Capacitor

JEE Physics · 62 questions · Page 2 of 7 · Click an option or "Show Solution" to reveal answer

Q11
An electron is made to enter symmetrically between two parallel and equally but oppositely charged metal plates, each of 10 cm length. The electron emerges out of the electric field region with a horizontal component of velocity 106 m/s10^6 \mathrm{~m} / \mathrm{s}. If the magnitude of the electric field between the plates is 9.1 V/cm9.1 \mathrm{~V} / \mathrm{cm}, then the vertical component of velocity of electron is (mass of electron =9.1×1031 kg=9.1 \times 10^{-31} \mathrm{~kg} and charge of electron =1.6×1019C=1.6 \times 10^{-19} \mathrm{C} )
A 1×106 m/s1 \times 10^6 \mathrm{~m} / \mathrm{s}
B 16×106 m/s16 \times 10^6 \mathrm{~m} / \mathrm{s}
C 16×104 m/s16 \times 10^4 \mathrm{~m} / \mathrm{s}
D 0
Correct Answer
Option B
Solution

No force in horizontal direction, i.e., Fx=0F_x=0 ax=0\Rightarrow a_x=0 So, vxv_x = constant hence, t=lvxt=\dfrac{l}{v_x} .....

(1) Now, for y-direction, using Ist equation of motion,

vy=uy+ayt{v_y} = {u_y} + {a_y}t
vy=0+eEm(lvx)\Rightarrow {v_y} = 0 + {{eE} \over m}\left( {{l \over {{v_x}}}} \right)

(from (1) and usiung F=maF=ma and a=Fma=\dfrac{F}{m})

vy=1.6×1019×9.1×102×0.19.1×1031×106\Rightarrow {v_y} = {{1.6 \times {{10}^{ - 19}} \times 9.1 \times {{10}^2} \times 0.1} \over {9.1 \times {{10}^{ - 31}} \times {{10}^6}}}
=1.6×107= 1.6 \times {10^7}

m/s

vy=16×106\Rightarrow {v_y} = 16 \times {10^6}

m/s.

Q12
Three capacitors each of 4 μ\mu F are to be connected in such a way that the effective capacitance is 6 μ\mu F. This can be done by connecting them :
A all in series
B two in series and one in parallel
C all in parallel
D two in parallel and one in series
Correct Answer
Option B
Solution

(a)

1Ceq=14+14+14=34{1 \over {{C_{eq}}}} = {1 \over 4} + {1 \over 4} + {1 \over 4} = {3 \over 4}

\Rightarrow

Ceq=43μF{C_{eq}} = {4 \over 3}\,\mu F

(b)

Ceq=4×44+4+4=6μF{C_{eq}} = {{4 \times 4} \over {4 + 4}} + 4 = 6\mu F

(c)

Ceq=4+4+4=12μF{C_{eq}} = 4 + 4 + 4 = 12\,\mu F

(d)

Ceq=(4+4)×4(4+4)+4=83μF{C_{eq}} = {{\left( {4 + 4} \right) \times 4} \over {\left( {4 + 4} \right) + 4}} = {8 \over 3}\mu F
Q13
The energy stored in the electric field produced by a metal sphere is 4.5 J. If the sphere contains 4 μ\mu C charge, its radius will be : [ Take : 14π0={1 \over {4\,\pi { \in _0}}} = 9 × \times 109 N - m2/C2 ]
A 20 mm
B 32 mm
C 28 mm
D 16 mm
Correct Answer
Option D
Solution

Energy of sphere =

Q22C{{{Q^2}} \over {2C}}
\therefore\,\,\,
16×10122C{{16 \times {{10}^{ - 12}}} \over {2C}}

= 4.5 \Rightarrow

\,\,\,

C =

16×10129{{16 \times {{10}^{ - 12}}} \over 9}

We know capacity of spherical conductor, C = 4π\pi

ε\varepsilon

0R

\therefore\,\,\,

4π\pi

ε\varepsilon

0R =

16×10129{{16 \times {{10}^{ - 12}}} \over 9}

\Rightarrow

\,\,\,

R =

14πε0×16×10129{1 \over {4\pi {\varepsilon _0}}} \times {{16 \times {{10}^{ - 12}}} \over 9}

= 9 ×\times 109 ×\times

16×10129{{16 \times {{10}^{ - 12}}} \over 9}

= 16 mm

Q14
A parallel plate capacitor of capacitance 2 F2 \mathrm{~F} is charged to a potential V\mathrm{V}, The energy stored in the capacitor is E1E_{1}. The capacitor is now connected to another uncharged identical capacitor in parallel combination. The energy stored in the combination is E2\mathrm{E}_{2}. The ratio E2/E1\mathrm{E}_{2} / \mathrm{E}_{1} is :
A 1 : 2
B 2 : 3
C 2 : 1
D 1 : 4
Correct Answer
Option A
Solution

To determine the ratio

E2/E1\mathrm{E}_{2} / \mathrm{E}_{1}

, we will follow these steps: 1. Calculate the initial energy stored in the original capacitor

E1\mathrm{E}_{1}

. 2. Determine the energy stored in the system when two capacitors are connected in parallel, which is

E2\mathrm{E}_{2}

. 3. Find the ratio

E2/E1\mathrm{E}_{2} / \mathrm{E}_{1}

. Step 1: Calculate the initial energy stored in the original capacitor

E1\mathrm{E}_{1}

. The energy stored in a capacitor is given by the formula:

E=12CV2E = \frac{1}{2} CV^2

Given that the capacitance

CC

is

2 F2 \mathrm{~F}

, and the potential difference is

V\mathrm{V}

, the initial energy

E1\mathrm{E}_{1}

is:

E1=122 FV2E_{1} = \frac{1}{2} \cdot 2 \mathrm{~F} \cdot V^2
E1=V2 JE_{1} = V^2 \mathrm{~J}

Step 2: Determine the energy stored when two capacitors are connected in parallel When the charged capacitor (capacitor 1) is connected to an identical uncharged capacitor (capacitor 2), the charge will redistribute between the two capacitors.

The total capacitance of the parallel combination is:

Ctotal=2 F+2 F=4 FC_{\text{total}} = 2 \mathrm{~F} + 2 \mathrm{~F} = 4 \mathrm{~F}

The initial charge on capacitor 1 is:

Q1=CV=2 FV=2V CQ_1 = CV = 2 \mathrm{~F} \cdot V = 2V \mathrm{~C}

After connection, this charge will be shared equally by the two capacitors because they are identical.

Therefore, the voltage across each capacitor in the parallel combination will be:

Vacross each capacitor=Total chargeTotal capacitance=2V4 F=V2V_{\text{across each capacitor}} = \frac{\text{Total charge}}{\text{Total capacitance}} = \frac{2V}{4 \mathrm{~F}} = \frac{V}{2}

The energy stored in the parallel combination is:

E2=124 F(V2)2E_{2} = \frac{1}{2} \cdot 4 \mathrm{~F} \cdot \left(\frac{V}{2}\right)^2
E2=124 FV24E_{2} = \frac{1}{2} \cdot 4 \mathrm{~F} \cdot \frac{V^2}{4}
E2=V212 JE_{2} = V^2 \cdot \frac{1}{2} \mathrm{~J}

Step 3: Find the ratio

E2/E1\mathrm{E}_{2} / \mathrm{E}_{1}

We know that:

E1=V2 JE_{1} = V^2 \mathrm{~J}
E2=12V2 JE_{2} = \frac{1}{2} V^2 \mathrm{~J}

The ratio is then:

E2E1=12V2V2=12=1:2\frac{E_{2}}{E_{1}} = \frac{\frac{1}{2} V^2}{V^2} = \frac{1}{2} = 1 : 2

Therefore, the correct answer is: Option A: 1 : 2

Q15
A parallel plate capacitor of capacitance 90 pF is connected to a battery of emf 20 V. If a dielectric material of dielectric constant K = 5/3 is inserted between the plates, the magnitude of the induced charge will be :
A 0.9 n C
B 1.2 n C
C 0.3 n C
D 2.4 n C
Correct Answer
Option B
Solution

Charge on Capacitor initially, Qi = CV After inserting dielectric of dielectric constant = K, new capacitance, Qf = (KC)

\vee
\therefore\,\,\,

Induced charges on dielectric = Qf - Qi = KCV - CV = (K - ) CV =

(531)\left( {{5 \over 3} - 1} \right)

×\times 90 ×\times 10-12 ×\times 20 = 1.2 ×\times 10-9 C = 1.2 nC

Q16
Two equal capacitors are first connected in series and then in parallel. The ratio of the equivalent capacities in the two cases will be :
A 4 : 1
B 1 : 2
C 2 : 1
D 1 : 4
Correct Answer
Option D
Solution

Given, C1 = C2 = C When both capacitors are connected in series, their equivalent capacitance will be

1Cs=1C+1C=2C{1 \over {{C_s}}} = {1 \over C} + {1 \over C} = {2 \over C}
Cs=C2\Rightarrow {C_s} = {C \over 2}

When both capacitors are connected in parallel, their equivalent capacitance will be Cp = C + C = 2C \therefore The ratio of equivalent capacitance in series and parallel combination is

CsCp=C/22C=14{{{C_s}} \over {{C_p}}} = {{C/2} \over {2C}} = {1 \over 4}

\therefore Cs : Cp = 1 : 4

Q17
A parallel plate capacitor has plate of length 'l', width ‘w’ and separation of plates is ‘d’. It is connected to a battery of emf V. A dielectric slab of the same thickness ‘d’ and of dielectric constant k = 4 is being inserted between the plates of the capacitor. At what length of the slab inside plates, will the energy stored in the capacitor be two times the initial energy stored?
A l4{l \over 4}
B l2{l \over 2}
C 2l3{{2l} \over 3}
D l3{l \over 3}
Correct Answer
Option D
Solution

Ci =

ε0Ad=ε0lwd{{{\varepsilon _0}A} \over d} = {{{\varepsilon _0}lw} \over d}

Ui =

12CiV2{1 \over 2}{C_i}{V^2}

=

12ε0lwdV2{1 \over 2}{{{\varepsilon _0}lw} \over d}{V^2}

Cf = C1 + C2 =

Kε0A1d+ε0A2d{{K{\varepsilon _0}{A_1}} \over d} + {{{\varepsilon _0}{A_2}} \over d}

=

Kε0wxd+ε0w(lx)d{{K{\varepsilon _0}wx} \over d} + {{{\varepsilon _0}w\left( {l - x} \right)} \over d}

=

ε0wd[Kx+lx]{{{\varepsilon _0}w} \over d}\left[ {Kx + l - x} \right]

\therefore Uf =

12CfV2{1 \over 2}{C_f}{V^2}

=

12ε0wd[Kx+lx]V2{1 \over 2}{{{\varepsilon _0}w} \over d}\left[ {Kx + l - x} \right]{V^2}

Given Uf = 2Ui \Rightarrow

12ε0wd[Kx+lx]V2{1 \over 2}{{{\varepsilon _0}w} \over d}\left[ {Kx + l - x} \right]{V^2}

= 2 ×\times

12ε0lwdV2{1 \over 2}{{{\varepsilon _0}lw} \over d}{V^2}

\Rightarrow kx + l – x = 2l \Rightarrow 4x – x = l \Rightarrow 3x = l \Rightarrow x =

l3{l \over 3}
Q18
A parallel plate capacitor is formed by two plates each of area 30π\pi cm2 separated by 1 mm. A material of dielectric strength 3.6 ×\times 107 Vm-1 is filled between the plates. If the maximum charge that can be stored on the capacitor without causing any dielectric breakdown is 7 ×\times 10-6C, the value of dielectric constant of the material is : [Use 14πε0=9×109{1 \over {4\pi {\varepsilon _0}}} = 9 \times {10^9} Nm2 C-2]
A 1.66
B 1.75
C 2.25
D 2.33
Correct Answer
Option D
Solution

Field inside the dielectric

=σkε0= {\sigma \over {k{\varepsilon _0}}}

According to the given information,

σkε0=3.6×107{\sigma \over {k{\varepsilon _0}}} = 3.6 \times {10^7}
QAkε0=3.6×107\Rightarrow {{{Q \over A}} \over {k{\varepsilon _0}}} = 3.6 \times {10^7}
k=2.33\Rightarrow k = 2.33
Q19
Two capacitors of capacitances C and 2C are charged to potential differences V and 2V, respectively. These are then connected in parallel in such a manner that the positive terminal of one is connected to the negative terminal of the other. The final energy of this configuration is :
A Zero
B 32CV2{3 \over 2}C{V^2}
C 92CV2{9 \over 2}C{V^2}
D 256CV2{{25} \over 6}C{V^2}
Correct Answer
Option B
Solution

By conservation of charge,

q1+q2=q1+q2{q_1} + {q_2} = {q_1}' + {q_2}'

\Rightarrow

CV+(2C)(2V)=(C+2C)V- CV + (2C)(2V) = (C + 2C)V'
V=3CV3C=VV' = {{3CV} \over {3C}} = V
Uf=12Cv2+12(2C)V2{U_f} = {1 \over 2}C{v^2} + {1 \over 2}(2C){V^2}
Uf=32CV2{U_f} = {3 \over 2}C{V^2}
Q20
Effective capacitance of parallel combination of two capacitors C1 and C2 is 10 μF. When these capacitors are individually connected to a voltage source of 1V, the energy stored in the capacitor C2 is 4 times that of C1. If these capacitors are connected in series, their effective capacitance will be :
A 4.2 μF
B 8.4 μF
C 1.6 μF
D 3.2 μF
Correct Answer
Option C
Solution

C1 + C2 = 10 ......(1)

12C2V2=4×12C1V2{1 \over 2}{C_2}{V^2} = 4 \times {1 \over 2}{C_1}{V^2}

\Rightarrow C2 = 4C1 .....(2) From (1) ans (2), C1 = 2 and C2 = 8 For series combination Ceq =

C1C2C1+C2{{{C_1}{C_2}} \over {{C_1} + {C_2}}}

=

8×28+2{{8 \times 2} \over {8 + 2}}

= 1.6 μ\muF

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