Physics Objective Questions and Answers: Electrostatic Potential and Capacitance
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Multiple Choice Questions
(a) 9 km
(b) 10 m
(c) 1.11 m
(d) 1.11 cm
Show Answer & Explanation
Answer: (a) 9 km
Explanation:
1. \( C=4\pi\varepsilon_0R\Rightarrow R=\dfrac{C}{4\pi\varepsilon_0}=9\times10^9\times10^{-6}=9\times10^3 \) m = 9 km.
Teacher's Note:
1. A farad is a very large unit.
2. Use \( 1/4\pi\varepsilon_0=9\times10^9 \).
(a) flow from A to B
(b) oscillate between A and B
(c) remain stationary
(d) flow from B to A
Show Answer & Explanation
Answer: (a) flow from A to B
Explanation:
1. Potentials: \( V_A=\dfrac{kQ}{R} \) and \( V_B=\dfrac{kQ}{2R} \).
2. A is at the higher potential, so positive charge flows from A to B until the potentials are equal.
Teacher's Note:
1. Charge moves from higher to lower potential.
(a) C/2
(b) C/4
(c) \( 2C \)
(d) 4C
Show Answer & Explanation
Answer: (c) \( 2C \)
Explanation:
1. \( C=\varepsilon_0A/d\propto1/d \), so halving \( d \) doubles \( C \).
Teacher's Note:
1. Capacitance is inversely proportional to the separation.
(a) \( N^{5/3} \) times
(b) \( N^{2/3} \) times
(c) N times
(d) \( N^{1/3} \) times
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Answer: (d) \( N^{1/3} \) times
Explanation:
1. Volume conservation: \( R=N^{1/3}r \).
2. Capacitance of a sphere is proportional to its radius, so \( C'=N^{1/3}C \).
Teacher's Note:
1. Volume is conserved, not surface area.
2. C ∝ R for a sphere.
(a) 4 J
(b) 2 erg
(c) \( 4\times10^{-3} \) erg
(d) 2 J
Show Answer & Explanation
Answer: (d) 2 J
Explanation:
1. \( U=\tfrac12CV^2=\tfrac12\times4\times10^{-6}\times(10^3)^2=2 \) J.
Teacher's Note:
1. Use SI units: μF → 10⁻⁶ F, kV → 10³ V.
(a) \( 600\ \mu\text J \)
(b) \( 900\ \mu\text J \)
(c) \( 300\ \mu\text J \)
(d) \( 450\ \mu\text J \)
Show Answer & Explanation
Answer: (a) \( 600\ \mu\text J \)
Explanation:
1. Charges 20 μC and 80 μC; opposite joining gives net 60 μC on 6 μF: \( V=10 \) V.
2. Initial energy \( \tfrac12\cdot2\cdot100+\tfrac12\cdot4\cdot400=900 \) μJ; final \( \tfrac12\cdot6\cdot100=300 \) μJ.
3. Heat \( =600 \) μJ.
Teacher's Note:
1. Heat = initial energy − final energy.
(a) 2 : 1
(b) 1 : 2
(c) 4 : 1
(d) 1 : 4
Show Answer & Explanation
Answer: (d) 1 : 4
Explanation:
1. In series both carry the same charge, so \( V\propto1/C \).
2. \( V_1:V_2=C_2:C_1=1:4 \).
Teacher's Note:
1. Smaller capacitance takes the larger share of voltage.
(a) \( 37\times10^{-12} \) C²N⁻¹m⁻²
(b) \( 28\times10^{-12} \) C²N⁻¹m⁻²
(c) \( 25\times10^{-12} \) C²N⁻¹m⁻²
(d) \( 27\times10^{-12} \) C²N⁻¹m⁻²
Show Answer & Explanation
Answer: (d) \( 27\times10^{-12} \) C²N⁻¹m⁻²
Explanation:
1. At constant charge \( V\propto1/K \): \( K=3000/1000=3 \).
2. Permittivity \( \varepsilon=K\varepsilon_0=27\times10^{-12} \) SI.
Teacher's Note:
1. Isolated capacitor: voltage falls by factor K.
(a) \( \dfrac{KCE}{K+1} \)
(b) \( \dfrac{(K+1)CE}{2(K-1)} \)
(c) \( \dfrac{(K-1)CE}{2(K+1)} \)
(d) \( \dfrac{CE}{2K} \)
Show Answer & Explanation
Answer: (c) \( \dfrac{(K-1)CE}{2(K+1)} \)
Explanation:
1. Initial charge \( CE/2 \); final \( \dfrac{KCE}{K+1} \).
2. Difference \( =CE\dfrac{2K-(K+1)}{2(K+1)}=\dfrac{(K-1)CE}{2(K+1)} \).
Teacher's Note:
1. Same reasoning as for two identical capacitors in series.
(a) 100 V
(b) 600 V
(c) zero
(d) 400 V
Show Answer & Explanation
Answer: (b) 600 V
Explanation:
1. The charge is unchanged, so the field in the air gaps stays 200 V/cm.
2. The field inside the metal is zero, so the voltage is \( 200\times(5-2)=600 \) V.
Teacher's Note:
1. Isolated capacitor: charge, hence field, is fixed.
(a) \( C_0/5 \), \( W_0/5 \)
(b) \( 5C_0 \), \( W_0/5 \)
(c) \( 5C_0 \), \( 5W_0 \)
(d) \( C_0/5 \), \( 5W_0 \)
Show Answer & Explanation
Answer: (b) \( 5C_0 \), \( W_0/5 \)
Explanation:
1. Capacitance becomes \( KC_0=5C_0 \).
2. At constant charge \( U=Q^2/2C \) falls to \( W_0/5 \).
Teacher's Note:
1. Constant charge: energy ∝ 1/C.
(a) the intensity of the electric field
(b) the charge
(c) the capacity
(d) the energy of the condenser
Show Answer & Explanation
Answer: (b) the charge
Explanation:
1. The condenser is isolated, so the charge remains constant.
2. The capacity rises by \( K \), the field and the energy fall by \( K \).
Teacher's Note:
1. Isolated: Q constant.
(a) \( 200\ \mu C \)
(b) \( 1280\ \mu C \)
(c) \( 160\ \mu C \)
(d) \( 320\ \mu C \)
Show Answer & Explanation
Answer: (c) \( 160\ \mu C \)
Explanation:
1. Charge limits: \( 8\times20=160 \) μC and \( 16\times80=1280 \) μC.
2. In series the same charge flows on both, so the smaller limit, 160 μC, applies.
Teacher's Note:
1. Use the smaller charge limit.
(a) \( 1300\ \mu J \)
(b) \( 1600\ \mu J \)
(c) \( 1500\ \mu J \)
(d) \( 1200\ \mu J \)
Show Answer & Explanation
Answer: (d) \( 1200\ \mu J \)
Explanation:
1. Total charge \( 120 \) μC drawn at 10 V: \( W=QV=120\times10=1200 \) μJ.
2. Half of this (600 μJ) is stored and half is dissipated.
Teacher's Note:
1. Battery work is QV, twice the stored energy.
(a) \( \dfrac{2\varepsilon_0A}{d}\,\dfrac{K_1+K_2}{K_1K_2} \)
(b) \( \dfrac{2\varepsilon_0A}{d}\,\dfrac{K_1K_2}{K_1+K_2} \)
(c) \( \dfrac{d}{2\varepsilon_0A} \)
(d) \( \dfrac{2\varepsilon_0A}{d}(K_1+K_2) \)
Show Answer & Explanation
Answer: (b) \( \dfrac{2\varepsilon_0A}{d}\,\dfrac{K_1K_2}{K_1+K_2} \)
Explanation:
1. Two layers in series: \( C_1=\dfrac{2K_1\varepsilon_0A}{d} \) and \( C_2=\dfrac{2K_2\varepsilon_0A}{d} \).
2. Series: \( C=\dfrac{C_1C_2}{C_1+C_2}=\dfrac{2\varepsilon_0A}{d}\dfrac{K_1K_2}{K_1+K_2} \).
Teacher's Note:
1. Layers parallel to the plates are in series.
(a) 0.33
(b) 3
(c) 7.5
(d) 4
Show Answer & Explanation
Answer: (b) 3
Explanation:
1. Parallel combination: \( C=\dfrac{C_0}{2}+\dfrac{KC_0}{2}=\dfrac{C_0}{2}(1+K) \).
2. So \( 5=1.25(1+K) \) and \( K=3 \).
Teacher's Note:
1. Side-by-side regions are in parallel.
(a) 1
(b) 2
(c) 4
(d) 3
Show Answer & Explanation
Answer: (d) 3
Explanation:
1. Final charge \( =60+120=180 \) μC at the same voltage.
2. Charge is proportional to capacitance: \( K=180/60=3 \).
Teacher's Note:
1. The battery keeps the potential fixed.
(a) \( 900\ \mu J \)
(b) \( 1800\ \mu J \)
(c) \( 2700\ \mu J \)
(d) \( 3600\ \mu J \)
Show Answer & Explanation
Answer: (b) \( 1800\ \mu J \)
Explanation:
1. Battery voltage \( V=60/2=30 \) V; battery work \( =120\times30=3600 \) μJ.
2. Stored energy rises from \( \tfrac12\times60\times30=900 \) μJ to \( \tfrac12\times180\times30=2700 \) μJ, an increase of 1800 μJ.
3. Heat \( =3600-1800=1800 \) μJ.
Teacher's Note:
1. Heat = work by battery − increase in stored energy.
(a) decreased to one-half
(b) decreased to \( 1/\sqrt2 \)
(c) increased by a factor \( \sqrt2 \)
(d) increased to twice
Show Answer & Explanation
Answer: (a) decreased to one-half
Explanation:
1. With the same free charge, \( E=\dfrac{E_0}{K}=\dfrac{E_0}{2} \).
Teacher's Note:
1. Dielectrics weaken the field by the factor K.
(a) 60 μC
(b) 70 μC
(c) 30 μC
(d) 80 μC
Show Answer & Explanation
Answer: (b) 70 μC
Explanation:
1. \( \tau=RC=2 \) s. Charge after 4 s of charging: \( q=600(1-e^{-2})=519 \) μC.
2. Discharging for another 4 s: \( q=519\,e^{-2}\approx70 \) μC.
Teacher's Note:
1. First find the charge at the end of charging.
(a) (n + 1)C
(b) C
(c) \( (n-1)C \)
(d) nC
Show Answer & Explanation
Answer: (c) \( (n-1)C \)
Explanation:
1. \( n \) plates form \( (n-1) \) gaps, each of capacitance \( C \), all connected in parallel.
2. Total \( (n-1)C \).
Teacher's Note:
1. Count the gaps, not the plates.
(a) \( \dfrac{mC\Delta T}{s} \)
(b) \( \sqrt{\dfrac{2mC\Delta T}{s}} \)
(c) \( \dfrac{ms\Delta T}{C} \)
(d) \( \sqrt{\dfrac{2ms\Delta T}{C}} \)
Show Answer & Explanation
Answer: (d) \( \sqrt{\dfrac{2ms\Delta T}{C}} \)
Explanation:
1. All the stored energy becomes heat: \( \tfrac12CV^2=ms\Delta T \).
2. So \( V=\sqrt{\dfrac{2ms\Delta T}{C}} \).
Teacher's Note:
1. Energy conservation.
(a) \( 6\times10^{4} \) C/m²
(b) \( 6\times10^{-7} \) C/m²
(c) \( 3\times10^{4} \) C/m²
(d) \( 3\times10^{-7} \) C/m²
Show Answer & Explanation
Answer: (b) \( 6\times10^{-7} \) C/m²
Explanation:
1. Free charge density \( \sigma=K\varepsilon_0E=2.2\times8.85\times10^{-12}\times3\times10^4 \).
2. This equals \( 5.8\times10^{-7}\approx6\times10^{-7} \) C/m².
Teacher's Note:
1. In a dielectric \( E=\sigma/K\varepsilon_0 \).
(a) \( \dfrac{Q\rho}{K\varepsilon_0} \)
(b) \( \dfrac{QK}{\varepsilon_0\rho} \)
(c) \( \dfrac{Q}{K\varepsilon_0\rho^2} \)
(d) \( \dfrac{Q}{K\varepsilon_0\rho} \)
Show Answer & Explanation
Answer: (d) \( \dfrac{Q}{K\varepsilon_0\rho} \)
Explanation:
1. Resistance of the dielectric \( R=\rho\dfrac dA \); capacitance \( C=\dfrac{K\varepsilon_0A}{d} \).
2. Voltage \( V=Q/C \), current \( i=\dfrac VR=\dfrac{Q}{RC}=\dfrac{Q}{K\varepsilon_0\rho} \).
Teacher's Note:
1. RC = Kε₀ρ is independent of geometry.
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Practice MCQs for JEE Physics Electrostatic Potential and Capacitance
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