Exercises 3 and 4 Solutions Electric Power System 2015 1(4) Exercises 3 and 4 3.1 V0=0, V1=2200 V, V2=0 Only positive sequence! 3.2 V0=0, V1=0, V2=2200 V Only negative sequence! 3.3 V0=2200 V, V1=0, V2=0 Only zero sequence! 3.4 I1 ZTH1 Pos seq X eq VF + V1 – I2 ZTH2 + X eq Neg seq 3R V2 – I0 ZTH0 Zero seq X eq 3Xn V0 – a) b) + Determine sequence diagrams impedances that will carry current when the load R is connected: Z1=ZTH1+jXeq=j0.12 p.u. Z2=ZTH2+jXeq=j0.12 p.u.Z0=3jXn+jXeq=j0.25 p.u. Zbase=0.42/10 =0.016 R=0.016/0.016 p.u.=1 p.u. VTH 1 1 I1 I2 I0 0.329 9.3p.u. Z1 Z2 Z0 3R j 0.12 j0.12 j0.25 3 1 c) There are no zero-sequence currents on the 10kV-side since these are blocked by the -winding. I1 X”d X eq Znet1 Bus 1 VF Z1 VF VF + V1 – I2 X2 X eq Znet2 Z2 Bus 1 + V2 – I0 X0 X eq Znet0 Z0 Bus 1 V0 – 3.5 OS + IEA Exercises 3 and 4 Solutions Electric Power System 2015 2(4) Max. initial fault current = Subtransient fault current at three-phase short-circuit Least severe fault type = Single-line to ground Convert all values to common base Sbase=100MVA: Network: Vbase=50kV Zbase=(50kV)2/100MVA=25, Rfault=10/25=0.4p.u., Znet1=Znet2=Znet0=ZBUS(1,1)=j0.2p.u., Ibase=100MVA/( 3 50kV)=1.15kA Transformer: Change from 50MVA to 100MVA: Xeq=100/50·0.1=0.2p.u. Generator: From 25MVA to 100MVA: X"d=0.4p.u., X2=0.4p.u., X0=0.2p.u. a) Positive sequence Thévenin equivalent: VF=55kV/50kV=1.1p.u., Z1=(jX"d+jXeq)//Znet1=j(0.4+0.2)//j0.2=j0.15p.u. Three-phase fault: I1=VF/Z1=1.1/j0.15p.u.=-j7.33p.u., I2=I0=0 Ia I 0 7.33 90 Phase currents are: I b A I1 7.33150 p. u. Ic I 2 7.3330 The breaker must be able to interrupt a current of 7.33p.u. or 8468A. b) Negative sequence Thévenin equivalent: Z2=(jX2+jXeq)//Znet2=j0.15p.u. Zero sequence Thévenin equivalent: Z0=Znet0=j0.2p.u. (X0 and Xeq not involved since -winding gives open-circuit) I0=I1=I2=VF/(Z0+Z1+Z2+3Rfault)=1.1/(j0.15+j0.15+j0.2+1.2)=0.84622.6°p.u. Ia I 0 2.54 22.6 A 0 I Phase currents are: b I1 p.u. 0 Ic I 2 A phase current of 2.54p.u. or 2930A should be classified as a fault. 3.6 a) SLG fault phase A at bus 2 with ZF=0: I0 I1 I2 VF Z 0 Z1 Z 2 where VF=1.05 and Z0 is element (2,2) of Zbus0, Z1 is element (2,2) of Zbus1, Z2 is element (2,2) of Zbus2: I0 I1 I2 1.05 j 4.71 j 0.1089 j 0.057 j 0.057 Ia=I0+I1+I2=3I1=14.13 p.u., which agrees with Table 9.4. b) LL fault phases B and C at bus 2 with ZF=0: I0=0, I1 I2 I1 I2 VF where VF=1.05, Z1 and Z2 as in a): Z1 Z 2 1.05 j 9.21 j 0.057 j 0.057 c) LLG fault phases B and C at bus 2 with ZF=0: OS IEA Exercises 3 and 4 Solutions Electric Power System 2015 I1 3(4) Z0 Z2 VF ; I2 I1 ; I0 I1 ; Z2Z0 Z Z Z Z 0 2 0 2 Z1 Z2 Z0 where VF=1.05, Z0, Z1 and Z2 as in a): 1.05 j11.12 j0.057 j0.1089 j0.057 j0.057 j0.1089 j0.1089 I2 j11.12 j7.30 j0.1089 j0.057 j0.057 I0 j11.12 j3.82 j0.1089 j0.057 I1 3.7 Sequence current characteristics and A matrix from formula sheet. Double line-to-ground (I): I1= - (I0+I2) (b), Ib2 Two non-zero phase currents that need not balance each other (C). Ib1 Ic1 Ib Ic I0 Ia=0 Ia1 Ia2 Line-to-line fault (III): Ib2 Ic2 Ib1 Ic1 Ic2 I1= - I2 and I0=0 (a), Ib Two non-zero phase currents must balance each other (B). Ic Ia1 Ia2 Single line-to-ground fault (II): Ib2 I0=I1=I2 (c) Ic2 I0 Ib1 One non-zero phase current (A). Ic1 Ia1 Ia2 Ib=Ic=0 OS IEA I0=Ia=0 Exercises 3 and 4 Solutions Electric Power System 2015 3.8 a ZTH1 Pos. seq. Xeq 3.8 b VTH B1 ZTH2 VTH B1 Xeq Neg. seq. B2 ZTH0 Zero seq. 3.8 c 4(4) B2 Xeq 3Xn 3Xn B0 B0 B0=2504.410-940=5610-6 -1. 20 3 √3 ∙ 10 ∙ 56 ∙ 10 0,65 Ic=|Ia|=3|I1|=1,9 A 3.8 d Z0= 3 ∙ ∙ // ∙ ∙ ∙ ∙ >106 which makes the fault current (very close to) zero. 3.8 e (20/3)/6 kV/k=1,9 A This is equal to Ic, which makes sense: To cancel the fault current, the coil should produce a current equal to Ic but with opposite phase. 3.9 B0=2500.3310-640=4,110-3 -1 3 20 3 3 ∙ 10 ∙ 4.1 ∙ 10 144 3 √3 Changing from overhead line to cable changes Ic by a factor of 48/1.9=75 =(0,33 F/km)/(4.4 nF/km) 3.10 a. IR = (20/3)/3 kV/k=3.8 A b. OS IEA