Class 12 Physics Chapter 2: Electrostatic Potential and Capacitance worksheet with answer key
A 20-mark worksheet on Electrostatic Potential and Capacitance for about 40 minutes of class or homework: 5 multiple-choice, 3 very short answer and 3 short answer questions, written from the NCERT chapter and checked by a second reviewer. Print the PDF for the class; the answer key carries the marking scheme. Teachers may photocopy it freely.
Show answer
Answer: (d) concentric spheres centred at the charge
V = q/(4πε₀r) depends only on r, so V is constant wherever r is constant: on spheres centred at the charge. The radial field lines cross them normally.
Show answer
Answer: (d) 2 μF
1/C = 1/6 + 1/3 = 1/2, so C = 2 μF. 9 μF is the parallel value; in series the combination is smaller than the smallest capacitor.
Show answer
Answer: (d) [M⁻¹ L⁻² T⁴ A²]
C = Q/V: charge is [A T] and potential is [M L² T⁻³ A⁻¹], so C = [A T]/[M L² T⁻³ A⁻¹] = [M⁻¹ L⁻² T⁴ A²]. [M L² T⁻³ A⁻¹] is the dimension of potential itself.
Show answer
Answer: (b) 0.40 J
U = ½QV = ½ × 4.0 × 10⁻³ × 200 = 0.40 J. QV alone gives 0.80 J; halving twice gives 0.20 J.
Show answer
Answer: (a) 400 pF
C = ε₀A/d = 8.85 × 10⁻¹² × 4.0 × 10⁻² / (0.885 × 10⁻³) = 4.0 × 10⁻¹⁰ F = 400 pF.
Show answer
In a non-polar molecule (O₂, H₂) the centres of positive and negative charge coincide, so it has no permanent dipole moment; a field displaces the charges in opposite directions and induces a dipole moment. In a polar molecule (H₂O, HCl) the centres are separated even without a field, giving a permanent dipole moment; a field tends to align these randomly oriented dipoles, against thermal agitation.
- definitions with one example of each (1)
- induced dipole for non-polar; alignment of permanent dipoles for polar (1)
Show answer
Series: 1/Cs = 1/C + 1/2C = 3/2C, so Cs = 2C/3, and each carries the same charge Q = 2CV/3. Then V₁ = Q/C = 2V/3 across C and V₂ = Q/2C = V/3 across 2C; they add to V. The smaller capacitor takes the larger share of the voltage.
- equivalent 2C/3 and the same charge 2CV/3 on each (1)
- 2V/3 across C and V/3 across 2C (1)
Show answer
(a) Each has charge of magnitude e and falls through 2.0 kV, so each gains eΔV = 2.0 keV = 2.0 × 10³ × 1.6 × 10⁻¹⁹ J = 3.2 × 10⁻¹⁶ J. (b) Equal kinetic energies: ½me ve² = ½mp vp², so ve/vp = √(mp/me) = √1836 ≈ 43.
- 2.0 keV = 3.2 × 10⁻¹⁶ J for each (1)
- ve/vp = √1836 ≈ 43 (1)
Show answer
(a) Q₀ = CV = 10 × 10⁻⁶ × 100 = 1.0 × 10⁻³ C. With the battery connected V is fixed and C becomes 30 μF, so Q = 3.0 × 10⁻³ C: an extra 2.0 × 10⁻³ C flows. (b) U₀ = ½ × 10 × 10⁻⁶ × 100² = 0.050 J; U = ½ × 30 × 10⁻⁶ × 100² = 0.15 J; increase 0.10 J. (c) The battery moves 2.0 × 10⁻³ C through a potential difference of 100 V: W = qV = 0.20 J, twice the increase in stored energy; the other 0.10 J does not stay in the capacitor's field.
- extra charge 2.0 × 10⁻³ C (1)
- stored energy rises from 0.050 J to 0.15 J, by 0.10 J (1)
- battery work 0.20 J, twice the increase (1)
Show answer
(a) C = ε₀A/d = 8.85 × 10⁻¹² × 2.0 × 10⁻²/2.0 × 10⁻³ = 8.85 × 10⁻¹¹ F ≈ 89 pF. (b) Vmax = Emax d = 3 × 10⁶ × 2.0 × 10⁻³ = 6.0 × 10³ V. (c) Qmax = CVmax = 8.85 × 10⁻¹¹ × 6.0 × 10³ ≈ 5.3 × 10⁻⁷ C. Beyond this the air ionises and the charge leaks away.
- C ≈ 8.9 × 10⁻¹¹ F (1)
- Vmax = 6.0 × 10³ V (1)
- Qmax ≈ 5.3 × 10⁻⁷ C (1)
Show answer
Each layer acts as a capacitor of plate area A and separation d/2, and the two are in series (the same charge sits on each). C₁ = 2ε₀A/(d/2) = 4C₀ and C₂ = 4ε₀A/(d/2) = 8C₀. Then 1/C = 1/4C₀ + 1/8C₀ = 3/8C₀, so C = (8/3)C₀.
- layers treated as two capacitors in series (1)
- C₁ = 4C₀ and C₂ = 8C₀ (1)
- 1/C = 3/8C₀, so C = 8C₀/3 (1)
← Chapter 1: Electric Charges and FieldsChapter 3: Current Electricity →