Capacitor

NEET Physics · 98 questions · Page 4 of 10 · Click an option or "Show Solution" to reveal answer

Q31
A parallel plate air capacitor is charged to a potential difference of V volts. After disconnecting the charging battery the distance between the plates of the capacitor is increased using an insulting handle. As a result the potential difference between the plates
A increases
B decreases
C does not charge
D becomes zero
Correct Answer
Option A
Solution

If we increase the distance between the plates its capacity decreases resulting in higher potential as we know Q = CV.

Since Q is constant (battery has been disconnected), on decreasing C, V will increase.

Q32
A network of four capacitors of capacity equal to C 1 = C, C 2 = 2C, C 3 = 3C and C 4 = 4C are connected to a battery as shown in the figure. The ratio of the charges on C 2 and C 4 is
A 4/7
B 3/22
C 7/4
D 22/3
Correct Answer
Option B
Solution

Equivalent capacitance for three capacitors (C 1 , C 2 & C 3 ) in series is given by

1Ceq.=1C1+1C2+1C3{1 \over {{C_{eq.}}}} = {1 \over {{C_1}}} + {1 \over {{C_2}}} + {1 \over {{C_3}}}
=C2C3+C3C1+C1C2C1C2C3= {{{C_2}{C_3} + {C_3}{C_1} + {C_1}{C_2}} \over {{C_1}{C_2}{C_3}}}
Ceq.=C1C2C3C2C3+C3C1+C1C2\Rightarrow {C_{eq.}} = {{{C_1}{C_2}{C_3}} \over {{C_2}{C_3} + {C_3}{C_1} + {C_1}{C_2}}}
Ceq.=2(2C)(3C)C(2C)+(2C)(3C)+(3C)C=611C\Rightarrow {C_{eq.}} = {{2\left( {2C} \right)\left( {3C} \right)} \over {C\left( {2C} \right) + \left( {2C} \right)\left( {3C} \right) + \left( {3C} \right)C}} = {6 \over {11}}C

\Rightarrow Charge on capacitors (C 1 , C 2 & C 3 ) in series

=CeqV=6C11V= {C_{eq}}V = {{6C} \over {11}}V

Charge on capacitor

C4=C4V=4CV{C_4} = {C_4}V = 4CV
ChargeonC2ChargeonC4=6C11V4CV=611×14=322{{Charg e\,on\,{C_2}} \over {Charg e\,on\,{C_4}}} = {{{{6C} \over {11}}V} \over {4CV}} = {6 \over {11}} \times {1 \over 4} = {3 \over {22}}
Q33
Three capacitors each of capacity 4 μ\mu F are to be connected in such a way that the effective capacitance is 6μF.6\mu F. This can be done by
A connecting all of them in series
B connecting them in parallel
C connecting two in series and one in parallel
D connecting two in parallel and one in series
Correct Answer
Option C
Solution

For series,

C=C1×C2C1+C2=4×44+4=2μFC' = {{{C_1} \times {C_2}} \over {{C_1} + {C_2}}} = {{4 \times 4} \over {4 + 4}} = 2\mu F

For parallel

Ceq=C+C3=2+4=6μF{C_{eq}} = C' + {C_3} = 2 + 4 = 6\mu F
Q34
A capacitor of capacity C 1 charged upto V volt and then connected to an uncharged capacitor of capacity C 2 . The final potential difference across each will be
A C1VC1+C2{{{C_1}V} \over {{C_1} + {C_2}}}
B C2VC1+C2{{{C_2}V} \over {{C_1} + {C_2}}}
C (1C2C1)V\left( {1 - {{{C_2}} \over {{C_1}}}} \right)V
D (1+C2C1)\left( {1 + {{{C_2}} \over {{C_1}}}} \right)
Correct Answer
Option A
Solution

Charge Q = C 1 V Total capacity of combination (parallel) C = C 1 + C 2

P.D.=QC=C1VC1+C2P.D. = {Q \over C} = {{{C_1}V} \over {{C_1} + {C_2}}}
Q35
Energy per unit volume for a capacitor having area A and separation d kept at potential difference V is given by
A 12ε0V2d2{1 \over 2}{\varepsilon _0}{{{V^2}} \over {{d^2}}}
B 12ε0V2d2{1 \over {2{\varepsilon _0}}}{{{V^2}} \over {{d^2}}}
C 12CV2{1 \over 2}C{V^2}
D Q22C.{{{Q^2}} \over {2C}}.
Correct Answer
Option A
Solution

Energy stored per unit volume

=12ε0E2=12ε0(Vd)2=12ε0V2d2= {1 \over 2}{\varepsilon _0}{E^2} = {1 \over 2}{\varepsilon _0}{\left( {{V \over d}} \right)^2} = {1 \over 2}{\varepsilon _0}{{{V^2}} \over {{d^2}}}
(E=Vd)\left(\because {E = {V \over d}} \right)
Q36
A capacitor is charged with a battery and energy stored is U. After disconnecting battery another capacitor of same capacity is connected in parallel to the first capacitor. Then energy stored in each capacitor is
A U/2U/2
B U/4
C 4U
D 2U
Correct Answer
Option B
Solution

Let q be the charge on each capacitor. \therefore Energy stored,

U=12CV2=12q2CU = {1 \over 2}C{V^2} = {1 \over 2}{{{q^2}} \over C}

Now, when battery is disconnected and another capacitor of same capacity is connected in parallel to the first capacitor, then voltage across each capacitor,

V=q2CV = {q \over {2C}}

\therefore Energy stored =

12C(q2C)2=14.12q2C=14U.{1 \over 2}C{\left( {{q \over {2C}}} \right)^2} = {1 \over 4}.{1 \over 2}{{{q^2}} \over C} = {1 \over 4}U.
Q37
A capacitor has air as dielectric medium and two conducting plates of area 12 cm212 \mathrm{~cm}^2 and they are 0.6 cm0.6 \mathrm{~cm} apart. When a slab of dielectric having area 12 cm212 \mathrm{~cm}^2 and 0.6 cm0.6 \mathrm{~cm} thickness is inserted between the plates, one of the conducting plates has to be moved by 0.2 cm0.2 \mathrm{~cm} to keep the capacitance same as in previous case. The dielectric constant of the slab is : (Given ϵ0=8.834×1012 F/m\epsilon_0=8.834 \times 10^{-12} \mathrm{~F} / \mathrm{m})
A 1.50
B 0.66
C 1.33
D 1
Correct Answer
Option A
Solution
0Ad=ϵ0Adk+0.210.60.2=0.6kk=0.60.4=1.5\begin{aligned} & \frac{\in_0 A}{d}=\frac{\epsilon_0 A}{\frac{d}{k}+\frac{0.2}{1}} \\ & \Rightarrow \quad 0.6-0.2=\frac{0.6}{k} \\ & \quad k=\frac{0.6}{0.4}=1.5 \end{aligned}
Q38
Capacitance (in FF) of a spherical conductor with radius 11 mm is
A 1.1×10101.1 \times {10^{ - 10}}
B 106{10^{ - 6}}
C 9×1099 \times {10^{ - 9}}
D 103{10^{ - 3}}
Correct Answer
Option A
Solution

For an isolated sphere, the capacitance is given by

C=4π0rC = 4\pi \,{ \in _0}\,r
=19×109×1= {1 \over {9 \times {{10}^9}}} \times 1
=1.1×1010F= 1.1 \times {10^{ - 10}}F
Q39
Two capacitors of capacities 2C and C are joined in parallel and charged up to potential V. The battery is removed and the capacitor of capacity C is filled completely with a medium of dielectric constant K. The potential difference across the capacitors will now be :
A VK+2{V \over {K + 2}}
B VK{V \over K}
C 3VK+2{{3V} \over {K + 2}}
D 3VK{{3V} \over K}
Correct Answer
Option C
Solution
VC=2CV+CVKC+2C{V_C} = {{2CV + CV} \over {KC + 2C}}
=3VK+2= {{3V} \over {K + 2}}
Q40
If the charge on a capacitor is increased by 2 C, the energy stored in it increases by 44%. The original charge on the capacitor is (in C)
A 10
B 20
C 30
D 40
Correct Answer
Option A
Solution

Let initially the charge is q so

12q2C=Ui{1 \over 2}{{{q^2}} \over C} = {U_i}

And

12(q+2)2C=Uf{1 \over 2}{{{{(q + 2)}^2}} \over C} = {U_f}

Given

UfUiUi×100=44{{{U_f} - {U_i}} \over {{U_i}}} \times 100 = 44
(q+2)2q2q=.44{{{{(q + 2)}^2} - {q^2}} \over q} = .44
q=10C\Rightarrow q = 10C
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