Physics Objective Questions and Answers: Electromagnetic Induction
Explore reliable objective questions for Electromagnetic Induction tailored for JEE learners. Utilizing these Physics multiple-choice formats ensures thorough preparation and strengthens problem-solving speed for upcoming school assessments.
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Access the complete set of multiple-choice questions for Electromagnetic Induction below. This focused format allows students to isolate specific topics for thorough review and uninterrupted practice alongside official JEE textbooks.
Multiple Choice Questions
(a) 10 mV
(b) 1 mV
(c) 100 mV
(d) 5 mV
Show Answer & Explanation
Answer: (a) 10 mV
Explanation:
1. Area \( A=\pi r^2=\pi\times\frac{100}{\pi}\times10^{-4}=10^{-2}\ \text{m}^2 \).
2. Rate of change of field \( \frac{dB}{dt}=\frac{0.5}{0.5}=1\ \text{T/s} \) (steady, so the emf is the same at 0.25 s).
3. \( \varepsilon=A\frac{dB}{dt}=10^{-2}\ \text{V}=10\ \text{mV} \).
Teacher's Note:
1. A steady rate of change gives a constant emf.
2. Convert 10/√π cm to metres before squaring.
(a) \( \frac14B^2L\omega \)
(b) \( \frac14BL^2\omega \)
(c) \( \frac12B L^2\omega \)
(d) \( \frac12BL\omega^2 \)
Show Answer & Explanation
Answer: (c) \( \frac12B L^2\omega \)
Explanation:
1. Speed of an element at distance x from the axis: \( v=\omega x \).
2. \( \varepsilon=\int_0^LB\omega x\,dx=\frac12B\omega L^2 \).
Teacher's Note:
1. The emf is the sum of the motional emfs B v dx of all small elements.
2. The average speed of the rod is ωL/2.
(a) 3 A
(b) 1 A
(c) 4 A
(d) 0.75 A
Show Answer & Explanation
Answer: (a) 3 A
Explanation:
1. Long after closing the switch, the current is steady, so the ideal inductors have no voltage across them and behave like plain wires.
2. Each branch then has a resistance of 12 ohm, and three 12 ohm branches in parallel give \( \frac{12}{3}=4\ \Omega \).
3. \( I=\frac{12}{4}=3\ \text{A} \).
Teacher's Note:
1. In steady state di/dt = 0, so the induced emf of an ideal inductor is zero.
2. The inductance affects only the transient period.
(a) 10 mV
(b) 20 mV
(c) 5 mV
(d) 1.6 mV
Show Answer & Explanation
Answer: (a) 10 mV
Explanation:
1. \( \varepsilon=\left|\frac{d\Phi}{dt}\right|=B\frac{d(\pi r^2)}{dt}=2\pi rB\left|\frac{dr}{dt}\right| \).
2. \( \varepsilon=2\pi(0.1)(0.8)(0.02)\approx1.0\times10^{-2}\ \text{V}=10\ \text{mV} \).
Teacher's Note:
1. Differentiate the flux B π r² with respect to time.
2. Convert cm to m: r = 0.1 m and dr/dt = 0.02 m/s.
(a) 20 V
(b) 8 V
(c) 12 V
(d) 16 V
Show Answer & Explanation
Answer: (d) 16 V
Explanation:
1. \( \varepsilon=Blv=2\times1\times8=16\ \text{V} \).
Teacher's Note:
1. Motional emf = B l v when B, l and v are mutually perpendicular.
2. Units: T m (m/s) = V.
(a) \( \frac{\mu_0I}{2\pi a} \)
(b) 0
(c) \( \frac{\mu_0I}{4\pi a} \)
(d) \( \frac{\mu_0I}{\pi a} \)
Show Answer & Explanation
Answer: (b) 0
Explanation:
1. Each wire is straight and ends at a corner, so use \( B=\frac{\mu_0I}{4\pi d}(\sin\theta_2-\sin\theta_1) \) with perpendicular distance \( d=\frac a2 \) for every wire.
2. Wires AB and ED each subtend angles from 45° to 90° or -90° to -45° (factor 0.29), and wires BC and TE each subtend factors 1.71, in units of \( \frac{\mu_0I}{2\pi a} \).
3. By the right-hand rule AB and TE give fields into the page: \( 0.29+1.71=2 \). BC and ED give fields out of the page: \( 1.71+0.29=2 \).
4. The net field at O is zero.
Teacher's Note:
1. Find the direction of each field with the right-hand rule before adding magnitudes.
2. The arrangement is symmetric about the point O, which makes the contributions cancel in pairs.
(a) \( M=\frac{\sqrt2\mu_0R^2}{L} \)
(b) \( M=\frac{2\sqrt2\mu_0R}{L} \)
(c) \( M=\frac{2\sqrt2\mu_0R^2}{L} \)
(d) \( M=\frac{\sqrt2\mu_0R}{L^2} \)
Show Answer & Explanation
Answer: (c) \( M=\frac{2\sqrt2\mu_0R^2}{L} \)
Explanation:
1. Field at the centre due to one side of the square (distance \( \frac L2 \), angles 45° each way): \( B_1=\frac{\mu_0I}{4\pi(L/2)}(2\sin45^\circ)=\frac{\sqrt2\mu_0I}{2\pi L} \).
2. Four sides: \( B=\frac{2\sqrt2\mu_0I}{\pi L} \).
3. The small loop sees an almost uniform field: \( \Phi=B\pi R^2=\frac{2\sqrt2\mu_0R^2}{L}I \), so \( M=\frac\Phi I=\frac{2\sqrt2\mu_0R^2}{L} \).
Teacher's Note:
1. Put the current in the large loop and find the flux through the small loop.
2. Because L is much larger than R, the field over the small loop is nearly constant.
(a) 2 T
(b) 4 T
(c) 8 T
(d) 16 T
Show Answer & Explanation
Answer: (a) 2 T
Explanation:
1. The wire length is fixed: \( 4\times2\pi r=2\pi r'\Rightarrow r'=4r \).
2. \( B=\frac{\mu_0NI}{2r}\propto\frac Nr \): the original has \( \frac4r \), the new coil has \( \frac1{4r} \).
3. \( B'=32\times\frac{1/4r}{4/r}=32\times\frac1{16}=2\ \text{T} \).
Teacher's Note:
1. Unwinding keeps the total wire length constant, so the radius becomes four times larger.
2. N decreases by 4 and r increases by 4, so B falls by 16.
(a) 44 V
(b) 88 V
(c) 22 V
(d) 66 V
Show Answer & Explanation
Answer: (a) 44 V
Explanation:
1. \( \omega=\frac{2\pi\times500}{60}=\frac{2\times22\times500}{7\times60}=52.4\ \text{rad/s} \).
2. The plane at 60° to the field means the normal is at 30° to the field: \( \varepsilon=NBA\omega\sin30^\circ \).
3. \( \varepsilon=600\times0.4\times70\times10^{-4}\times52.4\times0.5=44\ \text{V} \).
Teacher's Note:
1. Flux = NBA cos(angle between the normal and B), so the emf is NBAω sin(angle).
2. If the plane makes 60° with the field, the normal makes 30°.
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