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MHT CET 202623 AprilEvening Shift
Exam
MHT CET
Year
2026
Date
23 April
Shift
Evening Shift
Subject
Physics
Chapter
Electromagnetic Induction

MHT CET 2026 · 23 April · Evening Shift · Physics · Electromagnetic Induction

A very small circular loop of radius 'a' is initially (at t = 0 )...

A very small circular loop of radius 'a' is initially (at t=0t = 0) coplanar and concentric with a much larger fixed circular loop of radius 'b'. A constant current I flows in the larger loop. The smaller loop is rotated with a constant angular speed ω\omega about the common diameter. The emf induced in the smaller loop as a function of time t is
(\mu_0=permeabilityoffreespace)= permeability of free space)

Options

  1. A(πa2μ0I2b)ωcos⁡ωt\left(\dfrac{\pi a^2\mu_0 I}{2b}\right)\omega\cos\omega t
  2. B(πa2μ0I2b)ωsin⁡ω2t2\left(\dfrac{\pi a^2\mu_0 I}{2b}\right)\omega\sin\omega^2 t^2
  3. C(πa2μ0I2b)ωsin⁡ωt\left(\dfrac{\pi a^2\mu_0 I}{2b}\right)\omega\sin\omega t
  4. D(πa2μ0I2b)ω(sin⁡)2ωt\left(\dfrac{\pi a^2\mu_0 I}{2b}\right)\omega(\sin)^2\omega t

Correct answer

C. (πa2μ0I2b)ωsin⁡ωt\left(\dfrac{\pi a^2\mu_0 I}{2b}\right)\omega\sin\omega t

Step-by-step solution

The magnetic field produced by the larger loop at its centre is given by

B=μ0I2bB = \dfrac{\mu_0 I}{2b}

Since the smaller loop is very small (a \ll b),themagneticfieldoveritsareacanbeassumedtobeuniformandequalto), the magnetic field over its area can be assumed to be uniform and equal toB.<br><br>Themagneticfluxlinkedwiththesmallerloopatanytime.<br><br>The magnetic flux linked with the smaller loop at any timetis<br><br>Φ=B⃗⋅A⃗=BAcos⁡(ωt)is<br><br>\Phi = \vec{B} \cdot \vec{A} = B A \cos(\omega t)

Substituting A=πa2A = \pi a^2 and B=μ0I2bB = \dfrac{\mu_0 I}{2b}, we get

Φ=(μ0I2b)(πa2)cos⁡(ωt)\Phi = \left(\dfrac{\mu_0 I}{2b}\right) (\pi a^2) \cos(\omega t)

According to Faraday's law of induction, the induced emf is

e=−dΦdt=−ddte = -\dfrac{d\Phi}{dt} = -\dfrac{d}{dt}\left[\left(\dfrac{\mu_0 I \pi a^2}{2b}\right) \cos(\omegat) \right]

e=e =\left(\dfrac{\pi a^2 \mu_0 I}{2b}\right) \omega \sin(\omegat)<br><br>Answer: \left(\dfrac{\pi a²\mu_0 I}{2b}\right)\omega\sin\omegat
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