Electrostatics

JEE Physics · 130 questions · Page 2 of 13 · Click an option or "Show Solution" to reveal answer

Q11
A charged oil drop is suspended in a uniform field of 3×1043 \times {10^4} v/mv/m so that it neither falls nor rises. The charge on the drop will be (Take the mass of the charge =9.9×1015kg = 9.9 \times {10^{ - 15}}\,\,kg and g=10m/s2g = 10\,m/{s^2})
A 1.6×1018C1.6 \times {10^{ - 18}}\,C
B 3.2×1018C3.2 \times {10^{ - 18}}\,C
C 3.3×1018C3.3 \times {10^{ - 18}}\,C
D 4.8×1018C4.8 \times {10^{ - 18}}\,C
Correct Answer
Option C
Solution

At equilibrium, electric force on drop balances weight of drop.

qE=mgqqE = mg \Rightarrow q
=mgE=9.9×1015×103×104= {{mg} \over E} = {{9.9 \times {{10}^{ - 15}} \times 10} \over {3 \times {{10}^4}}}
=3.3×1018C= 3.3 \times {10^{ - 18}}C
Q12
Two thin wire rings each having a radius RR are placed at a distance dd apart with their axes coinciding. The charges on the two rings are +q+q and q.-q. The potential difference between the centres of the two rings is
A q2π0[1R1R2+d2]{q \over {2\pi \,{ \in _0}}}\left[ {{1 \over R} - {1 \over {\sqrt {{R^2} + {d^2}} }}} \right]
B qR4π0d2{{qR} \over {4\pi \,{ \in _0}\,{d^2}}}
C q4π0[1R1R2+d2]{q \over {4\pi \,{ \in _0}}}\left[ {{1 \over R} - {1 \over {\sqrt {{R^2} + {d^2}} }}} \right]
D zero
Correct Answer
Option A
Solution
VA=Vself+Vdue{V_A} = {V_{self}} + {V_{due}}

to

(2)(2)
VA=14πε0[qRqR2+d2]\Rightarrow {V_A} = {1 \over {4\pi {\varepsilon _0}}}\left[ {{q \over R} - {q \over {\sqrt {{R^2} + {d^2}} }}} \right]
VB=Vself+Vdue{V_B} = {V_{self}} + {V_{due}}

to

(1)(1)
VB=14πε0[qR+qR2+d2]\Rightarrow {V_B} = {1 \over {4\pi {\varepsilon _0}}}\left[ {{{ - q} \over R} + {q \over {\sqrt {{R^2} + {d^2}} }}} \right]
ΔV=VAVB\Delta V = {V_A} - {V_B}
=14πε0[qR+qRqR2+d2qR2+d2]= {1 \over {4\pi {\varepsilon _0}}}\left[ {{q \over R} + {q \over R} - {q \over {\sqrt {{R^2} + {d^2}} }} - {q \over {\sqrt {{R^2} + {d^2}} }}} \right]
=12πε0[qRqR2+d2]= {1 \over {2\pi {\varepsilon _0}}}\left[ {{q \over R} - {q \over {\sqrt {{R^2} + {d^2}} }}} \right]
Q13
Two point charges +8q+8q and 2q-2q are located at x=0x=0 and x=Lx=L respectively. The location of a point on the xx axis at which the net electric field due to these two point charges is zero is
A L4{L \over 4}
B 22 LL
C 44 LL
D 88 LL
Correct Answer
Option B
Solution
K2q(xL)2+K8qx2=01(xL)2=4x2{{ - K2q} \over {{{\left( {x - L} \right)}^2}}} + {{K8q} \over {{x^2}}} = 0 \Rightarrow {1 \over {{{\left( {x - L} \right)}^2}}} = {4 \over {{x^2}}}

or,

1xL=2xx=2x2L{1 \over {x - L}} = {2 \over x} \Rightarrow x = 2x - 2L

or,

x=2Lx=2L
Q14
An electric dipole is placed at an angle of 30{30^ \circ } to a non-uniform electric field. The dipole will experience
A a translation force only in the direction of the field
B a translation force only in a direction normal to the direction of the field
C a torque as well as a translational force
D a torque only
Correct Answer
Option C
Solution

The electric field will be different at the location of the two charges.

Therefore the two forces will be unequal.

This will result in a force as well as torque.

Q15
Two spherical conductors AA and BB of radii 11 mmmm and 22 mmmm are separated by a distance of 55 cmcm and are uniformly charged. If the spheres are connected by a conducting wire then in equilibrium condition, the ratio of the magnitude of the electric fields at the surfaces of spheres AA and BB is
A 4:14:1
B 1:21:2
C 2:12:1
D 1:41:4
Correct Answer
Option C
Solution

After connection,

V1=V2{V_1} = {V_2}
KQ1r1=KQ2r2\Rightarrow K{{{Q_1}} \over {{r_1}}} = K{{{Q_2}} \over {{r^2}}}
Q1r1=Q2r2\Rightarrow {{Q{}_1} \over {{r_1}}} = {{{Q_2}} \over {{r_2}}}

The ratio of electric fields

E1E2=KQ1r12KQ2r22=Q1r12×r22Q2{{{E_1}} \over {{E_2}}} = {{K{{{Q_1}} \over {r_1^2}}} \over {K{{{Q_2}} \over {r_2^2}}}} = {{{Q_1}} \over {r_1^2}} \times {{r_2^2} \over {{Q_2}}}
E1E2=r1×r22r12×r2E1E2=r2r1=21\Rightarrow {{{E_1}} \over {{E_2}}} = {{{r_1} \times r_2^2} \over {r_1^2 \times {r_2}}} \Rightarrow {{{E_1}} \over {{E_2}}} = {{{r_2}} \over {{r_1}}} = {2 \over 1}

Since the distance between the spheres is large as compared to their diameters, the induced effects may be ignored.

Q16
An electric charge 103μC{10^{ - 3}}\,\,\mu \,C is placed at the origin (0,0)(0,0) of XYX-Y co-ordinate system. Two points AA and BB are situated at (2,2)\left( {\sqrt 2 ,\sqrt 2 } \right) and (2,0)\left( {2,0} \right) respectively. The potential difference between the points AA and BB will be
A 4.54.5 volts
B 99 volts
C zero
D 22 volts
Correct Answer
Option C
Solution

The distance of point

A(2,2)A\left( {\sqrt 2 ,\sqrt 2 } \right)

from the origin,

OA=r1OA = \left| {\overrightarrow {{r_1}} } \right|
=(2)2+(2)2= \sqrt {{{\left( {\sqrt 2 } \right)}^2} + {{\left( {\sqrt 2 } \right)}^2}}
=4=2= \sqrt 4 = 2

The distance of point

B(2,0)B(2,0)

from the origin,

OB=r2=(2)2+(0)2=2OB = \left| {\overrightarrow {{r_2}} } \right| = \sqrt {{{\left( 2 \right)}^2} + {{\left( 0 \right)}^2}} = 2

units. Now, potential at

A,A,
VA=14π0.Q(OA){V_A} = {1 \over {4\pi { \in _0}}}.{Q \over {\left( {OA} \right)}}

Potential at

B,B,
VB=14π0.Q(Ob){V_B} = {1 \over {4\pi { \in _0}}}.{Q \over {\left( {Ob} \right)}}

\therefore Potential difference between the points

AA

and

BB

is zero.

Q17
The potential at a point xx (measured in μm\mu \,m) due to some charges situated on the xx-axis is given by V(x)=20/(x24)V\left( x \right) = 20/\left( {{x^2} - 4} \right) volt The electric field EE at x=4μmx = 4\,\mu \,m is given by
A (10/9)(10/9) volt / μ\mu mm and in the +ve + ve xx direction
B (5/3)\left( {5/3} \right) volt/ μ\mu mm and in the ve-ve xx direction
C (5/3)\left( {5/3} \right) volt/μ\mu mm and in the +ve+ve xx direction
D (10/9)\left( {10/9} \right) volt/ μm\mu \,m and in the ve-ve xx direction
Correct Answer
Option A
Solution

Here,

V(x)=20x24voltV\left( x \right) = {{20} \over {{x^2} - 4}}volt

We know that

E=dVdx=ddx(20x24)E = - {{dV} \over {dx}} = {d \over {dx}}\left( {{{20} \over {{x^2} - 4}}} \right)

or,

E=+40x(x24)2E = + {{40x} \over {{{\left( {{x^2} - 4} \right)}^2}}}

At

x=4μm,x = 4\mu m,
E=+40×4(424)2E = + {{40 \times 4} \over {{{\left( {{4^2} - 4} \right)}^2}}}
=+160144=+109volt/μm.= + {{160} \over {144}} = + {{10} \over 9}volt/\mu m.

Positive sign indicates that

E\overrightarrow E

is in

+ve+ve
xx

-direction.

Q18
A charge QQ is placed at each of the opposite corners of a square. A charge qq is placed at each of the other two corners. If the net electrical force on QQ is zero, then Q/qQ/q equals:
A 1-1
B 11
C 12 - {1 \over {\sqrt 2 }}
D 22 - 2\sqrt 2
Correct Answer
Option D
Solution

Let

FF

be the force between

QQ

and

Q.Q.

The force between

qq

and

QQ

should be attractive for net force on

QQ

to be zero. Let

FF'

be the force between

QQ

and

q.q.

For equilibrium

2F=F\sqrt 2 F' = - F
2×kQq2=kQ2(2)2\sqrt 2 \times k{{Qq} \over {{\ell ^2}}} = - k{{{Q^2}} \over {{{\left( {\sqrt 2 \ell } \right)}^2}}}
Qq=22\Rightarrow {Q \over q} = - 2\sqrt 2
Q19
Let P(r)=QπR4rP\left( r \right) = {Q \over {\pi {R^4}}}r be the change density distribution for a solid sphere of radius RR and total charge QQ. For a point p'p' inside the sphere at distance r1{r_1} from the center of the sphere, the magnitude of electric field is :
A Q4π0r12{Q \over {4\pi \,{ \in _0}\,r_1^2}}
B Qr124π0R4{{Qr_1^2} \over {4\pi \,{ \in _0}\,{R^4}}}
C Qr123π0R4{{Qr_1^2} \over {3\pi \,{ \in _0}\,{R^4}}}
D 00
Correct Answer
Option B
Solution

Let us consider a spherical shell of thickness

dxdx

and radius

x.x.

The volume of this spherical shell

=4πr2dr.= 4\pi {r^2}dr.

The charge enclosed within shell

=QrπR4[4πr2dr]= {{{Q_r}} \over {\pi {R^4}}}\left[ {4\pi {r^2}dr} \right]

The charge enclosed in a sphere of radius

r1{r_1}

is

4QR40r1r3dr{{4Q} \over {{R^4}}}\int\limits_0^{{r_1}} {{r^3}} dr
=4QR4[r44]0r1= {{4Q} \over {{R^4}}}\left[ {{{{r^4}} \over 4}} \right]_0^{{r_1}}
=QR4r14= {Q \over {{R^4}}}r_1^4

\therefore The electric field at point

pp

inside the sphere at a distance

r1{r_1}

from the center of the sphere is

E=14π0[QR4r14]r12E = {1 \over {4\pi { \in _0}}}{{\left[ {{Q \over {{R^4}}}r_1^4} \right]} \over {r_1^2}}
=14π0QR4r12= {1 \over {4\pi { \in _0}}}{Q \over {{R^4}}}r_1^2
Q20
Two points PP and QQ are maintained at the potentials of 1010 VV and 4-4 VV, respectively. The work done in moving 100100 electrons from PP to QQ is :
A 9.60×1017J9.60 \times {10^{ - 17}}J
B 2.24×1016J - 2.24 \times {10^{ - 16}}J
C 2.24×1016J 2.24 \times {10^{ - 16}}J
D 9.60×1017J- 9.60 \times {10^{ - 17}}J
Correct Answer
Option C
Solution
WPQq=(VQVP){{{W_{PQ}}} \over q} = \left( {{V_Q} - {V_P}} \right)
WPQ=q(VQVP)\Rightarrow {W_{PQ}} = q\left( {{V_Q} - {V_P}} \right)
=(100×1.6×1019)(410)= \left( { - 100 \times 1.6 \times {{10}^{ - 19}}} \right)\left( { - 4 - 10} \right)
=+2.24×1016J= + 2.24 \times {10^{ - 16}}J
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