong>the</strong> train run <strong>simul<strong>at</strong>ion</strong> using <strong>the</strong> computerprogram “Train dynamics” we chose a <strong>railway</strong> line section Zilina– Kosice, as this section has a considerable number <strong>of</strong> curves withsmall radii. (We used <strong>the</strong> parameter 1/r; r – track curve radius).curves confirmed <strong>the</strong> results <strong>of</strong> simplified calcul<strong>at</strong>ions; although,<strong>the</strong> difference, according to a more precise calcul<strong>at</strong>ion, was a bitsmaller. Moreover, in <strong>the</strong>se calcul<strong>at</strong>ions we considered speed limitsin <strong>the</strong> same sections as <strong>the</strong>y are <strong>at</strong> present, yet we also used <strong>the</strong>oreticalspeed limits for each curve while certainly <strong>the</strong> maximumspeed <strong>of</strong> train ETR 470, which is 200 km/h, could not be exceeded.Selected calcul<strong>at</strong>ion results are in <strong>the</strong> following table.The diagram <strong>of</strong> a run diagram and energy consumption onKošice – Zilina line, <strong>the</strong>oretical sections (considering maximumpossible <strong>the</strong>oretical speed in each curve on <strong>the</strong> line) is presentedin <strong>the</strong> figure below:Fig. 1 Track curves on Kosice-Zilina lineFig. 2 Tilting body <strong>vehicle</strong>s – <strong>the</strong>oretical line sections(Kosice – Zilina line)We compared <strong>the</strong> train <strong>set</strong>s with corresponding weights:• Conventional – locomotive series 163, plus passenger cars <strong>of</strong>total weight <strong>of</strong> 400 t, totally 484 t.• With a tilting body – train-<strong>set</strong> series ETR 470, total weight <strong>of</strong>490 t, permanent power <strong>of</strong> 5880 kW, maximum traction force258 kNAlthough <strong>the</strong> power <strong>of</strong> locomotive series 163 is remarkablylower, for <strong>the</strong> maximum speed <strong>of</strong> 120 km/h currently used on given<strong>railway</strong> lines this locomotive is good enough. Calcul<strong>at</strong>ed traveltimes for <strong>the</strong> conventional locomotive-hauled train and Pendolinotrain <strong>set</strong> series ETR 470 on <strong>the</strong> lines with existing speed limits donot differ by more than 1% in favour <strong>of</strong> Pendolino, which is a negligibledifference. However, benefits from <strong>the</strong> increased speed inTable: Travel times and energy consumption on selected sectionsZilina –KosiceTrack sectionsexisting st<strong>at</strong>eTraveltime(min)Energyconsumption(kWh)Existing sectionsfor tilting body<strong>vehicle</strong>sTraveltime(min)Energyconsumption(kWh)Theoreticalsections fortilting body<strong>vehicle</strong>sTraveltime(min)Energyconsumption(kWh)163 + 400 t 154.1 2374 — — — —ETR 470 153.6 1626 110.7 1879 102.3 2776In case <strong>of</strong> <strong>the</strong>oretical speed limits for each curve increasedenergy consumption has remarkably gone up, as <strong>the</strong>re were frequentchanges in velocity (acceler<strong>at</strong>ion in <strong>the</strong> sections with a higherpermissible speed).5. Parameters effecting choice <strong>of</strong> a suitable rail <strong>vehicle</strong>In <strong>the</strong> decision process on suitability <strong>of</strong> <strong>the</strong> use <strong>of</strong> a selected<strong>railway</strong> <strong>vehicle</strong> type on a given <strong>railway</strong> line it is necessary to investig<strong>at</strong>enot only design parameters <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> but also o<strong>the</strong>rparameters concerning its oper<strong>at</strong>ion have to be considered as well.These parameters in principle can be divided into <strong>the</strong> followingc<strong>at</strong>egories:a) Technical parameters:– parameters <strong>of</strong> railroad tracks and buildings– parameters <strong>of</strong> interlocking systems– parameters <strong>of</strong> traction power supply and electrotechnicalequipmentb) Parameters <strong>of</strong> effects on environment railroad surroundingsc) Parameters <strong>of</strong> effect on passengersd) Economic parameters– Oper<strong>at</strong>ional and maintenance costs– Disposal costs– Costs for increasing quality and reliability– Competitiveness with o<strong>the</strong>r transport modes48 ● COMMUNICATIONS 3/2008


REVIEWTechnical parametersThese parameters are based on valid legisl<strong>at</strong>ion (regul<strong>at</strong>ions,standards,…) and mostly in a designing phase <strong>of</strong> a suitable type <strong>of</strong><strong>railway</strong> <strong>vehicle</strong> it is not possible to influence <strong>the</strong>se parameters as<strong>the</strong>ir change requires high investments for modific<strong>at</strong>ion <strong>of</strong> <strong>the</strong><strong>railway</strong> track and o<strong>the</strong>r connected technical facilities. Moreover,<strong>the</strong>se parameters directly affect <strong>the</strong> oper<strong>at</strong>ional safety <strong>of</strong> <strong>the</strong> rail<strong>vehicle</strong>.Parameters <strong>of</strong> effects on environment railroad surroundingsParameters <strong>of</strong> effects on environment railroad surroundingsare also given by valid legisl<strong>at</strong>ion but <strong>the</strong>y can be affected bya <strong>vehicle</strong> design and its maintenance system. The main parametersbelonging to this group are especially:– Noise emitted by <strong>the</strong> <strong>vehicle</strong>;– Influence on soil, w<strong>at</strong>er and air pollution.Parameters <strong>of</strong> effect on passengersThese parameters are most important from <strong>the</strong> point <strong>of</strong>meeting passenger needs. They concern namely:– Personal comfort during <strong>the</strong> train run– Speed <strong>of</strong> transport from place A to place B– Train ticket price– Traffic safetyEconomic parametersEconomic parameters are <strong>the</strong> most important for assessmentsuitability <strong>of</strong> <strong>the</strong> use <strong>of</strong> a <strong>railway</strong> <strong>vehicle</strong> on <strong>the</strong> given <strong>railway</strong> lineas oper<strong>at</strong>ion should be economically effective. Individual types <strong>of</strong>costs rel<strong>at</strong>ed to <strong>the</strong> rail <strong>vehicle</strong> oper<strong>at</strong>ion can be affected alreadyduring <strong>the</strong> design phase.When considering <strong>the</strong> individual parameters with <strong>the</strong> aim <strong>of</strong>choice <strong>of</strong> <strong>the</strong> most suitable type for a given <strong>railway</strong> line it is goodnot to focus only on one parameter th<strong>at</strong> looks like <strong>the</strong> most important,but all <strong>the</strong> parameters should be evalu<strong>at</strong>ed and considered in<strong>the</strong>ir mutual connection. This is valid also for usage <strong>of</strong> tilting body<strong>vehicle</strong>s when one important parameter – an increased train velocityshould be considered with all <strong>the</strong> induced requirements foroper<strong>at</strong>ion <strong>of</strong> this train technology.References[1] SIMCO, J: Employment Tilting Body Trains – Altern<strong>at</strong>ive for Raising Speed in Railway Transport (in Slovak), Horizonty dopravy3/2002, Zilina, p. 1–8[2] SIMAN, P, PETRAS, J.: Programme „SP Dynamika“ (in Czech), Computer program, Praha, 1998[3] GRENCIK, J., KLINKO, M.: Potential Reduction <strong>of</strong> Travel Times and Energy Consumption <strong>of</strong> Tilting Body Vehicles on ZSR, Communic<strong>at</strong>ions– Scientific Letters <strong>of</strong> <strong>the</strong> University <strong>of</strong> Zilina, 1/2001, EDIS Žilina, p. 88–97.COMMUNICATIONS 3/2008 ●49


REVIEWBojan Cene – Aleksandar Radosavljevic – Branislav Gavrilovic *DRIVING ENERGY CONSUMPTION OF ELECTRICTRACTION VEHICLESThe paper presents some <strong>simul<strong>at</strong>ion</strong> and tests results <strong>of</strong> driving energy consumption <strong>of</strong> electric traction <strong>vehicle</strong>s both <strong>at</strong> Serbian andSlovenian Railways. On Serbian Railways <strong>the</strong>re are two series <strong>of</strong> electric locomotives: four-axles 441 series made in former Yugoslavia underlicense <strong>of</strong> ASEA (Sweden) and six-axles 461 series manufactured in Romania in co-oper<strong>at</strong>ion with ASEA. On Slovenian <strong>railway</strong>s are fourseries <strong>of</strong> electrical locomotives oper<strong>at</strong>ing: <strong>the</strong> Italian two axles locomotive series 342, <strong>the</strong> Italian six axles locomotive series 362, <strong>the</strong> Frenchsix axles locomotive series 363, and <strong>the</strong> three-system four axles Siemens locomotive series 541.Keywords: energy consumption, electric traction <strong>vehicle</strong>s, Slovene <strong>railway</strong>s, Serbian <strong>railway</strong>s, GPS1. IntroductionThe problem <strong>of</strong> driving energy savings during train tractionbecame very significant during <strong>the</strong> energetic crisis and <strong>the</strong>reforeall foreign <strong>railway</strong>s have conducted wide researches in order to finda solution <strong>of</strong> this problem. Apart from technical improvements <strong>of</strong>tractive and hauled stock <strong>the</strong>se researches have also been conductedin <strong>the</strong> field <strong>of</strong> s<strong>of</strong>tware development for finding optimalenergetic train running trajectories. Considering <strong>the</strong> fact th<strong>at</strong> <strong>the</strong>most <strong>of</strong> <strong>the</strong> driving energy r<strong>at</strong>ionaliz<strong>at</strong>ion possibilities have alreadybeen used <strong>the</strong> subject <strong>of</strong> <strong>the</strong> newest researches has become <strong>the</strong>way <strong>of</strong> train running (for <strong>the</strong> given line <strong>the</strong> running regimes with<strong>the</strong> low or <strong>the</strong> lowest possible energy consumption are chosen withall <strong>the</strong> o<strong>the</strong>r conditions defined by <strong>the</strong> timetable unchanged). With<strong>the</strong> optimal way <strong>of</strong> running it is possible for <strong>the</strong> train to run on <strong>the</strong>given line according to <strong>the</strong> given timetable and with minimal energyconsumption. The optimiz<strong>at</strong>ion results are used for making andmaintaining <strong>the</strong> optimal energy timetables.In Serbia such work was done by <strong>the</strong> Institute <strong>of</strong> Transport<strong>at</strong>ionCIP (SI CIP) and verified on <strong>the</strong> Serbian Railway network(ZS) [1, 2].The co-author in Slovenia is executing <strong>the</strong> inspectorial supervision<strong>of</strong> oper<strong>at</strong>ion and maintenance <strong>of</strong> <strong>railway</strong> <strong>vehicle</strong>s in Slovenia.2. The st<strong>at</strong>e <strong>of</strong> <strong>the</strong> electric traction <strong>vehicle</strong>sin Serbia and SloveniaThe first electric locomotive, 441 series (Fig. 1) (four-axleB o B o ), was put in exploit<strong>at</strong>ion on <strong>the</strong> former Yugoslav Railwaysnetwork in <strong>the</strong> mid <strong>of</strong> 1970. In 1971, a large number <strong>of</strong> <strong>the</strong>m weredelivered for <strong>the</strong> same network. “Rade Koncar”, <strong>the</strong> enterprisefrom Zagreb, manufactured those locomotives, licensed by ASEA,Sweden. Six-axle (C o C o ) electric locomotives, 461 series (Fig. 3),were manufactured in <strong>the</strong> mid <strong>of</strong> 1972 in Resice, Romania in cooper<strong>at</strong>ionwith <strong>the</strong> ASEA. They were delivered for <strong>the</strong> “eastern”part <strong>of</strong> <strong>the</strong> former Yugoslav Railways (ZTP Belgrade, Skopje andPodgorica) [3].The locomotives use single axle drive and diodes in drivecontrol system. Electric locomotives series 441 are developed forspeeds <strong>of</strong> 120 and 140 km/h (<strong>the</strong> r<strong>at</strong>ios between <strong>the</strong> cog number<strong>of</strong> <strong>the</strong> smaller and <strong>the</strong> larger cog-weel are 20:73 and 28:87) andseries 461 for <strong>the</strong> speed <strong>of</strong> 120 km/h only (20:73). The electricequipment is constructed to work with single-phase altern<strong>at</strong>e currentwith nominal voltage <strong>of</strong> 25 kV and frequency <strong>of</strong> 50 Hz. Bothseries have two driver’s cabs, one on each locomotive end, whichare used on electrified lines for passenger and freight train traction.30 diode electric locomotives series 441 had been modernizedinto thyristor locomotives series 444 (Fig. 2) between 2004and 2007 in <strong>the</strong> company “Rade Koncar”, Zagreb. New modernequipment is built into locomotives leading to improvements inperformance, reliability and availability. Moderniz<strong>at</strong>ion had includedsubstitution <strong>of</strong> all relay equipment with microprocessors for locomotivecontrol, protection and diagnostic <strong>of</strong> malfunctioning withmessages and instructions for maintenance. The old step regul<strong>at</strong>ion<strong>of</strong> traction motors was replaced with continuous control <strong>of</strong>tractive effort based on thyristor elements.The following objectives are intended to be achieved by moderniz<strong>at</strong>ion:lifetime extension, improvement in service parameters,service cost reduction, better working environment for drivers,* Bojan Cene 1 , Aleksandar Radosavljevic 2 , Branislav Gavrilovic 31 Ministry for Traffic, Ljubljana, Slovenia, Email: bojan.cene@gmail.com2 Institute <strong>of</strong> Transport<strong>at</strong>ion CIP, Belgrade, Serbia3 Serbian Railways, Belgrade, Serbia50 ● COMMUNICATIONS 3/2008


REVIEWhigh unific<strong>at</strong>ion <strong>of</strong> equipment on locomotives <strong>of</strong> series 441 and461 and maintenance cost reduction. Total number <strong>of</strong> locomotiveseries 441 is 76 (441: 46, 444: 30) and <strong>of</strong> series 461 is 53.Fig. 4 The electric locomotive series 342Fig. 1 The electric locomotive series 441Fig. 5 The electric locomotive series 362Fig. 2 The electric locomotive series 444Fig. 6 The electric locomotive series 363Fig. 3 The electric locomotive series 461The fourth (four axles B 0 B 0 locomotive <strong>of</strong> <strong>the</strong> DC System 3 kV,series 342 was manufactured by Ansaldo Italy and has been oper<strong>at</strong>ingin <strong>the</strong> region <strong>of</strong> Slovenian Railways since <strong>the</strong> year 1968 (Fig.4). The next (six axles B 0 B 0 B 0 ) DC system locomotive series 362was also manufactured by Ansaldo Italy and has been alreadyoper<strong>at</strong>ing in Slovenia since <strong>the</strong> year 1960 (Fig. 5). The Frenchlocomotive (six axles CC) series 363 has been oper<strong>at</strong>ing in Sloveniasince <strong>the</strong> year 1975 and is still representing <strong>the</strong> most frequentelectric locomotive on <strong>the</strong> Slovenian <strong>railway</strong>s today (Fig. 6). InFig. 7 The electric locomotive series 541COMMUNICATIONS 3/2008 ●51


REVIEW<strong>the</strong> year 2006 in Slovenia started oper<strong>at</strong>ing <strong>the</strong> three-system (fouraxles B 0 B 0 ) Siemens electric locomotive series 541, factory design<strong>at</strong>edas ES64U4. It can oper<strong>at</strong>e in <strong>the</strong> following electric tractionsystems: DC system 3 kV, single phase AC system 25 kV, 50 Hzand single phase AC system15 kV, 16 ⅔ Hz (Fig. 7).The Italian locomotives series 342, r<strong>at</strong>ed output 2 MW andseries 362, r<strong>at</strong>ed output 2.65 MW are classic resistance electriclocomotives, which are slowly termin<strong>at</strong>ing <strong>the</strong>ir service in Slovenia.The locomotive 363, r<strong>at</strong>ed output 2.75 MW is a more up-tod<strong>at</strong>eresistance locomotive with gear transmission <strong>of</strong> power acrossa reduction gear to <strong>the</strong> <strong>wheel</strong> <strong>set</strong>s. This locomotive is still expectedto oper<strong>at</strong>e for approxim<strong>at</strong>ely ten more years. The Siemens locomotiveseries 541 is an interoperable locomotive and was acquiredfor oper<strong>at</strong>ion on <strong>the</strong> <strong>railway</strong>s in Slovenia as well as in neighbouringcountries. It is equipped with st<strong>at</strong>ic convertors in transistorversion.3. Definition <strong>of</strong> <strong>the</strong> train movement differential equ<strong>at</strong>ionTrain movement equ<strong>at</strong>ion represents <strong>the</strong> dependence between<strong>the</strong> train acceler<strong>at</strong>ion and <strong>the</strong> efforts exerted during <strong>the</strong> trainrunning. The train movement equ<strong>at</strong>ion is <strong>the</strong> basis for solving all<strong>the</strong> traction-energy tasks. Some <strong>of</strong> <strong>the</strong>m are: running times, drivingenergy consumption, determin<strong>at</strong>ion <strong>of</strong> <strong>the</strong> corresponding trainload for <strong>the</strong> given line, determin<strong>at</strong>ion <strong>of</strong> <strong>the</strong> optimal energy runningtimes, etc. The train movement equ<strong>at</strong>ion is based on <strong>the</strong> well-knownmechanics rule: elementary work <strong>of</strong> efforts exerted on <strong>the</strong> runningtrain (resultant efforts) is equivalent to <strong>the</strong> elementary increase(or decrease) <strong>of</strong> quantity <strong>of</strong> motion [1]:dA dE (1)Where: dA [Nm] - elementary work <strong>of</strong> <strong>the</strong> resultant effort; dE[Nm] – elementary change <strong>of</strong> <strong>the</strong> live effort–train kinetic energy.During running <strong>the</strong> train is exposed to influence <strong>of</strong> differentefforts (considering <strong>the</strong> intensity and direction) but its movementis <strong>the</strong> result <strong>of</strong> influence <strong>of</strong> <strong>the</strong> resultant effort. When <strong>the</strong> trainmovement speed is changed <strong>the</strong> <strong>wheel</strong> rot<strong>at</strong>ing and rot<strong>at</strong>ing massesspeeds th<strong>at</strong> are rot<strong>at</strong>ing according to <strong>the</strong> train movement are alsochanged. Train movement equ<strong>at</strong>ions are as follows:dV-3Ml = 10 ^Fv-Fk-Wo-WdhdtdxV = , (3)dtWhere: V [m/s] – train speed, x [m] - distance, t [s] - time, M[t/m/s 2 ] – weight coefficient <strong>of</strong> <strong>the</strong> train, F v [daN] – tractive effort<strong>at</strong> <strong>the</strong> <strong>wheel</strong> rim, F k [daN] – braking effort <strong>of</strong> <strong>the</strong> train, W o [daN]– basic train resistance, W d [daN] – additional resistance.Additional resistance (Fig. 8) is <strong>the</strong> one th<strong>at</strong> arises from <strong>the</strong>line gradient and its curve radius and <strong>the</strong> basic resistance is <strong>the</strong>one th<strong>at</strong> arises during <strong>the</strong> <strong>vehicle</strong> movement (with defined speedalong <strong>the</strong> straight and horizontal line considering <strong>the</strong> averagewe<strong>at</strong>her conditions). M value is as follows:QL^1+ fLh+ QK^1+fKhMl=(4)gWhere: Q L [t] – locomotive weight ready for service, Q K [t] –load hauled, ε L – rot<strong>at</strong>ional inertia coefficient <strong>of</strong> a locomotive,ε K – rot<strong>at</strong>ional inertia coefficient <strong>of</strong> coaches, g 9,81 [m/s 2 ] –gravit<strong>at</strong>ional acceler<strong>at</strong>ion.(2)Fig. 8 Additional track resistance52 ● COMMUNICATIONS 3/2008


REVIEW5. Results <strong>of</strong> <strong>simul<strong>at</strong>ion</strong>s and experimental testsOn <strong>the</strong> Serbian Railway network <strong>the</strong>re are different lines considering<strong>the</strong> field configur<strong>at</strong>ion: level, mountain and mixed. TheBelgrade (Resnik)–Bar line is a typical mountain line with numerousup and downgrades and <strong>the</strong> small curve radiuses (R 300 m).This track, which is 405.1 km long, has 558 changes <strong>of</strong> specificresistance. The longitudinal line section is adapted for computer<strong>simul<strong>at</strong>ion</strong> by its reduction without connection <strong>of</strong> <strong>the</strong> successiverel<strong>at</strong>ed sections. The o<strong>the</strong>r line elements, such as: maximumsection speeds, train stops in st<strong>at</strong>ions, restricted-speed running,etc. are used according to <strong>the</strong> timetable.Simul<strong>at</strong>ion <strong>of</strong> various freight trains running hauled by electriclocomotives series 441 and 461, is done to estim<strong>at</strong>e <strong>the</strong> totalrunning time and consumed energy for <strong>the</strong> train traction. Simul<strong>at</strong>ionis done on <strong>the</strong>se lines: Beograd ranzirna “A” – Mala Krsna(Q V 1160 t), Nis – Tabanovci (Q V 1160 t), Beograd ranzirna“B” – Lapovo ranzirna (Q V 800 t), Mala Krsna – Rakovica(Q V 600 t), Resnik – Podgorica (Q V 1000 t, Fig. 9, 10) andPodgorica – Resnik (Q V 1060 t). On <strong>the</strong> basis <strong>of</strong> <strong>the</strong> obtainedvalues we can conclude th<strong>at</strong> average specific consumed energy for<strong>the</strong> locomotive series 441 is about 25.5 Wh/brtkm and for <strong>the</strong>locomotive series 461 is about 35.1 Wh/brtkm [4]. In <strong>the</strong> case <strong>of</strong>passenger trains <strong>the</strong> specific consumed energy for train traction ishigher by about 30% and more.The Slovenian Railways have started to install up-to-d<strong>at</strong>e digitalequipment for metering and reading <strong>the</strong> energy consumption with<strong>the</strong> use <strong>of</strong> <strong>the</strong> GPS system on electric traction <strong>vehicle</strong>s. The oper<strong>at</strong>ingprinciple is shown in Fig. 11.The following equipment is installed on <strong>the</strong> locomotive: Energymeter LEM EM4T, voltage transductor type LEM CV 4-6000/SP1,Fig. 9 D<strong>at</strong>a for st<strong>at</strong>ionsFig. 10 D<strong>at</strong>a for travelling regimes54 ● COMMUNICATIONS 3/2008


REVIEWth<strong>at</strong> <strong>the</strong> GPS does not recognize <strong>the</strong> curve <strong>of</strong> <strong>the</strong> <strong>railway</strong> track in<strong>the</strong> <strong>moment</strong> <strong>of</strong> reading, but it works along <strong>the</strong> bee-line. Therefore<strong>the</strong> accuracy <strong>of</strong> this system amounts to approxim<strong>at</strong>ely 94 %. If <strong>the</strong>number <strong>of</strong> squares is increased, <strong>the</strong> squares become smaller anda more accur<strong>at</strong>e result is obtained.Fig. 11 Measuring <strong>of</strong> consumption <strong>of</strong> energy on electric locomotives onSlovene <strong>railway</strong>sand current transductor type LF 2005-S/SP9. The consumed energyis read by <strong>the</strong> d<strong>at</strong>a memory, in which <strong>the</strong> d<strong>at</strong>a on consumedenergy and d<strong>at</strong>a from GPS are combined. These d<strong>at</strong>a are sent to<strong>the</strong> server EGIDA (where <strong>the</strong> d<strong>at</strong>a <strong>of</strong> all electric locomotives arecollected). From <strong>the</strong>re <strong>the</strong> d<strong>at</strong>a are sent to <strong>the</strong> server GEMA.R,which unites all <strong>the</strong> d<strong>at</strong>a from <strong>the</strong> inform<strong>at</strong>ion system <strong>of</strong> trafficperformance (ISUP) and from <strong>railway</strong> subst<strong>at</strong>ions (ENP). Thed<strong>at</strong>a on <strong>the</strong> consumer are sent to <strong>the</strong> INTRANET [5].In <strong>the</strong> continu<strong>at</strong>ion, <strong>the</strong> analysis <strong>of</strong> <strong>the</strong> run <strong>of</strong> <strong>the</strong> train No.47408, with a mass <strong>of</strong> 1708 tons and with a locomotive series 363– 004 is shown for <strong>the</strong> trip from Ljubljana to Maribor on 14 September2007. For better understanding <strong>the</strong> analysis <strong>of</strong> energy consumption<strong>of</strong> this train is given only for <strong>the</strong> distance travelled fromLjubljana to Ljubljana Moste (Table 1) [6].Analysis <strong>of</strong> electricity consumption <strong>at</strong> train 47408on <strong>railway</strong> line Ljubljana – Ljubljana Moste Table 1Consumed[kWh]Regener<strong>at</strong>ed[kWh]TracksectionSpeed[km/h]Width[m]Length[m]1 0 Ljubljana 0 46.0588 14.52671 0 Ljubljana 0 46.0588 14.52670 0 Ljubljana 17 46.0588 14.527920 0 Ljubljana –LjubljanaMoste35 46.0589 14.5339The fifth and <strong>the</strong> sixth column in <strong>the</strong> table represent <strong>the</strong> widthand <strong>the</strong> length <strong>of</strong> d<strong>at</strong>a acquisition from <strong>the</strong> locomotive by <strong>the</strong>GPS equipment. The GPS system divides <strong>the</strong> area <strong>of</strong> movement<strong>of</strong> <strong>the</strong> locomotive into small squares and each such square indic<strong>at</strong>estransmitted inform<strong>at</strong>ion about <strong>the</strong> energy consumed from<strong>the</strong> locomotive to <strong>the</strong> centre. It must be taken into consider<strong>at</strong>ionOver <strong>the</strong> total distance <strong>of</strong> 156 km <strong>the</strong> electric energy consumptionfor this train was 2893 kWh. This energy consumption amountsonly to 10.89 Wh/brtkm which is much less than average consumption<strong>of</strong> 35.1 Wh/brtkm with 461 series locomotives. This isdue to differences in <strong>railway</strong> line difficulty. Line Ljubljana – Mariborhas no ascending slopes, for <strong>the</strong> most part <strong>the</strong>re is a downgrade <strong>of</strong>10 ‰. Lines <strong>of</strong> <strong>the</strong> Serbia <strong>railway</strong>s, for which <strong>the</strong>se measurementsare made, are mainly steep with a slope up to 27 ‰.Line Koper – Divaca in Slovenija with a slope up to 26 ‰energy consumption with 363 series locomotives amounts about45 Wh/brtkm.6. ConclusionThe s<strong>of</strong>tware for <strong>the</strong> electric locomotive optimiz<strong>at</strong>ion controlfor driving energy savings purposes enables <strong>the</strong> user to find <strong>the</strong>optimal combin<strong>at</strong>ion (according to his needs) <strong>of</strong> <strong>the</strong> changeabletrain traction parameters. Almost every train traction parameter ischangeable: locomotive series with all characteristic parameters(<strong>wheel</strong> usage percentage, rot<strong>at</strong>ion masses affect factor, nominaltraction motors voltage value, continuous and maximum tractionmotors current, efficiency <strong>of</strong> cog-<strong>wheel</strong>s, deform<strong>at</strong>ion factor, locomotiveactive and apparent power on <strong>the</strong> pantograph, etc.), lineelements (maximum speeds, stopping, restricted-speed running,length <strong>of</strong> stops in st<strong>at</strong>ions, track resistance, etc.). The amount <strong>of</strong><strong>the</strong> output results is bigger than in all <strong>the</strong> o<strong>the</strong>r projects done s<strong>of</strong>ar. The train running <strong>simul<strong>at</strong>ion</strong> time is considerably shorter thanin all o<strong>the</strong>r traction-energy calcul<strong>at</strong>ion methods known so far. The<strong>simul<strong>at</strong>ion</strong> results can also be used for making <strong>the</strong> regime card <strong>of</strong>each train run in <strong>the</strong> whole timetable diagram.In order to verify in practice <strong>the</strong> calcul<strong>at</strong>ed driving energy consumption<strong>of</strong> electric locomotives <strong>at</strong> <strong>the</strong> Serbian Railway numerousmeasurements are conducted on <strong>the</strong> tracks. These measurementsshow high coincidence between <strong>the</strong>oretical and practical results.The s<strong>of</strong>tware for train driving energy consumption is alsoapplied on <strong>the</strong> diesel locomotives and <strong>the</strong> only electric-motor trainseries ZS 412/416 for urban-suburban traffic on <strong>the</strong> Serbian Railways.For this manner <strong>of</strong> analysis <strong>of</strong> consumption electricity energyare decided in Slovenia because <strong>of</strong> larger number <strong>of</strong> carriers.COMMUNICATIONS 3/2008 ●55


REVIEWReferences[1] RADOSAVLJEVIC, A. et al.: Optimiz<strong>at</strong>ion <strong>of</strong> Running Electric Locomotives Series 441 Because <strong>of</strong> Driving Energy Savings (in Serbian),SI CIP Belgrade, 1991[2] RADOSAVLJEVIC, A., MILUTINOVIC, D., BECEJAC, L.: Simul<strong>at</strong>ion <strong>of</strong> Electric Locomotives Running for <strong>the</strong> Driving EnergySavings Purposes, Fourth Intern<strong>at</strong>ional Conference Drives and Supply Systems for Modern Electric Traction in Integr<strong>at</strong>ed 21 stCentury Europe, Warsaw, Poland, 23–25 September 1999, pp. 226–230, 1999[3] RADOSAVLJEVIC, A., KOZULJ, T., BECEJAC, L.: Technical and Oper<strong>at</strong>ional Characteristics <strong>of</strong> Traction Units on Yugoslav Railways(in Serbian), Zelnid, Belgrade, 1998[4] RADOSAVLJEVIC A, MILUTINOVIC, D., JOVANOVIC, R., LUCANIN, V.: Experimental Determin<strong>at</strong>ion <strong>of</strong> Mixed Feight TrainRunning Resistance and Influence on Energy Consumption, 6 th World Congress on Railway Research WCRR 2003 – Topic: InteractiveSystems and Environment – Session: Energy Emissions, Edinburgh, Scotland, 2003, pp. 40–47, 2003[5] DREMELJ, B.: Onboard Metering Electricity Consumption System Architecture and D<strong>at</strong>a P<strong>at</strong>hs (in Slovenian), 2006[6] Slovene Railways, Intranet – D<strong>at</strong>a Concerning Train, No 47408 from day 14.09.2007.56 ● COMMUNICATIONS 3/2008


REVIEWRadomir Brkic – Zivoslav Adamovic *THE IMPLEMENTATION OF SAFETY AND RELIABILITY OF DATATRANSMISSION IN RAILWAY SIGNALLIZATION SYSTEMSThe focus <strong>of</strong> this paper is <strong>the</strong> safety and reliability <strong>of</strong> d<strong>at</strong>a transmission in <strong>railway</strong> systems <strong>at</strong> increased and high train speeds by means<strong>of</strong> technological devices <strong>of</strong> new gener<strong>at</strong>ion. Routes in <strong>railway</strong> traffic are protected with new microprocessing signalling devices, <strong>the</strong> reliabilityand availability <strong>of</strong> which, thanks to new techology, may be projected to a necessary, i. e. desired value.Key words: ETCS, autom<strong>at</strong>ic control, autom<strong>at</strong>ic guidance, safety, reliability, availability.1. IntroductionSo far, <strong>the</strong> conventional signalling system th<strong>at</strong> involves fixeddistances between <strong>the</strong> main signals and pre-signals makes <strong>the</strong> giventask harder and limits <strong>the</strong> existing riding power <strong>of</strong> <strong>the</strong> rail. Contraryto this, <strong>the</strong> ETCS (European Train Control System) – supportedline train leading – is independent <strong>of</strong> dividing <strong>the</strong> railroadinto track sections and it provides <strong>the</strong> possibility <strong>of</strong> viewing <strong>the</strong>actual condition <strong>of</strong> <strong>the</strong> railroad ahead and with no limits.Although mixed traffic railroads would require keeping <strong>of</strong> <strong>the</strong>conventional signals in <strong>the</strong> initial period – because <strong>of</strong> <strong>the</strong> lowerspeed freight trains – as emergency and lower hierarchy level incase <strong>of</strong> a main system failure, <strong>the</strong> main autom<strong>at</strong>ic leading systemworks as an ‘overlay-system’ representing <strong>the</strong> first safety systemcontrolled by s<strong>of</strong>tware.2. Concept <strong>of</strong> an electronic signal boxVery important advantages <strong>of</strong> electronic signal boxes lie in <strong>the</strong>possibilities <strong>of</strong>fered by a system-specific applic<strong>at</strong>ion <strong>of</strong> modernprocessing technology. O<strong>the</strong>r than this, <strong>the</strong>se advantages include:1. Lower purchasing value <strong>of</strong> <strong>the</strong> device;2. Considerably reduced construction requirements and fixedequipment;3. Minimized scope <strong>of</strong> maintenance;4. Ensured unific<strong>at</strong>ion <strong>of</strong> work places for <strong>the</strong> train disp<strong>at</strong>chers –independent <strong>of</strong> <strong>the</strong> equipment supplier – and high level ergonometricequipment in <strong>the</strong> work places <strong>of</strong> disp<strong>at</strong>chers and <strong>the</strong>oper<strong>at</strong>ive center disp<strong>at</strong>chers;5. Simple integr<strong>at</strong>ion <strong>of</strong> additional autom<strong>at</strong>iz<strong>at</strong>ion and disponingfunctions; standardiz<strong>at</strong>ion <strong>of</strong> <strong>the</strong> interface for computersystems higher up in <strong>the</strong> hierarchy;6. Cre<strong>at</strong>ing conditions necessary for an integr<strong>at</strong>ed system <strong>of</strong> autom<strong>at</strong>icleading.1.1. Starting points for <strong>the</strong> safety microcomputermodulePossible places <strong>of</strong> applic<strong>at</strong>ion for <strong>the</strong> safety microprocessormodule – safety microcomputer – are:• <strong>the</strong> electronic signal box, <strong>the</strong> vital ETCS computer• <strong>the</strong> terminal computer for handling signals and branches• <strong>the</strong> vital element <strong>of</strong> every module and <strong>the</strong> main element in <strong>the</strong>safe signal transmission and crypto communic<strong>at</strong>ion.All <strong>the</strong>se places in <strong>the</strong> signal structure differ very much in <strong>the</strong>quantity <strong>of</strong> <strong>the</strong> hardware necessary for <strong>the</strong> main module, s<strong>of</strong>twarenecessary in rel<strong>at</strong>ion to <strong>the</strong> function it performs, factors <strong>of</strong> <strong>the</strong>environment, necessary reliability, etc.Therefore, a global developing aim can be defined as follows:• To develop a microprocessor module for those applic<strong>at</strong>ion placesin <strong>the</strong> field <strong>of</strong> rail signalliz<strong>at</strong>ion where <strong>the</strong> systems i.e. subsystemsmust be fail-safe;• To construct a ‘hard core’ th<strong>at</strong> can be programmed by <strong>the</strong> ‘mainprogram’ to work fail-safe invariably, regardless <strong>of</strong> <strong>the</strong> loc<strong>at</strong>ion<strong>of</strong> <strong>the</strong> applic<strong>at</strong>ion places;• To compose <strong>the</strong> module from reliable components <strong>of</strong> <strong>the</strong> leadingworld producers;• To achieve an MTBF ‘reasonably’ longer than 1 year, th<strong>at</strong> isbetween 10,000–15,000 hours.Unlike <strong>the</strong> so far safety signalling systems based on relays,<strong>the</strong>re are nei<strong>the</strong>r electronic components, nor systems th<strong>at</strong> can befound on <strong>the</strong> market which show <strong>the</strong> necessary ‘fail-safe’ behavior.Since <strong>the</strong> processor itself has no inherent safety, an adequ<strong>at</strong>econcept must be found to guarantee fail-safe behavior using ‘redundancy’– which in fact means <strong>the</strong> management and control <strong>of</strong> <strong>the</strong>managing hardware with one special unit capable <strong>of</strong> detecting allfunctional mistakes th<strong>at</strong> may cause danger to <strong>the</strong> process.* Radomir Brkic 1 , Zivoslav Adamovic 21 Railway College Belgrade,E-mail: rbrkic@drenik.net2 Technical Faculty, Zrenjanin, SerbiaCOMMUNICATIONS 3/2008 ●57


REVIEWThe processing results from <strong>the</strong> two systems are comparedand in case <strong>the</strong>y are not identical, <strong>the</strong> comparing function itselfand <strong>the</strong> next safety action must redirect <strong>the</strong> system into a safe-sideposition. This concept is possible with <strong>the</strong> configur<strong>at</strong>ions ‘2 out <strong>of</strong>2’ and ‘2 out <strong>of</strong> 3’.These are <strong>the</strong> main problems th<strong>at</strong> every system must solveand <strong>the</strong> ‘internal mechanisms’ th<strong>at</strong> must achieve <strong>the</strong> above failsafebehavior:• Every single failure must be identified and must result in a safetyreaction <strong>of</strong> <strong>the</strong> system;• Double or multiple failures cannot happen if <strong>the</strong> safety concept<strong>of</strong> <strong>the</strong> system enables full comparison <strong>of</strong> results (during <strong>the</strong>entire course <strong>of</strong> <strong>the</strong> processing, and not only <strong>at</strong> its end) andcondition <strong>of</strong> both channels, including memories;• Not a single failure in one channel can have a similar effecton <strong>the</strong> o<strong>the</strong>r channel. The channels must be independent fromeach o<strong>the</strong>r;• Both channels and <strong>the</strong> whole module must be completely testedand with no mistakes in ei<strong>the</strong>r hardware or s<strong>of</strong>tware beforereleasing <strong>the</strong> system into work. In o<strong>the</strong>r words, <strong>the</strong> systemmust be guaranteed as mistake-free before starting up <strong>the</strong>system.So, this obviously shows th<strong>at</strong> <strong>the</strong> work <strong>of</strong> both processors andall <strong>the</strong> activities th<strong>at</strong> are rel<strong>at</strong>ed to fur<strong>the</strong>r process oper<strong>at</strong>ion arecontrolled in <strong>the</strong> earliest phase <strong>of</strong> every tact.This early control, as an internal mechanism for identifyingmistakes even in <strong>the</strong> earliest phase, is supported by a special additionalchecking program, which periodically checks <strong>the</strong> completest<strong>at</strong>us <strong>of</strong> <strong>the</strong> system. Also, all <strong>the</strong> inside d<strong>at</strong>a, before <strong>the</strong>ir entryinto <strong>the</strong> memory, are subject to autom<strong>at</strong>ic comparison and correction.It is clear th<strong>at</strong> this kind <strong>of</strong> safety concept assumes safety functions<strong>of</strong> <strong>the</strong> tact-giver and <strong>the</strong> compar<strong>at</strong>or, implying th<strong>at</strong> <strong>the</strong>y mustbe ‘fail-safe’ designed, i.e. th<strong>at</strong> every mistake on one <strong>of</strong> <strong>the</strong> elements<strong>of</strong> <strong>the</strong>se modules must be reflected in <strong>the</strong> ultim<strong>at</strong>e instancein <strong>the</strong> content <strong>of</strong> <strong>the</strong> BUS signal.Fig. 1 shows an illustr<strong>at</strong>ive example <strong>of</strong> a basic two-channelconfigur<strong>at</strong>ion <strong>of</strong> <strong>the</strong> safety microcomputer by Siemens Company.This configur<strong>at</strong>ion is safe-designed so th<strong>at</strong> <strong>the</strong> two identical microcomputerswork in synchrony with <strong>the</strong>ir:• Central processing units CPU 1 and CPU 2;• Belonging memories for entering and reading <strong>of</strong> <strong>the</strong> RAM 1and RAM 2 d<strong>at</strong>a;• Memories which are programmed for fixed values th<strong>at</strong> can bereprogrammed as needed, EPROM 1 and EPROM 2;• The configur<strong>at</strong>ion contains common ingoing and outgoingmodules;• Reception (1) and Release (2) which establish connection with<strong>the</strong> exterior elements; <strong>the</strong> system has one common tact-giverto synchronize <strong>the</strong> work <strong>of</strong> <strong>the</strong> two identical channels.The system checks if <strong>the</strong> signals from both channels are identicalin every tact step, in <strong>the</strong> following way: <strong>the</strong> tact-giver turns onboth processors (TACT 1 and TACT 2) and a compar<strong>at</strong>or (‘C’ signal– control in Fig. 1) The compar<strong>at</strong>or checks <strong>the</strong> content <strong>of</strong> <strong>the</strong> collectorsin both microcomputers (BUS 1 and BUS 2) and compares<strong>the</strong>m. Only in case th<strong>at</strong> <strong>the</strong> compar<strong>at</strong>or (in every tact)establishes <strong>the</strong> identical st<strong>at</strong>us <strong>of</strong> both channels, it gener<strong>at</strong>es <strong>the</strong>signals “OK” (no mistake) on its exit, which triggers <strong>the</strong> nextworking cycle <strong>of</strong> <strong>the</strong> tact-giver.O<strong>the</strong>rwise, in case <strong>the</strong>re is any discrepancy in <strong>the</strong> signalscoming from Channel 1 and Channel 2, which is transparentlyshown on BUS 1 and BUS 2, or in case <strong>of</strong> any mistake on <strong>the</strong>compar<strong>at</strong>or, <strong>the</strong> compar<strong>at</strong>or ‘chokes’ <strong>the</strong> ‘OK’ (no mistake) signaldriving <strong>the</strong> tact-giver into rest, which ultim<strong>at</strong>ely means stopping<strong>the</strong> process: <strong>the</strong> whole configur<strong>at</strong>ion (module) stops its work directing<strong>the</strong> system to <strong>the</strong> ‘safe side’.Fig. 1 Basic structure <strong>of</strong> <strong>the</strong> two-channel safety microcomputer2. Principles <strong>of</strong> safety in <strong>the</strong> <strong>railway</strong> signalling systemsThe signalling systems are not immune from failure and,<strong>the</strong>refore, due to <strong>the</strong>ir specific role, <strong>the</strong>y must be designed andconstructed so th<strong>at</strong> even in case <strong>of</strong> disturbance and failure <strong>the</strong>y donot endanger <strong>the</strong> safety <strong>of</strong> <strong>the</strong> traffic, which implies th<strong>at</strong> <strong>the</strong>y mustbe signal-safe and technically-safe.This ‘fail-safe’ behavior is achieved by implement<strong>at</strong>ion <strong>of</strong> <strong>the</strong>signalling principles and safety criteria and using highly reliabledevices regardless <strong>of</strong> <strong>the</strong> technology.As a defined measure <strong>of</strong> safety, <strong>the</strong> intern<strong>at</strong>ional <strong>railway</strong> organiz<strong>at</strong>ionUIC, i.e. its committee ORE, has defined in its recommend<strong>at</strong>ionson <strong>the</strong> basis <strong>of</strong> so far experience and <strong>the</strong> achievedlevel <strong>of</strong> technical development ‘<strong>the</strong> mean time between two dangerousfailures’ – ‘MTBF’, as a reliability measure in between two58 ● COMMUNICATIONS 3/2008


REVIEWfailures. For example, for an electronic signal box this means,respectively:• Th<strong>at</strong> <strong>the</strong> mean time between two dangerous failures (MTBF)must not be closer than 100 years;• Th<strong>at</strong> <strong>the</strong> mean time between two failures (MTBF) must not becloser than 4 months (2880 hours).2.1. The purpose and <strong>the</strong> functioning principle <strong>of</strong> <strong>the</strong>signalling/safety devicesFig. 2 illustr<strong>at</strong>es <strong>the</strong> role <strong>of</strong> <strong>the</strong> system <strong>of</strong> <strong>railway</strong> signalliz<strong>at</strong>ionwith modalities <strong>of</strong> implement<strong>at</strong>ion <strong>of</strong> <strong>the</strong> safety principles.Fig. 2 The role <strong>of</strong> <strong>the</strong> <strong>railway</strong> signalliz<strong>at</strong>ion system with modalities <strong>of</strong> implement<strong>at</strong>ion <strong>of</strong> <strong>the</strong> safety principlesCOMMUNICATIONS 3/2008 ●59


REVIEWFig. 2 clearly illustr<strong>at</strong>es th<strong>at</strong> <strong>the</strong> two basic purposes <strong>of</strong> <strong>the</strong><strong>railway</strong> signalliz<strong>at</strong>ion are:• control and management <strong>of</strong> <strong>the</strong> traffic;• ensuring safety in <strong>railway</strong> traffic.3. ConclusionThe issue <strong>of</strong> achieving complex safety with standardized modulesolutions has been laid down as a possible concept in this work.The possible applic<strong>at</strong>ions are in: electronic signal boxes, vital ETCScomputers, terminal computers for controlling signals and branches,and as basic elements in transmission <strong>of</strong> safety d<strong>at</strong>a and cryptocommunic<strong>at</strong>ion.In all <strong>the</strong>se possible applic<strong>at</strong>ions <strong>the</strong>re are considerable differencesin <strong>the</strong> scope <strong>of</strong> necessary hardware for <strong>the</strong> basic module,<strong>the</strong> necessary s<strong>of</strong>tware in rel<strong>at</strong>ion to <strong>the</strong> function, <strong>the</strong> factor <strong>of</strong>environment and also <strong>the</strong> necessary reliability in <strong>the</strong> safe d<strong>at</strong><strong>at</strong>ransmission.The new technology implies a close connection between <strong>the</strong>hardware and <strong>the</strong> s<strong>of</strong>tware, where <strong>the</strong> s<strong>of</strong>tware controls <strong>the</strong> hardwaresafety. The procedures, steps and <strong>the</strong> sequences <strong>of</strong> oper<strong>at</strong>ionare included in <strong>the</strong> s<strong>of</strong>tware, more precisely in <strong>the</strong> program, whichis especially important for <strong>the</strong> safe d<strong>at</strong>a transmission.References:[1] ADAMOVIC, Z. BRKIC, R.: The Reliability Engineering, The Associ<strong>at</strong>ion for Technical Diagnostics <strong>of</strong> Serbia – TEHDIS, Belgrade, 2004.[2] BUSSE, K., FELTEN, F.: Safe D<strong>at</strong>a Transmission through Airwaves for <strong>the</strong> First Time in a CBI, SIGNAL+DRAHT, 4/2005.[3] BRKIC, R.: Quality Analysis <strong>of</strong> Reliability and Safety <strong>of</strong> a Railway System, The scientific-pr<strong>of</strong>essional magazine Technical diagnostics- TEHDIS, Belgrade, 2006.[4] BRKIC, R.: Applic<strong>at</strong>ion <strong>of</strong> New Technology in <strong>the</strong> Integr<strong>at</strong>ed Railway System, XXIX May Convention <strong>of</strong> Railway Maintainers <strong>of</strong> Serbiaand Montenegro, Vrnjacka Banja, 2006.60 ● COMMUNICATIONS 3/2008


REVIEWJan Krmela *COMPUTATIONAL MODELLING OF TYRES CONSIDERINGOPERATING AND SAFETY REQUIREMENTSThis contribution deals with <strong>the</strong> structural concept <strong>of</strong> tyres considering oper<strong>at</strong>ing and safety aspects. Results obtained from experimentalmodelling <strong>of</strong> tyres considering oper<strong>at</strong>ing and functional aspects are an essential condition <strong>of</strong> gener<strong>at</strong>ion <strong>of</strong> “correct” comput<strong>at</strong>ional models <strong>of</strong>tyres. Achievement <strong>of</strong> harmony between all requirements on <strong>the</strong> tyre and resulting demands on safety which would lead, apart from o<strong>the</strong>rthings, to an increase <strong>of</strong> <strong>the</strong> life <strong>of</strong> <strong>the</strong> tyre, is a topical issue <strong>of</strong> computing algorithms in tyre-manufacturing plants.1. IntroductionThe rapid development <strong>of</strong> automotive industry is evidencedby <strong>the</strong> production <strong>of</strong> a large variety <strong>of</strong> <strong>vehicle</strong>s. New more powerfuland more perfect road and <strong>of</strong>f-road cars are placed on <strong>the</strong> market.Automobile manufacturers try to outstrip competitors by qualityand quantity <strong>of</strong> products, whereby <strong>the</strong>ir priority is to meet all oper<strong>at</strong>ingand safety requirements and, <strong>at</strong> <strong>the</strong> same time, to guaranteelong life and reliability <strong>of</strong> <strong>the</strong> car, which is considered as a comprehensivedynamic system. All this is required in spite <strong>of</strong> <strong>the</strong>increasing speed <strong>of</strong> cars and customer requirements for comfort,ergonomics, etc. Light m<strong>at</strong>erials are used to reduce car weight and,consequently, oper<strong>at</strong>ing costs.The extensive development <strong>of</strong> cars and all transport<strong>at</strong>ion meanscannot manage without predicting loading st<strong>at</strong>es by quick estim<strong>at</strong>es.A combin<strong>at</strong>ion is used <strong>of</strong> comput<strong>at</strong>ional modelling as a supportingtool and <strong>the</strong> classical experimental approach. Computer aidsshould facilit<strong>at</strong>e designers and development engineers drafting prototypesand models which are used for load tests <strong>of</strong> individualcomponents as well as <strong>of</strong> whole automobiles.Tyres are developed along with cars namely considering <strong>the</strong>irdesign, m<strong>at</strong>erial and safety. The reason for this is th<strong>at</strong> tyres as <strong>the</strong>elements assuring good interaction between car and road must meetcritical safety criteria <strong>at</strong> high speeds (<strong>the</strong> defect <strong>of</strong> a tyre ona highway <strong>at</strong> high speed has to be controllable and must not leadto f<strong>at</strong>al accidents). This is incidentally also a question <strong>of</strong> assigning<strong>the</strong> correct type <strong>of</strong> a tyre to a car and to its oper<strong>at</strong>ing conditions(tyres only for road oper<strong>at</strong>ion, for <strong>of</strong>f-road, combined oper<strong>at</strong>ion aswell as for summer or winter conditions). This is why <strong>the</strong> use <strong>of</strong>comput<strong>at</strong>ional modelling is applied also to <strong>the</strong> field <strong>of</strong> tyres (designmodific<strong>at</strong>ion – change <strong>of</strong> inclin<strong>at</strong>ion angle <strong>of</strong> reinforcing fibres,number <strong>of</strong> reinforcing layers, m<strong>at</strong>erials <strong>of</strong> cords, etc.).The work <strong>of</strong> <strong>the</strong> author over a long period <strong>of</strong> time is devotedto radial tyres for passenger motor cars and, particularly, to <strong>the</strong>ircomput<strong>at</strong>ional modelling [1, 2].In order to be able to adopt a comprehensive approach to <strong>the</strong>st<strong>at</strong>e <strong>of</strong> <strong>the</strong> art trend <strong>of</strong> comput<strong>at</strong>ional modelling, it is necessary tohave good knowledge <strong>of</strong> <strong>the</strong> function <strong>of</strong> <strong>wheel</strong>s with tyres, differenttypes <strong>of</strong> tyres, <strong>the</strong>ir design, structure, range <strong>of</strong> m<strong>at</strong>erials, oper<strong>at</strong>ingconditions, characteristic behaviour <strong>at</strong> particular modes <strong>of</strong> loadingand knowledge <strong>of</strong> more details and d<strong>at</strong>a. All <strong>the</strong>se can be consideredas input parameters absolutely necessary for comput<strong>at</strong>ional modellingwithout which present modelling engineers cannot manage.The present contribution deals with <strong>the</strong> structural concept <strong>of</strong>tyres considering oper<strong>at</strong>ing and safety requirements.For a comprehensive approach <strong>the</strong> functions <strong>of</strong> <strong>wheel</strong>s withtyres are a primary issue.2. Functions <strong>of</strong> <strong>wheel</strong>s with tyresThe function <strong>of</strong> <strong>wheel</strong>s with tyres is not only to align a carreliably. As can be seen in more detail from Fig. 1 <strong>the</strong>re are morerequirements on tyres. The main oper<strong>at</strong>ing requirements on cartyres are th<strong>at</strong> car <strong>wheel</strong>s should be as light as possible and, <strong>at</strong> <strong>the</strong>same time tough, st<strong>at</strong>ically and dynamically balanced.The main requirements on tyres are, apart from o<strong>the</strong>r things,high wear resistance, optimal deform<strong>at</strong>ion characteristics, low rollingresistance, high oper<strong>at</strong>ing life, etc. Wheels with tyres must meetparticular functional requirements given by parameters <strong>of</strong> tyreswhich affect <strong>the</strong> running properties <strong>of</strong> <strong>the</strong> car, i.e. affect <strong>the</strong>irdynamic behaviour (car manoeuvrability, stability, acceler<strong>at</strong>ion,deceler<strong>at</strong>ion, driving comfort, etc.).* Jan KrmelaDepartment <strong>of</strong> Transport Means and Diagnostic, Jan Perner Transport Faculty, University <strong>of</strong> Pardubice, Czech Republic;E-mail: Jan.Krmela@upce.cz, Jan2.Krmela@post.czCOMMUNICATIONS 3/2008 ●61


REVIEWFig. 1 Functions <strong>of</strong> <strong>wheel</strong>s with tyres and requirements on <strong>the</strong>m [2]Fur<strong>the</strong>r specific requirements on tyres, e.g. <strong>vehicle</strong>s handlingm<strong>at</strong>erial in metalworks close to metallurgical furnaces where tyresare exposed to extremely high temper<strong>at</strong>ures are as well as to sharpobjects.3. Definition <strong>of</strong> a tyreTyres as heterogeneous composite bodies can be defined fromvarious viewpoints as shown in Fig. 2. From a geometrical point<strong>of</strong> view <strong>the</strong> tyre is an annulus, from <strong>the</strong> viewpoint <strong>of</strong> strength andflexibility it can be considered as a pressure vessel and with respectto <strong>the</strong> structure <strong>of</strong> individual parts <strong>of</strong> <strong>the</strong> tyre casing and respectivedifferent properties a tyre can be considered as a part withanisotropic properties. Fur<strong>the</strong>rmore, a tyre can be st<strong>at</strong>ically anddynamically loaded, which is given by <strong>the</strong> actual oper<strong>at</strong>ing condition.A specific requirement on tyres is safety <strong>at</strong> high speeds and <strong>the</strong>consequential measures aimed <strong>at</strong> preventing f<strong>at</strong>al road accidents.62 ● COMMUNICATIONS 3/2008


REVIEWFor this reason tyres and <strong>wheel</strong>s as a unit are modified from<strong>the</strong> structural point <strong>of</strong> view, particularly for special army <strong>vehicle</strong>swhere even a sudden drop <strong>of</strong> pressure does not put an end to <strong>the</strong>oper<strong>at</strong>ing capability <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> (system with a central collarproviding circular indexing <strong>of</strong> <strong>the</strong> casing with respect to <strong>the</strong> <strong>wheel</strong>rim).Fig. 2 Definition <strong>of</strong> tyre from various viewpoints [2]4. Tyres for high speeds from <strong>the</strong> viewpoint <strong>of</strong> safetyTyre safety is passive and active – see Fig. 3. Passive safetydepends on <strong>the</strong> quality <strong>of</strong> <strong>the</strong> production <strong>of</strong> a tyre casing, <strong>the</strong> appliedtechnology and used m<strong>at</strong>erials and in <strong>the</strong> case <strong>of</strong> comput<strong>at</strong>ionalmodelling also on <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong> performed calcul<strong>at</strong>ions andappropri<strong>at</strong>e choice <strong>of</strong> <strong>the</strong> computing algorithm.Requirements on active safeness are particularly high runningsafety on various types <strong>of</strong> road surfaces, breakdown resistance,speed resistance and high life <strong>of</strong> m<strong>at</strong>erials used for <strong>the</strong> production<strong>of</strong> tyres, namely reinforcing m<strong>at</strong>erials.The aim is to avoid f<strong>at</strong>al road accidents which might be causedby tyre casing defects ei<strong>the</strong>r by neglecting oper<strong>at</strong>ing conditions <strong>of</strong>tyres (depth <strong>of</strong> tyre tread p<strong>at</strong>tern, tyre infl<strong>at</strong>ion pressure, use <strong>of</strong> inappropri<strong>at</strong>etyres with a different structure, etc.) or by bad vulcaniz<strong>at</strong>ionduring <strong>the</strong> manufacturing process cre<strong>at</strong>ing delamin<strong>at</strong>ions.Fig. 3 Viewpoints <strong>of</strong> tyre safety [2]New fe<strong>at</strong>ures are introduced for high speeds, e.g. electronicsystems which warn <strong>the</strong> drivers in <strong>the</strong> case a gradual drop <strong>of</strong> <strong>the</strong>tyre pressure or adjusting systems for infl<strong>at</strong>ion based on <strong>the</strong> temper<strong>at</strong>ureload <strong>of</strong> <strong>the</strong> tyre casing. Each manufacturer protects <strong>the</strong>results <strong>of</strong> his developments and p<strong>at</strong>ents considering <strong>the</strong>m as priv<strong>at</strong>e“know-how”. Consequently, all new inform<strong>at</strong>ion is only very scarcelyavailable.The listing <strong>of</strong> various structural modific<strong>at</strong>ions would lie outside<strong>the</strong> scope <strong>of</strong> this contribution. Obviously this is an actual topicwhere <strong>the</strong> use <strong>of</strong> modern comput<strong>at</strong>ional methods is advanced andpurposeful.Tyres are subject to internal and external effects which canmore or less cause limit st<strong>at</strong>es leading to degrad<strong>at</strong>ion processes(delamin<strong>at</strong>ion, etc.).During <strong>the</strong> oper<strong>at</strong>ion <strong>of</strong> a <strong>vehicle</strong> combined loading <strong>of</strong> <strong>the</strong>tyre occurs both from a mechanical (st<strong>at</strong>ical, dynamic) and a temper<strong>at</strong>urepoint <strong>of</strong> view (local he<strong>at</strong>ing in subzones, global he<strong>at</strong>ingin <strong>the</strong> tyre-tread area perme<strong>at</strong>ing into <strong>the</strong> tyre during breaking).Also this has to be considered in defining tyre safety <strong>at</strong> highspeeds.5. Requirements on tyre lifeTyres must resist during oper<strong>at</strong>ing to surrounding effects, toneg<strong>at</strong>ive effects <strong>of</strong> oper<strong>at</strong>ion and to o<strong>the</strong>r effects, which couldlead e.g. to delamin<strong>at</strong>ion. Resistance to <strong>the</strong> following effects isconsidered:• puncture – capability <strong>of</strong> tyre to resist puncture by sharp objects• cut-through – capability <strong>of</strong> tyre (especially <strong>of</strong> <strong>the</strong> tread and sidewall)to resist contact with sharp objects• breakdown – capability <strong>of</strong> tyre to resist damage during shorttermloading by concentr<strong>at</strong>ed forces• f<strong>at</strong>igue – capability <strong>of</strong> tyre to resist m<strong>at</strong>erial f<strong>at</strong>igue and defectsin consequence <strong>of</strong> repe<strong>at</strong>ed loading cycles• separ<strong>at</strong>ion and delamin<strong>at</strong>ion – capability <strong>of</strong> structural tyre componentsto maintain integrity <strong>of</strong> <strong>the</strong> system during oper<strong>at</strong>ion• humidity – tyre elements must be able to resist degrad<strong>at</strong>ion bycontact with w<strong>at</strong>er• ozone influence – capability <strong>of</strong> tyre and <strong>of</strong> its components toresist degrad<strong>at</strong>ion caused by ozone present in <strong>at</strong>mosphere• temper<strong>at</strong>ure – tyre components must be able to resist high andlow ambient temper<strong>at</strong>ures and also consequences <strong>of</strong> contactwith <strong>the</strong> road• chemicals – capability <strong>of</strong> tyres and <strong>the</strong>ir components to resistdegrad<strong>at</strong>ion caused by chemicals (in winter – influence <strong>of</strong> saltsolutions).COMMUNICATIONS 3/2008 ●63


REVIEWKnowledge <strong>of</strong> <strong>the</strong> extent <strong>of</strong> resistance <strong>of</strong> tyres to various modes<strong>of</strong> loading and effects <strong>of</strong> <strong>the</strong> environment is gained from tests <strong>of</strong>strength and life – in o<strong>the</strong>r words from destructive tests (Fig. 4).6. Tests <strong>of</strong> tyres for comput<strong>at</strong>ional modelsComput<strong>at</strong>ional modelling requires confirm<strong>at</strong>ion analyses combinedwith experiments. This is <strong>the</strong> reason why it is necessary torun not only tests <strong>of</strong> tyres as a whole, as shown in Fig. 4, but alsotests <strong>of</strong> individual tyre casing components [3], purposely separ<strong>at</strong>edparts etc.This is how an overview which structural modific<strong>at</strong>ions canlead to an increase <strong>of</strong> <strong>the</strong> level <strong>of</strong> safety criteria, increase <strong>of</strong> resistance,life etc. can be obtained.Basic st<strong>at</strong>ical deform<strong>at</strong>ion characteristics <strong>of</strong> tyres can beobtained from a device called st<strong>at</strong>ical adhesor (Fig. 5), which isavailable to author. The st<strong>at</strong>ical adhesor also enables measurement<strong>of</strong> d<strong>at</strong>a from <strong>the</strong> contact surface under defined conditions,as presented in Fig. 5.7. Comput<strong>at</strong>ional modelling <strong>of</strong> tyresIf relevant results are obtained from experimental modelling<strong>of</strong> whole tyres and individual components and all input d<strong>at</strong>a areavailable, gener<strong>at</strong>ion <strong>of</strong> comput<strong>at</strong>ional models <strong>of</strong> <strong>the</strong> tyre casingcan proceed [4]. On <strong>the</strong> basis <strong>of</strong> <strong>the</strong> author’s long experience <strong>the</strong>FEM model <strong>of</strong> an actual radial tyre (Fig. 6) was gener<strong>at</strong>ed whichis “open” to different modes <strong>of</strong> loading and analyses assumingnecessary input d<strong>at</strong>a are completed into <strong>the</strong> calcul<strong>at</strong>ions.8. ConclusionsThis contribution deals only with a specific field which <strong>the</strong>computing engineer has to be well acquainted with from an oper<strong>at</strong>ingand safety point <strong>of</strong> view and from <strong>the</strong> resulting requirementsfor tyre resistance. This is <strong>the</strong> only way how to obtain highlysophistic<strong>at</strong>ed comput<strong>at</strong>ional models <strong>of</strong> tyres, n<strong>at</strong>urally assumingknowledge <strong>of</strong> accur<strong>at</strong>e m<strong>at</strong>erial parameters <strong>of</strong> all parts <strong>of</strong> <strong>the</strong> tyrecasing and <strong>of</strong> <strong>the</strong> o<strong>the</strong>r necessary d<strong>at</strong>a such as inputs <strong>of</strong> road characteristics,load, type <strong>of</strong> car, etc.Fig. 4 Tests <strong>of</strong> <strong>the</strong> tyre as a whole [1]64 ● COMMUNICATIONS 3/2008


REVIEWFig. 6 Comput<strong>at</strong>ional model “open“ to fur<strong>the</strong>r analyses (cross section)Approach to <strong>the</strong> compiling <strong>of</strong> <strong>the</strong> comput<strong>at</strong>ional models <strong>of</strong><strong>the</strong> tyre shown in [2] can be applied also to <strong>the</strong> o<strong>the</strong>r constructiontypes <strong>of</strong> <strong>the</strong> tyres, different sizes, etc.Fig. 5 St<strong>at</strong>ical adhesor and measureable d<strong>at</strong>a <strong>of</strong> <strong>the</strong> tyreReferences[1] KRMELA, J.: Design <strong>of</strong> <strong>the</strong> Comput<strong>at</strong>ional Three-Dimensional Model <strong>of</strong> <strong>the</strong> Radial-ply Tyre (in Czech), [Dissert<strong>at</strong>ion <strong>the</strong>sis], CeskaTrebova, Jan Perner Transport Faculty, University <strong>of</strong> Pardubice, Czech Republic, 2004, p. 226[2] KRMELA, J.: Systems Approach to <strong>the</strong> Comput<strong>at</strong>ional Modelling <strong>of</strong> Tyres – I. Part (in Czech), Monograph, Brno, Czech Republic,2008, p. 102, ISBN 978-80-7399-365-8, Online: [3] KRMELA, J., PESLOVA, F., HAJDUCHOVA, L.: Composite with Elastomer’s M<strong>at</strong>rix (in Czech), M<strong>at</strong>erial Engineering, University<strong>of</strong> Zilina, 3/2004, pp. 17–24, ISSN 1335-0803.[4] KRMELA, J.: The Comput<strong>at</strong>ional Modelling <strong>of</strong> Multi-Layer Composites’ M<strong>at</strong>erials (in Czech), Proc. <strong>of</strong> conference Dynamic Rigid andDeformable Bodies 2006, Usti nad Labem, Czech Republic, 2006, pp. 103–110, ISBN 80-7044-782-6.[5] RUSNAKOVA, S. et al.: Assessment <strong>of</strong> Espi Technique for Detection <strong>of</strong> Vibr<strong>at</strong>ion Behaviour <strong>of</strong> Composite Lamin<strong>at</strong>es, Proc. <strong>of</strong> 12thIntern<strong>at</strong>ional conference on Problems <strong>of</strong> M<strong>at</strong>erial Engineering, Mechanics and Design, Jasna, Slovakia: 2007, CD-ROM – Full texts<strong>of</strong> paper, p. 3, ISBN 978-80-969728-0-7.[6] KRMELA, J., HAJDUCHOVA, L., PESLOVA, F., JANICEK, P.: Composite Structures Used in Tyre, Proc. <strong>of</strong> 22 nd Intern<strong>at</strong>ionalColloquium Advanced Manufacturing and Repair Technologies in Vehicle Industry, Poland, 2005, pp. 15–16, ISBN 80-8070-393-0.COMMUNICATIONS 3/2008 ●65


REVIEWJarmila Sosedova – Jan Slesinger – Miroslav Bariak *TELEMATICS IN INLAND NAVIGATIONOne <strong>of</strong> <strong>the</strong> goals <strong>of</strong> EU transport policy is <strong>the</strong> implement<strong>at</strong>ion <strong>of</strong> integr<strong>at</strong>ed control systems to control transport processes in all means <strong>of</strong>transport, including <strong>the</strong> systems for w<strong>at</strong>er transport<strong>at</strong>ion. Recent deployment <strong>of</strong> inform<strong>at</strong>ion and communic<strong>at</strong>ion technologies on inland w<strong>at</strong>erwaysbrings noticeable impact in security and efficiency <strong>of</strong> transport. Based on this, <strong>the</strong> European Council and Parliament issued <strong>the</strong> directiveconcerning harmonized River Inform<strong>at</strong>ion Services (RIS) on inland w<strong>at</strong>erways around European Union Member St<strong>at</strong>es. Its aim is <strong>the</strong> harmonizedimplement<strong>at</strong>ion <strong>of</strong> inform<strong>at</strong>ion and communic<strong>at</strong>ion systems on <strong>the</strong> network <strong>of</strong> European inland w<strong>at</strong>erways.1. IntroductionThe applic<strong>at</strong>ion issue <strong>of</strong> inform<strong>at</strong>ion, communic<strong>at</strong>ion and telem<strong>at</strong>icservices in transport<strong>at</strong>ion including w<strong>at</strong>er transport falls intokey areas <strong>of</strong> WHITE PAPER “European transport policy for 2010:time to decide” [KOM(2001)370 d<strong>at</strong>ed 12 th September 2001].In <strong>the</strong> past few years <strong>the</strong> penetr<strong>at</strong>ion <strong>of</strong> inform<strong>at</strong>ion servicesapplic<strong>at</strong>ions on inland w<strong>at</strong>erways raised quickly around EU MemberSt<strong>at</strong>es. Many <strong>of</strong> <strong>the</strong>se applic<strong>at</strong>ions have nowadays noticeable impactin security and efficiency <strong>of</strong> transport processes. The EuropeanCommission <strong>the</strong>refore emphasizes <strong>the</strong> necessity to negoti<strong>at</strong>ecommon requirements and technical specific<strong>at</strong>ions for this area.As a result <strong>of</strong> such negoti<strong>at</strong>ions a harmonized system <strong>of</strong> navig<strong>at</strong>ionassistance and an inform<strong>at</strong>ion system covering inland w<strong>at</strong>erwaysin EU should be established.Based on mentioned requirements <strong>the</strong> European Council andParliament issued <strong>the</strong> directive 2005/44/EU d<strong>at</strong>ed 7 th September2005 concerning harmonized River Inform<strong>at</strong>ion Services on inlandw<strong>at</strong>erways around European Union [2].The applic<strong>at</strong>ion <strong>of</strong> directive fully covers <strong>the</strong> establishmentand oper<strong>at</strong>ion <strong>of</strong> River Inform<strong>at</strong>ion Services around all class IVand up w<strong>at</strong>erways in EU Member St<strong>at</strong>es which are interconnectedtoge<strong>the</strong>r with neighbor st<strong>at</strong>es by class IV and up w<strong>at</strong>erways. Thisdirective also covers harbor infrastructure on such w<strong>at</strong>erways.2. The purpose <strong>of</strong> RIS project implement<strong>at</strong>ionThe River Inform<strong>at</strong>ion Services in this case represent harmonizedinform<strong>at</strong>ion services supporting inland navig<strong>at</strong>ion and transport<strong>at</strong>ionprocesses administr<strong>at</strong>ion including interconnection too<strong>the</strong>r means <strong>of</strong> transport. River Inform<strong>at</strong>ion Services concentr<strong>at</strong>eservices for all parties concerned (freighters, shippers, transportoper<strong>at</strong>ors etc.). Such services deal with actual w<strong>at</strong>erway st<strong>at</strong>usinform<strong>at</strong>ion – tactical planning, st<strong>at</strong>istics, inland navig<strong>at</strong>ion support,harbor fees, custom services, accident recovery support and o<strong>the</strong>r.The directive forms <strong>the</strong> framework for deployment and utiliz<strong>at</strong>ion<strong>of</strong> harmonized River Inform<strong>at</strong>ion Services around EuropeanUnion with <strong>the</strong> aim to support inland navig<strong>at</strong>ion, enhance transportsecurity, efficiency and environmental friendliness. This frameworkalso covers <strong>the</strong> issue <strong>of</strong> interconnection between w<strong>at</strong>ertransport and o<strong>the</strong>r means <strong>of</strong> transport around Union [2].Ano<strong>the</strong>r important part <strong>of</strong> this directive establishes <strong>the</strong> outlinefor negoti<strong>at</strong>ion <strong>of</strong> common requirements and technical specific<strong>at</strong>ionsin this area. Basic requirements and technical specific<strong>at</strong>ionsare due to be developed by European Commission taking in account<strong>the</strong> directives already issued by intern<strong>at</strong>ional organiz<strong>at</strong>ions (PIANC,CCNR a UNECE). This step should guarantee fur<strong>the</strong>r continuity<strong>of</strong> development services for transport process control in o<strong>the</strong>rmeans <strong>of</strong> transport including <strong>the</strong> interconnection to maritime transportsystems.In case <strong>of</strong> River Inform<strong>at</strong>ion Services (RIS) deployment toEU Member St<strong>at</strong>es it is very important to guarantee fur<strong>the</strong>r systeminteroperability and system applic<strong>at</strong>ion efficiency. Such inform<strong>at</strong>ionsystem should easily cooper<strong>at</strong>e with inform<strong>at</strong>ion systems alreadyin service in o<strong>the</strong>r means <strong>of</strong> transport <strong>at</strong> least around EuropeanUnion countries. Therefore all Member St<strong>at</strong>es for purposes <strong>of</strong>system establishment should:– provide to RIS users all relevant d<strong>at</strong>a concerning navig<strong>at</strong>ionand transport planning in inland navig<strong>at</strong>ion,– supply geographical inform<strong>at</strong>ion system maps suitable for inlandnavig<strong>at</strong>ion for all inland w<strong>at</strong>erways class Va and up,– arrange administr<strong>at</strong>ion reports reception with required d<strong>at</strong>afrom communic<strong>at</strong>ion with vessels for responsible RIS authorities,* Jarmila Sosedova, Jan Slesinger, Miroslav BariakDepartment <strong>of</strong> W<strong>at</strong>er Transport, Faculty <strong>of</strong> Oper<strong>at</strong>ion and Economics <strong>of</strong> Transport and Communic<strong>at</strong>ions, Zilinská univerzitaE-mail: Jarmila.Sosedova@fpedas.uniza.sk66 ● COMMUNICATIONS 3/2008


REVIEW- guarantee th<strong>at</strong> <strong>the</strong> messages for bo<strong>at</strong>masters are provided asa standard downloadable encrypted messages. Such messagesshould carry inform<strong>at</strong>ion <strong>at</strong> least with d<strong>at</strong>a necessary for safenavig<strong>at</strong>ion. Optionally <strong>the</strong>se messages should also carry additionalinform<strong>at</strong>ion concerning ice rung, maximal allowed draftetc.The local law regul<strong>at</strong>ions, rules and directives around allintended Member St<strong>at</strong>es concerning such w<strong>at</strong>erways should comein force before 20th October 2007. This step should lead to accordancewith global RIS harmoniz<strong>at</strong>ion and EU directives [2].3. The scope <strong>of</strong> <strong>the</strong> RIS projectAs a result <strong>of</strong> last research studies in <strong>the</strong> area <strong>of</strong> River Inform<strong>at</strong>ionServices around several EU Member St<strong>at</strong>es <strong>the</strong> projectIRIS Europe (Implement<strong>at</strong>ion <strong>of</strong> River Inform<strong>at</strong>ion Services inEurope) was issued in l<strong>at</strong>e 2005. Its aim is to stimul<strong>at</strong>e activitiesin field <strong>of</strong> telem<strong>at</strong>ics and intelligent transport systems in inlandnavig<strong>at</strong>ion by implement<strong>at</strong>ion <strong>of</strong> a testing pl<strong>at</strong>form <strong>of</strong> harmonizedRiver Inform<strong>at</strong>ion Systems. This effort should result in early deployment<strong>of</strong> RIS around EU inland w<strong>at</strong>erways, should lead to elimin<strong>at</strong>ion<strong>of</strong> existing barriers and to demarc<strong>at</strong>ion <strong>of</strong> consequentialfunctions and services in Danube and Rhine – Seine regions.The IRIS Europe project is a part <strong>of</strong> European program TEN-T(Trans-European Transport Networks) covered by European Commissionwith <strong>the</strong> highest investment priority.The project RIS Europe is maintained and developed by Austria,Slovak Republic, Hungary, Ne<strong>the</strong>rlands, Belgium and France st<strong>at</strong>eauthorities. By affili<strong>at</strong>ion <strong>of</strong> Bulgaria and Romania to EU also<strong>the</strong>se countries joined <strong>the</strong> project development. O<strong>the</strong>r Europeancountries – Czech Republic, Serbia and Ukraine are involved asobservers to interchange experiences and know-how.The membership <strong>of</strong> Slovakia in IRIS Europe project is a n<strong>at</strong>uralconsequence <strong>of</strong> successful activity <strong>of</strong> Slovak government and commercialorganiz<strong>at</strong>ions in projects aimed to define, harmonize andspecify River Inform<strong>at</strong>ion Services.4. The structure and goals <strong>of</strong> RIS projectThe project is formally divided into 6 separ<strong>at</strong>e sections:Section 1: Infrastructure for tactical traffic situ<strong>at</strong>ion planningapplic<strong>at</strong>ionsIn this field in <strong>the</strong> area <strong>of</strong> RIS testing pl<strong>at</strong>form install<strong>at</strong>ion <strong>the</strong>Slovak Republic aims to cover establishment <strong>of</strong> coast-line infrastructureand to cover prepar<strong>at</strong>ion <strong>of</strong> support program for shipequipment with necessary devices (install<strong>at</strong>ion <strong>of</strong> AIS base st<strong>at</strong>ionson <strong>the</strong> Slovak part <strong>of</strong> <strong>the</strong> river Danube and on borderlineparts <strong>of</strong> <strong>the</strong> river, establishment <strong>of</strong> n<strong>at</strong>ional RIS centre, trackingand tracing electronic d<strong>at</strong>a interchange with a group <strong>of</strong> RIS users)[3].Section 2: Inter-border services <strong>of</strong> electronic public administr<strong>at</strong>ion– “e-government”Slovak Republic should define requirements <strong>of</strong> administr<strong>at</strong>ionconcerning “e-government” services (for example electronic reporting<strong>of</strong> dangerous goods transport, electronic reports for customprocedures, st<strong>at</strong>istic d<strong>at</strong>a acquisition etc.). This definition shouldalso cover <strong>the</strong> needs <strong>of</strong> commercial users. Very important part <strong>of</strong>this area is <strong>the</strong> definition <strong>of</strong> legisl<strong>at</strong>ion and <strong>the</strong> definition <strong>of</strong> <strong>the</strong><strong>set</strong> <strong>of</strong> service and technical conditions for intern<strong>at</strong>ional RIS d<strong>at</strong>ainterchange including pilot infrastructure implement<strong>at</strong>ion. Thegoal is to allow n<strong>at</strong>ional public administr<strong>at</strong>ion authorities to receiveelectronic reports <strong>of</strong> goods being transported in Austria, Slovakia,Hungary and France [4].Section 3: Environmental services testing infrastructureIn this area <strong>the</strong> Slovak Republic covers <strong>the</strong> vessel waste managementissue and <strong>the</strong> issues <strong>of</strong> navig<strong>at</strong>ion inform<strong>at</strong>ion interchangewith <strong>the</strong> aim to decrease accidents and to provide disaster recoverysolutions.Section 4: Coordin<strong>at</strong>ion in corridor VII (candid<strong>at</strong>e countriesand third-parties), <strong>the</strong> Rhine – Seine region coordin<strong>at</strong>ion and Balticcountries coordin<strong>at</strong>ion – <strong>the</strong> knowledge transferActivities in this area are covered by project partners in Austriaand The Ne<strong>the</strong>rlands.Section 5: Open issues in harmoniz<strong>at</strong>ion and standardiz<strong>at</strong>ion<strong>of</strong> RISThe Slovak Republic based on requirements defined in RISdirective covers <strong>the</strong> harmoniz<strong>at</strong>ion and standardiz<strong>at</strong>ion issues in<strong>the</strong> area <strong>of</strong> River Inform<strong>at</strong>ion Services. Its applic<strong>at</strong>ion aims to <strong>the</strong>field <strong>of</strong> Intelligent Transport Systems, where <strong>the</strong> Slovak Republicdefines <strong>the</strong> framework for cooper<strong>at</strong>ion <strong>of</strong> interconnected systemsin transport services. The solution includes also risk analysis forpassenger and crew members, identific<strong>at</strong>ion <strong>of</strong> services and functionsfor crew and passengers safety in inland navig<strong>at</strong>ion includinglaw and technical regul<strong>at</strong>ions in this area [3] and [5].Section 6: The project controlLast section deals with control and supervision activities, knowledgetransfer and applic<strong>at</strong>ion including n<strong>at</strong>ional and intern<strong>at</strong>ionalactivities in w<strong>at</strong>er transport not covered directly by this projectand <strong>the</strong> initi<strong>at</strong>ives in <strong>the</strong> area <strong>of</strong> <strong>of</strong>f-shore maritime navig<strong>at</strong>ion.4. ConclusionThe Slovak Republic joined <strong>the</strong> project prepar<strong>at</strong>ion and planningin accordance with its n<strong>at</strong>ional policy directive (“Dopravnapolitika Slovenskej republiky do roku 2015” – Slovak governmentdecree No. 445 issued on 8 June 2005) with <strong>the</strong> aim to fulfill itscommitments from RIS directive (2005/44/EU). The intention <strong>of</strong><strong>the</strong> RIS directive places liability for local governmental institutions(in case <strong>of</strong> Slovakia responsible person is The Ministry <strong>of</strong> Transport,Post and Telecommunic<strong>at</strong>ion <strong>of</strong> <strong>the</strong> Slovak Republic) toprovide expert capacity and to control <strong>the</strong> process <strong>of</strong> project financingto reach <strong>the</strong> demarked targets.COMMUNICATIONS 3/2008 ●67


REVIEWDuring passed few years <strong>the</strong> main activity <strong>of</strong> Slovakia in <strong>the</strong>River Inform<strong>at</strong>ion Services project concentr<strong>at</strong>ed on <strong>the</strong> COMPRIS(Consortium Oper<strong>at</strong>ional Management River Inform<strong>at</strong>ion Services)project. Local n<strong>at</strong>ional institutions mainly involved in this projectwere Transport Research Institute, Inc. Zilina, a branch for developmentin w<strong>at</strong>er transport in Br<strong>at</strong>islava, St<strong>at</strong>e Navig<strong>at</strong>ion Administr<strong>at</strong>ionBr<strong>at</strong>islava, Slovensky vodohospodarsky podnik, <strong>the</strong> companyOZ Br<strong>at</strong>islava Ltd. in <strong>the</strong> area <strong>of</strong> digital maps for inland navig<strong>at</strong>ionand KIOS, Ltd. Piestany in <strong>the</strong> area <strong>of</strong> s<strong>of</strong>tware applic<strong>at</strong>iondevelopment and electronic d<strong>at</strong>a interchange with public administr<strong>at</strong>ionauthorities. The company Slovenská plavba a prístavy,a.s. Br<strong>at</strong>islava, which provided vessels for <strong>the</strong> COMPRIS projecttesting and assisted in development <strong>of</strong> <strong>the</strong> messaging system forbo<strong>at</strong>masters, particip<strong>at</strong>ed in this project as a cooper<strong>at</strong>or. The institutionSlovenský hydrometeorologický ústav provided necessaryd<strong>at</strong>a concerning w<strong>at</strong>er-level stage and meteo-d<strong>at</strong>a [1].Total project cost estim<strong>at</strong>ion value figures 4.146 million EUR.The project is financed from <strong>the</strong> European Union TEN-T programup to 50% <strong>of</strong> its costs for solution and test projects.References[1] SOSEDOVA, J. et al.: Project VEGA MS SR 1/3831/06 – Transport – Juridical Conditions <strong>of</strong> Inland Shipping and <strong>the</strong>ir Economic Consequencesfor Carriers after <strong>the</strong> Entrance <strong>of</strong> <strong>the</strong> Slovak Republic to <strong>the</strong> European Union[2] DIRECTIVE 2005/44/EC OF THE EUROPEAN PARLIAMENT AND OF THE COUNCIL <strong>of</strong> 7 September 2005 on harmonizedriver inform<strong>at</strong>ion services (RIS) on inland w<strong>at</strong>erways in <strong>the</strong> Community, Official Journal L 255, 30/09/2005 P. 0152 – 0159[3] COMMISSION REGULATION (EC) No 414/2007 <strong>of</strong> 13 March 2007 concerning <strong>the</strong> technical guidelines for <strong>the</strong> planning, implement<strong>at</strong>ionand oper<strong>at</strong>ional use <strong>of</strong> river inform<strong>at</strong>ion services (RIS) referred to in Article 5 <strong>of</strong> Directive 2005/44/EC <strong>of</strong> <strong>the</strong> EuropeanParliament and <strong>of</strong> <strong>the</strong> Council on harmonized river inform<strong>at</strong>ion services (RIS) on inland w<strong>at</strong>erways in <strong>the</strong> Community, O.J. L 105<strong>of</strong> 23 April 2007, pp. 1–34[4] COMMISSION REGULATION (EC) No 415/2007 <strong>of</strong> 13 March 2007 concerning <strong>the</strong> technical specific<strong>at</strong>ions for vessel trackingand tracing systems referred to in Article 5 <strong>of</strong> Directive 2005/44/EC <strong>of</strong> <strong>the</strong> European Parliament and <strong>of</strong> <strong>the</strong> Council on harmonizedriver inform<strong>at</strong>ion services (RIS) on inland w<strong>at</strong>erways in <strong>the</strong> Community, O.J. L 105 <strong>of</strong> 23 April 2007, pp. 35–87[5] COMMISSION REGULATION (EC) No 416/2007 <strong>of</strong> 22 March 2007 concerning <strong>the</strong> technical specific<strong>at</strong>ions for Notices to Skippersas referred to in Article 5 <strong>of</strong> Directive 2005/44/EC <strong>of</strong> <strong>the</strong> European Parliament and <strong>of</strong> <strong>the</strong> Council on harmonized river inform<strong>at</strong>ionservices (RIS) on inland w<strong>at</strong>erways in <strong>the</strong> Community, O.J. L 105 <strong>of</strong> 23 April 2007, pp. 88–253[6] www.iris-europe.net[7] www.iris-europe.sk[8] www.telecom.gov.sk68 ● COMMUNICATIONS 3/2008


REVIEWIvana Olivkova *PASSENGER INFORMATION SYSTEMSIN PUBLIC TRANSPORTThe article deals with establishment <strong>of</strong> passenger inform<strong>at</strong>ion systems which are comprehensive and not limited to one or more individualoper<strong>at</strong>ors or transport modes. The systems should be multi-lingual, disabled adapted, both inside and outside interchanges, and combine st<strong>at</strong>ic(i.e. timetable) and dynamic d<strong>at</strong>a on both public and priv<strong>at</strong>e transport services.1. IntroductionPassenger inform<strong>at</strong>ion systems in transit applic<strong>at</strong>ions refer to<strong>the</strong> use <strong>of</strong> technology to provide travel inform<strong>at</strong>ion to passengersin order to assist <strong>the</strong>ir trip-making or route choice decisions ei<strong>the</strong>rprior to departure or en route. The inform<strong>at</strong>ion provided may varyfrom st<strong>at</strong>ic route, schedule and fare inform<strong>at</strong>ion to real-time <strong>vehicle</strong>loc<strong>at</strong>ion and/or estim<strong>at</strong>ed arrival time. Real-time inform<strong>at</strong>ion canbe <strong>of</strong>fered to passengers when <strong>the</strong> passenger inform<strong>at</strong>ion systemis used in conjunction with GPS systems. Fur<strong>the</strong>rmore, passengerinform<strong>at</strong>ion might be dissemin<strong>at</strong>ed through <strong>the</strong> use <strong>of</strong> transitoper<strong>at</strong>ions s<strong>of</strong>tware such as itinerary planning systems.Passenger inform<strong>at</strong>ion is generally expected to improve <strong>the</strong>quality <strong>of</strong> transit service by improving <strong>the</strong> passenger experience.Passenger inform<strong>at</strong>ion may grant passengers a better sense <strong>of</strong> controlover <strong>the</strong>ir trip-making decisions and/or enable <strong>the</strong>m to take actionto minimize <strong>the</strong>ir waiting times <strong>at</strong> stops, plan <strong>the</strong>ir transfer connectionsand thus reduce <strong>the</strong>ir overall travel time.2. C<strong>at</strong>egories <strong>of</strong> inform<strong>at</strong>ion systems in public transportInform<strong>at</strong>ion systems may be provided in three c<strong>at</strong>egories(Fig. 1):• Pre-trip passenger inform<strong>at</strong>ion systems• In-terminal/wayside inform<strong>at</strong>ion systems• In-<strong>vehicle</strong> inform<strong>at</strong>ion systemsPre-tripPassenger Inform<strong>at</strong>ion Systemsin Public transportIn-terminalVarious factors affect passenger trip-making decisions, includingservice characteristics such as frequency and coverage. Differenttypes <strong>of</strong> inform<strong>at</strong>ion (e.g. st<strong>at</strong>ic or real-time) and differentmethods for accessing th<strong>at</strong> inform<strong>at</strong>ion (e.g. via <strong>the</strong> internet <strong>at</strong>home or in <strong>vehicle</strong> announcements) will likely have different effectson how passengers use different types <strong>of</strong> service (e.g. high frequencyand low frequency). There is a wide variety <strong>of</strong> passenger inform<strong>at</strong>ionsystems th<strong>at</strong> are designed to influence specific passenger behaviorsand decisions. Below, each <strong>of</strong> <strong>the</strong> c<strong>at</strong>egories <strong>of</strong> passengerinform<strong>at</strong>ion systems listed above is discussed.3. Pre-Trip Passenger Inform<strong>at</strong>ion SystemsPre-trip passenger inform<strong>at</strong>ion systems imparts to <strong>the</strong> userinform<strong>at</strong>ion relevant to <strong>the</strong> choices th<strong>at</strong> are made prior to departure.These pre-trip decisions include choice <strong>of</strong> mode, route anddeparture time, thus enabling passengers to choose a course <strong>of</strong>action th<strong>at</strong> best serves <strong>the</strong>ir trip purpose.There are two types <strong>of</strong> pre-trip passenger inform<strong>at</strong>ion:• General Service Inform<strong>at</strong>ion,• Itinerary Planning.In-<strong>vehicle</strong>Fig. 1 C<strong>at</strong>egories <strong>of</strong> passenger inform<strong>at</strong>ion systemsGeneral Service Inform<strong>at</strong>ion systems <strong>of</strong>fer st<strong>at</strong>ic inform<strong>at</strong>ion,such as route, schedule and fare inform<strong>at</strong>ion. This inform<strong>at</strong>ion canbe accessed by phone or by consulting maps and timetables th<strong>at</strong>are posted on <strong>vehicle</strong>s, <strong>at</strong> stops, or on <strong>the</strong> Internet.Itinerary planning systems allow passengers to consider a variety<strong>of</strong> factors such as travel time, walking distance, cost, and number* Ivana OlivkovaInstitut <strong>of</strong> Transport, Faculty <strong>of</strong> Civil Engineering, Technical University <strong>of</strong> Ostrava, Ostrava – Poruba, Czech Republic,E-mail: ivana.olivkova@vsb.czCOMMUNICATIONS 3/2008 ●69


REVIEW<strong>of</strong> transfers. With <strong>the</strong>se criteria in mind, <strong>the</strong> passenger may choosefrom <strong>the</strong> altern<strong>at</strong>ive trip plans th<strong>at</strong> connect <strong>the</strong>ir origin to <strong>the</strong>irdestin<strong>at</strong>ion.Passenger response to pre-trip inform<strong>at</strong>ion has been hypo<strong>the</strong>sizedand modeled in <strong>the</strong> liter<strong>at</strong>ure. It is important to distinguishbetween low frequency, regular services (e.g. suburban and <strong>of</strong>f-peakurban routes) and high frequency, irregular services (e.g. urbanroutes) when considering transit passenger route choice. It is generallyassumed th<strong>at</strong>, for low frequency services, passengers chooseboth <strong>the</strong> stop and <strong>the</strong> trip (i.e. scheduled departure time) before<strong>the</strong> trip begins. With high frequency services, passengers areassumed to choose only <strong>the</strong> stop prior to starting <strong>the</strong> trip.The choice <strong>of</strong> various stops on routes th<strong>at</strong> serve <strong>the</strong> passenger’sdestin<strong>at</strong>ion can be modeled according to random utility <strong>the</strong>ory,where each candid<strong>at</strong>e stop in <strong>the</strong> choice <strong>set</strong> has some utility valueth<strong>at</strong> is a function <strong>of</strong> <strong>the</strong> stop’s <strong>at</strong>tributes. Therefore, various types<strong>of</strong> pre-trip inform<strong>at</strong>ion (e.g. schedules, estim<strong>at</strong>ed arrival times)might contribute to <strong>the</strong> perceived utility <strong>of</strong> a stop and have a significantimpact on passenger pre-trip stop choice. For high frequencyservices, it is assumed th<strong>at</strong> passengers develop, prior todeparture, a choice <strong>set</strong> <strong>of</strong> candid<strong>at</strong>e routes th<strong>at</strong> serve <strong>the</strong> originstop. Choice <strong>of</strong> <strong>the</strong> actual trip from <strong>the</strong> <strong>set</strong> <strong>of</strong> altern<strong>at</strong>ive routes isassumed to take place en-route. However, pre-trip st<strong>at</strong>ic and/orreal-time inform<strong>at</strong>ion can play an important role in <strong>the</strong> passenger’sconsider<strong>at</strong>ion <strong>of</strong> possible routes.4. In-Terminal Inform<strong>at</strong>ion SystemsPassenger inform<strong>at</strong>ion systems th<strong>at</strong> provide inform<strong>at</strong>ion topassengers while <strong>the</strong>y wait <strong>at</strong> stops are designed to provide waitingcustomers with current inform<strong>at</strong>ion regarding delays, estim<strong>at</strong>edarrival times and o<strong>the</strong>r real-time <strong>vehicle</strong> performance d<strong>at</strong>a.The dynamic stop inform<strong>at</strong>ion system (DIS) makes it possibleto inform visually and acoustically <strong>the</strong> passengers in <strong>the</strong> publictransport<strong>at</strong>ion about <strong>the</strong> actual situ<strong>at</strong>ion on <strong>the</strong> particular stop(Fig. 2). The system compares <strong>the</strong> time table with <strong>the</strong> actual trafficsitu<strong>at</strong>ion monitored by <strong>the</strong> following <strong>of</strong> <strong>the</strong> <strong>vehicle</strong>s position withFig. 2 The dynamic stop inform<strong>at</strong>ion system<strong>the</strong> help <strong>of</strong> <strong>the</strong> s<strong>at</strong>ellite navig<strong>at</strong>ion system GPS. The d<strong>at</strong>a about<strong>the</strong> bus loc<strong>at</strong>ion are transmitted from <strong>the</strong> <strong>vehicle</strong>s by means <strong>of</strong> <strong>the</strong>radio communic<strong>at</strong>ion adapter with <strong>the</strong> GSM /GPRS modulus into<strong>the</strong> central traffic inform<strong>at</strong>ion centre (CETIS). In <strong>the</strong> CETIS <strong>the</strong>d<strong>at</strong>a are processed and <strong>the</strong>y can be completed by <strong>the</strong> time table.The inform<strong>at</strong>ion about time devi<strong>at</strong>ions <strong>of</strong> <strong>the</strong> buses from <strong>the</strong> timetable is conveyed in <strong>the</strong> real-time with <strong>the</strong> help <strong>of</strong> <strong>the</strong> Internet(Intranet) to <strong>the</strong> applic<strong>at</strong>ion computer <strong>at</strong> <strong>the</strong> stop or <strong>at</strong> <strong>the</strong> st<strong>at</strong>ion.The passengers are in a position to w<strong>at</strong>ch <strong>the</strong> inform<strong>at</strong>ion about<strong>the</strong> actual traffic situ<strong>at</strong>ion on <strong>the</strong> large area colour display panel.The visually impaired and handicapped persons outfitted by <strong>the</strong>command transmitter can solicit <strong>the</strong> inform<strong>at</strong>ion in <strong>the</strong> acousticform [4].The inform<strong>at</strong>ion provided <strong>at</strong> transit stops may or may not influencepassenger route choice. For low frequency, regular services,it is assumed th<strong>at</strong> passengers have already chosen a stop and a tripprior to departure. Therefore, in <strong>the</strong> case <strong>of</strong> low frequency services,in-terminal/wayside inform<strong>at</strong>ion may be used to ease customer frustr<strong>at</strong>ionand imp<strong>at</strong>ience during delays. However, in-terminal/waysideinform<strong>at</strong>ion can influence <strong>the</strong> passenger’s en-route decision-makingbehavior in <strong>the</strong> case <strong>of</strong> high frequency services. For example, ifmore than one route serves <strong>the</strong> origin stop, <strong>the</strong> passenger maychoose from among a <strong>set</strong> <strong>of</strong> approaching <strong>vehicle</strong>s th<strong>at</strong> serve <strong>the</strong>destin<strong>at</strong>ion.According to random utility <strong>the</strong>ory, each approaching candid<strong>at</strong>etrip has some utility associ<strong>at</strong>ed with it, which might be a function<strong>of</strong> passenger inform<strong>at</strong>ion [3]. The utility <strong>of</strong> an approachingtrip in <strong>the</strong> choice <strong>set</strong> as a function <strong>of</strong>:• Waiting time (<strong>the</strong> difference between <strong>the</strong> estim<strong>at</strong>ed arrival time<strong>of</strong> a trip and <strong>the</strong> estim<strong>at</strong>ed arrival time <strong>of</strong> <strong>the</strong> base trip), providedby <strong>the</strong> inform<strong>at</strong>ion system• In-<strong>vehicle</strong> travel time• Transfer time to <strong>the</strong> connecting trip• Number <strong>of</strong> passengers• On-board comfort (i.e. level <strong>of</strong> crowding on-board between <strong>the</strong>origin and destin<strong>at</strong>ion stops)• Time already spent <strong>at</strong> <strong>the</strong> stop5. In-Vehicle Inform<strong>at</strong>ion SystemsIn-<strong>vehicle</strong> inform<strong>at</strong>ion systems use public address systems,ei<strong>the</strong>r autom<strong>at</strong>ed or performed by <strong>the</strong> oper<strong>at</strong>or, variable messagesigns and o<strong>the</strong>r on-board systems to communic<strong>at</strong>e inform<strong>at</strong>ion to<strong>the</strong> passengers. In-<strong>vehicle</strong> inform<strong>at</strong>ion might include <strong>the</strong> name <strong>of</strong><strong>the</strong> next stop, transfer opportunities <strong>at</strong> <strong>the</strong> stop, points <strong>of</strong> interestnear <strong>the</strong> stop, and o<strong>the</strong>r inform<strong>at</strong>ion rel<strong>at</strong>ing to upcoming stops.There is less opportunity to influence a passenger’s route choicedecision-making on a transit <strong>vehicle</strong>, since <strong>the</strong> passenger has alreadychosen a stop <strong>at</strong> which to board, <strong>the</strong> <strong>vehicle</strong> (or trip) and, presumably,a destin<strong>at</strong>ion. However, some real-time inform<strong>at</strong>ion, suchas <strong>the</strong> whereabouts <strong>of</strong> connecting <strong>vehicle</strong>s <strong>at</strong> downstream stopsmight be conveyed using in-<strong>vehicle</strong> inform<strong>at</strong>ion systems. The user,<strong>the</strong>n, may upd<strong>at</strong>e <strong>the</strong> destin<strong>at</strong>ion stop choice or begin planning<strong>the</strong> next leg <strong>of</strong> <strong>the</strong> trip based on <strong>the</strong> prevailing connection prospects.70 ● COMMUNICATIONS 3/2008


REVIEWLike <strong>the</strong> o<strong>the</strong>r inform<strong>at</strong>ion systems, <strong>the</strong> provision <strong>of</strong> real-time inform<strong>at</strong>ionregarding connecting routes depends on <strong>the</strong> GPS systemin place [2].Components <strong>of</strong> in-<strong>vehicle</strong> inform<strong>at</strong>ion systems [4] – Fig. 3:• on-board computer and control unit• exterior signs• interior inform<strong>at</strong>ion signs• digital acoustic annunci<strong>at</strong>orOn-board computer and control unit with back lighted keyboardand d<strong>at</strong>a record on memory card are determined for controlling<strong>of</strong> all peripheries in public transport <strong>vehicle</strong>s as part <strong>of</strong>control and passenger inform<strong>at</strong>ion system in <strong>the</strong> required configur<strong>at</strong>ion:exterior and interior signs, digital acoustic unit, ticketingsystem, switches and traffic lights <strong>set</strong>up and GPS loc<strong>at</strong>ion. Theconstruction solution and s<strong>of</strong>tware enable its using both for manualoper<strong>at</strong>ion mode and mode with autom<strong>at</strong>ical next stop switching,autonomous <strong>vehicle</strong> loc<strong>at</strong>ion by means <strong>of</strong> GPS and time tablescanning [2].Exterior and interior inform<strong>at</strong>ion signs indic<strong>at</strong>ed line number,destin<strong>at</strong>ion, real time, tariff zone, duty announcement and o<strong>the</strong>rinform<strong>at</strong>ion. Digital acoustic annunci<strong>at</strong>or provides acoustic inform<strong>at</strong>ionparalelly up to three independent channels for passengersinside <strong>the</strong> <strong>vehicle</strong>, outside <strong>the</strong> <strong>vehicle</strong> and driver.In-<strong>vehicle</strong> traveler inform<strong>at</strong>ion systems, however, may influence<strong>the</strong> behavior <strong>of</strong> passengers aboard <strong>the</strong> bus. For example, <strong>the</strong>announcement <strong>of</strong> a stop may prompt passengers expecting toalight <strong>at</strong> <strong>the</strong> stop, especially those not familiar with <strong>the</strong> system, tobegin <strong>the</strong> approach to <strong>the</strong> exit doors. If this is <strong>the</strong> case, <strong>the</strong> timerequired to discharge all passengers <strong>at</strong> <strong>the</strong> stop may be reducedwith <strong>the</strong> provision <strong>of</strong> in-<strong>vehicle</strong> inform<strong>at</strong>ion. Reduced alightingtime may lead to a reduction in total dwell time <strong>at</strong> <strong>the</strong> stop, andthus affect <strong>the</strong> progression <strong>of</strong> <strong>the</strong> <strong>vehicle</strong> from stop to stop alongits route.Real-time Inform<strong>at</strong>ion makes use <strong>of</strong> GPS d<strong>at</strong>a to provide current<strong>vehicle</strong> performance inform<strong>at</strong>ion to users. Performance d<strong>at</strong>a mightbe used to provide ei<strong>the</strong>r <strong>the</strong> current loc<strong>at</strong>ions <strong>of</strong> transit <strong>vehicle</strong>sor <strong>the</strong> estim<strong>at</strong>ed arrival times <strong>of</strong> <strong>vehicle</strong>s <strong>at</strong> stops along <strong>the</strong> route.The fourth type <strong>of</strong> pre-trip inform<strong>at</strong>ion is Multimodal TravelerInform<strong>at</strong>ion, which provides real-time and/or st<strong>at</strong>ic traffic andtransit inform<strong>at</strong>ion. Multimodal inform<strong>at</strong>ion requires transporttelem<strong>at</strong>ics technologies th<strong>at</strong> measure and estim<strong>at</strong>e <strong>the</strong> currentst<strong>at</strong>e <strong>of</strong> <strong>the</strong> traffic network as well as transit-specific technologiesth<strong>at</strong> provide transit inform<strong>at</strong>ion.Exterior signExterior signInterior inform<strong>at</strong>ion signsFig. 3 Components <strong>of</strong> in-<strong>vehicle</strong> inform<strong>at</strong>ion systemsOn-board computerand control unitDigital acousticannunci<strong>at</strong>or6. ConclusionsWith increasing demands on <strong>the</strong> transport network, systemsproviding accur<strong>at</strong>e, reliable and timely dynamic inform<strong>at</strong>ion to passengersare becoming increasingly important. Many public authoritieswish to promote <strong>the</strong> use <strong>of</strong> public transport as a viable altern<strong>at</strong>iveto <strong>the</strong> priv<strong>at</strong>e car. To travel door to door using public transportmeans passengers must, on occasion, use several modes. Thisincreases potential uncertainty about <strong>the</strong> journey and interchanges.Real time inform<strong>at</strong>ion can reduce this uncertainty and can promotepublic transport.References:[1] PRIBYL, P.: Inteligent Transport Systems and Transport Telem<strong>at</strong>ics II., Vydav<strong>at</strong>elstvi CVUT Praha, 2007.[2] OLIVKOVA, I.: Inform<strong>at</strong>ion Systems in Public Transport, VSB-TU Ostrava, 2004.[3] KRIVDA, V., OLIVKOVA, I., FRIC, J.: Transport Telem<strong>at</strong>ics – part I., VSB-TU Ostrava, 2004.[4] NUZZOLO, A., RUSSO, F., CRISSALI, U.: Dynamic Schedule-Based Assignment Models for Public Transport Networks, Submittedto Springer-Verlag, 2005.[5] http://www.apex.cz.COMMUNICATIONS 3/2008 ●71


T<strong>at</strong>iana Olejnikova *TWO AND THREE-REVOLUTION CYCLICAL SURFACESThe cre<strong>at</strong>ion <strong>of</strong> two-revolution and three-revolution cyclical surfaces is presented in <strong>the</strong> paper. Classific<strong>at</strong>ion and vector equ<strong>at</strong>ions <strong>of</strong> <strong>the</strong>surfaces are given. The surfaces are cre<strong>at</strong>ed by transl<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle along <strong>the</strong> curves and its centre is on <strong>the</strong> curve. The curves are cre<strong>at</strong>edby revolution <strong>of</strong> a point about any edge <strong>of</strong> <strong>the</strong> trihedron <strong>of</strong> <strong>the</strong> previous curve and this trihedron moves simultaneously along this curve. Allspecific forms <strong>of</strong> surfaces are illustr<strong>at</strong>ed in figures visualized in Maple.1. IntroductionThe point S 1 revolves about <strong>the</strong> coordin<strong>at</strong>e axis z with angularvelocity w 1 in <strong>the</strong> distance d 1 from <strong>the</strong> origin <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>esystem (O, x, y, z). For every value <strong>of</strong> <strong>the</strong> angle w 1 <strong>the</strong>re exists onlyone position <strong>of</strong> <strong>the</strong> point R 1 and <strong>the</strong> trajectory <strong>of</strong> this point R 1 is<strong>the</strong> curve k 1 (circle). The trihedron (R 1 , t 1 , n 1 , b 1 ) defined in everypoint R 1 ∈ k 1 is determined by tangent, principal normal andbinormal <strong>of</strong> <strong>the</strong> curve k 1 . The point S 2 revolves <strong>at</strong> an angularvelocity w 2 about any axis <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>e system, which is identicalwith <strong>the</strong> trihedron (R 1 , t 1 , n 1 , b 1 ) <strong>of</strong> <strong>the</strong> curve k 1 , in <strong>the</strong> distanced 2 from <strong>the</strong> origin <strong>of</strong> this coordin<strong>at</strong>e system which is movingsimultaneously along <strong>the</strong> curve k 1 . For every value <strong>of</strong> <strong>the</strong> angle w 2<strong>the</strong>re exists only one position <strong>of</strong> <strong>the</strong> point R 2 . The trajectory <strong>of</strong>this point R 2 is <strong>the</strong> curve k g 2, where g t, n, b. The trihedron (R 2 ,t 2 , n 2 , b 2 ) in every point R 2 ∈ k g 2 is determined by <strong>the</strong> tangent,principal normal and binormal <strong>of</strong> <strong>the</strong> curve k g 2. The point S 3 revolvesabout any axis <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>e system identical with <strong>the</strong> trihedron(R 2 , t 2 , n 2 , b 2 ) <strong>of</strong> <strong>the</strong> curve k g 2 <strong>at</strong> an angular velocity w 3 in<strong>the</strong> distance d 3 from <strong>the</strong> origin <strong>of</strong> this coordin<strong>at</strong>e system which ismoving simultaneously along <strong>the</strong> curve k g 2. For every value <strong>of</strong> <strong>the</strong>angle w 3 <strong>the</strong>re exists only one position <strong>of</strong> <strong>the</strong> point R 3 . The trajectory<strong>of</strong> <strong>the</strong> point R 3 is <strong>the</strong> curve k g 3 h , where g, h t, n, b. Thetrihedron (R 3 , t 3 , n 3 , b 3 ) in every point R 3 ∈ k g 3 h is determined by<strong>the</strong> tangent, principal normal and binormal <strong>of</strong> <strong>the</strong> curve k g 3 h .The surface <strong>of</strong> <strong>the</strong> type P 1 (u,v) is cre<strong>at</strong>ed by transl<strong>at</strong>ion <strong>of</strong> <strong>the</strong>circle c 1 (R 1 , r 1 ) along <strong>the</strong> curve k 1 , <strong>the</strong> surface <strong>of</strong> <strong>the</strong> typeP g 2(u,v) is cre<strong>at</strong>ed by transl<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle c 2 (R 2 , r 2 ) along<strong>the</strong> curve k g 2 and <strong>the</strong> surface <strong>of</strong> <strong>the</strong> type P g 3 h (u,v) is cre<strong>at</strong>ed bytransl<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle c 3 (R 3 , r 3 ) along <strong>the</strong> curve k g 3 h . Theindex g t, n, b determines th<strong>at</strong> <strong>the</strong> point S 2 revolves about <strong>the</strong>tangent t 1 , or principal normal n 1 or binormal b 1 <strong>of</strong> <strong>the</strong> curve k 1and <strong>the</strong> index h t, n, g determines th<strong>at</strong> <strong>the</strong> point S 3 revolvesabout tangent t 2 , principal normal n 2 or binormal b 2 <strong>of</strong> <strong>the</strong> curvek g 2.REVIEW2. Vector functions <strong>of</strong> <strong>the</strong> curves k 1 , k2, g k3 ghLet <strong>the</strong> curve k 1 be a circle cre<strong>at</strong>ed by revolution <strong>of</strong> <strong>the</strong> pointS 1 S 1 (d 1 , 0, 0, 1) about <strong>the</strong> axis z <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>e system (O,x, y, z) <strong>at</strong> an angular velocity w 1 v and k 1 is determined by <strong>the</strong>vector functionr 1 (v) (x k1 (v), y k1 (v), z k1 (v), 1) S 1 . T z1 (w 1 ) (d 1 cos v, s 1 q 1 sin v, 0,1), v ∈ 0, 2π. (1)The m<strong>at</strong>rix T z1 (w 1 ) represents <strong>the</strong> revolution <strong>of</strong> <strong>the</strong> point S 1about <strong>the</strong> coordin<strong>at</strong>e axis z given by (5) (3 rd m<strong>at</strong>rix for i 1),where <strong>the</strong> parameter q 1 1 determines <strong>the</strong> right-turned or leftturnedrevolution movement <strong>of</strong> <strong>the</strong> point (Fig. 1, i 1, j z) [3].We will define <strong>the</strong> trihedron (R 1 , t 1 , n 1 , b 1 ) <strong>of</strong> <strong>the</strong> curve k 1 in everypoint R 1 ∈ k 1 by <strong>the</strong> tangent t 1 , principal normal n 1 and by binormalb 1 with <strong>the</strong>ir unit vectors t 1 (v), n 1 (v), b 1 (v) by equ<strong>at</strong>ions (2),(3), (4) for i 1, v ∈ 0, 2π1 dr1t^vh1 = ^<strong>at</strong>i, bti,ctih= =h1i dv(2)1 dx ^vh kidy ^ki vh dz ^ki vh dr1= e , , o , h1i =h dv dv dv dv1i21 dr1n^vh1 = ^ani, bni,cnih= =2h2i dv22221 dx^ ki vh dy^ ki vh dz^ki vh dr1= f , , p , h222 2i=2h2i dv dv dv dv1b,. (4)h t v n v h t v n vi = _ ^ hi # ^ihi3i = ^ hi # ^ hi3iThe curve k2 g is cre<strong>at</strong>ed by revolution <strong>of</strong> <strong>the</strong> point S 2 in <strong>the</strong>distance d 2 from <strong>the</strong> origin <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>e system (O, x, y, z)about any coordin<strong>at</strong>e axis x, y, or z through <strong>the</strong> angle w 2 into <strong>the</strong>point S 2 (Fig. 1, i 2 for , j x, y, z). Angular velocity w 2 m 1 v(3)* T<strong>at</strong>iana OlejnikovaInstitute <strong>of</strong> Technology, Economics and Management in Civil Engineering, Civil Engineering Faculty, Technical University <strong>of</strong> Kosice, Slovakia,E-mail: t<strong>at</strong>iana.olejnikova@tuke.sk72 ● COMMUNICATIONS 3/2008


REVIEWFig. 1 Revolution <strong>of</strong> <strong>the</strong> point about axes x, y, z<strong>of</strong> <strong>the</strong> point S 2 is m 1 -multiple <strong>of</strong> angular velocity w 1 v <strong>of</strong> <strong>the</strong>point S 1 The point S 2 is transformed into <strong>the</strong> point R 2 in <strong>the</strong> coordin<strong>at</strong>esystem (R 1 , t 1 , n 1 , b 1 ). If we cre<strong>at</strong>e a surface <strong>of</strong> <strong>the</strong> typeP g 2(u,v), where g t (or g n, or g b), we will revolve <strong>the</strong> pointS 2 about <strong>the</strong> axis j x, or j y, or j z. The revolution <strong>of</strong> <strong>the</strong>point S 2 is represented by a m<strong>at</strong>rix T j2 (w 2 ). j x, y, z in (5), where<strong>the</strong> parameter q 2 1 determines <strong>the</strong> right-turned or left-turnedrevolution and <strong>the</strong> transform<strong>at</strong>ion <strong>of</strong> <strong>the</strong> point S 2 into <strong>the</strong> pointR 2 is represented by a m<strong>at</strong>rix M 2 (w 2 ) given by (5) [4]. The pointS 2 . will be situ<strong>at</strong>ed always on any coordin<strong>at</strong>e axis x, y, z.J10 0K0 cos wiqisinwiTxi^wih =KK0- qisinwicos wiKL00 0J cos wi0 qisinwiK0 1 0Tzi^wih =KK - qisinwi0 cos wiKL 0 0 0J cos wiqisinwi0Kqisinwicos wi0Tzi^wih =K -K 0 0 1KL 0 0 0J<strong>at</strong>i bticti0NK Oanibnicni0Mw i^ih=K OK.abibbicbi0OK OL0 0 0 1P0NO0O,0OO1P0NO0O,0OO1P0NO0O,0OO1PThe elements <strong>of</strong> <strong>the</strong> m<strong>at</strong>rix M 1 (w 1 ) in (5) are <strong>the</strong> coordin<strong>at</strong>es<strong>of</strong> unit vectors t i (v), n i (v), b i (v) <strong>of</strong> tangent t i , principal normal n iand binormal b i in trihedron (R i , t i , n i , b i ), i 1, 2, 3. Then <strong>the</strong>vector function <strong>of</strong> <strong>the</strong> curve k g 2 isr 2 (v) (x k2 (v), y k2 (v), z k2 (v), 1) S 1 . T z1 (w 1 ) (5) S 2 . T j2 (w 2 ) . M 2 (w 2 ), j x, y, z. (6)and S 2 S 2 (d 2 , 0, 0, 1) or S 2 S 2 (0, 0, d 2 , 1).The trihedron (R 2 , t 2 , n 2 , b 2 ) is determined in every point R 2∈ k g 2 by <strong>the</strong> tangent t 2 , principal normal n 2 and binormal b 2 with<strong>the</strong> unit vectors t 2 (v), n 2 (v), b 2 (v) expressed by equ<strong>at</strong>ions (2), (3),(4) for i 2.The curve k g 3 h is cre<strong>at</strong>ed by revolution <strong>of</strong> <strong>the</strong> point R 3 in <strong>the</strong>distance d 3 from <strong>the</strong> origin <strong>of</strong> <strong>the</strong> coordin<strong>at</strong>e system (O, x, y, z)about any coordin<strong>at</strong>e axis x, y, or z through <strong>the</strong> angle w 3 into <strong>the</strong>point S 3 (Fig. 2, i 3 for, j x, y, z). Angular velocity w 3 m 2 w 2 m 2 m 1 v <strong>of</strong> <strong>the</strong> point S 3 is m 2 -multiple <strong>of</strong> angular velocityw 2 m 1 v <strong>of</strong> <strong>the</strong> point S 2 . The point S 3 is transformed into <strong>the</strong>point R 3 in <strong>the</strong> coordin<strong>at</strong>e system (R 2 , t 2 , n 2 , b 2 ). If we cre<strong>at</strong>e <strong>the</strong>surface <strong>of</strong> type P g 3 h (u,v), where h t (or h n, or h b), we willrevolve <strong>the</strong> point S 3 about <strong>the</strong> axis j x, or j y, or j z. Therevolution <strong>of</strong> <strong>the</strong> point S 3 is represented by a m<strong>at</strong>rix T j3 (w 3 ), j x, y, z, where <strong>the</strong> parameter q 3 1 determines <strong>the</strong> rightturnedor left-turned revolution and transform<strong>at</strong>ion <strong>of</strong> <strong>the</strong> pointS 3 into <strong>the</strong> point R 3 is represented by <strong>the</strong> m<strong>at</strong>rix M 3 (w 3 ) by equ<strong>at</strong>ions(5) [4]. The point S 3 .will always be situ<strong>at</strong>ed on any coordin<strong>at</strong>eaxis x, y, or z.Then <strong>the</strong> vector function <strong>of</strong> <strong>the</strong> curve k g 3 h for j x, y, z isr 3 (v) (x k3 (v), y k3 (v), z k3 (v), 1) S 1 . T z1 (w 1 ) S 2 . T j2 (w 2 ) . M 2 (w 2 ) S 3 . T j3 (w 3 ) . M 3 (w 3 ) ,j x, y, z. (7)The trihedron (R 3 , t 3 , n 3 , b 3 ) in every point R 3 ∈ k g 3 h is determinedby <strong>the</strong> tangent t 3 , principal normal n 3 and binormal b 3with <strong>the</strong> unit vectors t 3 (v), n 3 (v), b 3 (v) by equ<strong>at</strong>ions (2), (3), (4)for i 3.In Fig. 2 <strong>the</strong>re is displayed a revolution <strong>of</strong> <strong>the</strong> point S 1 about<strong>the</strong> coordin<strong>at</strong>e axis z through <strong>the</strong> angle w 1 into <strong>the</strong> point R 1 , whereits revolutionary movement cre<strong>at</strong>es <strong>the</strong> curve k 1 , revolution <strong>of</strong> <strong>the</strong>point S 2 about <strong>the</strong> coordin<strong>at</strong>e axis z through <strong>the</strong> angle w 2 into <strong>the</strong>point S 2 and its transform<strong>at</strong>ion into <strong>the</strong> point R 2 , where its revolutionarymovement cre<strong>at</strong>es <strong>the</strong> curve k g 2, revolution <strong>of</strong> <strong>the</strong> pointS 3 about <strong>the</strong> coordin<strong>at</strong>e axis z through <strong>the</strong> angle w 3 into <strong>the</strong> pointS 3 and its transform<strong>at</strong>ion into <strong>the</strong> point R 3 , where its revolutionarymovement cre<strong>at</strong>es <strong>the</strong> curve k g 3 h . In <strong>the</strong> points R 1 , R 2 , R 3 <strong>the</strong>reare displayed trihedrons (R 1 , t 1 , n 1 , b 1 ), (R 2 , t 2 , n 2 , b 2 ), (R 3 , t 3 , n 3 ,b 3 ).In Fig. 3 <strong>the</strong>re are displayed for illustr<strong>at</strong>ion only three combin<strong>at</strong>ions<strong>of</strong> <strong>the</strong> curves k 1 , k t 2, k t 3 t , k 1 , k n 2, k n 3 n and k 1 , k b 2, k b 3 b .COMMUNICATIONS 3/2008 ●73


REVIEWThe two-revolution cyclical surface <strong>of</strong> <strong>the</strong> type P g 2(u,v) is cre<strong>at</strong>edby transl<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle c 2 (R 2 , r 2 ) along <strong>the</strong> curve k g 2 <strong>at</strong> anangular velocity w 2 m 1 v, where <strong>the</strong> circle is always in <strong>the</strong> plane(n 2 , b 2 ) if <strong>the</strong> index g t, or in <strong>the</strong> plane (t 2 , b 2 )ifg n, or in<strong>the</strong> plane (t 2 , n 2 )ifg b and its centre is <strong>the</strong> point R 2 ∈ k g 2. Wewill cre<strong>at</strong>e it so th<strong>at</strong> <strong>the</strong> circle c 02 determined by <strong>the</strong> vector functionc 02 (u) (0, r 2 cos u, r 2 sin u, 1) if g t, or c 02 (u) (r 2 cos u,0, r 2 sin u, 1) if g n, or c 02 (u) (r 2 cos u, r 2 sin u, 0, 1) if g bwe will transform into <strong>the</strong> circle c 2 in <strong>the</strong> coordin<strong>at</strong>e system (R 2 ,t 2 , n 2 , b 2 ) using <strong>the</strong> m<strong>at</strong>rix M 2 (w 2 ) by equ<strong>at</strong>ions (5) (Fig. 4). Thevector function <strong>of</strong> <strong>the</strong> cyclical surface <strong>of</strong> <strong>the</strong> type P g 2(u,v) isP g 2(u,v) r 2 (v) c 02 (u) . M 2 (w 2 ),u ∈ 0, 2π. v ∈ 0, 2π. (9)Fig. 2 Cre<strong>at</strong>ion <strong>the</strong> curves k 1 , k g 2, k g 3 h and <strong>the</strong>ir trihedronswhere r 2 (v) is <strong>the</strong> vector function <strong>of</strong> <strong>the</strong> curve k g 2 determinedby (6).Fig. 3 Combin<strong>at</strong>ions <strong>of</strong> <strong>the</strong> curves k 1 , k t 2, k t 3 t , k 1 , k n 2, k n 3 n and k 1 , k b 2, k b 3 b .3. Vector functions <strong>of</strong> cyclical surfaces <strong>of</strong> <strong>the</strong> typeP 1 (u,v), P g 2(u,v), P g 3 h (u,v)The cyclical surface <strong>of</strong> <strong>the</strong> type P 1 (u,v) is cre<strong>at</strong>ed by transl<strong>at</strong>ion<strong>of</strong> <strong>the</strong> circle c 1 (R 1 , r 1 ) in <strong>the</strong> plane (n 1 , b 1 ) along <strong>the</strong> curvek 1 <strong>at</strong> an angular velocity w 1 v. We will cre<strong>at</strong>e it so th<strong>at</strong> <strong>the</strong> circlec 01 determined by <strong>the</strong> vector function c 01 (u) (0, r 1 cos u, r 1 sin u,1) will be transformed into <strong>the</strong> circle c 1 in <strong>the</strong> coordin<strong>at</strong>e system(R 1 , t 1 , n 1 , b 1 ) using <strong>the</strong> m<strong>at</strong>rix M 1 (w 1 ) expressed by equ<strong>at</strong>ions (5)(Fig. 4).isThe vector function <strong>of</strong> <strong>the</strong> cyclical surface <strong>of</strong> <strong>the</strong> type P 1 (u,v)P 1 (u,v) r 1 (v) c 01 (u) . M 1 (w 1 ),u ∈ 0, 2π. v ∈ 0, 2π. (8)where r 1 (v) is <strong>the</strong> vector function <strong>of</strong> <strong>the</strong> curve k 1 determined byequ<strong>at</strong>ion (1). This surface is surface <strong>of</strong> torus.The three-revolution cyclical surface <strong>of</strong> <strong>the</strong> type P g 3 h (u,v) iscre<strong>at</strong>ed by transl<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle c 3 (R 3 , r 3 ) along <strong>the</strong> curvek 3 <strong>at</strong> an angular velocity w 3 m 2 m 1 v, where <strong>the</strong> circle is alwaysin <strong>the</strong> plane (n 3 , b 3 ) if <strong>the</strong> index h t, or in <strong>the</strong> plane (t 3 , b 3 ) ifh n, or in <strong>the</strong> plane (t 3 , n 3 ) if h b and its centre is <strong>the</strong> pointR 3 ∈ k g 3 h . We will cre<strong>at</strong>e it so th<strong>at</strong> <strong>the</strong> circle c 03 determined <strong>the</strong> byvector function c 03 (u) (0, r 3 cos u, r 3 sin u, 1) if h t, orc 03 (u) (r 3 cos u, 0, r 3 sin u, 1) if h n, or c 03 (u) (r 3 cos u, r 3sin u, 0, 1) if h b we will transform into <strong>the</strong> circle c 3 in <strong>the</strong> coordin<strong>at</strong>esystem (R 3 , t 3 , n 3 , b 3 ) using <strong>the</strong> m<strong>at</strong>rix M 3 (w 3 ) by equ<strong>at</strong>ions(5). The vector function <strong>of</strong> <strong>the</strong> cyclical surface <strong>of</strong> <strong>the</strong> typeP g 3 h (u,v) isP g 3 h (u,v) r 3 (v) c 03 (u) . M 3 (w 3 ),u ∈ 0, 2π. v ∈ 0, 2π. (10)where r 3 (v) is <strong>the</strong> vector function <strong>of</strong> <strong>the</strong> curve k g 3 h determined by(7).74 ● COMMUNICATIONS 3/2008


REVIEWFig. 4 Transform<strong>at</strong>ion <strong>of</strong> <strong>the</strong> circle c 0i into <strong>the</strong> circle c i4. Classific<strong>at</strong>ion <strong>of</strong> cyclical surfaces <strong>of</strong> <strong>the</strong> typeP g 2(u,v), P g 3 h (u,v)The two-revolution cyclical surface <strong>of</strong> <strong>the</strong> type P g 2(u,v) can beclassified according to <strong>the</strong> index g:Table 1: Classific<strong>at</strong>ion <strong>of</strong> cyclical surfaces <strong>of</strong> <strong>the</strong> type P g 2(u,v)g t n bP t2(u,v) P n 2(u,v) P b 2(u,v)The three-revolution cyclical surface <strong>of</strong> <strong>the</strong> type P g 3 h (u,v) canbe classified according to <strong>the</strong> index g and h:Table 2: Classific<strong>at</strong>ion <strong>of</strong> cyclical surfaces <strong>of</strong> <strong>the</strong> type P g 3 h (u,v)g/h t n btP t3 t (u,v) P t3 n (u,v) P t3 b (u,v)n P n 3 t (u,v) P n 3 n (u,v) P n 3 b (u,v)5. Illustr<strong>at</strong>ions <strong>of</strong> cyclical surfaces <strong>of</strong> <strong>the</strong> typeP 1 (u,v), P g 2(u,v), P g 3 h (u,v)In Fig. 5 <strong>the</strong>re are displayed three combin<strong>at</strong>ions <strong>of</strong> cyclicalsurfaces <strong>of</strong> <strong>the</strong> type P 1 (u,v), P t 2(u,v), P t 3t (u,v) in fig. a), P 1 (u,v),P t 2(u,v), P t 3n (u,v) in fig.b), P 1 (u,v), P t 2(u,v), P t 3b (u,v) in fig. c).In Fig. 6 <strong>the</strong>re are displayed three combin<strong>at</strong>ions <strong>of</strong> cyclicalsurfaces <strong>of</strong> <strong>the</strong> type P 1 (u,v), P n 2(u,v), P n 3t (u,v) in fig. a), P 1 (u,v),P n 2(u,v), P n 3n (u,v) in fig. b), P 1 (u,v), P n 2(u,v), P n 3b (u,v) in fig. c).In Fig. 7 <strong>the</strong>re are displayed three combin<strong>at</strong>ions <strong>of</strong> cyclicalsurfaces <strong>of</strong> <strong>the</strong> type P 1 (u,v), P b 2(u,v), P b 3t (u,v) in fig. a), P 1 (u,v),P b 2(u,v), P b 3n (u,v) in fig.b), P 1 (u,v), P b 2(u,v), P b 3b (u,v) in fig. c).The surfaces mentioned above can be used in design practiceas constructive or ornamental structural components.The paper was supported by <strong>the</strong> grant VEGA 1 / 4002 / 07.b P b 3 t (u,v) P b 3 n (u,v) P b 3 b (u,v)a) b) c)Fig. 5 Combin<strong>at</strong>ions <strong>of</strong> cyclical surfaces for g tCOMMUNICATIONS 3/2008 ●75


REVIEWa) b) c)Fig. 6 Combin<strong>at</strong>ions <strong>of</strong> cyclical surfaces for g na) b) c)Fig 7 Combin<strong>at</strong>ions <strong>of</strong> cyclical surfaces for g bReferences[1] OLEJNIKOVA, T.: Straight-lines Spiral-rotary Planes (in Slovak), Proc. <strong>of</strong> 26. konference o geometrii a pocitacove grafice, 2006,Nove Mesto na Morave, CR, 2006, p. 15–28, ISBN 80-7040-902-9.[2] OLEJNIKOVA, T.: Straight-lines Spiral-rotary Planes II (in Slovak), Proc. <strong>of</strong> 6th Intern<strong>at</strong>ional Conference APLIMAT 2007,Br<strong>at</strong>islava, 2007, p. 231–236, ISBN 978-80-969562-4-1[3] KOHOUT, V.: Differential Geometry (in Czech), SNTL-Publishers <strong>of</strong> Technical Liter<strong>at</strong>ure, Praha, 1971.[4] GRANAT, L., SECHOVSKY, H.: Computer Graphics (in Slovak), SNTL – Publishers <strong>of</strong> Technical Liter<strong>at</strong>ure, Br<strong>at</strong>islava, 197476 ● COMMUNICATIONS 3/2008


BOOK REVIEWKavicka, A., Klima, V., Adamko, N.:Agent-oriented Simul<strong>at</strong>ion <strong>of</strong> Traffic Nodes,ISBN 80-8070-477-5The edition house EDIS released a very interesting (and for <strong>the</strong> Slovak and/or Czech speakingpeople very important) book titled Agentovo orientovana simulacia dopravnych uzlov (Agent-orientedSimul<strong>at</strong>ion <strong>of</strong> Traffic Nodes). The authors are A. Kavicka, V. Klima a N. Adamko and <strong>the</strong> book iswritten in Slovakian. The first phrase presented <strong>at</strong> <strong>the</strong> last page <strong>of</strong> <strong>the</strong> book cover can be transl<strong>at</strong>edas follows: “The subject <strong>of</strong> <strong>the</strong> monograph is methodology <strong>of</strong> developing really applicable <strong>simul<strong>at</strong>ion</strong>models <strong>of</strong> complex service systems, especially models <strong>of</strong> traffic nodes as systems with domin<strong>at</strong>ingor prevailing function to reloc<strong>at</strong>e elements.” Th<strong>at</strong> st<strong>at</strong>ement well characterizes <strong>the</strong> contents <strong>of</strong> <strong>the</strong>book. Really, <strong>the</strong> rich concluding chapter <strong>of</strong> <strong>the</strong> book concerns <strong>the</strong> <strong>railway</strong> traffic and we candisclose th<strong>at</strong> <strong>the</strong> whole contents <strong>of</strong> <strong>the</strong> book arose under <strong>the</strong> influence <strong>of</strong> <strong>the</strong> demands <strong>of</strong> <strong>railway</strong>transport, though it can be applied as a <strong>set</strong> <strong>of</strong> efficient stimuli outside <strong>the</strong> <strong>railway</strong> systems <strong>simul<strong>at</strong>ion</strong>,too – <strong>the</strong> oper<strong>at</strong>ion transport in production systems, <strong>the</strong> road transport and <strong>the</strong> dynamics in sea portsand container terminals can be presented as examples.In <strong>the</strong> introductory chapter, a system analysis <strong>of</strong> marshalling yard is presented. Although onecould view it as a certain preparing to <strong>the</strong> last chapter <strong>of</strong> <strong>the</strong> book, <strong>the</strong> essence <strong>of</strong> this chapter is topresent a more or less elementary r<strong>at</strong>ional steps th<strong>at</strong> have to be present before realizing anyapplicable <strong>simul<strong>at</strong>ion</strong> model: from <strong>the</strong> pedagogical point <strong>of</strong> view, <strong>the</strong> marshalling yard servesa certain represent<strong>at</strong>ive <strong>of</strong> o<strong>the</strong>r systems th<strong>at</strong> could be studied by using <strong>simul<strong>at</strong>ion</strong>, a represent<strong>at</strong>iveth<strong>at</strong> needs no special pr<strong>of</strong>essional knowledge <strong>of</strong> a branch (almost every expert in production, design,management and o<strong>the</strong>r branches <strong>of</strong> technology knows something on trains, wagons, st<strong>at</strong>ions andlinks among <strong>the</strong>m, so th<strong>at</strong> he understands even in case he is not a pr<strong>of</strong>essional in traffic problems).The second chapter contains an analysis <strong>of</strong> general notions rel<strong>at</strong>ed to <strong>simul<strong>at</strong>ion</strong>. The contents <strong>of</strong>this chapter is important not only th<strong>at</strong> it forms a logical and semantic base for understanding <strong>the</strong>following chapters (let us accept th<strong>at</strong> <strong>the</strong> terms like <strong>simul<strong>at</strong>ion</strong>, model, systems and th<strong>at</strong> derivedfrom <strong>the</strong>m are understood in a lot <strong>of</strong> public<strong>at</strong>ions over <strong>the</strong> world in a r<strong>at</strong>her chaotic way); it appearsas a good stimulus independently <strong>of</strong> <strong>the</strong> reader’s pr<strong>of</strong>essional orient<strong>at</strong>ion and can be fruitful als<strong>of</strong>or <strong>the</strong> readers whose interest is e.g. production, services and ecology. In a similar way, <strong>the</strong> bookoverpasses <strong>the</strong> transport domain frontiers also in <strong>the</strong> following chapter, which presents and welldeclares <strong>the</strong> pr<strong>of</strong>essional contents and importance <strong>of</strong> (computing) agents, including <strong>the</strong>ir classific<strong>at</strong>ionand near rel<strong>at</strong>ion to computer <strong>simul<strong>at</strong>ion</strong>. Simul<strong>at</strong>ion leads to problems <strong>of</strong> synchroniz<strong>at</strong>ion <strong>of</strong>agents, which concerns two aspects: modeling <strong>of</strong> agents functioning during <strong>the</strong> same simul<strong>at</strong>ed(Newtonian) time, and synchroniz<strong>at</strong>ion <strong>of</strong> computing with visual present<strong>at</strong>ion <strong>of</strong> its st<strong>at</strong>e, namelywith anim<strong>at</strong>ion <strong>of</strong> <strong>simul<strong>at</strong>ion</strong> models, in real time.The fifth chapter is a certain focus <strong>of</strong> a lot <strong>of</strong> work th<strong>at</strong> <strong>the</strong> authors undertook in programmingand implementing <strong>simul<strong>at</strong>ion</strong> s<strong>of</strong>tware. It is known th<strong>at</strong> <strong>the</strong> results <strong>of</strong> <strong>the</strong>ir effort were applied inSwitzerland and China, i.e. th<strong>at</strong> <strong>the</strong> s<strong>of</strong>tware forms a more or less universal package <strong>of</strong> <strong>simul<strong>at</strong>ion</strong>and anim<strong>at</strong>ion routines, blocks and modules, composed <strong>of</strong> more or less autonomous agents. For<strong>the</strong> implement<strong>at</strong>ion <strong>of</strong> <strong>the</strong>m, <strong>the</strong> authors applied programming language Pascal, which is a populartool embedded in an editing and debugging environment, but which has never been oriented to <strong>the</strong>agent programming paradigm. In Pascal, <strong>the</strong> authors had to program all wh<strong>at</strong> is essential foragents, especially everything rel<strong>at</strong>ed <strong>the</strong>ir initi<strong>at</strong>ive and dynamics, and <strong>the</strong>y decided to use Petri netsas tools for this purpose. This chapter reflects <strong>the</strong> hardest work <strong>of</strong> <strong>the</strong> authors and may appear mostdifficult for many readers, but one can quiet <strong>the</strong>m not to be disturbed, as <strong>the</strong>re are programmingtools th<strong>at</strong> allow elude Petri nets. Beside <strong>the</strong> described chapters, <strong>the</strong> book contains 40 page appendix<strong>of</strong> Pascal source code; <strong>the</strong> readers knowing Pascal language will surely appreci<strong>at</strong>e it.Pr<strong>of</strong>. Eugene KindlerCOMMUNICATIONS 3/2008 ●77


COMMUNICATIONS – Scientific Letters <strong>of</strong> <strong>the</strong> University <strong>of</strong> ZilinaWriter’s Guidelinesl. Submissions for public<strong>at</strong>ion must be unpublished and not be a multiple submission.2. Manuscripts written in English language must include abstract also written in English. Thesubmission should not exceed 10 pages with figures and tables (form<strong>at</strong> A4, Times Romansize 12). The abstract should not exceed 10 lines.3. Submissions should be sent: by e-mail (as <strong>at</strong>tachment in applic<strong>at</strong>ion MS WORD) to one <strong>of</strong><strong>the</strong> following addresses: holesa@nic.utc.sk or vrablova@nic.utc.sk or polednak@fsi.utc.sk withahard copy(to be assessed by <strong>the</strong> editorial board) or on a CD with a hard copy to <strong>the</strong> followingaddress: Zilinska univerzita, OVaV, Univerzitná 1, SK-10 26 Zilina, Slovakia.4. 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The editorial board will assess <strong>the</strong> submission in its following session. In <strong>the</strong> case th<strong>at</strong> <strong>the</strong>article is accepted for future volumes, <strong>the</strong> board submits <strong>the</strong> manuscript to <strong>the</strong> editors forreview and language correction. After reviewing and incorpor<strong>at</strong>ing <strong>the</strong> editor’s remarks, <strong>the</strong>final draft (before printing) will be sent to authors for final review and adjustment.9. The deadlines for submissions are as follows: September 30, December 31, March 31 andJune 30.10. Topics for issues: 4/2008 – Networks for New Gener<strong>at</strong>ions, 1/2009 – M<strong>at</strong>erial Engineering.POKYNY PRE AUTOROV PRÍSPEVKOV DO ČASOPISUKOMUNIKÁCIE – vedecké listy Žilinskej univerzity1. Redakcia prijíma iba príspevky doteraz nepublikované alebo inde nezaslané na uverejnenie.2. Rukopis musí byť v jazyku anglickom. Príspevok by nemal prekročiť 10 strán vrátane obrázkova tabuliek (formát A4, písmo Times Roman 12 bodové). K článku dodá autor resumév rozsahu maximálne 10 riadkov (v anglickom jazyku).3. Príspevok prosíme poslať: e-mailom, ako prílohu spracovanú v aplikácii Micros<strong>of</strong>t WORD,na adresu: holesa@nic.utc.sk alebo polednak@fsi.utc.sk príp. vrablova@nic.utc.sk (alebodoručiť na diskete 3,5) a jeden výtlačok článku na adresu Žilinská univerzita, OVaV, Univerzitná1,010 26 Žilina.4. Skr<strong>at</strong>ky, ktoré nie sú bežné, je nutné pri ich prvom použití rozpísať v plnom znení.5. Obrázky, grafy a schémy, pokiaľ nie sú spracované v Micros<strong>of</strong>t WORD, je potrebnédoručiť buď v digitálnej forme (ako GIF, JPG, TIFF, BMP súbory), prípadne nakresliťkontrastne na bielom papieri a predložiť v jednom exemplári. Pri požiadavke na uverejneniefotografie priložiť ako podklad kontrastnú fotografiu alebo diapozitív.6. Odvolania na liter<strong>at</strong>úru sa označujú v texte alebo v poznámkach pod čiarou príslušnýmporadovým číslom v hran<strong>at</strong>ej zátvorke. Zoznam použitej liter<strong>at</strong>úry je uvedený za príspevkom.Citovanie liter<strong>at</strong>úry musí byť podľa STN 01 0197 (ISO 690) „Bibliografické odkazy“.7. K rukopisu treba pripojiť plné meno a priezvisko autora a adresu inštitúcie v ktorej pracuje,e-mail adresu alebo číslo telefónu event. faxu.8. Príspevok posúdi redakčná rada na svojom najbližšom zasadnutí a v prípade jeho zaradeniado niektorého z budúcich čísiel podrobí rukopis recenziám a jazykovej korektúre. Predtlačou bude poslaný autorovi na definitívnu kontrolu.9. Termíny na dodanie príspevkov do čísiel v roku sú: 30. september, 31. december, 31. mareca 30. jún.10. Nosná téma pre č. 1/2008: Bezpečnostné inžinierstvo.SCIENTIFIC LETTERS OF THE UNIVERSITY OF ZILINAVOLUME 10Editor-in-chief:Pr<strong>of</strong>. Ing. Pavel Poledňák, PhD.Editorial board:Pr<strong>of</strong>. Ing. Jan Bujnak, CSc. – SKPr<strong>of</strong>. Ing. Otakar Bokuvka, CSc. – SKPr<strong>of</strong>. RNDr. Peter Bury, CSc. – SKPr<strong>of</strong>. RNDr. Jan Cerný, DrSc. – CZPr<strong>of</strong>. Eduard I. Danilenko, DrSc. – UKRPr<strong>of</strong>. Ing. Branislav Dobrucky, CSc. – SKPr<strong>of</strong>. Dr. Stephen Dodds – UKDr. Robert E. Caves – UKDr.hab Inž. Stefania Grzeszczyk, pr<strong>of</strong>. PO – PLDoc. PhDr. Anna Hlavnova, CSc. – SKPr<strong>of</strong>. Ing. Vladimír Hlavna, PhD. – SKPr<strong>of</strong>. RNDr. Jaroslav Janacek, CSc. – SKPr<strong>of</strong>. Ing. Hermann Kn<strong>of</strong>lacher – ADr. Ing. Helmut König, Dr.h.c. – CHPr<strong>of</strong>. Ing. Milan Moravcik, CSc. – SKPr<strong>of</strong>. Ing. Gianni Nicoletto – IPr<strong>of</strong>. Ing. Ludovít Parilak, CSc. – SKIng. Miroslav Pfliegel, CSc. – SKPr<strong>of</strong>. Ing. Pavel Polednak, PhD. – SKPr<strong>of</strong>. Bruno Salgues – FPr<strong>of</strong>. Andreas Steimel – DPr<strong>of</strong>. Ing. Miroslav Steiner, DrSc. – CZPr<strong>of</strong>. Ing. Pavel Surovec, CSc. – SKPr<strong>of</strong>. Josu Takala – SUPhDr. Radoslava Turska, CSc. – SKDoc. Ing. Martin Vaculik, CSc. – SKAddress <strong>of</strong> <strong>the</strong> editorial <strong>of</strong>fice:Zilinská univerzitaOffice for Science and Research(OVaV)Univerzitna 1SK 010 26 ZilinaSlovakiaE-mail: komunikacie@nic.utc.sk, polednak@fsi.utc.sk,Each paper was reviewed by two reviewers.Journal is excerpted in CompendexIt is published by <strong>the</strong> University <strong>of</strong> Zilina inEDIS - Publishing Institution <strong>of</strong> Zilina UniversityRegistered No: 1989/98ISSN 1335-4205Published quarterlySingle issues <strong>of</strong> <strong>the</strong> journal can be found on:http://www.utc.sk/komunikacie78 ● COMMUNICATIONS 3/2008

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