About this set. These are original practice questions written
in GATE style for the 2026 Power Electronics syllabus, with fully worked
solutions. They are not reproductions of the official GATE 2026 question paper.
Question 01 · 1 markQuestion 1
Among the devices listed below, the one that cannot block a reverse voltage
across its main terminals, because a parasitic diode is formed as an inherent
part of its structure, is the
- silicon controlled rectifier (SCR)
- symmetric-blocking gate turn-off thyristor (GTO)
- n-channel power MOSFET
- reverse-blocking IGBT
Solution
A vertical n-channel power MOSFET is built on an \(n^{+}\) substrate (drain) with an
\(n^{-}\) drift region, a \(p\) body and an \(n^{+}\) source. The source metallisation
deliberately shorts the \(n^{+}\) source to the \(p\) body to suppress the parasitic
\(npn\) transistor. That short leaves the \(p\) body and the \(n^{-}\) drift region
permanently connected between source and drain as a \(pn\) junction, which is the
body diode. When the drain is taken negative with respect to the source this
diode is forward biased and conducts, so no reverse voltage can be sustained.
The SCR and the symmetric GTO both contain a reverse-blocking junction by design,
and the reverse-blocking IGBT is fabricated with a deep isolation diffusion
precisely to give it that capability. Only the MOSFET has an unavoidable
antiparallel diode. The characteristics of the switch family are collected in
Chapter 5.
C
Final Answer
Correct answer: (C) n-channel power MOSFET
Question 02 · 2 marksQuestion 2
A thyristor is connected in series with a load consisting of \(R = 20\,\Omega\) in
series with \(L = 0.5\) H, the combination being fed from a 100 V DC supply. The
thyristor is triggered by a single gate pulse of duration 50 \(\mu\)s. The
anode current at the instant the gate pulse ends is _____ mA.
Solution
With the thyristor in conduction the loop equation is
Equation
\[V = Ri + L\frac{di}{dt}, \qquad i(0) = 0\]
whose solution is the standard first-order rise
Equation
\[i(t) = \frac{V}{R}\left(1 - e^{-Rt/L}\right)\]
The time constant is \(L/R = 0.5/20 = 25\) ms, so in 50 \(\mu\)s the exponent is very
small:
Equation
\[\frac{Rt}{L} = \frac{20 \times 50\times 10^{-6}}{0.5} = 2\times 10^{-3}\]
Equation
\[i(50\,\mu s) = \frac{100}{20}\left(1 - e^{-0.002}\right) = 5\left(1.998\times 10^{-3}\right) = 9.99\times 10^{-3}~\text{A}\]
So the anode current reaches only 9.99 mA. The same figure comes out of the
short-time approximation \(i \approx (V/L)t = (100/0.5)(50\times10^{-6}) = 10\) mA,
which confirms the arithmetic. If the latching current of this device were, say,
50 mA, the thyristor would revert to the blocking state the moment the gate pulse
was withdrawn; a highly inductive load therefore demands a pulse train or a
sustained gate signal, as discussed in
Chapter 4.
✓
Final Answer
Correct answer: 9.99 mA
Question 03 · 1 markQuestion 3
A single-phase fully controlled bridge converter is supplied from a 230 V, 50 Hz
source of negligible impedance. The load is highly inductive, so the load current
is continuous and ripple-free at 10 A. For a firing angle of 45°, the average
output voltage is _____ V.
Solution
With continuous conduction each pair of thyristors conducts for a half cycle
beginning at \(\omega t = \alpha\), so the output voltage over one repetition
interval of \(\pi\) is \(v_o = V_m\sin\omega t\) for
\(\alpha \le \omega t \le \alpha + \pi\). Averaging,
Equation
\[V_{dc} = \frac{1}{\pi}\int_{\alpha}^{\alpha+\pi} V_m \sin\omega t\; d(\omega t) = \frac{2V_m}{\pi}\cos\alpha\]
With \(V_m = \sqrt{2}\times 230 = 325.27\) V,
Equation
\[\frac{2V_m}{\pi} = \frac{2 \times 325.27}{\pi} = 207.08~\text{V}\]
Equation
\[V_{dc} = 207.08 \times \cos 45^\circ = 207.08 \times 0.7071 = 146.4~\text{V}\]
The load current does not enter the result at all, provided conduction stays
continuous. See
Chapter 8.
✓
Final Answer
Correct answer: 146.4 V
Question 04 · 2 marksQuestion 4
A single-phase AC voltage controller uses two thyristors in antiparallel to feed
a purely resistive load of 10 \(\Omega\) from a 230 V, 50 Hz supply. Both devices
are fired symmetrically at a firing angle of 90°. The power delivered to the
load is _____ W.
Solution
With a resistive load each thyristor conducts from \(\alpha\) to \(\pi\) in its own
half cycle, and the output voltage is the supply voltage over that interval and
zero otherwise. Over a half-cycle repetition interval,
Equation
\[V_{o,rms}^{2} = \frac{1}{\pi}\int_{\alpha}^{\pi} \left(V_m \sin\omega t\right)^{2} d(\omega t) = \frac{V_m^{2}}{2\pi}\int_{\alpha}^{\pi}\left(1 - \cos 2\omega t\right) d(\omega t)\]
Equation
\[V_{o,rms} = V_s \sqrt{\frac{1}{\pi}\left[\pi - \alpha + \frac{\sin 2\alpha}{2}\right]}\]
At \(\alpha = 90^\circ = \pi/2\) the term \(\sin 2\alpha = \sin 180^\circ = 0\), so
Equation
\[V_{o,rms} = 230\sqrt{\frac{\pi - \pi/2}{\pi}} = 230\sqrt{0.5} = 162.63~\text{V}\]
The load being resistive, the power follows directly:
Equation
\[P = \frac{V_{o,rms}^{2}}{R} = \frac{230^{2}\times 0.5}{10} = \frac{26450}{10} = 2645~\text{W}\]
Firing at 90° halves the power relative to full conduction (5290 W), not the
voltage. More on this converter in
Chapter 21.
✓
Final Answer
Correct answer: 2645 W
Question 05 · 2 marksQuestion 5
A type-A (first-quadrant) chopper operates from a 200 V DC source and feeds a
load consisting of a resistance of 0.5 \(\Omega\) in series with a constant
counter-emf of 100 V and a large smoothing inductance. The chopping frequency is
high enough that the load current may be taken as ripple-free. For a duty ratio
of 0.7, the average load current is _____ A.
Solution
In a step-down chopper the load is connected to the source for \(DT\) and
freewheels through the diode for \((1-D)T\), so the average output voltage is
Equation
\[V_o = D\,V_s = 0.7 \times 200 = 140~\text{V}\]
Averaging the load loop equation over one chopping period, the inductor voltage
averages to zero in steady state, leaving
Equation
\[V_o = I_a R + E\]
Equation
\[I_a = \frac{V_o - E}{R} = \frac{140 - 100}{0.5} = \frac{40}{0.5} = 80~\text{A}\]
Note how sensitive the current is to duty ratio when the counter-emf is large:
raising \(D\) from 0.7 to 0.75 would take \(V_o\) to 150 V and the current to 100 A.
This is the sizing problem that dominates chopper-fed drives, treated in
Chapter 11.
✓
Final Answer
Correct answer: 80 A
Question 06 · 2 marksQuestion 6
A single-phase full-bridge voltage source inverter operates in square-wave mode
from a 200 V DC link, producing an output voltage that alternates between
\(+200\) V and \(-200\) V with equal half-periods. The total harmonic distortion of
the output voltage, referred to the fundamental, is _____ %.
Solution
The Fourier series of a symmetrical square wave of amplitude \(V_{dc}\) contains
only odd harmonics:
Equation
\[v_o(t) = \sum_{n = 1,3,5,\dots} \frac{4V_{dc}}{n\pi}\sin\left(n\omega t\right)\]
The rms value of the fundamental is therefore
Equation
\[V_1 = \frac{4V_{dc}}{\pi\sqrt{2}} = \frac{4 \times 200}{\pi\sqrt{2}} = \frac{800}{4.4429} = 180.06~\text{V}\]
The total rms value is read straight off the waveform, since the magnitude is
\(V_{dc}\) at every instant:
Equation
\[V_{rms} = V_{dc} = 200~\text{V}\]
The harmonic content is what is left when the fundamental is removed in the
mean-square sense:
Equation
\[\text{THD} = \frac{\sqrt{V_{rms}^{2} - V_1^{2}}}{V_1} = \frac{\sqrt{200^{2} - 180.06^{2}}}{180.06}\]
Equation
\[= \frac{\sqrt{40000 - 32421.6}}{180.06} = \frac{\sqrt{7578.4}}{180.06} = \frac{87.05}{180.06} = 0.4834\]
So the distortion is 48.34 %, and note that it does not depend on \(V_{dc}\): both
numerator and denominator scale with it. This fixed, large distortion is the
reason square-wave operation is replaced by modulation whenever the load is a
motor. See
Chapter 16.
✓
Final Answer
Correct answer: 48.34 %
Question 07 · 2 marksQuestion 7
A three-phase voltage source inverter with a DC-link voltage of 600 V is
controlled by sinusoidal pulse width modulation with a modulation index (amplitude
modulation ratio) of 0.9. The frequency modulation ratio is large and the
inverter operates in the linear modulation range. The rms value of the
fundamental component of the line-to-line output voltage is _____ V.
Solution
In the linear range of sinusoidal PWM the peak of the fundamental pole voltage,
measured with respect to the DC-link midpoint, is
Equation
\[\hat{V}_{a0,1} = m_a \frac{V_{dc}}{2}\]
The fundamental line-to-line voltage is built from two pole voltages displaced by
120°, which multiplies the magnitude by \(\sqrt{3}\):
Equation
\[\hat{V}_{ab,1} = \sqrt{3}\, m_a \frac{V_{dc}}{2}\]
Dividing by \(\sqrt{2}\) to convert peak to rms,
Equation
\[V_{ab,1(rms)} = \frac{\sqrt{3}}{2\sqrt{2}}\, m_a V_{dc} = 0.6124\, m_a V_{dc}\]
Equation
\[V_{ab,1(rms)} = 0.6124 \times 0.9 \times 600 = 330.7~\text{V}\]
For comparison, six-step operation of the same DC link would give
\(V_{ab,1(rms)} = (\sqrt{6}/\pi)V_{dc} = 0.7797 \times 600 = 467.8\) V, so linear
sinusoidal PWM reaches at most about 78.5 % of that even at \(m_a = 1\). Recovering
the shortfall is the motivation for third-harmonic injection and space vector
modulation, covered in
Chapter 18.
✓
Final Answer
Correct answer: 330.7 V
Question 08 · 2 marksQuestion 8
A buck converter in a switched-mode power supply operates from a 48 V input at a
switching frequency of 20 kHz with a duty ratio of 0.5, delivering 24 V to a
12 \(\Omega\) load. The filter inductance is 500 \(\mu\)H and the output capacitor is
large enough that the output voltage may be treated as constant. The converter
works in continuous conduction mode. The peak-to-peak ripple in the inductor
current is _____ A.
Solution
During the on-interval \(DT\) the inductor sees the difference between input and
output voltage, and the current ramps up linearly:
Equation
\[\Delta I_L = \frac{\left(V_s - V_o\right)D T}{L} = \frac{\left(V_s - V_o\right)D}{L f_s}\]
With \(T = 1/20\,\text{kHz} = 50\,\mu\text{s}\),
Equation
\[\Delta I_L = \frac{(48 - 24)(0.5)(50\times 10^{-6})}{500\times 10^{-6}} = \frac{24 \times 25\times 10^{-6}}{500\times 10^{-6}} = 1.2~\text{A}\]
The off-interval gives the same figure, as it must in steady state, since the
inductor then carries \(-V_o\) across it for \((1-D)T\):
Equation
\[\Delta I_L = \frac{V_o(1-D)T}{L} = \frac{24 \times 0.5 \times 50\times 10^{-6}}{500\times 10^{-6}} = 1.2~\text{A}\]
The average inductor current equals the load current,
\(I_L = 24/12 = 2\) A. Since \(\Delta I_L/2 = 0.6\) A is less than 2 A, the inductor
current never reaches zero and the assumed continuous conduction is confirmed.
Converter waveforms are derived in
Chapter 12.
✓
Final Answer
Correct answer: 1.2 A
Question 09 · 2 marksQuestion 9
A separately excited DC motor is fed from a single-phase fully controlled bridge
converter supplied at 230 V, 50 Hz. The armature resistance is 1.0 \(\Omega\) and
the armature current is continuous and ripple-free at 10 A. The field is held
constant, giving a back-emf constant of
\(K_a\phi = 1.2\;\text{V}\cdot\text{s/rad}\). For a firing angle of 30°, the motor
speed is _____ rpm.
Solution
The converter applies an average armature voltage of
Equation
\[V_a = \frac{2V_m}{\pi}\cos\alpha = \frac{2\left(\sqrt{2}\times 230\right)}{\pi}\cos 30^\circ = 207.08 \times 0.8660 = 179.33~\text{V}\]
Averaging the armature circuit equation over a supply period, the armature
inductance contributes nothing in steady state, so
Equation
\[E_b = V_a - I_a R_a = 179.33 - (10)(1.0) = 169.33~\text{V}\]
The back-emf fixes the mechanical speed:
Equation
\[\omega_m = \frac{E_b}{K_a \phi} = \frac{169.33}{1.2} = 141.11~\text{rad/s}\]
Equation
\[N = \frac{60\,\omega_m}{2\pi} = \frac{60 \times 141.11}{2\pi} = 1347.5~\text{rpm}\]
The torque developed is \(T = K_a\phi I_a = 1.2 \times 10 = 12\) N·m, unaffected by
\(\alpha\); the firing angle sets speed, and the load sets current. Drive
behaviour across the quadrants is developed in
Chapter 25.
✓
Final Answer
Correct answer: 1347.5 rpm
Question 10 · 1 markQuestion 10
A single-phase AC voltage controller with two antiparallel thyristors feeds a
series R–L load whose impedance angle is
\(\varphi = \tan^{-1}\!\left(\omega L / R\right)\). The range of firing angle over
which the output voltage can actually be varied is
- \(0 \le \alpha \le \pi\)
- \(\varphi \le \alpha \le \pi\)
- \(0 \le \alpha \le \varphi\)
- \(\pi/2 \le \alpha \le \pi\)
Solution
Fire a thyristor at \(\omega t = \alpha\) into the R–L load. The current is the sum
of a steady-state and a transient term,
Equation
\[i(\omega t) = \frac{V_m}{Z}\left[\sin\left(\omega t - \varphi\right) - \sin\left(\alpha - \varphi\right)e^{-\left(\omega t - \alpha\right)/\tan\varphi}\right]\]
If \(\alpha = \varphi\) the transient term vanishes and the current is the pure
sinusoid \(\left(V_m/Z\right)\sin(\omega t - \varphi)\), which extinguishes exactly
at \(\omega t = \alpha + \pi\). Each device then conducts for a full 180° and the
next device is fired precisely as the previous one turns off, so the load
receives the full supply voltage.
For \(\alpha\) less than \(\varphi\) the extinction angle would exceed
\(\alpha + \pi\), meaning one thyristor is still conducting when its partner is
gated. The partner cannot turn on with reverse voltage across it, and the
outcome is a single device conducting continuously with the load current becoming
the full sinusoid again. The output is therefore stuck at the uncontrolled value
for every \(\alpha \le \varphi\); control only begins once \(\alpha\) exceeds
\(\varphi\), and ends at \(\alpha = \pi\) where the conduction angle shrinks to zero.
B
Final Answer
Correct answer: (B) \(\varphi \le \alpha \le \pi\)