About this set. These are original practice questions written
in GATE style for the 2026 Power Systems syllabus, with fully worked
solutions. They are not reproductions of the official GATE 2026 question paper.
A completely transposed single-circuit three-phase overhead line has its three conductors
placed in one horizontal plane. The spacings are \(D_{ab}=4\) m, \(D_{bc}=4\) m and
\(D_{ca}=8\) m. Each conductor has a geometric mean radius of 1.2 cm. The inductance per
phase per kilometre of the line is
- 0.804 mH/km
- 1.208 mH/km
- 1.398 mH/km
- 2.416 mH/km
Solution
For a transposed line the mutual spacing is replaced by the geometric mean of the three
pairwise distances (see Inductance of a Transmission Line):
Equation
\[D_{eq} = \sqrt[3]{D_{ab}D_{bc}D_{ca}} = \sqrt[3]{4 \times 4 \times 8} = \sqrt[3]{128} = 5.0397~\text{m}\]
The inductance per phase per unit length of a transposed line with conductors of geometric
mean radius \(D_s\) is
Equation
\[L = 2 \times 10^{-7}\,\ln\!\left(\frac{D_{eq}}{D_s}\right) \quad \text{H/m}\]
Equation
\[\frac{D_{eq}}{D_s} = \frac{5.0397}{0.012} = 419.98, \qquad \ln(419.98) = 6.0402\]
Equation
\[L = 2 \times 10^{-7} \times 6.0402 = 1.2080 \times 10^{-6}~\text{H/m} = 1.208~\text{mH/km}\]
B
Final Answer
Correct answer: (B) 1.208 mH/km.
A three-phase, 50 Hz medium transmission line is represented by its nominal-\(\pi\)
equivalent. The total series impedance is \(Z = 20 + j60~\Omega\) per phase and the total
shunt admittance is \(Y = j4 \times 10^{-4}~\text{S}\) per phase, the latter being split
equally between the two ends. The line delivers 100 MVA at 0.8 power factor lagging at a
receiving-end line voltage of 220 kV. The sending-end line voltage, in kV, is _____
(round off to one decimal place).
Solution
For the nominal-\(\pi\) model the generalised constants are \(A = D = 1 + \tfrac{ZY}{2}\)
and \(B = Z\) (see Medium Transmission Line). First evaluate \(A\):
Equation
\[ZY = (20 + j60)(j4\times 10^{-4}) = j8\times10^{-3} - 2.4\times10^{-2} = -0.024 + j0.008\]
Equation
\[A = 1 + \frac{ZY}{2} = 1 + (-0.012 + j0.004) = 0.988 + j0.004\]
Take the receiving-end phase voltage as the reference phasor:
Equation
\[V_R = \frac{220 \times 10^{3}}{\sqrt{3}} \angle 0^\circ = 127017.1 \angle 0^\circ~\text{V}\]
Equation
\[|I_R| = \frac{S}{\sqrt{3}\,V_L} = \frac{100 \times 10^{6}}{\sqrt{3} \times 220 \times 10^{3}} = 262.43~\text{A}\]
At 0.8 power factor lagging the current lags \(V_R\) by \(36.87^\circ\):
Equation
\[I_R = 262.43\angle -36.87^\circ = 209.95 - j157.46~\text{A}\]
Now apply \(V_S = A V_R + B I_R\):
Equation
\[A V_R = (0.988 + j0.004)(127017.1) = 125492.9 + j508.1~\text{V}\]
Equation
\[Z I_R = (20 + j60)(209.95 - j157.46) = 13646.5 + j9447.6~\text{V}\]
Equation
\[V_S = 139139.4 + j9955.7~\text{V}, \qquad |V_S| = \sqrt{139139.4^2 + 9955.7^2} = 139495.0~\text{V}\]
This is the phase value; the sending-end line voltage is \(\sqrt{3}\) times as large:
Equation
\[|V_{S,\text{line}}| = \sqrt{3} \times 139495.0 = 241612~\text{V} = 241.6~\text{kV}\]
✓
Final Answer
Correct answer: 241.6 kV.
A synchronous generator is rated 100 MVA, 13.8 kV and has a subtransient reactance of
0.20 pu on its own rating as base. When this machine is included in a system study that
uses a base of 200 MVA and 13.2 kV at the generator terminals, its subtransient reactance
in per unit is _____ (round off to three decimal places).
Solution
Per-unit impedance scales directly with the base MVA and inversely with the square of the
base voltage (see Per-Unit Quantities):
Equation
\[X_{new} = X_{old} \times \frac{S_{base,new}}{S_{base,old}} \times \left(\frac{V_{base,old}}{V_{base,new}}\right)^{2}\]
Equation
\[X_{new} = 0.20 \times \frac{200}{100} \times \left(\frac{13.8}{13.2}\right)^{2} = 0.20 \times 2 \times 1.09298\]
Equation
\[X_{new} = 0.4372~\text{pu}\]
The reactance grows because the new base MVA is larger, and grows a little further because
the new base voltage is smaller than the machine rating.
✓
Final Answer
Correct answer: 0.437 pu.
A two-bus system has bus 1 as the slack bus with \(V_1 = 1.0\angle 0^\circ\) pu. The two
buses are joined by a single line of series admittance \(y_{12} = 2 - j6\) pu, and the line
charging is neglected. Bus 2 is a load bus drawing \(0.5 + j0.2\) pu. Starting from a flat
start \(V_2^{(0)} = 1.0\angle 0^\circ\) pu, the magnitude of \(V_2\) after one Gauss-Seidel
iteration is _____ pu (round off to four decimal places).
Solution
With no shunt elements the bus admittance matrix entries for bus 2 are
\(Y_{22} = y_{12} = 2 - j6\) and \(Y_{21} = -y_{12} = -2 + j6\). The scheduled injection at
a load bus is negative: \(P_2 = -0.5\) pu and \(Q_2 = -0.2\) pu. The Gauss-Seidel update
(see Gauss-Seidel Load Flow) is
Equation
\[V_2^{(1)} = \frac{1}{Y_{22}}\left[\frac{P_2 - jQ_2}{\left(V_2^{(0)}\right)^{*}} - Y_{21}V_1\right]\]
Evaluate the two terms in the bracket:
Equation
\[\frac{P_2 - jQ_2}{\left(V_2^{(0)}\right)^{*}} = \frac{-0.5 - j(-0.2)}{1.0} = -0.5 + j0.2\]
Equation
\[-Y_{21}V_1 = -(-2 + j6)(1.0) = 2 - j6\]
Equation
\[\text{bracket} = (-0.5 + j0.2) + (2 - j6) = 1.5 - j5.8\]
Divide by \(Y_{22}\), rationalising with the conjugate \(2 + j6\):
Equation
\[V_2^{(1)} = \frac{1.5 - j5.8}{2 - j6} = \frac{(1.5 - j5.8)(2 + j6)}{2^2 + 6^2} = \frac{37.8 - j2.6}{40} = 0.9450 - j0.0650\]
Equation
\[\left|V_2^{(1)}\right| = \sqrt{0.9450^2 + 0.0650^2} = \sqrt{0.89725} = 0.9472~\text{pu} \;\angle -3.93^\circ\]
✓
Final Answer
Correct answer: 0.9472 pu.
An unloaded 50 MVA, 11 kV synchronous generator has its neutral solidly grounded. Its
sequence reactances on the machine rating as base are \(X_1 = 0.25\) pu, \(X_2 = 0.20\) pu
and \(X_0 = 0.05\) pu; all resistances are negligible. With the prefault terminal voltage
at 1.0 pu, a single line-to-ground fault occurs on phase a at the machine terminals. The
magnitude of the fault current is
- 2.62 kA
- 5.25 kA
- 15.75 kA
- 47.24 kA
Solution
For a single line-to-ground fault the three sequence networks are connected in series, so
the three sequence currents are equal (see Single Line-to-Ground Fault):
Equation
\[I_{a1} = I_{a2} = I_{a0} = \frac{E_a}{j(X_1 + X_2 + X_0)} = \frac{1.0}{j(0.25 + 0.20 + 0.05)} = \frac{1.0}{j0.50} = -j2.0~\text{pu}\]
The faulted phase current is the sum of the three sequence components:
Equation
\[I_a = I_{a0} + I_{a1} + I_{a2} = 3I_{a1} = -j6.0~\text{pu}, \qquad |I_a| = 6.0~\text{pu}\]
Convert to amperes using the base current at the 11 kV level:
Equation
\[I_{base} = \frac{S_{base}}{\sqrt{3}\,V_{base}} = \frac{50 \times 10^{6}}{\sqrt{3} \times 11 \times 10^{3}} = 2624.3~\text{A}\]
Equation
\[|I_f| = 6.0 \times 2624.3 = 15746~\text{A} = 15.75~\text{kA}\]
C
Final Answer
Correct answer: (C) 15.75 kA.
The line currents of a three-phase, four-wire system are measured as
\(I_a = 6\angle 0^\circ\) A, \(I_b = 4\angle -90^\circ\) A and \(I_c = 8\angle 150^\circ\) A.
The zero-sequence component of the phase-a current is
- 0 A
- \(0.309\angle 180^\circ\) A
- \(0.928\angle 180^\circ\) A
- \(3.000\angle 0^\circ\) A
Solution
The zero-sequence current is the average, not the sum, of the three phase currents
(see Symmetrical Components):
Equation
\[I_{a0} = \frac{1}{3}\left(I_a + I_b + I_c\right)\]
Resolve each phasor into rectangular form:
Equation
\[I_a = 6 + j0, \qquad I_b = -j4, \qquad I_c = 8(\cos 150^\circ + j\sin 150^\circ) = -6.9282 + j4\]
Equation
\[I_a + I_b + I_c = (6 - 6.9282) + j(-4 + 4) = -0.9282 + j0\]
Equation
\[I_{a0} = \frac{-0.9282}{3} = -0.3094 = 0.3094\angle 180^\circ~\text{A}\]
The neutral current, for reference, is \(I_n = 3I_{a0} = 0.928\angle 180^\circ\) A, which is
choice C. That is the trap: option C omits the factor of one third.
B
Final Answer
Correct answer: (B) \(0.309\angle 180^\circ\) A.
A lossless synchronous generator with inertia constant \(H = 5\) MJ/MVA is connected to an
infinite bus through a transmission link. In the prefault condition the power-angle
characteristic is \(P_e = 2.0\sin\delta\) pu and the constant mechanical input is
\(P_m = 1.0\) pu. A three-phase fault at the generator terminals reduces the electrical
power output to zero, and the fault is cleared by restoring the original prefault network.
For a system frequency of 50 Hz, the critical clearing time is _____ s (round off to three
decimal places).
Solution
The initial rotor angle follows from \(P_m = P_{max}\sin\delta_0\):
Equation
\[\delta_0 = \sin^{-1}\!\left(\frac{1.0}{2.0}\right) = 30^\circ = 0.5236~\text{rad}\]
Because the postfault characteristic is identical to the prefault one, the maximum swing
angle is
Equation
\[\delta_{max} = 180^\circ - \delta_0 = 150^\circ = 2.6180~\text{rad}\]
Applying the equal-area criterion with zero power transfer during the fault, the
accelerating area from \(\delta_0\) to \(\delta_{cc}\) must equal the decelerating area from
\(\delta_{cc}\) to \(\delta_{max}\) (see Equal Area Criterion):
Equation
\[\cos\delta_{cc} = \frac{P_m(\delta_{max} - \delta_0)}{P_{max}} + \cos\delta_{max}\]
Equation
\[\cos\delta_{cc} = \frac{1.0(2.6180 - 0.5236)}{2.0} + \cos 150^\circ = 1.0472 - 0.8660 = 0.1812\]
Equation
\[\delta_{cc} = \cos^{-1}(0.1812) = 79.56^\circ = 1.3886~\text{rad}\]
During the fault the electrical power is zero, so the swing equation integrates in closed
form and the clearing time corresponding to \(\delta_{cc}\) is
Equation
\[t_{cc} = \sqrt{\frac{2H(\delta_{cc} - \delta_0)}{\pi f P_m}} = \sqrt{\frac{2 \times 5 \times (1.3886 - 0.5236)}{\pi \times 50 \times 1.0}}\]
Equation
\[t_{cc} = \sqrt{\frac{8.650}{157.08}} = \sqrt{0.05507} = 0.2347~\text{s}\]
✓
Final Answer
Correct answer: 0.235 s (critical clearing angle \(79.56^\circ\)).
Two thermal units supply a total load of 250 MW. Their fuel cost characteristics, in
Rs./h with the outputs in MW, are
Equation
\[C_1 = 0.02P_1^{2} + 16P_1 + 50, \qquad C_2 = 0.04P_2^{2} + 12P_2 + 80\]
The generation limits are \(50 \le P_1 \le 200\) MW and \(30 \le P_2 \le 100\) MW.
Transmission losses are neglected. For the economic dispatch, the output of unit 1 is
_____ MW.
Solution
The incremental cost of each unit is the derivative of its cost characteristic:
Equation
\[\frac{dC_1}{dP_1} = 0.04P_1 + 16, \qquad \frac{dC_2}{dP_2} = 0.08P_2 + 12\]
Ignoring the limits for the moment, equal incremental cost with
\(P_1 + P_2 = 250\) gives (see Economic Load Dispatch)
Equation
\[0.04(250 - P_2) + 16 = 0.08P_2 + 12 \Rightarrow 26 - 0.04P_2 = 0.08P_2 + 12\]
Equation
\[0.12P_2 = 14 \Rightarrow P_2 = 116.67~\text{MW}, \qquad P_1 = 133.33~\text{MW}\]
This trial value of \(P_2\) exceeds its 100 MW upper limit, so it is not feasible. Unit 2
is therefore held at its limit and the balance is taken by unit 1:
Equation
\[P_2 = 100~\text{MW}, \qquad P_1 = 250 - 100 = 150~\text{MW}\]
The system incremental cost is now set by the free unit:
Equation
\[\lambda = 0.04(150) + 16 = 22~\text{Rs./MWh}\]
The solution is consistent because the fixed unit sits at its maximum and its incremental
cost there, \(0.08(100) + 12 = 20\) Rs./MWh, is below \(\lambda\); loading it further would
still be cheap, but the limit forbids it. Both outputs lie within the stated ranges.
✓
Final Answer
Correct answer: \(P_1 = 150\) MW (with \(P_2 = 100\) MW, \(\lambda = 22\) Rs./MWh).
A feeder is protected by an IDMT overcurrent relay of the normal inverse type fed from a
current transformer of ratio 400/5 A. The relay plug setting is 125 percent and the time
multiplier setting is 0.3. The relay operating time is given by
Equation
\[t = \frac{0.14 \times \text{TMS}}{(\text{PSM})^{0.02} - 1}~\text{s}\]
For a symmetrical fault current of 4000 A in the primary, the relay operating time is
_____ s (round off to three decimal places).
Solution
Refer the fault current to the relay coil through the CT ratio:
Equation
\[I_{relay} = 4000 \times \frac{5}{400} = 50~\text{A}\]
A plug setting of 125 percent means the relay picks up at 1.25 times the CT secondary
rated current:
Equation
\[I_{pickup} = 1.25 \times 5 = 6.25~\text{A}\]
The plug setting multiplier is the ratio of the two:
Equation
\[\text{PSM} = \frac{50}{6.25} = 8\]
Evaluate the characteristic. Since \(8^{0.02} = e^{0.02\ln 8} = e^{0.041589} = 1.042466\),
Equation
\[t = \frac{0.14 \times 0.3}{1.042466 - 1} = \frac{0.042}{0.042466} = 0.989~\text{s}\]
✓
Final Answer
Correct answer: 0.989 s.
A lossless 400 kV three-phase transmission line has a series inductance of 1.0 mH/km and a
shunt capacitance of 11.1 nF/km per phase. The surge impedance loading of the line is
- 267 MW
- 533 MW
- 800 MW
- 1066 MW
Solution
For a lossless line the surge impedance depends only on the ratio of the distributed
parameters, not on the line length (see Surge Impedance Loading):
Equation
\[Z_c = \sqrt{\frac{L}{C}} = \sqrt{\frac{1.0 \times 10^{-3}}{11.1 \times 10^{-9}}} = \sqrt{90090} = 300.2~\Omega\]
The surge impedance loading is the three-phase power delivered when the line is terminated
in \(Z_c\), with \(V_L\) the rated line-to-line voltage:
Equation
\[\text{SIL} = \frac{V_L^{2}}{Z_c} = \frac{(400 \times 10^{3})^{2}}{300.2} = \frac{1.6 \times 10^{11}}{300.2}\]
Equation
\[\text{SIL} = 5.33 \times 10^{8}~\text{W} = 533~\text{MW}\]
B
Final Answer
Correct answer: (B) 533 MW.