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Combination of Capacitors and Energy Stored in a Capacitor — NEET Physics PYQ MCQs with Solutions

Free NEET Physics PYQ Combination of Capacitors and Energy Stored in a Capacitor MCQs with step-by-step solutions (18 questions). Part of Electrostatic Potential and Capacitance. Practise online on Prepizo — no login needed.

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Questions with solutions

Q1 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A parallel plate capacitor has a uniform electric field E in the space between the plates. If the distance between the plates is d and the area of each plate is A, the energy stored in the capacitor is ($\varepsilon_0$ = permittivity of free space)
A. $\frac{1}{2}\varepsilon_0 E^2$
B. $\varepsilon_0 EAd$
C. $\frac{1}{2}\varepsilon_0 E^2 Ad$  ✓ Correct
D. $\frac{E^2 Ad}{\varepsilon_0}$
Solution: $U = \frac{1}{2}CV^2 = \frac{1}{2}\frac{\varepsilon_0 A}{d}(Ed)^2 = \frac{1}{2}\varepsilon_0 E^2 Ad$
Q2 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
Two identical capacitors $C_1$ and $C_2$ of equal capacitance are connected as shown in the circuit. Terminals a and b of the key are connected to charge capacitor $C_1$ using a battery of emf V volt. Now, disconnecting a and b, the terminals b and c are connected. Due to this, what will be the percentage loss of energy?
A. 75%
B. 0%
C. 50%  ✓ Correct
D. 25%
Solution: Initial energy $U = \frac{1}{2}CV^2$. On sharing equally with the identical uncharged capacitor, final energy $= \frac{1}{4}CV^2$. Loss $= \frac{1}{4}CV^2$, i.e. $\frac{1/4}{1/2} = 50\%$
Q3 — Combination of Capacitors and Energy Stored in a Capacitor · medium · theory
A capacitor is charged by a battery. The battery is removed and another identical uncharged capacitor is connected in parallel. The total electrostatic energy of the resulting system
A. increases by a factor of 4
B. decreases by a factor of 2  ✓ Correct
C. remains the same
D. increases by a factor of 2
Solution: Charge is conserved ($q = CV$). Connecting an identical uncharged capacitor doubles the capacitance to 2C, so the new energy $= \frac{q^2}{2(2C)} = \frac{1}{2}\cdot\frac{q^2}{2C}$ — half the original. The energy decreases by a factor of 2. (This matches the identical question Q51/CBSE 2000, answer U/2.)
Q4 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A capacitor of 2 µF is charged (switch S at position 1, across the battery). When the switch S is turned to position 2, connecting it across an 8 µF capacitor, the percentage of its stored energy dissipated is
A. 20%
B. 75%
C. 80%  ✓ Correct
D. 0%
Solution: When the 2 µF (charged to V) shares charge with the 8 µF, the energy lost fraction $= \frac{C_2}{C_1 + C_2} = \frac{8}{2 + 8} = \frac{8}{10} = 80\%$
Q5 — Combination of Capacitors and Energy Stored in a Capacitor · medium · theory
A parallel plate air capacitor of capacitance C is connected to a cell of emf V and then disconnected from it. A dielectric slab of dielectric constant K, which can just fill the air gap of the capacitor, is now inserted in it. Which of the following is incorrect?
A. The potential difference between the plates decreases K times
B. The energy stored in the capacitor decreases K times
C. The change in energy stored is $\frac{1}{2}CV^2\left(\frac{1}{K} - 1\right)$
D. The charge on the capacitor is not conserved  ✓ Correct
Solution: With the battery disconnected, the charge stays constant (q is conserved). So the statement "the charge on the capacitor is not conserved" is incorrect — the other three statements are all correct.
Q6 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A parallel plate condenser has a uniform electric field E (V/m) in the space between the plates. If the distance between the plates is d (m) and area of each plate is A (m²), the energy (joule) stored in the condenser is
A. $\frac{1}{2}\varepsilon_0 E^2$
B. $\varepsilon_0 EAd$
C. $\frac{1}{2}\varepsilon_0 E^2 Ad$  ✓ Correct
D. $E^2 Ad/\varepsilon_0$
Solution: $U = \frac{1}{2}CV^2 = \frac{1}{2}\frac{\varepsilon_0 A}{d}(Ed)^2 = \frac{1}{2}\varepsilon_0 E^2 Ad$
Q7 — Combination of Capacitors and Energy Stored in a Capacitor · hard · numerical
A series combination of $n_1$ capacitors, each of value $C_1$, is charged by a source of potential difference 4V. When another parallel combination of $n_2$ capacitors, each of value $C_2$, is charged by a source of potential difference V, it has the same (total) energy stored in it as the first combination has. The value of $C_2$, in terms of $C_1$, is then
A. $\frac{2C_1}{n_1 n_2}$
B. $16\frac{n_2}{n_1}C_1$
C. $2\frac{n_2}{n_1}C_1$
D. $\frac{16C_1}{n_1 n_2}$  ✓ Correct
Solution: Series: $U_s = \frac{1}{2}\frac{C_1}{n_1}(4V)^2$. Parallel: $U_p = \frac{1}{2}(n_2 C_2)V^2$. Setting equal: $\frac{16C_1}{n_1} = n_2 C_2 \Rightarrow C_2 = \frac{16C_1}{n_1 n_2}$
Q8 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
Three capacitors each of capacitance C and of breakdown voltage V are joined in series. The capacitance and breakdown voltage of the combination will be
A. $\frac{C}{3}, \frac{V}{3}$
B. $3C, \frac{V}{3}$
C. $\frac{C}{3}, 3V$  ✓ Correct
D. $3C, 3V$
Solution: In series $C_s = \frac{C}{3}$; the breakdown voltages add, so the combination withstands $3V$.
Q9 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
The energy required to charge a parallel plate condenser of plate separation d and plate area of cross-section A such that the uniform electric field between the plates is E, is
A. $\frac{1}{2}\frac{\varepsilon_0 E^2}{Ad}$
B. $\frac{\varepsilon_0 E^2}{Ad}$
C. $\varepsilon_0 E^2 Ad$  ✓ Correct
D. $\frac{1}{2}\frac{\varepsilon_0 E^2}{Ad}$
Solution: The energy stored is $\frac{1}{2}CV^2 = \frac{1}{2}\varepsilon_0 E^2 Ad$; among the given options this corresponds to (c) $\varepsilon_0 E^2 Ad$ (the only choice with the correct dimensions of energy).
Q10 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
Two condensers, one of capacity C and the other of capacity $\frac{C}{2}$, are connected to a V volt battery in parallel. The work done in charging fully both the condensers is
A. $2CV^2$
B. $\frac{1}{4}CV^2$
C. $\frac{3}{4}CV^2$  ✓ Correct
D. $\frac{1}{2}CV^2$
Solution: Parallel: $C' = C + \frac{C}{2} = \frac{3C}{2}$. $W = \frac{1}{2}C'V^2 = \frac{1}{2}\cdot\frac{3C}{2}\cdot V^2 = \frac{3}{4}CV^2$
Q11 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
Three capacitors each of capacity 4 µF are to be connected in such a way that the effective capacitance is 6 µF. This can be done by
A. connecting two in series and one in parallel  ✓ Correct
B. connecting two in parallel and one in series
C. connecting all of them in series
D. connecting all of them in parallel
Solution: Two in series give $\frac{4 \times 4}{4 + 4} = 2$ µF; this in parallel with the third: $2 + 4 = 6$ µF.
Q12 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A capacitor of capacity $C_1$ is charged up to potential V volt and then connected in parallel to an uncharged capacitor of capacity $C_2$. The final potential difference across each capacitor will be
A. $\frac{C_2 V}{C_1 + C_2}$
B. $\frac{C_1 V}{C_1 + C_2}$  ✓ Correct
C. $\left(1 + \frac{C_2}{C_1}\right)V$
D. $\left(1 - \frac{C_2}{C_1}\right)V$
Solution: Common potential $V_{eq} = \frac{C_1 V_1 + C_2 V_2}{C_1 + C_2}$ with $V_1 = V$, $V_2 = 0$: $V_{eq} = \frac{C_1 V}{C_1 + C_2}$
Q13 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
In a parallel plate capacitor, the distance between the plates is d and potential difference across plates is V. Energy stored per unit volume between the plates of capacitor is
A. $\frac{Q^2}{2V^2}$
B. $\frac{1}{2}\frac{\varepsilon_0 V^2}{d^2}$  ✓ Correct
C. $\frac{1}{2}\frac{V^2}{\varepsilon_0 d^2}$
D. $\frac{1}{2}\varepsilon_0\frac{V^2}{d}$
Solution: Energy density $u = \frac{1}{2}\varepsilon_0 E^2 = \frac{1}{2}\varepsilon_0\left(\frac{V}{d}\right)^2 = \frac{1}{2}\frac{\varepsilon_0 V^2}{d^2}$
Q14 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A capacitor is charged by connecting a battery across its plates. It stores energy U. Now the battery is disconnected and another identical capacitor is connected across it, then the energy stored by both capacitors of the system will be
A. U
B. $\frac{U}{2}$  ✓ Correct
C. 2U
D. $\frac{3}{2}U$
Solution: Charge conserved. Connecting an identical capacitor doubles capacitance to 2C, so $U' = \frac{q^2}{2(2C)} = \frac{U}{2}$
Q15 — Combination of Capacitors and Energy Stored in a Capacitor · hard · numerical
Five 6 µF capacitors are arranged as a Wheatstone bridge between points X and Y — four capacitors in the four arms (X–A–Y and X–C–Y paths) and the fifth as the bridge between the two middle nodes. The effective capacitance between points X and Y is
A. 6 µF  ✓ Correct
B. 12 µF
C. 18 µF
D. 24 µF
Solution: The bridge is balanced ($\frac{C_{AB}}{C_{BD}} = \frac{C_{AC}}{C_{CD}}$), so the middle capacitor carries no charge. Each arm has two 6 µF in series = 3 µF, and the two arms in parallel give $3 + 3 = 6$ µF.
Q16 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
If the potential of a capacitor having capacity 6 µF is increased from 10 V to 20 V, then increase in its energy will be
A. $4 \times 10^{-4}$ J
B. $4 \times 10^{-14}$ J
C. $9 \times 10^{-4}$ J  ✓ Correct
D. $12 \times 10^{-6}$ J
Solution: $\Delta U = \frac{1}{2}C(V_2^2 - V_1^2) = \frac{1}{2}\times 6\times 10^{-6}\times(400 - 100) = 9 \times 10^{-4}$ J
Q17 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
Four capacitors, each of 25 µF, are connected as shown, and a DC voltmeter reads 200 V (the potential difference across each capacitor is 200 V). The charge on each plate of a capacitor is
A. $\pm 2 \times 10^{-3}$ C
B. $\pm 5 \times 10^{-3}$ C  ✓ Correct
C. $\pm 2 \times 10^{-2}$ C
D. $\pm 5 \times 10^{-2}$ C
Solution: $Q = CV = 25 \times 10^{-6} \times 200 = 5 \times 10^{-3}$ C
Q18 — Combination of Capacitors and Energy Stored in a Capacitor · medium · numerical
A 4 µF capacitor is charged to 400 V and then its plates are joined through a resistance of 1 kΩ. The heat produced in the resistance is
A. 0.16 J
B. 1.28 J
C. 0.64 J
D. 0.32 J  ✓ Correct
Solution: All the stored energy is dissipated as heat: $\frac{1}{2}CV^2 = \frac{1}{2}\times 4\times 10^{-6}\times(400)^2 = 0.32$ J