Physics Objective Questions and Answers: Electrostatic Potential and Capacitance
Review structured MCQ sets for JEE Physics Electrostatic Potential and Capacitance. Built according to official JEE guidelines, these downloadable questions support daily revision and core concept reinforcement.
Download Electrostatic Potential and Capacitance MCQs with Answers
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Multiple Choice Questions
(a) \( v\propto\dfrac r{r_0} \)
(b) \( \sqrt{\ln\left(\dfrac r{r_0}\right)} \)
(c) \( v\propto e^{+r/r_0} \)
(d) \( v\propto\ln\left(\dfrac r{r_0}\right) \)
Show Answer & Explanation
Answer: (b) \( \sqrt{\ln\left(\dfrac r{r_0}\right)} \)
Explanation:
1. Line charge field \( E=\dfrac\lambda{2\pi\epsilon_0r} \), so the potential difference is \( \dfrac\lambda{2\pi\epsilon_0}\ln\dfrac r{r_0} \).
2. \( \tfrac12mv^2=q\Delta V\propto\ln\dfrac r{r_0}\Rightarrow v\propto\sqrt{\ln(r/r_0)} \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( \dfrac{-q}{1+\sqrt2} \)
(b) \( -2q \)
(c) \( +q \)
(d) \( \dfrac{-\sqrt2\,q}{\sqrt2+1} \)
Show Answer & Explanation
Answer: (d) \( \dfrac{-\sqrt2\,q}{\sqrt2+1} \)
Explanation:
1. Pairs: \( Q\text{-}q_1 \) at a, \( q_1\text{-}q_2 \) at a, \( Q\text{-}q_2 \) at \( a\sqrt2 \). \( U=k\left[\dfrac{Qq}a+\dfrac{q^2}a+\dfrac{Qq}{a\sqrt2}\right]=0 \).
2. \( Q\left(1+\dfrac1{\sqrt2}\right)=-q\Rightarrow Q=\dfrac{-\sqrt2q}{\sqrt2+1} \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( \dfrac{Q(a^2+b^2+c^2)}{4\pi\epsilon_0(a^3+b^3+c^3)} \)
(b) \( \dfrac{Q(a+b+c)}{4\pi\epsilon_0(a^2+b^2+c^2)} \)
(c) \( \dfrac Q{4\pi\epsilon_0(a+b+c)} \)
(d) \( \dfrac Q{12\pi\epsilon_0}\cdot\dfrac{ab+bc+ca}{abc} \)
Show Answer & Explanation
Answer: (b) \( \dfrac{Q(a+b+c)}{4\pi\epsilon_0(a^2+b^2+c^2)} \)
Explanation:
1. \( Q=4\pi\sigma(a^2+b^2+c^2) \), and inside all the shells \( V=\dfrac\sigma{\epsilon_0}(a+b+c) \).
2. \( V=\dfrac{Q(a+b+c)}{4\pi\epsilon_0(a^2+b^2+c^2)} \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) 120 V
(b) -120 V
(c) 80 V
(d) -80 V
Show Answer & Explanation
Answer: (d) -80 V
Explanation:
1. \( V_A-V_O=-\int_0^2E\,dx=-\int_0^230x^2dx \).
2. \( =-10x^3\Big|_0^2=-80 V \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) positive
(b) zero
(c) negative
(d) depends on the path connecting the initial and final positions
Show Answer & Explanation
Answer: (b) zero
Explanation:
1. Both points lie in the plane \( z=0 \), the perpendicular bisector plane of the dipole, which is an equipotential \( (V = 0) \).
2. The work \( q(V_i-V_f)=0 \), independent of path.
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( V_A\lt V_B \)
(b) \( V_A\lt V_C \)
(c) \( V_A\gt V_B \)
(d) \( V_A\gt V_C \)
Show Answer & Explanation
Answer: (c) \( V_A\gt V_B \)
Explanation:
1. Potential falls in the direction of the field, so \( V_B\lt V_A \).
2. A and \( C \) lie on the same equipotential line (perpendicular to the field), so \( V_A=V_C \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) +2
(b) -1
(c) -2
(d) zero
Show Answer & Explanation
Answer: (a) +2
Explanation:
1. The integral equals \( V(0)-V(\infty)=V_{centre} \).
2. Whatever the distribution on the ring, \( V_{centre}=\dfrac{kQ}R=\dfrac{9\times10^9\times1.11\times10^{-10}}{0.5}\approx2 V \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( +8 \) V/m along the x-axis
(b) \( -16 \) V/m along the x-axis
(c) \( -8 \) V/m along the x-axis
(d) zero
Show Answer & Explanation
Answer: (c) \( -8 \) V/m along the x-axis
Explanation:
1. \( E_x=-\dfrac{\partial V}{\partial x}=-8x \), and \( E_y=E_z=0 \).
2. At \( x=1 \): \( E=-8 V/m \), i.e. \( 8 V/m \) directed along the negative x-axis.
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( 5.82\,\dfrac{q^2}{4\pi\epsilon_0a} \)
(b) \( -5.82\,\dfrac{q^2}{4\pi\epsilon_0a} \)
(c) \( 3\,\dfrac{q^2}{4\pi\epsilon_0a} \)
(d) \( 12\,\dfrac{q^2}{4\pi\epsilon_0a} \)
Show Answer & Explanation
Answer: (a) \( 5.82\,\dfrac{q^2}{4\pi\epsilon_0a} \)
Explanation:
1. For one corner: 3 neighbours at a (unlike): \( -3 \); 3 face-diagonal at \( a\sqrt2 \) (like): \( +\dfrac3{\sqrt2} \); 1 body-diagonal at \( a\sqrt3 \) (unlike): \( -\dfrac1{\sqrt3} \). Sum \( =-1.456 \).
2. \( U=\dfrac12\times8\times(-1.456)\dfrac{kq^2}a=-5.82\dfrac{kq^2}a \). The work needed to disassemble is \( +5.82\dfrac{q^2}{4\pi\epsilon_0a} \).
Teacher's Note:
1. Potential is a scalar: add potentials of point charges, and use \( U = k q1 q2 / r \) summed over pairs for the energy of a system.
2. The work done by the field is \( q \) times the fall in potential, and equipotential surfaces carry zero work.
(a) \( \dfrac{(K_1+K_2+K_3)(K_2K_3+K_3K_1+K_1K_2)}{K_1K_2K_3} \)
(b) \( \dfrac{9K_1K_2K_3}{(K_1+K_2+K_3)(K_2K_3+K_3K_1+K_1K_2)} \)
(c) \( \dfrac{K_1K_2K_3}{(K_1+K_2+K_3)(K_1K_2+K_2K_3+K_3K_1)} \)
(d) \( \dfrac{(K_1+K_2+K_3)(K_2K_3+K_3K_1+K_1K_2)}{9K_1K_2K_3} \)
Show Answer & Explanation
Answer: (b) \( \dfrac{9K_1K_2K_3}{(K_1+K_2+K_3)(K_2K_3+K_3K_1+K_1K_2)} \)
Explanation:
1. Layers (series): \( C_1=\dfrac{3C}{1/K_1+1/K_2+1/K_3}=\dfrac{3CK_1K_2K_3}{K_1K_2+K_2K_3+K_3K_1} \). Side by side (parallel): \( C_2=\dfrac{C(K_1+K_2+K_3)}3 \).
2. At the same \( V \), \( E\propto C \): \( \dfrac{E_1}{E_2}=\dfrac{9K_1K_2K_3}{(K_1+K_2+K_3)(K_1K_2+K_2K_3+K_3K_1)} \).
Teacher's Note:
1. For capacitors use \( C = K epsilon_0 A / d \), add in parallel and add reciprocals in series, and decide first whether the battery stays connected (\( V \) fixed) or is removed (\( Q \) fixed).
2. Energy stored is \( Q^2/2C = CV^2/2 \); compare before and after to get the work done.
(a) \( \dfrac{nV}{K+n} \)
(b) \( V \)
(c) \( \dfrac V{K+n} \)
(d) \( \dfrac{(n+1)V}{K+n} \)
Show Answer & Explanation
Answer: (d) \( \dfrac{(n+1)V}{K+n} \)
Explanation:
1. Total charge \( Q=(C+nC)V=(n+1)CV \), conserved after the battery is removed.
2. New capacitance \( KC+nC \): \( V'=\dfrac{(n+1)CV}{(K+n)C}=\dfrac{(n+1)V}{K+n} \).
Teacher's Note:
1. For capacitors use \( C = K epsilon_0 A / d \), add in parallel and add reciprocals in series, and decide first whether the battery stays connected (\( V \) fixed) or is removed (\( Q \) fixed).
2. Energy stored is \( Q^2/2C = CV^2/2 \); compare before and after to get the work done.
(a) \( 3.75\times10^{-6}\ \text{J} \)
(b) \( 6.25\times10^{-6}\ \text{J} \)
(c) \( 2.16\times10^{-6}\ \text{J} \)
(d) \( 2.55\times10^{-6}\ \text{J} \)
Show Answer & Explanation
Answer: (a) \( 3.75\times10^{-6}\ \text{J} \)
Explanation:
1. Charge is constant: \( W=\dfrac{Q^2}2\left(\dfrac1{C_2}-\dfrac1{C_1}\right) \).
2. \( W=\dfrac{25\times10^{-12}}2\left(\dfrac1{2\times10^{-6}}-\dfrac1{5\times10^{-6}}\right)=3.75\times10^{-6} J \).
Teacher's Note:
1. For capacitors use \( C = K epsilon_0 A / d \), add in parallel and add reciprocals in series, and decide first whether the battery stays connected (\( V \) fixed) or is removed (\( Q \) fixed).
2. Energy stored is \( Q^2/2C = CV^2/2 \); compare before and after to get the work done.
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Multiple Choice Questions (MCQs) for JEE Physics Electrostatic Potential and Capacitance
Download Multiple Choice Questions: Electrostatic Potential and Capacitance (JEE Physics)
Review structured objective questions for JEE Physics Electrostatic Potential and Capacitance. Built according to official JEE guidelines, these MCQ sets support daily revision and core concept reinforcement.
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FAQs
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