Magnetic Effect of Current MCQ Questions & Answers in Electrostatics and Magnetism | Physics
Learn Magnetic Effect of Current MCQ questions & answers in Electrostatics and Magnetism are available for students perparing for IIT-JEE, NEET, Engineering and Medical Enternace exam.
71.
Three infinitely long wires are placed equally apart on the circumference of a circle of radius $$a,$$ perpendicular to its plane. Two of the wires carry current $$I$$ each, in the same direction, while the third carries current $$2I$$ along the direction opposite to the other two. The magnitude of the magnetic induction $$\vec B$$ at a distance $$r$$ from the centre of the circle, for $$r >a,$$ is
A
0
B
$$\frac{{2{\mu _0}}}{\pi }\frac{I}{r}$$
C
$$ - \frac{{2{\mu _0}}}{\pi }\frac{I}{r}$$
D
$$\frac{{2{\mu _0}}}{\pi }\frac{{Ia}}{{{r^2}}}$$
Answer :
0
From ampere circuital law
$$\oint {B.dl} = {\mu _0}i$$
Where, $$i$$ = Net current passing through the loop
Now $$i = I + I - 2I = 0$$
$$\therefore B.2\pi \,r = 0 \Rightarrow B = 0$$
72.
A $$10\,eV$$ electron is circulating in a plane at right angles to a uniform field at magnetic induction $${10^{ - 4}}\,Wb/{m^2}\left( { = 1.0\,{\text{gauss}}} \right).$$ The orbital radius of the electron is
73.
Two similar coils of radius $$R$$ are lying concentrically with their planes at right angles to each other. The currents flowing in them are $$I$$ and $$2\,I,$$ respectively. The resultant magnetic field induction at the centre will be:
A
$$\frac{{\sqrt 5 {\mu _0}I}}{{2R}}$$
B
$$\frac{{3{\mu _0}I}}{{2R}}$$
C
$$\frac{{{\mu _0}I}}{{2R}}$$
D
$$\frac{{{\mu _0}I}}{R}$$
Answer :
$$\frac{{\sqrt 5 {\mu _0}I}}{{2R}}$$
The magnetic field, due the coil, carrying current $$I$$ Ampere
$${B_1} = \frac{{{\mu _0}I}}{{2R}}$$
The magnetic field due to the coil, carrying current $$2\,I$$ Ampere
$${B_2} = \frac{{{\mu _0}\left( {2I} \right)}}{{2R}}$$
The resultant $$B$$
$$\eqalign{
& {B_{{\text{net}}}} = \sqrt {B_1^2 + B_2^2 + 2{B_1}{B_2}\cos \theta ,} \,\theta = {90^ \circ } \cr
& {B_{{\text{net}}}} = \sqrt {B_1^2 + B_2^2} = \frac{{{\mu _0}\left( {2I} \right)}}{{2R}}\sqrt {1 + 4} \cr
& = \frac{{\sqrt 5 {\mu _0}I}}{{2R}} \cr} $$
74.
A long solenoid has 200 turns per $$cm$$ and carries a current $$i.$$ The magnetic field at its centre is $$6.28 \times {10^{ - 2}}Weber/m^2.$$ Another long solenoid has 100 turns per $$cm$$ and it carries a current $$\frac{i}{3}.$$ The value of the magnetic field at its centre is
75.
Under the influence of a uniform magnetic field a charged particle is moving in a circle of radius $$R$$ with constant speed $$v.$$ The time period of the motion
A
depends on both $$R$$ and $$v$$
B
is independent of both $$R$$ and $$v$$
C
depends on $$R$$ and not on $$v$$
D
depends on $$v$$ and not on $$R$$
Answer :
is independent of both $$R$$ and $$v$$
When a test charge $${q_0}$$ enters a magnetic field $${\vec B}$$ directed along $$z$$-axis, with a velocity $${\vec v}$$ making angles $$d$$ with the $$z$$-axis. The time period of the motion is independent of $$R$$ and $$v.$$
76.
The length of a magnet is large compared to its width and
breadth. The time period of its oscillation in a vibration
magnetometer is $$2s.$$ The magnet is cut along its length into three equal parts and these parts are then placed on each other with their like poles together. The time period of this combination will be
A
$$2\sqrt 3 \,s$$
B
$$\frac{2}{3}\,s$$
C
$$2 s$$
D
$$\frac{2}{{\sqrt 3 }}\,s$$
Answer :
$$\frac{2}{3}\,s$$
$$T = 2\pi \sqrt {\frac{I}{{M \times B}}} \,{\text{where}}\,I = \frac{1}{{12}}m{\ell ^2}$$
When the magnet is cut into three pieces the pole strength will remain the same and
M.I. $$\left( {I'} \right) = \frac{1}{{12}}\left( {\frac{m}{3}} \right){\left( {\frac{\ell }{3}} \right)^2} \times 3 = \frac{I}{9}$$
We have, Magnetic moment $$\left( M \right)$$ = Pole strength $$\left( m \right) \times \ell $$
∴ New magnetic moment,
$$M' = m \times \left( {\frac{\ell }{3}} \right) \times 3 = m\ell = M\,\,\,\therefore T' = \frac{T}{{\sqrt 9 }} = \frac{2}{3}s.$$
77.
A rigid square of loop of side $$'a'$$ and carrying current $${I_2}$$ is lying on a horizontal surface near a long current $${I_1}$$ carrying wire in the same plane as shown in figure. The net force on the loop due to the wire will be:
A
Repulsive and equal to $$\frac{{{\mu _0}{I_1}{I_2}}}{{2\pi }}$$
B
Attractive and equal to $$\frac{{{\mu _0}{I_1}{I_2}}}{{3\pi }}$$
C
Repulsive and equal to $$\frac{{{\mu _0}{I_1}{I_2}}}{{4\pi }}$$
D
Zero
Answer :
Repulsive and equal to $$\frac{{{\mu _0}{I_1}{I_2}}}{{4\pi }}$$
78.
A bar magnet is demagnetized by inserthing it inside a solenoid of length $$0.2 m,$$ 100 turns, and carrying a current of $$5.2 A.$$ The coercivity of the bar magnet is:
79.
A coil of one turn is made of a wire of certain length and then from the same length a coil of two turns is made. If the same current is passed in both the cases, then the ratio of the magnetic induction at their centres will be
A
$$2:1$$
B
$$1:4$$
C
$$4:1$$
D
$$1:2$$
Answer :
$$1:4$$
Magnetic induction at the centre of current carrying coil of $$N$$ turns carrying current is given by
$$B = \frac{{{\mu _0}Ni}}{{2r}}\,\,......\left( {\text{i}} \right)$$
Suppose the length of the wire be $$L.$$ I
For coil of one turn, let radius be $${r_1}.$$
$$\eqalign{
& \therefore L = 2\pi {r_1} \times N \cr
& {\text{or}}\,\,{r_1} = \frac{L}{{2\pi \times N}} = \frac{L}{{2\pi }}\,\,\left( {\because N = 1} \right) \cr} $$ II
For coil of two turns, let radius be $${r_2}.$$
$$\eqalign{
& \therefore L = 2\pi {r_2} \times N \cr
& {\text{or}}\,\,{r_2} = \frac{L}{{2\pi \times N}} = \frac{L}{{2\pi \times 2}}\,\,\left( {\because N = 2} \right) \cr
& {\text{or}}\,\,{r_2} = \frac{{{r_1}}}{2} \cr} $$
By comparing two different cases from Eq. (i),
$$\eqalign{
& \frac{{{B_1}}}{{{B_2}}} = \frac{{{N_1}}}{{{r_1}}} \times \frac{{{r_2}}}{{{N_2}}}\,\,{\text{or}}\,\,\frac{{{B_1}}}{{{B_2}}} = \frac{{1 \times \frac{{{r_1}}}{2}}}{{{r_1} \times 2}} \cr
& \therefore \frac{{{B_1}}}{{{B_2}}} = \frac{1}{4} \cr} $$
80.
A long straight wire carries a certain current and produces a magnetic field of $$2 \times {10^{ - 4}}weber/{m^2}$$ at a perpendicular distance of $$5\,cm$$ from the wire. An electron situated at $$5\,cm$$ from the wire moves with a velocity $${10^7}\,m/s$$ towards the wire along perpendicular to it. The force experienced by the electron will be (charge on electron $$ = 1.6 \times {10^{ - 19}}C$$ )