Magnetic Effect of Current

JEE Physics · 124 questions · Page 2 of 13 · Click an option or "Show Solution" to reveal answer

Q11
The current sensitivity of a galvanometer can be increased by : (A) decreasing the number of turns (B) increasing the magnetic field (C) decreasing the area of the coil (D) decreasing the torsional constant of the spring Choose the most appropriate answer from the options given below :
A (B) and (C) only
B (C) and (D) only
C (A) and (C) only
D (B) and (D) only
Correct Answer
Option D
Solution
NiAB=kθNiAB = k\theta
θi=NABk\Rightarrow {\theta \over i} = {{NAB} \over k}

\Rightarrow Sensitivity increases if

BB \uparrow

and

kk \downarrow
Q12
Proton, deuteron and alpha particle of same kinetic energy are moving in circular trajectories in a constant magnetic field. The radii of proton, denuteron and alpha particle are respectively rp,rd{r_p},{r_d} and rα{r_\alpha }. Which one of the following relation is correct?
A rα=rp=rd{r_\alpha } = {r_p} = {r_d}
B rα=rp<rd{r_\alpha } = {r_p} < {r_d}
C rα>rd>rp{r_\alpha } > {r_d} > {r_p}
D rα=rd>rp{r_\alpha } = {r_d} > {r_p}
Correct Answer
Option B
Solution
r=2mvqBr×vmqr = {{\sqrt {2mv} } \over {qB}} \Rightarrow r \times v{{\sqrt m } \over q}

Thus we have,

rα=rp<rd{r_\alpha } = {r_p} < {r_d}
Q13
Two thin, long, parallel wires, separated by a distance d'd' carry a current of i'i' AA in the same direction. They will
A repel each other with a force of μ0i2/(2πd){\mu _0}{i^2}/\left( {2\pi d} \right)
B attract each other with a force of μ0i2/(2πd){\mu _0}{i^2}/\left( {2\pi d} \right)
C repel each other with a force 0i2/(2πd2)_0{i^2}/\left( {2\pi {d^2}} \right)
D attract each other with a force of μ0i2/(2πd2){\mu _0}{i^2}/\left( {2\pi {d^2}} \right)
Correct Answer
Option B
Solution
F=μ0i12πd=μ0i22πd{F \over \ell } = {{{\mu _0}{i_1}} \over {2\pi d}} = {{{\mu _0}{i^2}} \over {2\pi d}}

(attractive as current is in the same direction)

Q14
If in a circular coil AA of radius R,R, current II is flowing and in another coil BB of radius 2R2R a current 2I2I is flowing, then the ratio of the magnetic fields BA{B_A} and BB{B_B}, produced by them will be
A 11
B 22
C 1/21/2
D 44
Correct Answer
Option A
Solution

KEY CONCEPT : We know that the magnetic field produced by a current carrying circular coil of radius

rr

at its center is

B=μ04πIr×2πB = {{{\mu _0}} \over {4\pi }}{I \over r} \times 2\pi

Here

BA=μ04πIR×2π{B_A} = {{{\mu _0}} \over {4\pi }}{I \over R} \times 2\pi

and

BB=μ04π2I2R×2π{B_B} = {{{\mu _0}} \over {4\pi }}{{2I} \over {2R}} \times 2\pi
BABB=1\Rightarrow {{{B_A}} \over {B{}_B}} = 1
Q15
The time period of a charged particle undergoing a circular motion in a uniform magnetic field is independent of its
A speed
B mass
C charge
D magnetic induction
Correct Answer
Option A
Solution

KEY CONCEPT : The time period of a charged particle

(m,q)\left( {m,q} \right)

moving in a magnetic field

(B)(B)

is

T=2πmqBT = {{2\pi m} \over {qB}}

The time period does not depend on the speed of the particle.

Q16
A particle of mass MM and charge QQ moving with velocity v\overrightarrow v describe a circular path of radius RR when subjected to a uniform transverse magnetic field of induction B.B. The network done by the field when the particle completes one full circle is
A (Mv2R)2πR\left( {{{M{v^2}} \over R}} \right)2\pi R
B zero
C BQ2πRB\,\,Q\,2\pi R
D BQv2πRB\,Qv\,2\pi R
Correct Answer
Option B
Solution

The work done,

dW=FdscosθdW = Fds\,\cos \,\theta

The angle between force and displacement is

90.{90^ \circ }.

Therefore work done is zero.

Q17
A uniform electric field and a uniform magnetic field are acting along the same direction in a certain region. If an electron is projected along the direction of the fields with a certain velocity then
A its velocity will increase
B Its velocity will decrease
C it will turn towards left of a direction of motion
D it will turn towards right of direction of motion
Correct Answer
Option B
Solution

Due to electric field, it experiences force and decelerates i.e. its velocity decreases.

Q18
Two long conductors, separated by a distance dd carry current I1{I_1} and I2{I_2} in the same direction. They exert a force FF on each other. Now the current in one of them is increased to two times and its direction is reversed. The distance is also increased to 3d3d. The new value of the force between them is
A 2F3 - {{2F} \over 3}
B F3{F \over 3}
C 2F-2F
D F3 - {F \over 3}
Correct Answer
Option A
Solution

Force between two long conductor carrying current,

F=μ04π2I1I2d×F = {{{\mu _0}} \over {4\pi }}{{2{I_1}{I_2}} \over d} \times \ell
F=μ04π2(2I1)I23dF' = - {{{\mu _0}} \over {4\pi }}{{2\left( {2{I_1}} \right){I_2}} \over {3d}}\ell

\therefore

FF=23{{F'} \over F} = {{ - 2} \over 3}
Q19
A particle of charge 16×1018 - 16 \times {10^{ - 18}} coulomb moving with velocity 10ms110m{s^{ - 1}} along the xx-axis enters a region where a magnetic field of induction BB is along the yy-axis, and an electric field of magnitude 104V/m{10^4}V/m is along the negative zz-axis. If the charged particle continues moving along the xx-axis, the magnitude of BB is
A 103Wb/m2{10^3}Wb/{m^2}
B 105Wb/m2{10^5}Wb/{m^2}
C 1016Wb/m2{10^{16}}Wb/{m^2}
D 103Wb/m2{10^{ - 3}}Wb/{m^2}
Correct Answer
Option A
Solution

The situation is shown in the figure.

FE={F_E} =

Force due to electric field

FB={F_B} =

Force due to magnetic field It is given that the charged particle remains moving along

XX

-axis (i.e. undeviated). Therefore

FB=FE{F_B} = {F_E}
qvB=qE\Rightarrow qvB = qE
B=Ev=10410\Rightarrow B = {E \over v} = {{{{10}^4}} \over {10}}
=103weber/m2= {10^3}\,\,weber/{m^2}
Q20
A current ii ampere flows along an infinitely long straight thin walled tube, then the magnetic induction at any point inside the tube is
A μ04π,2ir{{{\mu _0}} \over {4\pi }},{{2i} \over r} tesla
B zero
C infinite
D 2ir{{2i} \over r} tesla
Correct Answer
Option B
Solution

Using Ampere's law at a distance

rr

from axis,

BB

is same from symmetry.

B.dl=μ0i\int {B.dl = {\mu _0}i}

i.e.,

B×2πr=μ0iB \times 2\pi r = {\mu _0}i

Here

ii

is zero, for

r<R,r < R,

whereas

RR

is the radius \therefore

B=0B=0
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