CBSE · Class 12 · Physics

Class 12 Electrostatic Potential and Capacitance Mock Test (CBSE)

3 practice questions from Electrostatic Potential and Capacitance, in the style of your board paper, each with a worked answer and the marks for every step. Then take a full chapter test on paper, snap the pages and get every step marked.

Topics in Electrostatic Potential and Capacitance

  • Electrostatic potential
  • Potential due to a point charge
  • Potential due to an electric dipole
  • Potential due to a system of charges
  • Equipotential surfaces
  • Potential energy of a system of charges
  • Potential energy in an external field
  • Electrostatics of conductors
  • Dielectrics and polarisation
  • Capacitors and capacitance
  • The parallel plate capacitor
  • Effect of dielectric on capacitance
  • Combination of capacitors
  • Energy stored in a capacitor

Electrostatic Potential and Capacitance practice questions with answers

  1. Q1Multiple choice1 mark
    Four equal point charges, each of magnitude qq, are placed at the four corners of a square of side aa. The total electric potential at the centre of the square is:
    1. (a)2qπε0a\frac{2q}{\pi\varepsilon_0 a}
    2. (b)42qπε0a\frac{4\sqrt{2}q}{\pi\varepsilon_0 a}
    3. (c)4qπε0a\frac{4q}{\pi\varepsilon_0 a}
    4. (d)2qπε0a\frac{\sqrt{2}q}{\pi\varepsilon_0 a}
    Show answer and step marks
    1. Correct option: (d) 2qπε0a\frac{\sqrt{2}q}{\pi\varepsilon_0 a}. The distance of each corner from the centre of the square of side aa is r=a2r = \frac{a}{\sqrt{2}}. The total potential is V=4×14πε0q(a/2)=2qπε0aV = 4 \times \frac{1}{4\pi\varepsilon_0} \frac{q}{(a/\sqrt{2})} = \frac{\sqrt{2}q}{\pi\varepsilon_0 a}.+1
    Answer: (d)
  2. Q2Multiple choice1 mark
    The electric potential at a distance r=1 mr = 1\text{ m} from the centre of a short electric dipole of dipole moment p=1×10−7 C mp = 1 \times 10^{-7}\text{ C m} along a line making an angle of 60∘60^\circ with the dipole axis is: (Given 14πε0=9×109 N m2 C−2\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9\text{ N m}^2\text{ C}^{-2})
    1. (a)225 V225\text{ V}
    2. (b)900 V900\text{ V}
    3. (c)450 V450\text{ V}
    4. (d)1800 V1800\text{ V}
    Show answer and step marks
    1. Correct option: (c) 450 V450\text{ V}. Using the formula V=14πε0pcos⁡θr2V = \frac{1}{4\pi\varepsilon_0} \frac{p \cos\theta}{r^2}, substituting p=1×10−7 C mp = 1 \times 10^{-7}\text{ C m}, r=1 mr = 1\text{ m}, θ=60∘\theta = 60^\circ, and 14πε0=9×109 N m2 C−2\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9\text{ N m}^2\text{ C}^{-2} gives V=9×109×10−7×0.512=450 VV = 9 \times 10^9 \times \frac{10^{-7} \times 0.5}{1^2} = 450\text{ V}.+1
    Answer: (c)
  3. Q3Short answer2 marks
    Why is the work done in moving a test charge from one point to another on an equipotential surface zero? Hence, show that the electric field is always directed normal to the equipotential surface at any point.
    Show answer and step marks
    1. On an equipotential surface VV is the same at every point, so ΔV=0\Delta V = 0 between any two points; since W=qΔVW = q\Delta V, the work done is W=0W = 0.+1
    2. For any small displacement dl⃗d\vec{l} along the surface, dV=−E⃗⋅dl⃗=−E dlcos⁡θ=0dV = -\vec{E} \cdot d\vec{l} = -E\, dl \cos\theta = 0; since E≠0E \ne 0 and dl≠0dl \ne 0, cos⁡θ=0\cos\theta = 0, so θ=90∘\theta = 90^\circ and E⃗\vec{E} is normal to the surface at every point.+1
    Answer: VV is constant on the surface, so W=qΔV=0W = q\Delta V = 0; for any displacement along it dV=−E⃗⋅dl⃗=0dV = -\vec{E} \cdot d\vec{l} = 0, so E⃗\vec{E} has no component along the surface and is normal to it.

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