L5 Examples Electric Power System 2014 1(2) Voltages, currents and power in AC circuits IL I12 Zth Vth Z ZL V V1 V2 Figure 1 The Thévenin equivalent can Figure 2 The voltage sources can represent represent any point in the electricity generators in a power system. Z represents network. ZL represents an impedance load impedance of power lines and transformers connected to this point. between the two sources. 1. One voltage source Use the circuit in Figure 1 and for each case below Determine numerical values of complex current IL, complex voltage V and magnitude of V in % of Vth. Draw Vth (phase angle = 0), V and IL in the complex plane. Adjust angles for clarity. Determine the complex power S=P+jQ leaving Zth to the right. Describe how angle and magnitude of V relates to those of Vth. a. Wall outlet, Vth=230 V, Zth=1Heater ZL=51. b. Transformer station, Vth=145/3 kV, transformers and cables Zth=j50eating in 1/3 city (we analyze only one of three phases) ZL=1000. c. Transformer station, Vth=145/3 kV, transformers and cables Zth=j50Shunt inductance in one phase ZL=j1400. d. Transformer station, Vth=145/3 kV, transformers and cables Zth=j50Shunt capacitor in one phase ZL=-j1400. 2. Two voltage sources Use the circuit in Figure 2 and for each case below Determine numerical values of the complex current I12. Draw V1, V2 and I12 in the complex plane. Adjust angles for clarity. Determine the complex power S=P+jQ leaving Z to the right. Describe how P and Q relate to magnitude difference between V1 and V2 and angle difference between V1 and V2. a. V1= V2=145/3 kV0, High voltage lines and transformers Z=j50. b. V1=145/3 kV0, V2=145/3 kV-30, High voltage lines and transformers Z=j50. c. V1=145/3 kV0, V2=140/3 kV0, High voltage lines and transformers Z=j50. d. V1=145/3 kV0, V2=150/3 kV0, High voltage lines and transformers Z=j50. OS IEA L5 Examples Electric Power System 2014 1. Solution Vth=230; Vth=145e3/sqrt(3); Vth=145e3/sqrt(3); Vth=145e3/sqrt(3); IL=Vth/(ZL+Zth) 145e3/sqrt(3)=83.7e3 Zth=1; Zth=j*50; Zth=j*50; Zth=j*50; V=ZL*IL IL (A) 1a 4.42 V (V) 98 %1a %1b %1c %1d S (VA) Zth ZL 998 83507 - 4175i, 100 6.99e6 0.0008 – 57.7i 80829 1d 0.0 +62.0i 97 86816 1a. V and Vth RR V<Vth, in phase XL R V<Vth, lags Vth 0.00 +4.67e6i XL XL V<Vth, in phase 104 0.00 - 5.38e6i XL XC V>Vth, in phase 1b. Vth Vth V I I 1c. 1d. I Vth V Vth V V I 2. Solution V1=145e3/sqrt(3); V1=145e3/sqrt(3); V1=145e3/sqrt(3); V1=145e3/sqrt(3); I12=(V1-V2)/Z, V2=145e3/sqrt(3); V2=145e3/sqrt(3)*exp(-j*pi*3/180); V2=140e3/sqrt(3); V2=150e3/sqrt(3); S=V2*conj(I12) I12 (A) 2a V% 226 1b 83.5 - 4.17i 1c ZL=51; ZL=1000; ZL=1400; ZL=-j*1400; S=V*conj(IL) 2(2) S (VA) %2a %2b %2c %2d P Q 0 =0 Arg(V1)=Arg(V2) 0 |V1|=|V2| 2b 87.6269 - 2.2946i 7.3358e+06 - 1.9209e+05i >0 Arg(V1)>Arg(V2) 0 |V1||V2| 2c 0 Z=j*50; Z=j*50; Z=j*50; Z=j*50; 0.0000 -57.7350i 0.0000e+00 + 4.6667e+06i =0 Arg(V1)=Arg(V2) >0 |V1|>|V2| 2d 0.0000 +57.7350i 0.0000e+00 - 5.0000e+06i =0 Arg(V1)=Arg(V2) <0 |V1|<|V2| 2a. 2b. V1=V2 I12=0 V1 I12 V2 2c. I12 OS I12 V1 2d. V1 V2 V2 IEA