Magnetic Effect of Current

JEE Physics · 124 questions · Page 7 of 13 · Click an option or "Show Solution" to reveal answer

Q61
A small circular loop of conducting wire has radius a and carries current I. It is placed in a uniform magnetic field B perpendicular to its plane such that when rotated slightly about its diameter and released, it starts performing simple harmonic motion of time period T. If the mass of the loop is m then :
A T=2mIBT = \sqrt {{{2m} \over {IB}}}
B T=πmIBT = \sqrt {{{\pi m} \over {IB}}}
C T=πm2IBT = \sqrt {{{\pi m} \over {2IB}}}
D T=2πmIBT = \sqrt {{{2\pi m} \over {IB}}}
Correct Answer
Option D
Solution

τ\tau = - MBsin θ\theta Iα\alpha = - MBsin θ\theta for small θ\theta, α\alpha =

MBIθ- {{MB} \over I}\theta

\therefore

ω2{\omega ^2}

=

MBI{{MB} \over I}

\Rightarrow ω\omega =

I(πR2)BmR22\sqrt {{{I\left( {\pi {R^2}} \right)B} \over {{{m{R^2}} \over 2}}}}

=

2IπBm\sqrt {{{2I\pi B} \over m}}

\therefore T =

2πω{{2\pi } \over \omega }

=

2πmIB\sqrt {{{2\pi m} \over {IB}}}
Q62
A proton, a deuteron and an α\alpha particle are moving with same momentum in a uniform magnetic field. The ratio of magnetic forces acting on them is _________ and their speed is _______, in the ratio.
A 2 : 1 : 1 and 4 : 2 : 1
B 4 : 2 : 1 and 2 : 1 : 1
C 1 : 2 : 4 and 2 : 1 : 1
D 1 : 2 : 4 and 1 : 1 : 2
Correct Answer
Option A
Solution

F = qvB = q

pm{p \over m}

B F \propto

qm{q \over m}

[as p, B are const.] \therefore F1 : F2 : F3 =

em:e2m:2e4m{e \over m}:{e \over {2m}}:{{2e} \over {4m}}

= 2 : 1 : 1 And v1 : v2 : v3 =

pm:p2m:p4m{p \over m}:{p \over {2m}}:{p \over {4m}}

= 4 : 2 : 1

Q63
Magnetic fields at two points on the axis of a circular coil at a distance of 0.05 m and 0.2 m from the centre are in the ratio 8 : 1. The radius of coil is ________.
A 1.0 m
B 0.15 m
C 0.2 m
D 0.1 m
Correct Answer
Option D
Solution
B=μ0NiR22(R2+x2)3/2B = {{{\mu _0}Ni{R^2}} \over {2{{({R^2} + {x^2})}^{3/2}}}}

at x1 = 0.05 m,

B1=μ0NiR22(R2+(0.05)2)3/2{B_1} = {{{\mu _0}Ni{R^2}} \over {2{{({R^2} + {{(0.05)}^2})}^{3/2}}}}

at x2 = 0.2 m,

B2=μ0NiR22(R2+(0.2)2)3/2{B_2} = {{{\mu _0}Ni{R^2}} \over {2{{({R^2} + {{(0.2)}^2})}^{3/2}}}}
B1B2=(R2+0.04)3/2(R2+0.0025)3/2{{{B_1}} \over {{B_2}}} = {{{{({R^2} + 0.04)}^{3/2}}} \over {{{({R^2} + 0.0025)}^{3/2}}}}
(81)2/3=R2+0.04R2+0.0025{\left( {{8 \over 1}} \right)^{2/3}} = {{{R^2} + 0.04} \over {{R^2} + 0.0025}}

4 (R2 + 0.0025) = R2 + 0.04 3R2 = 0.04 - 0.0100 R2 =

0.033{{0.03} \over 3}

= 0.01 R =

0.01\sqrt {0.01}

= 0.1 m

Q64
A proton and an α\alpha-particle, having kinetic energies Kp and Kα\alpha respectively, enter into a magnetic field at right angles. The ratio of the radii of trajectory of proton to that of α\alpha-particle is 2 : 1. The ratio of Kp : Kα\alpha is :
A 8 : 1
B 4 : 1
C 1 : 8
D 1 : 4
Correct Answer
Option B
Solution

Radius,

r=mvqB=2mKqBr = {{mv} \over {qB}} = {{\sqrt {2mK} } \over {qB}}
K=r2q2B22m\Rightarrow K = {{{r^2}{q^2}{B^2}} \over {2m}}

\therefore

KpKα=(rprα)2×(qpqα)2×mαmp{{{K_p}} \over {{K_\alpha }}} = {\left( {{{{r_p}} \over {{r_\alpha }}}} \right)^2} \times {\left( {{{{q_p}} \over {{q_\alpha }}}} \right)^2} \times {{{m_\alpha }} \over {{m_p}}}
=(21)2×(12)2×4= {\left( {{2 \over 1}} \right)^2} \times {\left( {{1 \over 2}} \right)^2} \times 4
=4= 4
Q65
A deuteron and an alpha particle having equal kinetic energy enter perpendicularly into a magnetic field. Let rd and rα\alpha be their respective radii of circular path. The value of rdrα{{{r_d}} \over {{r_\alpha }}} is equal to :
A 1
B 2
C 2\sqrt 2
D 12{1 \over {\sqrt 2 }}
Correct Answer
Option C
Solution

Given, kinetic energy of α\alpha-particle (Kα\alpha) = kinetic energy of deuteron (Kd) Since, kinetic energy, K =

12{1 \over 2}

mv2 \Rightarrow mv2 = 2K \Rightarrow v2 =

2Km{{2K} \over m}

\Rightarrow v =

2Km\sqrt {{{2K} \over m}}

.... (i) We know that, r =

mvBq{{mv} \over {Bq}}

.... (ii) where, r = radius of curvature of path of a charged particle, m = mass of the charged particle, q = charge of the particle, v = velocity of charged particle and B = magnetic field.

From Eqs. (i) and (ii), we get

r=m2KmBqr = {{m\sqrt {{{2K} \over m}} } \over {Bq}}
r=2KmBq\Rightarrow r = {{\sqrt {2Km} } \over {Bq}}

.... (iii) Since, m, K and B are same for both deuteron and α\alpha-particle. From Eq. (iii), we get

γmq\gamma \propto {{\sqrt m } \over q}

\therefore

rdrα=mdmα.qαqd=24(21){{{r_d}} \over {{r_\alpha }}} = \sqrt {{{{m_d}} \over {{m_\alpha }}}} .{{{q_\alpha }} \over {{q_d}}} = \sqrt {{2 \over 4}} \left( {{2 \over 1}} \right)

[\because md = 2mp and mα\alpha = 4mp qα\alpha = 2e and qd = e.]

rdrα=2{{{r_d}} \over {{r_\alpha }}} = \sqrt 2
Q66
The fractional change in the magnetic field intensity at a distance 'r' from centre on the axis of current carrying coil of radius 'a' to the magnetic field intensity at the centre of the same coil is : (Take r < a)
A 32a2r2{3 \over 2}{{{a^2}} \over {{r^2}}}
B 23a2r2{2 \over 3}{{{a^2}} \over {{r^2}}}
C 23r2a2{2 \over 3}{{{r^2}} \over {{a^2}}}
D 32r2a2{3 \over 2}{{{r^2}} \over {{a^2}}}
Correct Answer
Option D
Solution
Baxis=μ0iR22(R2+x2)3/2{B_{axis}} = {{{\mu _0}i{R^2}} \over {2{{({R^2} + {x^2})}^{3/2}}}}
Bcentre=μ0i2R{B_{centre}} = {{{\mu _0}i} \over {2R}}

\therefore

Bcentre=μ0i2a{B_{centre}} = {{{\mu _0}i} \over {2a}}

\therefore

Baxis=μ0ia22(a2+r2)3/2{B_{axis}} = {{{\mu _0}i{a^2}} \over {2{{({a^2} + {r^2})}^{3/2}}}}

\therefore fractional change in magnetic field =

μ0i2aμ0ia22(a2+r2)3/2μ0i2a=11[1+(r2a2)]3/2{{{{{\mu _0}i} \over {2a}} - {{{\mu _0}i{a^2}} \over {2{{({a^2} + {r^2})}^{3/2}}}}} \over {{{{\mu _0}i} \over {2a}}}} = 1 - {1 \over {{{\left[ {1 + \left( {{{{r^2}} \over {{a^2}}}} \right)} \right]}^{3/2}}}}
1[132r2a2]=32r2a2\approx 1 - \left[ {1 - {3 \over 2}{{{r^2}} \over {{a^2}}}} \right] = {3 \over 2}{{{r^2}} \over {{a^2}}}

Note :

(1+r2a2)3/2(132r2a2){\left( {1 + {{{r^2}} \over {{a^2}}}} \right)^{ - 3/2}} \approx \left( {1 - {3 \over 2}{{{r^2}} \over {{a^2}}}} \right)

[True only if r << a] Hence, option (d) is the most suitable option.

Q67
Two ions of masses 4 amu and 16 amu have charges +2e and +3e respectively. These ions pass through the region of constant perpendicular magnetic field. The kinetic energy of both ions is same. Then :
A lighter ion will be deflected less than heavier ion
B lighter ion will be deflected more than heavier ion
C both ions will be deflected equally
D no ion will be deflected
Correct Answer
Option B
Solution
r=PqB=2mkqBr = {P \over {qB}} = {{\sqrt {2mk} } \over {qB}}

Given they have same kinetic energy

rmqr \propto {{\sqrt m } \over q}
r1r2=42×316=34{{{r_1}} \over {{r_2}}} = {{\sqrt 4 } \over 2} \times {3 \over {\sqrt {16} }} = {3 \over 4}
r2=4r13{r_2} = {{4{r_1}} \over 3}

(r2 is for heavier ion and and r1 is for lighter ion)

sinθ=dR\sin \theta = {d \over R}

θ\theta \to Deflection

θ1R\theta \propto {1 \over R}

(R \to Radius of path) \because R2 > R1 \Rightarrow θ\theta2 < θ\theta1

Q68
A coaxial cable consists of an inner wire of radius 'a' surrounded by an outer shell of inner and outer radii 'b' and 'c' respectively. The inner wire carries an electric current i0, which is distributed uniformly across cross-sectional area. The outer shell carries an equal current in opposite direction and distributed uniformly. What will be the ratio of the magnetic field at a distance x from the axis when (i) x < a and (ii) a < x < b ?
A x2a2{{{x^2}} \over {{a^2}}}
B a2x2{{{a^2}} \over {{x^2}}}
C x2b2a2{{{x^2}} \over {{b^2} - {a^2}}}
D b2a2x2{{{b^2} - {a^2}} \over {{x^2}}}
Correct Answer
Option A
Solution

when x < a

B1(2πx)=μ0(i0πa2)πx2{B_1}(2\pi x) = {\mu _0}\left( {{{{i_0}} \over {\pi {a^2}}}} \right)\pi {x^2}
B(2πx)=μ0i0x2a2B(2\pi x) = {{{\mu _0}{i_0}{x^2}} \over {{a^2}}}
B1=μ0i0x2πa2{B_1} = {{{\mu _0}{i_0}x} \over {2\pi {a^2}}}

.... (1) when a < x < b

B2(2πx)=μ0i0{B_2}(2\pi x) = {\mu _0}{i_0}
B2=μ0i02πx{B_2} = {{{\mu _0}{i_0}} \over {2\pi x}}

..... (2)

B1B2=μ0i0x2πa2μ0i02πx=x2a2{{{B_1}} \over {{B_2}}} = {{{\mu _0}{i_0}{x \over {2\pi {a^2}}}} \over {{{{\mu _0}{i_0}} \over {2\pi x}}}} = {{{x^2}} \over {{a^2}}}
Q69
A current of 1.5 A is flowing through a triangle, of side 9 cm each. The magnetic field at the centroid of the triangle is : (Assume that the current is flowing in the clockwise direction.)
A 3 ×\times 10-7 T, outside the plane of triangle
B 232\sqrt 3 ×\times 10-7 T, outside the plane of triangle
C 232\sqrt 3 ×\times 10-5 T, inside the plane of triangle
D 3 ×\times 10-5 T, inside the plane of triangle
Correct Answer
Option D
Solution
B=3[μ0i4πr(sin60+sin60)]B = 3\left[ {{{{\mu _0}i} \over {4\pi r}}(\sin 60^\circ + \sin 60^\circ )} \right]
tan60=l/2r\tan 60^\circ = {{l/2} \over r}

where

r=9×10223r = {{9 \times {{10}^{ - 2}}} \over {2\sqrt 3 }}

M \therefore B = 3 ×\times 10-5 T Current is flowing in clockwise direction so,

B\overrightarrow B

is inside plane of triangle by right hand rule.

Q70
Two long current carrying conductors are placed to each other at a distance of 8 cm between them. The magnitude of magnetic field produced at mid-point between the two conductors due to current flowing in them is 300 μ\muT. The equal current flowing in the two conductors is :
A 30A in the same direction.
B 30A in the opposite direction.
C 60A in the opposite direction.
D 300A in the opposite direction.
Correct Answer
Option B
Solution

As Bnet \ne 0 that is the wires are carrying current in opposite direction.

μ0I×22π(4×102)=30×106{{{\mu _0}I \times 2} \over {2\pi (4 \times {{10}^{ - 2}})}} = 30 \times {10^{ - 6}}

T

I=30×106106\Rightarrow I = {{30 \times {{10}^{ - 6}}} \over {{{10}^{ - 6}}}}

A = 30 A in opposite direction.

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