Prepizo
Learn › NEET · Physics PYQ › Electrostatic Potential and Capacitance

Electrostatic Potential and Capacitance — NEET Physics PYQ MCQs with Solutions

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

▶ Practise Electrostatic Potential and Capacitance online (free)

Subtopics

Sample questions with solutions

Q1 — Electrostatic Potential and Potential Energy · easy · numerical
In a certain region of space with volume 0.2 m³, the electric potential is found to be 5 V throughout. The magnitude of electric field in this region is
A. 0.5 N/C
B. 1 N/C
C. 5 N/C
D. zero  ✓ Correct
Solution: $E = -\frac{dV}{dr}$. Since the potential is constant (5 V everywhere), its gradient is zero, so E = 0.
Q2 — Electrostatic Potential and Potential Energy · easy · theory
Some charge is being given to a conductor, then its potential is
A. maximum at surface
B. maximum at centre
C. same throughout the conductor  ✓ Correct
D. maximum somewhere between surface and centre
Solution: A charged conductor is an equipotential body — its surface and interior are all at the same potential.
Q3 — Electrostatic Potential and Potential Energy · easy · theory
In bringing an electron towards another electron, the electrostatic potential energy of the system
A. decreases
B. increases  ✓ Correct
C. remains same
D. becomes zero
Solution: $U = \frac{1}{4\pi\varepsilon_0}\frac{e^2}{r}$ (positive for like charges). As r decreases, U increases — work must be done against the repulsion.
Q4 — Electrostatic Potential and Potential Energy · easy · numerical
An electron of mass m and charge e is accelerated from rest through a potential difference of V volt in vacuum. Its final speed will be
A. $\frac{eV}{2m}$
B. $\frac{eV}{m}$
C. $\sqrt{\frac{2eV}{m}}$  ✓ Correct
D. $\sqrt{\frac{eV}{2m}}$
Solution: $eV = \frac{1}{2}mv^2 \Rightarrow v = \sqrt{\frac{2eV}{m}}$
Q5 — Electrostatic Potential and Potential Energy · easy · theory
A hollow metal sphere of radius 10 cm is charged such that the potential on its surface is 80 V. The potential at the centre of the sphere is
A. zero
B. 80 V  ✓ Correct
C. 800 V
D. 8 V
Solution: Inside a conductor the potential is constant and equal to the surface value. So the potential at the centre is also 80 V.
Q6 — Capacitors and Capacitance · easy · numerical
A parallel plate condenser with oil (dielectric constant 2) between the plates has capacitance C. If oil is removed, the capacitance of capacitor becomes
A. $\sqrt{2}C$
B. $2C$
C. $\frac{C}{\sqrt{2}}$
D. $\frac{C}{2}$  ✓ Correct
Solution: With oil $C = K C_0 = 2C_0$. Removing it gives $C_0 = \frac{C}{K} = \frac{C}{2}$
Q7 — Electrostatic Potential and Potential Energy · hard · numerical
Two metal spheres, one of radius R and the other of radius 2R respectively have the same surface charge density σ. They are brought in contact and separated. What will be the new surface charge densities on them?
A. $\sigma_1 = \frac{5}{6}\sigma, \sigma_2 = \frac{5}{2}\sigma$
B. $\sigma_1 = \frac{5}{2}\sigma, \sigma_2 = \frac{5}{6}\sigma$
C. $\sigma_1 = \frac{5}{2}\sigma, \sigma_2 = \frac{5}{3}\sigma$
D. $\sigma_1 = \frac{5}{3}\sigma, \sigma_2 = \frac{5}{6}\sigma$  ✓ Correct
Solution: Total charge $Q_t = 4\pi\sigma R^2 + 16\pi\sigma R^2 = 20\pi\sigma R^2$. On contact charges share in ratio 1:2 (potentials equal), so $Q_1 = \frac{Q_t}{3}$, $Q_2 = \frac{2Q_t}{3}$. $\sigma_1 = \frac{Q_t/3}{4\pi R^2} = \frac{5}{3}\sigma$; $\sigma_2 = \frac{2Q_t/3}{4\pi(2R)^2} = \frac{5}{6}\sigma$
Q8 — Electrostatic Potential and Potential Energy · hard · numerical
In a region, the potential is represented by V(x, y, z) = 6x − 8xy − 8y + 6yz, where V is in volts and x, y, z are in metres. The electric force experienced by a charge of 2 C situated at point (1, 1, 1) is
A. $6\sqrt{5}$ N
B. 30 N
C. 24 N
D. $4\sqrt{35}$ N  ✓ Correct
Solution: $\vec{E} = -\nabla V = -[(6 - 8y)\hat{i} + (-8x - 8 + 6z)\hat{j} + 6y\,\hat{k}]$ At (1,1,1): $\vec{E} = -(-2\hat{i} - 10\hat{j} + 6\hat{k})$, so $|E| = \sqrt{4 + 100 + 36} = 2\sqrt{35}$ N/C $F = qE = 2 \times 2\sqrt{35} = 4\sqrt{35}$ N
Q9 — Electrostatic Potential and Potential Energy · hard · numerical
Four electric charges +q, +q, −q and −q are placed at the corners of a square of side 2L (the two +q charges on the left corners, the two −q charges on the right corners). The electric potential at point A, mid-way between the two charges +q (i.e. the midpoint of the left side), is
A. $\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}\left(1 + \frac{1}{\sqrt{5}}\right)$
B. $\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}\left(1 - \frac{1}{\sqrt{5}}\right)$  ✓ Correct
C. zero
D. $\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1 + \sqrt{5})$
Solution: A is at distance L from each +q and $\sqrt{(2L)^2 + L^2} = \sqrt{5}L$ from each −q. $V = 2\cdot\frac{kq}{L} - 2\cdot\frac{kq}{\sqrt{5}L} = \frac{2q}{4\pi\varepsilon_0 L}\left(1 - \frac{1}{\sqrt{5}}\right)$
Q10 — Electrostatic Potential and Potential Energy · hard · theory
Three concentric spherical shells have radii a, b and c (a < b < c) and have surface charge densities σ, −σ and σ respectively. If $V_A$, $V_B$ and $V_C$ denote the potentials of the three shells, then for c = a + b, we have
A. $V_C = V_A \neq V_B$
B. $V_C = V_B \neq V_A$
C. $V_C \neq V_B \neq V_A$
D. $V_C = V_B = V_A$  ✓ Correct
Solution: Computing each potential from the three charged shells and substituting c = a + b gives $V_A = \frac{\sigma}{\varepsilon_0}(a - b + c) = \frac{\sigma}{\varepsilon_0}(2a)$, and $V_B = V_C = \frac{\sigma}{\varepsilon_0}(2a)$ as well. Hence $V_A = V_B = V_C$.
Q11 — Electrostatic Potential and Potential Energy · hard · numerical
Charges +q and −q are placed at points A and B respectively which are a distance 2L apart. C is the midpoint between A and B. The work done in moving a charge +Q along the semicircle CRD (from C to a point D located a distance L beyond B, i.e. 3L from A) is
A. $\frac{qQ}{4\pi\varepsilon_0 L}$
B. $\frac{qQ}{2\pi\varepsilon_0 L}$
C. $\frac{qQ}{6\pi\varepsilon_0 L}$
D. $-\frac{qQ}{6\pi\varepsilon_0 L}$  ✓ Correct
Solution: Potential at C (distance L from both): $V_C = \frac{kq}{L} - \frac{kq}{L} = 0$. At D (distance 3L from +q, L from −q): $V_D = \frac{kq}{3L} - \frac{kq}{L} = -\frac{2kq}{3L}$. $W = Q(V_D - V_C) = Q\left(-\frac{2kq}{3L}\right) = -\frac{qQ}{6\pi\varepsilon_0 L}$
Q12 — Electrostatic Potential and Potential Energy · hard · numerical
Identical charges (−q) are placed at each of the eight corners of a cube of side b. The electrostatic potential energy of a charge (+q) placed at the centre of the cube will be
A. $-\frac{4\sqrt{2}q^2}{\pi\varepsilon_0 b}$
B. $\frac{8\sqrt{2}q^2}{\pi\varepsilon_0 b}$
C. $-\frac{4q^2}{\sqrt{3}\pi\varepsilon_0 b}$  ✓ Correct
D. $\frac{8\sqrt{2}q^2}{4\pi\varepsilon_0 b}$
Solution: Each corner is at half the body-diagonal from the centre: $\frac{\sqrt{3}b}{2}$. $U = 8 \times \frac{1}{4\pi\varepsilon_0}\frac{(+q)(-q)}{\frac{\sqrt{3}b}{2}} = -\frac{4q^2}{\sqrt{3}\pi\varepsilon_0 b}$
Q13 — 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: $\frac{16C_1}{n_1} = n_2 C_2 \Rightarrow C_2 = \frac{16C_1}{n_1 n_2}$
Q14 — 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.
Q15 — Electrostatic Potential and Potential Energy · medium · numerical
Twenty seven drops of same size are charged at 220 V each. They combine to form a bigger drop. Calculate the potential of the bigger drop.
A. 660 V
B. 1320 V
C. 1520 V
D. 1980 V  ✓ Correct
Solution: 27 small drops → one big drop: $R = 27^{1/3}r = 3r$, and total charge $Q = 27q$. $V' = \frac{KQ}{R} = \frac{K \cdot 27q}{3r} = 9\frac{Kq}{r} = 9V = 9 \times 220 = 1980$ V
Q16 — Electrostatic Potential and Potential Energy · medium · theory
Two charged spherical conductors of radii $R_1$ and $R_2$ are connected by a wire. Then, the ratio of surface charge densities of the spheres $(\sigma_1/\sigma_2)$ is
A. $\frac{R_1}{R_2}$
B. $\frac{R_2}{R_1}$  ✓ Correct
C. $\left(\frac{R_1}{R_2}\right)$
D. $\frac{R_1^2}{R_2^2}$
Solution: Connected → same potential: $\frac{q_1}{R_1} = \frac{q_2}{R_2}$. With $\sigma = \frac{q}{4\pi R^2}$: $\frac{\sigma_1}{\sigma_2} = \frac{q_1}{q_2}\cdot\frac{R_2^2}{R_1^2} = \frac{R_1}{R_2}\cdot\frac{R_2^2}{R_1^2} = \frac{R_2}{R_1}$
Q17 — Electrostatic Potential and Potential Energy · medium · numerical
A short electric dipole has a dipole moment of $16 \times 10^{-9}$ C·m. The electric potential due to the dipole at a point at a distance of 0.6 m from the centre of the dipole, situated on a line making an angle of 60° with the dipole axis is ($\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9$ N·m²/C²)
A. 200 V  ✓ Correct
B. 400 V
C. zero
D. 50 V
Solution: $V = \frac{1}{4\pi\varepsilon_0}\frac{p\cos\theta}{r^2} = \frac{9 \times 10^9 \times 16 \times 10^{-9} \times \frac{1}{2}}{(0.6)^2} = 200$ V
Q18 — Electrostatic Potential and Potential Energy · medium · theory
Four diagrams show regions of equipotentials, each with a 20 V and a 40 V equipotential line (and 10 V, 30 V lines), arranged with different spacings and orientations. A positive charge q is moved from A (on the 20 V equipotential) to B (on the 40 V equipotential) in each diagram. Which statement is correct?
A. Maximum work is required to move q in figure (iii)
B. In all the four cases, the work done is the same  ✓ Correct
C. Minimum work is required to move q in figure (i)
D. Maximum work is required to move q in figure (ii)
Solution: Work done $W = q\Delta V$. In every diagram the charge moves from the 20 V line to the 40 V line, so $\Delta V = 20$ V is the same — hence the work done is the same in all four cases (work is path-independent, depending only on the potential difference).
Q19 — Electrostatic Potential and Potential Energy · medium · numerical
If potential (in volts) in a region is expressed as V(x, y, z) = 6xy − y + 2yz, the electric field (in N/C) at point (1, 1, 0) is
A. $-(3\hat{i} + 5\hat{j} + 3\hat{k})$
B. $-(6\hat{i} + 5\hat{j} + 2\hat{k})$  ✓ Correct
C. $-(2\hat{i} + 3\hat{j} + \hat{k})$
D. $-(6\hat{i} + 9\hat{j} + \hat{k})$
Solution: $\vec{E} = -\nabla V = -[6y\,\hat{i} + (6x - 1 + 2z)\hat{j} + 2y\,\hat{k}]$ At (1, 1, 0): $\vec{E} = -(6\hat{i} + 5\hat{j} + 2\hat{k})$ N/C
Q20 — Electrostatic Potential and Potential Energy · medium · theory
A conducting sphere of radius R is given a charge Q. The electric potential and the electric field at the centre of the sphere respectively are
A. zero and $\frac{Q}{4\pi\varepsilon_0 R^2}$
B. $\frac{Q}{4\pi\varepsilon_0 R}$ and zero  ✓ Correct
C. $\frac{Q}{4\pi\varepsilon_0 R}$ and $\frac{Q}{4\pi\varepsilon_0 R^2}$
D. Both are zero
Solution: Charge lies on the surface, so the field inside is zero. The potential is constant inside and equal to its surface value $\frac{Q}{4\pi\varepsilon_0 R}$.
Q21 — Electrostatic Potential and Potential Energy · medium · numerical
Four point charges −Q, −q, 2q and 2Q are placed, one at each corner of a square. The relation between Q and q for which the potential at the centre of the square is zero, is
A. $Q = -q$  ✓ Correct
B. $Q = -\frac{1}{q}$
C. $Q = q$
D. $Q = \frac{1}{q}$
Solution: All four corners are equidistant (r) from the centre, so $V = \frac{k}{r}(-Q - q + 2q + 2Q) = 0$ $Q + q = 0 \Rightarrow Q = -q$
Q22 — Electrostatic Potential and Potential Energy · medium · numerical
The electric potential at a point (x, y, z) is given by $V = -x^2y - xz^3 + 4$. The electric field $\vec{E}$ at that point is
A. $\vec{E} = (2xy + z^3)\hat{i} + x^2\hat{j} + 3xz^2\hat{k}$  ✓ Correct
B. $\vec{E} = 2xy\,\hat{i} + (x^2 + y^2)\hat{j} + (3xz - y^2)\hat{k}$
C. $\vec{E} = z^3\hat{i} + xyz\,\hat{j} + z^2\hat{k}$
D. $\vec{E} = (2xy - z^3)\hat{i} + xy^2\hat{j} + 3z^2x\hat{k}$
Solution: $\vec{E} = -\nabla V = -\left(\frac{\partial V}{\partial x}\hat{i} + \frac{\partial V}{\partial y}\hat{j} + \frac{\partial V}{\partial z}\hat{k}\right)$ $= -[(-2xy - z^3)\hat{i} + (-x^2)\hat{j} + (-3xz^2)\hat{k}] = (2xy + z^3)\hat{i} + x^2\hat{j} + 3xz^2\hat{k}$
Q23 — Electrostatic Potential and Potential Energy · medium · numerical
The electric potential at a point in free space due to a charge Q coulomb is $Q \times 10^{11}$ V. The electric field at that point is
A. $4\pi\varepsilon_0 Q \times 10^{22}$ V/m  ✓ Correct
B. $12\pi\varepsilon_0 Q \times 10^{20}$ V/m
C. $4\pi\varepsilon_0 Q \times 10^{20}$ V/m
D. $12\pi\varepsilon_0 Q \times 10^{22}$ V/m
Solution: $V = \frac{Q}{4\pi\varepsilon_0 r} = Q \times 10^{11}$, so $\frac{1}{4\pi\varepsilon_0 r} = 10^{11}$, giving $r = \frac{1}{4\pi\varepsilon_0 \times 10^{11}}$. $E = \frac{V}{r} = \frac{Q \times 10^{11}}{r} = 4\pi\varepsilon_0 Q \times 10^{22}$ V/m
Q24 — Electrostatic Potential and Potential Energy · medium · numerical
Two charges $q_1$ and $q_2$ are placed 30 cm apart. A third charge $q_3$ is moved along the arc of a circle of radius 40 cm from C to D (at C, $q_3$ is 40 cm from $q_1$ and 50 cm from $q_2$; at D, it is 40 cm from $q_1$ and 10 cm from $q_2$). The change in the potential energy of the system is $\frac{q_3}{4\pi\varepsilon_0}k$, where k is
A. $8q_2$  ✓ Correct
B. $8q_1$
C. $6q_2$
D. $6q_1$
Solution: $\Delta U = U_D - U_C = \frac{q_3}{4\pi\varepsilon_0}\left(\frac{q_2}{0.1} - \frac{q_2}{0.5}\right)$ (the $q_1$ term is unchanged at 0.4 m). $k = q_2(10 - 2) = 8q_2$
Q25 — Electrostatic Potential and Potential Energy · medium · theory
A point charge +q is placed at the origin O. Work done in taking another point charge −Q from the point A [coordinates (0, a)] to another point B [coordinates (a, 0)] along the straight path AB is
A. zero  ✓ Correct
B. $\left(\frac{-qQ}{4\pi\varepsilon_0}\frac{1}{a^2}\right)\sqrt{2}a$
C. $\left(\frac{qQ}{4\pi\varepsilon_0}\frac{1}{a^2}\right)\frac{a}{\sqrt{2}}$
D. $\left(\frac{qQ}{4\pi\varepsilon_0}\frac{1}{a^2}\right)\sqrt{2}a$
Solution: A and B are both at distance a from the origin, so $V_A = V_B = \frac{q}{4\pi\varepsilon_0 a}$. $W = -Q(V_B - V_A) = 0$
Q26 — Electrostatic Potential and Potential Energy · medium · numerical
A bullet of mass 2 g is having a charge of 2 µC. Through what potential difference must it be accelerated, starting from rest, to acquire a speed of 10 m/s?
A. 5 kV
B. 50 kV  ✓ Correct
C. 5 V
D. 50 V
Solution: $qV = \frac{1}{2}mv^2 \Rightarrow V = \frac{mv^2}{2q} = \frac{2 \times 10^{-3} \times 100}{2 \times 2 \times 10^{-6}} = 50 \times 10^3$ V = 50 kV
Q27 — Electrostatic Potential and Potential Energy · medium · numerical
There is an electric field E in the x-direction. If the work done on moving a charge of 0.2 C through a distance of 2 m along a line making an angle 60° with the x-axis is 4 J, then what is the value of E?
A. 3 N/C
B. 4 N/C
C. 5 N/C
D. 20 N/C  ✓ Correct
Solution: $W = qEd\cos\theta \Rightarrow E = \frac{W}{qd\cos\theta} = \frac{4}{0.2 \times 2 \times \cos 60°} = \frac{4}{0.2} = 20$ N/C
Q28 — Electrostatic Potential and Potential Energy · medium · numerical
Two concentric spheres of radii R and r have similar charges with equal surface charge densities (σ). What is the electric potential at their common centre?
A. $\frac{\sigma}{\varepsilon_0}$
B. $\frac{\sigma}{\varepsilon_0}(R - r)$
C. $\frac{\sigma}{\varepsilon_0}(R + r)$  ✓ Correct
D. None of these
Solution: $V = \frac{1}{4\pi\varepsilon_0}\left(\frac{Q}{R} + \frac{q}{r}\right)$; with $\frac{Q}{4\pi R^2} = \frac{q}{4\pi r^2} = \sigma$: $V = \frac{1}{\varepsilon_0}(\sigma R + \sigma r) = \frac{\sigma}{\varepsilon_0}(R + r)$
Q29 — Capacitors and Capacitance · medium · numerical
A parallel plate capacitor having cross-sectional area A and separation d has air in between the plates. Now, an insulating slab of same area but thickness d/2 is inserted between the plates having dielectric constant K = 4. The ratio of new capacitance to its original capacitance will be
A. 2 : 1
B. 8 : 5  ✓ Correct
C. 6 : 5
D. 4 : 1
Solution: With a slab of thickness $t = \frac{d}{2}$, $K = 4$: $C = \frac{\varepsilon_0 A}{(d - t) + \frac{t}{K}} = \frac{\varepsilon_0 A}{\frac{d}{2} + \frac{d}{8}} = \frac{8}{5}\frac{\varepsilon_0 A}{d}$ $\frac{C}{C_0} = \frac{8}{5}$
Q30 — Capacitors and Capacitance · medium · numerical
The capacitance of a parallel plate capacitor with air as medium is 6 µF. With the introduction of a dielectric medium, the capacitance becomes 30 µF. The permittivity of the medium is ($\varepsilon_0 = 8.85 \times 10^{-12}$ C²N⁻¹m⁻²)
A. $1.77 \times 10^{-12}$ C²N⁻¹m⁻²
B. $0.44 \times 10^{-10}$ C²N⁻¹m⁻²  ✓ Correct
C. 5.00 C²N⁻¹m⁻²
D. $0.44 \times 10^{-13}$ C²N⁻¹m⁻²
Solution: Dielectric constant $K = \frac{C_m}{C_0} = \frac{30}{6} = 5$. $\varepsilon_m = K\varepsilon_0 = 5 \times 8.85 \times 10^{-12} = 0.44 \times 10^{-10}$ C²N⁻¹m⁻²