For the case of parallel buried pipes former analyticalcalculati<strong>on</strong>s by Rizkallah <strong>and</strong> Achmus usingLe<strong>on</strong>hardt‘s theory showed a reducti<strong>on</strong> of the verticalstresses between the two pipes [6]. The system usedfor these calculati<strong>on</strong>s with the ―shear resistant beam <strong>on</strong>elastic bedding‖ for two parallel buried pipes is shownin Fig. 2.The <str<strong>on</strong>g>12th</str<strong>on</strong>g> <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g> <strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong> <strong>Cooling</strong>,September 5 th to September 7 th , 2010, Tallinn, Est<strong>on</strong>iaFig. 4. Ratio B2/ B dependent <strong>on</strong> relative overburdenheight <strong>and</strong> pipe distancesFig. 2. Shear resistant beam for parallel buried pipesThe c<strong>on</strong>centrati<strong>on</strong> factors B . B for the area beside <strong>and</strong>between the pipes were found with the followingassumpti<strong>on</strong>s:The influenced area for the determinati<strong>on</strong> ofthe c<strong>on</strong>centrati<strong>on</strong> factor B beside the pipe( B1 ) is defined by a line with an inclinati<strong>on</strong> of60° shown in Fig. 3. This angle coincides withthe theoretical slope inclinati<strong>on</strong> of a n<strong>on</strong>cohesivesoil with an internal angle of fricti<strong>on</strong>of ' = 30°.Between the pipes ( B2 ) the full interspace istaken as the area of influence.A calculati<strong>on</strong> method for parallel buried pipes instepped trenches was proposed by Hornung <strong>and</strong> Kittel[7]. With this calculati<strong>on</strong> method the total loading <strong>on</strong><strong>on</strong>e pipe is derived from the sum of the partial loadings,which corresp<strong>on</strong>d to the trench shape to the right <strong>and</strong>left of the pipe. The typical trench c<strong>on</strong>diti<strong>on</strong> for districtheating pipes provides a n<strong>on</strong> stepped trench with theflow <strong>and</strong> return pipes installed <strong>on</strong> the sameunderground level. The presented study was thereforecarried out without employing the Hornung <strong>and</strong> Kittelcalculati<strong>on</strong> method.NUMERICAL INVESTIGATIONSNumerical calculati<strong>on</strong>s were carried out with the twodimensi<strong>on</strong>al finite element program PLAXIS, versi<strong>on</strong>8.6. Two st<strong>and</strong>ard situati<strong>on</strong>s with different outer pipediameters D (DN65, D=140 mm; DN250, D= 400 mm)of two parallel buried district heating pipes wereinvestigated. The distance between the pipes waschosen to be A=10 cm (see Fig. 1). The overburdenheight of the backfill material of the trench wasH/D=3.0. The finite element mesh used for the DN65pipe is shown in Fig. 5 as an example.Fig. 3. Method to determine the c<strong>on</strong>centrati<strong>on</strong> factors forparallel buried pipesThe calculati<strong>on</strong>s by Rizkallah <strong>and</strong> Achmus showed <strong>on</strong>lysmall deviati<strong>on</strong>s for the c<strong>on</strong>centrati<strong>on</strong> factor B of singlepipes <strong>and</strong> the c<strong>on</strong>centrati<strong>on</strong> factor B1 for parallelburied pipes. However, a significant reducti<strong>on</strong> of thevertical stresses (i.e. B2 < B ) was determined betweenthe pipes. As an example, the ratio of the stress factorsis shown in Fig. 4, dependent <strong>on</strong> the relativeoverburden height H/D <strong>and</strong> the relative distance of thepipes A/D.Fig. 5. Finite element mesh for the case DN65, H/D=3The installati<strong>on</strong> process was simulated by a ―stagedc<strong>on</strong>structi<strong>on</strong>‖ process, c<strong>on</strong>sidering a retained trench<strong>and</strong> the backfilling procedure with several layers. Thecompacti<strong>on</strong> process was accounted for by applying astatic distributed load of p=10 kN/m² <strong>on</strong> each of thelayers. Ground water was not c<strong>on</strong>sidered in thisinvestigati<strong>on</strong>.13
S<strong>and</strong> in a medium dense to dense state was assumedas backfill material. The mechanical behaviour of thesoil was modelled with the Mohr-Coulomb c<strong>on</strong>stitutivelaw, which is a linear elastic / ideal plastic materialmodel. The parameters used for the model are shownin Table I.Table I. – Soil parameters used for s<strong>and</strong> in Mohr-Coulombmaterial modelThe <str<strong>on</strong>g>12th</str<strong>on</strong>g> <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g> <strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong> <strong>Cooling</strong>,September 5 th to September 7 th , 2010, Tallinn, Est<strong>on</strong>iaDefiniti<strong>on</strong> <strong>and</strong> UnitSizeUnit weight [kN/m³] 18Oedometric Elasticity Modulus E oed [MPa] 70.5Poiss<strong>on</strong>‘s ratio 0.3Internal angle of fricti<strong>on</strong> ‘ [°] 40Angle of dilatancy [°] 10Interface fricti<strong>on</strong> R inter [1] 0.536Between pipe <strong>and</strong> soil, the Coulomb fricti<strong>on</strong> law with aaccording to Eq. (1).tan Rinter *tan 'i (1)Fig. 7. Horiz<strong>on</strong>tal effective stresses h (DN250 pipe,H/D=3)In Fig. 8 the stress c<strong>on</strong>centrati<strong>on</strong> is shown by thedistributi<strong>on</strong> of the radial c<strong>on</strong>tact pressure for the lefth<strong>and</strong>pipe. In the springline area a maximum value of r =21.44 kN/m² for the radial pressure was obtained.Compared with the calculated average radial pressureof r,avg,calc = 18.81 kN/m² the deviati<strong>on</strong> is about 12.2%.In order to keep the model as simple as possible thepipes were assumed to be rigid.In the numerical calculati<strong>on</strong>s the initial soil stress statedue to the soil unit weight was established first. Theinstallati<strong>on</strong> procedure was then simulated <strong>and</strong> theresults were evaluated.In the first model of pipes with an outer diameter ofD=140mm (DN65), no significant stress c<strong>on</strong>centrati<strong>on</strong>between the pipes was observed. The radial c<strong>on</strong>tactpressure obtained for both pipes is shown in Fig. 6.Fig. 8. C<strong>on</strong>tact pressure <strong>on</strong> the left-h<strong>and</strong> DN250 pipe,H/D=3From the DIN EN 13941 regulati<strong>on</strong> the average radialpressure <strong>on</strong> a single buried pipe can be derived for theinvestigated trench c<strong>on</strong>diti<strong>on</strong> according to Eq. (2).r,avg,13941 D 1k * H * 2 2 (2)Fig. 6. C<strong>on</strong>tact pressure <strong>on</strong> the DN65 pipes, H/D=3However, in the sec<strong>on</strong>d numerical model of pipes withan outer diameter of D=400 mm (DN250), a stressc<strong>on</strong>centrati<strong>on</strong> between the pipes was evident. Thedistributi<strong>on</strong> of horiz<strong>on</strong>tal effective stresses acting afterthe installati<strong>on</strong> process is shown in Fig. 7. The stressesare significantly larger between the pipes than beneaththem.In Table II the results of the numerical investigati<strong>on</strong> arecompared to the expected radial pressure from the DINEN 13941 regulati<strong>on</strong>.Table II. – Average c<strong>on</strong>tact pressure r,avg for H/D=3.0DNSingle pipe according toDIN EN 1394165 6.15 kN/m² 7.25 kN/m²Parallel buried pipeaccording to numericalresults250 17.58 kN/m² 18.81 kN/m²Regarding the average radial c<strong>on</strong>tact pressure thedifference between the expected values from the DIN14
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P-1P-4P-9P-7E-5P-14P-8The 1
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academic access is facilitated as t
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1. CHP system operation in A2. Ther
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is covered by operating HOB. In oth
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produce heat and electricity. Fluct
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In addition, it can also be observe
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