[12.] W.H. Zhang, S.J. Lee, M.S. Choi and S. Oda,"Considerations on Distance Relay Setting forTransmission Line with STATCOM", 2010 IEEE, Powerand Energy Society General Meeting, USA, 25‐29 July2010.[13.] F.A. Albasri, T.S. Sidhu and R.K. Varma, "PerformanceComparison of Distance Protection Schemes for Shunt‐FACTS Compensated Transmission Lines", IEEETransactions on Power Delivery, Vol. 22, No. 4, pp.2116‐2125, October 2007.[14.] S. Jamali, A. Kazemi and H. Shateri, "MeasuredImpedance by Distance Relay for Inter Phase Faults inthe Presence of SVC on Double‐circuit Lines", IET 11 thConference on Developments in Power SystemProtection (DPSP’12), Birmingham, UK, 23 ‐ 26 April2012.[15.] J. G. Agrawal and K.D. Joshi, "Experimental Study ofSome Variable Impedance Type FACTS Devices", 4 thInternational Conference on Emerging Trends inEngineering & Technology (ICETET’11), Nagpur, India,18‐20 November, 2011.[16.] L. F. W. de S o w E. H. Watanabe and M. Aredes, "GTOControlled Series Capacitors: Multi‐module and MultipulseArrangements", IEEE Transaction on PowerDelivery, Vol. 15, No. 2. pp. 725‐731, April 2000.[17.] K.K. Sen and M.L. Sen, Introduction to FACTSControllers: Theory, Modeling and Applications, JohnWiley & Sons, Inc., and IEEE Press, New Jersey, USA,2009.[18.] M. Zellagui and A. Chaghi, "MHO Distance Relay ofTransmission Line High Voltage using SeriesCompensation in Algerian Networks", Journal of ACTAElectrotehnica, Vol. 52, No. 3, pp. 126‐133, October 2011.[19.] L. Gérin‐Lajoie, "A MHO Distance Relay Device in EMTPWorks", Electric Power Systems Research (EPSR), Vol.79, No. 3, pp. 484‐49, March 2009.[20.] D. Sweeting, "Applying IEC 60909, Short‐circuitCurrent Calculations", 58 th Annual IEEE, 2011 Record ofConference Papers Industry Applications Society, 19‐21September 2011.[21.] Ha Heng Xu and Zhang BaoHui, "Study on ReactanceRelays for Single Phase to Earth Fault on EHVTransmission Lines", International Conference onPower System Technology (PowerCon’04), 21‐24November 2004.[22.] S. Jamali and H. Shateri, "Impedance Based FaultLocation Method for Single Phase to Earth Faults inTransmission Systems", 10 th IET InternationalConference on Developments in Power SystemProtection (DPSP’10), 29 March ‐ 1 April, 2010.[23.] Sonelgaz Group,"Electrical Networks High Voltage 220kV", Company of Electrical Transmission, GRTE, Alger,Algeria, 30 December 2011.ACTA TECHNICA CORVINIENSIS – Bulletin of EngineeringACTA TECHNICA CORVINIENSIS – BULLETIN of ENGINEERINGISSN: 2067‐3809 [CD‐Rom, online]copyright © UNIVERSITY POLITEHNICA TIMISOARA,FACULTY OF ENGINEERING HUNEDOARA,5, REVOLUTIEI, 331128, HUNEDOARA, ROMANIAhttp://acta.fih.upt.ro862012. Fascicule 3 [July–September]
1. Emil RAGAN, 2. Marcel FEDÁK, 3. Pavol SEMANČOHEATING PROCESS MODELING FOR DIE‐CASTING JETS ON THEMACHINES WITH HOT CHAMBER1. FACULTY OF MANUFACTURING TECHNOLOGIES OF TECHNICAL UNIVERSITY OF KOŠICE WITH A SEAT IN PREŠOV, DEPARTAMENT OF TECHNOLOGICALSYSTEMS OPERATION, PREŠOV, SLOVAKIA2‐3. FACULTY OF MANUFACTURING TECHNOLOGIES OF TECHNICAL UNIVERSITY OF KOŠICE WITH A SEAT IN PREŠOV, DEPARTMENT OF MANUFACTURINGMANAGEMENT, PREŠOV, SLOVAKIAABSTRACT: In general the application of die‐casting technology in foundries that are focused on non ferrous metals allowsproducing cast parts with specific properties. Another advantage of pressure die‐casting technology with hot chamber isthe possibility of production of precision cast parts in low dimensional tolerances, often without further machining.Castings have got smooth surface, good mechanical properties, and they also may have complex construction workability.Required qualitative properties of castings produced with the pressure die‐casting technology with hot chamber aredependent on several parameters, which include holding stable temperature of the die‐casting nozzle. Therefore in thispaper we proposed the mathematical model as one of the method how to control heating die‐casting nozzle of the hotchamber pressure die‐casting machine using a gas torch.KEYWORDS: Pressure die‐casting, die‐casting nozzle, hot chamber pressure die‐casting machineINTRODUCTIONHigh pressure die‐casting technology in foundriesprocessing non‐ferrous molten metal metals allowsproducing casting of various shapes with specificproperties. The advantages of applying the technologyof high pressure die casting using hot chamber is thepossibility of precision castings in low dimensionaltolerance [1,2] .These castings have a smooth surface often withoutany further machining, and they also have goodmechanical properties [3]. This technology mayproduce castings with complex construction. Thequality of the castings depends on several parameters.One of the important parameter is control andregulation of temperature stability of nozzle [4,5].During the operation of pressure die‐casting machineswith hot chamber dynamic changes occur mainly intemperature time casting nozzle according to thecasting machine cycle. It is needed to hold thetemperature of casting nozzle at optimum valuetherefore it is necessary to eliminate dynamic changes.Given the operation consuming conditions during thedie‐casting process the nozzle is regulated bycontrolled gas torch. For regulation of nozzletemperature, there are several types of regulation[2,6].In this paper we focus on the compilation of modelwith simple control loop with a mathematicaldescription of the regulated system, and also on thecreation of transitional characteristic with regulatorydesign. Simple control‐loop that is formed by thetorch that heats the nozzle of pressure die‐castingmachine uses the proposed proportional regulatory.EQUATION MODEL DEFINITION OF REGULATORY SYSTEMFor appropriateness of the solutions it is firstlynecessary to derive an equation describing thedependence of torch gas flow on temperature ofcasting nozzle as the equation of the regulatorysystem. In the regulatory system the gas flow of thegas torch is referred as input value q and thetemperature difference of the nozzle expressed as T‐T 0 and surroundings temperature is an output variable[4].For the casting nozzle we can determine equation forthermal balance:nQ = Q +(1)1 2 Q3where: Q 1 ‐ amount of the heat per time unitgenerated by burning gas in torch, nQ 1 ‐ amount of theheat per time unit generated by burning gas in torchthat crossed into nozzle, Q 2 ‐ amount of the heat pertime unit generated by burning gas in torch that heatsnozzle, Q 3 ‐ heat loss per time unit.Variable Q 1 can be expressed as:Q 1 = ql(2)where: q ‐ gas flow of the torch, l ‐ calorific value ofthe gas.Variable Q 2 is expressed as:dTQ 2 = cm(3)dtwhere: c ‐ specific heat of the nozzle, m ‐ weight of thenozzle, T ‐ nozzle temperature, t ‐ time.Q = kSp ( T − T 0 )(4)where: k ‐ heat transfer coefficient from the nozzleinto the surroundings, S p ‐ surface area of the nozzle,T 0 ‐ surroundings temperature.© copyright FACULTY of ENGINEERING ‐ HUNEDOARA, ROMANIA 87
- Page 2 and 3:
ACTA TECHNICA CORVINIENSIS- BULLETI
- Page 4 and 5:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 6 and 7:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 8 and 9:
Regional Editors from MALAYSIAAbdel
- Page 10 and 11:
Imre TIMÁRUniversity of Pannonia,
- Page 12 and 13:
Ioan MILOŞANTransilvania Universit
- Page 14 and 15:
Member from GREECENicolaos VAXEVANI
- Page 16 and 17:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 18 and 19:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 20 and 21:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 22 and 23:
two decades are seismically deficie
- Page 24 and 25:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 26 and 27:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 28 and 29:
The Euler ecuation about the condit
- Page 30 and 31:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 32 and 33:
examination centre of the Hungarian
- Page 34 and 35:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 36 and 37: elieve that they are communicating
- Page 38 and 39: converting the data also increases
- Page 40 and 41: REFERENCES[1.] Bhavyesh Divecha, Aj
- Page 42 and 43: In addition, API (Application Progr
- Page 44 and 45: The new protocol has to be implemen
- Page 46 and 47: compressor, the now hot and highly
- Page 48 and 49: Figure 7. Pressure ratio of evapora
- Page 50 and 51: Physical data model (MFD) is obtain
- Page 52 and 53: The new project which now includes
- Page 54 and 55: Figure 3. Materials evolutionThe pr
- Page 56 and 57: (GPa) and weight used in the textil
- Page 58 and 59: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 60 and 61: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 62 and 63: A machine vision‐guided plant sen
- Page 64 and 65: During the experiment, non‐unifor
- Page 66 and 67: espectively velocities hodograph (v
- Page 68 and 69: generation and thermal‐diffusion
- Page 70 and 71: 70(Pr−1)=bGm( R −cPr)( − M+c
- Page 72 and 73: 72Figure 12: Sherwood Number for di
- Page 74 and 75: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 76 and 77: The hardware components offer the p
- Page 78 and 79: Markers 1 (t=‐60 ms) and 2 (t=‐
- Page 80 and 81: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 82 and 83: compensation, apply dynamic control
- Page 84 and 85: A. Impact on transmission line prot
- Page 88 and 89: Substituting equations (2), (3), (4
- Page 90 and 91: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 92 and 93: the tribological experiment to simu
- Page 94 and 95: It is difficult to determine temper
- Page 96 and 97: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 98 and 99: where: “ν ” represents the con
- Page 100 and 101: Figure 10. The velocity field in a
- Page 102 and 103: made on demand. In this type of pro
- Page 104 and 105: traditional MANET routing protocol
- Page 106 and 107: and classification,” In Journal o
- Page 108 and 109: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 110 and 111: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 112 and 113: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 114 and 115: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 116 and 117: equipped with tube made from stainl
- Page 118 and 119: Fig. 10 ‐ The die, the blank hold
- Page 120 and 121: desktop, it must be based on runtim
- Page 122 and 123: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 124 and 125: database, which makes it possible t
- Page 126 and 127: technology - „Applied logistics
- Page 128 and 129: increase in one of the factors lead
- Page 130 and 131: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 132 and 133: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 134 and 135: ACTA TECHNICA CORVINIENSIS - Bullet
- Page 136 and 137:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 138 and 139:
ACTA TECHNICA CORVINIENSIS - Bullet
- Page 140 and 141:
ACTA TECHNICA CORVINIENSIS - Bullet