Transmission Line Models

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Transmission LineEPO341 Prepared by Fuad Latip TRANSMISSION LINE MODELS 1.Short Transmission Line: below 80km (50 miles) 2.Medium Transmission Line: 80km (50 miles) < Medium TL < 240km (150 miles) 3.Long Transmission Line: above 240km (150 miles) TRANSMISSION LINE PER-PHASE MODEL Figure 1: General Transmission Line per-phase model Thetotalseriesresistance,seriesreactanceandshuntadmittanceoftransmissionlinecanbecalculated from the following equation. R = rd X = xd Y = yd Wherer = resistance /km x = reactance /km y = admittance S/km d = length of transmission line THE SHORT-LENGTH TRANSMISSION LINE ForShorttransmissionline,thecapacitancecanbeneglected.Thisproducesinaper-phasemodel consisting of a series resistance and inductance only. Figure 2: Short-Length Transmission Line per-phase model VS = Sending end VoltageVR = Receiving end Voltage IS = Sending end Current IR = Receiving end Current Transmission LineEPO341 Prepared by Fuad Latip From equivalent circuit it is obvious that I = IS = IR Applying KVL into the per-phase model, the sending voltage VS is related to the receiving voltage VR by the equation VS = VR + ZI = VR + RI + jXLI Or VR = VS - RI - jXLI THE MEDIUM-LENGTH TRANSMISSION LINE Figure 3: Medium-Length Transmission Line per-phase model The values R and L are the total resistance and inductance for the entire line, and the total admittance Y is the shunt admittance distributed over the entire line. To find the equation of medium-length transmission line, Two-port network (ABCD model) analysis has applied. Figure 4: Two port network Transmission LineEPO341 Prepared by Fuad Latip If the network is linear, then an elementary circuit theorem (analogous to Thevenins theorem) states that therelationshipbetweenthesendingandreceivingendvoltagesandcurrentswillbegivenbythe following equations: Refer to figure 3, The current in the receiving end capacitance is given by IC2= IR2 And the current in the series impedance elements will be Isc=IR2+IR Therefore by KVL, the voltage on the sending end of the transmission line will be IS= ZIsc+IR= Z(IC2+ IR) +IR = Z _IR2+ IR] + IR = [z2+1 IR+ZIR----------------------Equation (1) Comparing Equation (1) with ABCD constant equation A =Z2+ 1 AndB = Z The current following in the source will be IS= IC1+Isc= IC1+ IC2+ IR = IS2+ IR2+ IR-------------------------------Equation (2) Transmission LineEPO341 Prepared by Fuad Latip Substituting Equation (1) into Equation (2), we get IS= [z4+ 1 IR+ [z2+ 1 IR------------------Equation (3) Comparing Equation (3) with ABCD constant equation C = _Z4+ 1] And =Z2+ 1 Or D = A Medium Length Transmission Line Constant Note:Ifweignoretheshuntcapacitanceofatransmissionline,theshuntadmittanceY=0,andthe ABCD constant reduce to the short transmission line constant i.e. Short Length Transmission Line Constant A = 1B = ZC = 0D = 1 Transmission LineEPO341 Prepared by Fuad Latip Example A 220kV, 150MVA, 60 Hz three phase transmission line is 140km long. The characteristic parameters of the transmission line are r = 0.12/kmx = 0.88/kmy = 4.1 x 10-6 S/km The voltage at the receiving end of the transmission line is 210kV. Answer the following questions about this transmission line by assuming 1) Short transmission line and 2) Medium transmission line a)What the series impedance and shunt admittance of this transmission line? b)What is the sending end voltage if the line is supplying rated voltage and apparent power at 0.85 PF lagging? at unity PF? At 0.85 PF leading? c)What is the voltage regulation of the transmission line for each of the cases in (b) d)What is the efficiency of the transmission line when it is supplying rated apparent power at 0.85 PF lagging? (Answer will be discussed in class)