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SLG fault at bus 3, currents and voltages

Short answer

Bus 3 lies between two delta windings, so Z0 is infinite. Consequently, SLG fault current is zero. Phase voltages: Va=0, Vb=1.732∠-150° pu (115 kV line-to-ground), Vc=1.732∠150° pu (115 kV).

In a power system network shown in figure below, single line to ground (SLG) fault occurs at bus 3. i. Draw the positive, negative and zero sequence networks; ii. Determine phase currents in per units and amperes; iii. Phase voltages in per units and kilovolts. Specifications of the equipments are as under: G1: 100 MVA, 13.8 kV, X1 = X2 = 15% and X0 = 5%; G2: 100 MVA, 13.8 kV, X1 = X2 = 15% and X0 = 5%; G3: 100 MVA, 13.8 kV, X1 = X2 = 15% and X0 = 5%; T1: 100 MVA, 13.8/115 kV, X1 = X2 = X0 = 20%; T2: 100 MVA, 115/13.8 kV, X1 = X2 = X0 = 18%; Line: 100 MVA, 115 kV, X1 = X2 = 30% and X0 = 90%. [Figure: G1 (Y, ungrounded) and G2 (Y grounded) at bus 1 - T1 (Y grounded through j0.01 pu on bus 1 side / Δ) - bus 2 - line - bus 3 - T2 (Δ / Y grounded through 0.02 pu on bus 4 side) - bus 4 - G3 (Y grounded through j0.03 pu)]

Base: 100 MVA; 13.8 kV (generator buses 1 and 4), 115 kV (buses 2 and 3). Pre-fault voltage 1 pu, no load. From the figure: T1 is Yg (through j0.01) on the bus 1 side and Δ on the bus 2 side; T2 is Δ on the bus 3 side and Yg (through 0.02) on the bus 4 side; G1 is ungrounded, G2 solidly grounded, G3 grounded through j0.03.

(i) Sequence networks

Positive (emfs at G1, G2, G3):

 G1 j0.15 \
           (1)-j0.2-(2)-j0.3-(3)-j0.18-(4)-j0.15-G3
 G2 j0.15 /                   |
                              F

Negative: same reactances, no emfs.

Zero:

 G2: ref-j0.05-(1)        G1: open (ungrounded)
 T1: (1)-[3(j0.01)+j0.2]-ref  ;  Δ side (2): open
 line: (2)-j0.9-(3)  -> floating, no ground path
 T2: Δ side (3): open ; (4)-[0.06+j0.18]-ref
 G3: (4)-[j0.05+3(j0.03)]-ref
 -> bus 3 has NO connection to the reference

Because bus 3 sits between the Δ windings of T1 and T2, the zero-sequence impedance seen from bus 3 is infinite: Z0=∞Z_0 = \infty.

Thevenin values: Z1=Z2=j(0.075+0.2+0.3) ∥ j(0.18+0.15)=j0.575∥j0.33=j0.2097Z_1 = Z_2 = j(0.075+0.2+0.3)\ \|\ j(0.18+0.15) = j0.575\|j0.33 = j0.2097 pu.

(ii) Phase currents

Ia0=Ia1=Ia2=1Z1+Z2+Z0=1∞=0I_{a0} = I_{a1} = I_{a2} = \frac{1}{Z_1+Z_2+Z_0} = \frac{1}{\infty} = 0 Ia=Ib=Ic=0 pu=0 AI_a = I_b = I_c = 0\ \text{pu} = 0\ \text{A}

No fault current flows: the 115 kV section between the two deltas is an ungrounded system (only a small capacitive current would flow in practice).

(iii) Phase voltages at bus 3

With no current, Va1=1V_{a1} = 1, Va2=0V_{a2} = 0, and the condition Va=0V_a = 0 forces Va0=−1V_{a0} = -1 pu (the whole neutral shifts):

Va=Va0+Va1+Va2=0Vb=Va0+a2Va1=−1+1∠−120∘=1.732∠−150∘ puVc=Va0+aVa1=−1+1∠120∘=1.732∠150∘ pu\begin{aligned} V_a &= V_{a0}+V_{a1}+V_{a2} = 0 \\ V_b &= V_{a0} + a^2V_{a1} = -1 + 1\angle{-120^\circ} = 1.732\angle{-150^\circ}\ \text{pu} \\ V_c &= V_{a0} + aV_{a1} = -1 + 1\angle{120^\circ} = 1.732\angle{150^\circ}\ \text{pu} \end{aligned}

Base phase voltage at bus 3 =115/3=66.40= 115/\sqrt3 = 66.40 kV:

  • Va=0V_a = 0 kV
  • ∣Vb∣=∣Vc∣=1.732×66.40=115|V_b| = |V_c| = 1.732 \times 66.40 = 115 kV

Results

QuantitypuActual
Ia,Ib,IcI_a, I_b, I_c00 A
VaV_a00 kV
VbV_b1.732∠−150°115 kV
VcV_c1.732∠150°115 kV

The healthy phases rise to full line voltage, showing why ungrounded sections need insulation for line voltage to ground.

✓ Answer checked by Claude Sonnet 5.5

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