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8/10/2019 Tutorial 3 - July 2010
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1. Three 15 MVA, 30 kV synchronous generators A, B, and C are connected via threereactors to a common bus bar, as shown in Figure 1. The neutrals of generators Aand B are solidly grounded, and the neutral of generator C is grounded through a
reactor of 2.0 . The generator data and the reactance of the reactors are tabulatedbelow. A line-to-ground fault occurs on phase a of the common bus bar. Neglect
prefault currents and assume generators are operating at their rated voltage.Determine the fault current in phasea.
Figure 1
The generator base impedance is
== 6015
(30)Z
2
B
The reactor per-unit reactance, and the per-unit generator C neutral reactor are
pu1.0==60
6XR
pu3333.0==602Xn
The positive-sequence impedance network is shown in Figure (a), and the zerosequence impedance network is shown in Figure (b).
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The positive-sequence impedance is
3.0
1
3.0
1
35.0
1++=
1X
1 pu105.0X1 =
The negative-sequence impedance network is the same as the positive-sequenceimpedance network, except for the value of the generator negative-sequencereactance. Therefore, the negative-sequence impedance is
255.0
1
255.0
1
255.0
1++=
2X
1 pu085.0X 2 =
The zero-sequence impedance is
26.0
1
156.0
1
156.0
1++=
0X
1 pu06.0X 0 =
The line-to-ground fault current in phasea is
pu12j)06.0085.0105.0(j
3I3I )0(aa =
++==
2. The reactance data for the power system shown in Figure 2 in per unit on a commonbase is as follows:
X1 = 10 %
X0 = 5 %
X1 = 25 %
X0 = 25 %
X1 = 25 %
X0 = 25 %
XG1 = 10 %
XG0 = 5 %
X1 = 30 %
X0 = 50 %
Figure 2
Obtain the Thevenin sequence impedances for the fault at bus 1 and compute thefault current in per unit for the following faults:(a) A bolted three-phase fault at bus 1.(b) A bolted single line-to-ground fault at bus 1.(c) A bolted line-to-line fault at bus 1.(d) A bolted double line-to-ground fault at bus 1.
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The positive-sequence impedance network is shown below, and impedanceto the point of fault is
pu2275.0j65.035.0
)65.0)(35.0(jZ1 =
+=
Since negative-sequence reactances are the same as positive-sequence reactances,X2=X1= 0.2275.
The zero-sequence impedance network is shown below, and impedance to the pointof fault is
pu1875.0j75.025.0
)75.0)(25.0(jZ0 =
+=
(a) For a bolted three-phase fault at bus 1, the fault current is
pu3956.4j2275.0
1jI f ==
(b) For a bolted single-line to ground fault at bus 1, the fault current is
pu669.4j)1875.02275.02275.0(j
3I3I )0(af =
++==
(c) For a bolted line-to-line fault at bus 1, the fault current in phase b is
pu1978.2j)2275.02275.0(j
1I )1(a =
+=
pu3jI f 3.8067-I(1)
a ==
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(d) For a bolted double line-to-line fault at bus 1, we have
pu02767.3j
)1875.02275.0(
)1875.0)(2275.0(j2275.0j
1I )1(a =
++
=
pu6597.1j02767.3jI )0(a =+
=0.1875)(0.2275
0.2275
pu9792.4jI3I )0(af ==
3. The zero-, positive-, and negative-sequence bus impedance matrices for athree-bus power system are
jZ0 = pu
0.300.080.12
0.080.100.050.120.050.20
1Z = jZ2 = pu
0.250.120.15
0.120.200.100.150.100.16
Determine the per unit fault current and the bus voltages during fault for(a) A bolted three-phase fault at bus 2.(b) A bolted single line-to-ground fault at bus 2.(c) A bolted line-to-line fault at bus 2.(d) A bolted double line-to-ground fault at bus 2.
(a) The symmetrical components of fault current for a bolted balanced three-phasefault at bus 2 is given by
(1)
afI = (1)22
f
Z
V=
j0.20
1= -j5 ; (2)afI = 0 ;
(0)
afI = 0
The fault current
fc
fb
fa
I
I
I
=
2
2
aa1
aa1
111
0
j5-
0
=
0
0
0
305
1505
90-5
For balanced fault we only have the positive-sequence component of voltage. Thus,bus voltages during fault for phasea are
0.50.2
0.11.0
Z
Z1.0V
1
22
1
12)F(1 === p.u.
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00.2
0
Z
ZV
22
F)F(2 === p.u.
0.4
0.2
0.121.0
Z
Z1.0V
1
22
1
32)F(3 === p.u.
(b) The symmetrical components of fault current for a single line-to-groundfault at bus 2 is given by
(1)
afI =(2)
afI =(0)
afI = (0)22
(2)
22
(1)
22
f
ZZZ
V
++
Let0
f 01.0V =
Then (1)afI =(2)
afI =(0)
afI =0.10)0.20(0.20j
01.0 0
++
= 2j
The fault current (1)af(2)
af(1)
af(0)
afaf I3IIII =++= = - j 6; bfI = cfI = 0
The sequence components of voltage at bus 2 are calculated as
0.20)j()0.10j(IZV(0)
af
(0)
22
(0)
a2 === 2
0.60)j2()0.20j(1.0IZVV (1)af(1)
22f
(1)
a2 ===
0.40)j2()j0.20(IZV (2)af(2)
22
(2)
a2 ===
Phase components of line to ground voltage of bus 2 are computed as
c2
b2
a2
V
V
V
=
2
2
aa1
aa1
111
0.40
0.60
0.20
=
The sequence components of voltage at bus 1 are calculated as
0.10)j()0.05j(IZV (0)af(0)
12
(0)
a1 === 2
0.80)j()0.10j(1.0IZVV (1)af(1)
12f
(1)
a1 === 2
0.20)j2()j0.10(IZV (2)af(2)12(2)a1 ===
Phase components of line to ground voltage of bus 1 are computed as
0
0.91650
109.11
0.9165 0109.11
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c1
b1
a1
V
V
V
=
2
2
aa1
aa1
111
0.20
0.80
0.10
=
The sequence components of voltage at bus 3 are calculated as
0.16)j()0.08j(IZV (0)af(0)
32
(0)
a3 === 2
0.76)j()0.12j(1.0IZVV(1)
af
(1)
32f
(1)
a3 === 2
0.24)j2()j0.12(IZV (2)af(2)
32
(2)
a3 ===
Phase components of line to ground voltage of bus 1 are computed as
c3
b3
a3
V
V
V
=
2
2
aa1
aa1
111
0.24
0.76
0.16
=
(c) The symmetrical components of fault current for line-to-line fault at bus 2 are
(0)
afI = 0
(1)
afI = -(2)
afI = (2)22
(1)
22
f
ZZ
V
+=
)0.20(0.20j
01.00
+
= -j2.5
The phase components of fault currents in the fault are
0IIII (2)af(1)
af
(0)
afaf =++=
==+= (1)af(2)
af
(1)
af
2
bf I3jIaIaI -4.33
== bfcf II 4.33
The sequence components of voltage at bus 2 are calculated as
0)()0.10j(IZV (0)af(0)
22
(0)
a2 === 0
0.50)j2.5()0.20j(1.0IZVV (1)af(1)22f(1)a2 ===
0.50)j2.5()j0.20(IZV(2)
af
(2)
22
(2)
a2 ===
Phase components of line to ground voltage of bus 2 are computed as
0.50 00
0.95390
114.79
0.9539 0114.79
0.36 00
0.96250
115.87
0.9625 0115.87
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c2
b2
a2
V
V
V
=
2
2
aa1
aa1
111
0.50
0.50
0
=
The sequence components of voltage at bus 1 are calculated as
0)()0.05j(IZV (0)af(0)
12
(0)
a1 === 0
0.75)j()0.10j(1.0IZVV(1)
af
(1)
12f
(1)
a1 === 5.2
0.25)j2.5()j0.10(IZV (2)af(2)
12
(2)
a1 ===
Phase components of line to ground voltage of bus 1 are computed as
c1
b1
a1
V
V
V
=
2
2
aa1
aa1
111
0.25
0.75
0
=
The sequence components of voltage at bus 3 are calculated as
0)()0.08j(IZV (0)af(0)
32
(0)
a3 === 0
0.70)j()0.12j(1.0IZVV(1)
af
(1)
32f
(1)
a3 === 5.2
0.30)j2.5()j0.12(IZV (2)af(2)
32
(2)
a3 ===
Phase components of line to ground voltage of bus 1 are computed as
c3
b3
a3
V
V
V
=
2
2
aa1
aa1
111
=
0.30
0.70
0
(d) The symmetrical components of fault current for a double line-to-ground fault atbus 2 is given by
.75j
0.10j0.20j
)0.10j()0.20j(0.20j
1.0
ZZ
ZZZ
VI
(0)
22
(2)
22
(0)
22
(2)
22(1)
22
f(1)
af 3=
++
=
++
=
1
0
0
0.6614 0139.11
0.6140130.11
10
0
0.5 0180
0.50
180
1 00
0.60830
145.285
0.6083 0145.285
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j1.25j0.10j0.20
j0.10)j3.75(
ZZ
ZII
(0)
22
(2)
22
(0)
22(1)
af
(2)
af =+
=+
=
j2.5
j0.10j0.20
j0.20)j3.75(
ZZ
ZII
(0)
22
(2)
22
(2)
22(1)
af
(0)
af =
+
=
+
=
Phase components of current at the fault bus are
=++= (2)af(1)
af
(0)
afaf IIII 0
00(2)
af
(1)
af
2(0)
afbf 21025150j2.5IaIaII ++=++= .175.3
= 5.7282 0139.11 0.175.3 302530j2.5IaIaII 0(2)af
2(1)
af
(0)
afcf ++=++=
= 5.7282 0.8940
Fault current =+= cfbff III 7.5090
The sequence components of voltage at bus 2 are calculated as
0.25)j()0.10j(IZV (0)af(0)
22
(0)
a2 === 5.2
0.25)j3.75()0.20j(1.0IZVV (1)af(1)
22f
(1)
a2 ===
0.25)j1.25()j0.20(IZV (2)af(2)
22
(2)
a2 ===
Phase components of line to ground voltage of bus 2 are computed as
c2
b2
a2
V
V
V
=
2
2
aa1
aa1
111
0.25
0.25
0.25
=
The sequence components of voltage at bus 1 are calculated as
0.125)j()0.05j(IZV (0)af(0)
12
(0)
a1 === 5.2
0.625)j3()0.10j(1.0IZVV (1)af(1)
12f
(1)
a1 === 75.
0.125)j1.25()j0.10(IZV (2)af(2)12
(2)a1 ===
Phase components of line to ground voltage of bus 1 are computed as
0.750
0 0
0
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c1
b1
a1
V
V
V
=
2
2
aa1
aa1
111
0.125
0.625
0.125
=
The sequence components of voltage at bus 3 are calculated as
0.20)j()0.08j(IZV (0)af(0)
32
(0)
a3 === 5.2
0.55)j()0.12j(1.0IZVV (1)af(1)
32f
(1)
a3 === 75.3
0.15)j1.25()j0.12(IZV (2)af(2)
32
(2)
a3 ===
Phase components of line to ground voltage of bus 1 are computed as
c3
b3
a3
V
V
V
=
2
2
aa1
aa1
111
0.15
0.55
0.20
=
0.87500
0.500
120
0.50 0120
0.90 00
0.37750
113.413
0.3775 0113.413