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Question: A conducting circular loop is placed in a uniform magnetic field \(B=0.025T\) with its plane perpend...

A conducting circular loop is placed in a uniform magnetic field B=0.025TB=0.025T with its plane perpendicular to the magnetic field. The radius of the loop starts shrinking at 1mms11mm{{s}^{-1}}. The induced emf in the loop when the radius is 2 cm is:
A. 2πμV2\pi \mu V
B. πμV\pi \mu V
C. π2μV\dfrac{\pi }{2}\mu V
D. 3.2πμV3.2\pi \mu V

Explanation

Solution

Use the formula for the induced emf due to a changing magnetic flux through a loop. Write an expression for the magnetic flux through the given loop in terms of the radius and differentiate it with respect to the radius. Then use the given data to calculate the induced emf when the radius is 2cm.

Formula used:
E=dϕdtE=\dfrac{d\phi }{dt}
ϕ=B.A=BAcosθ\phi =\overrightarrow{B}.\overrightarrow{A}=BA\cos \theta

Complete step by step answer:
When magnetic flux through a conducting loop changes with time, an emf is induced in the loop. As a result a current flows in the loop. The emf induced in the loop due to varying magnetic flux is given as E=dϕdtE=\dfrac{d\phi }{dt}, where E is the emf induced, ϕ\phi is the magnetic flux and t is time. We can also say that the induced emf is equal to the rate of change in the magnetic flux through the loop.

The magnetic flux through a loop of constant (uniform) magnetic field is given as
ϕ=B.A=BAcosθ\phi =\overrightarrow{B}.\overrightarrow{A}=BA\cos \theta …. (i).
Here, B is the magnitude of the magnetic field, A is the area enclosed by the loop and θ\theta is the angle between the magnetic field and the area vector.

It is said that that magnetic field is perpendicular to the plane of the loop. This means that the magnetic field and the area vector of the loop are parallel. Therefore, θ=0\theta =0.
And cos0=1\cos 0=1.

Also, it is given that B=0.025TB=0.025T and the area enclosed by the loop will be equal to A=πr2A=\pi {{r}^{2}} (r is the radius of the loop).
Substitute the value in (i).
ϕ=(0.025)(πr2)\Rightarrow \phi =(0.025)\left( \pi {{r}^{2}} \right) ….. (ii).

Now differentiate (ii) with respect to r.
dϕdt=ddt[(0.025)(πr2)]\dfrac{d\phi }{dt}=\dfrac{d}{dt}\left[ (0.025)\left( \pi {{r}^{2}} \right) \right]
dϕdt=0.05πrdrdt\Rightarrow \dfrac{d\phi }{dt}=0.05\pi r\dfrac{dr}{dt}.
It is given that the radius of the loop is shrinking at rate of 1mms1=103ms11mm{{s}^{-1}}={{10}^{-3}}m{{s}^{-1}}.
This means that drdt=103ms1\dfrac{dr}{dt}={{10}^{-3}}m{{s}^{-1}}.
And we know that E=dϕdtE=\dfrac{d\phi }{dt}.
E=0.05πrdrdt\Rightarrow E=0.05\pi r\dfrac{dr}{dt}.
Substitute the value of drdt\dfrac{dr}{dt}.
E=0.05πr(103) E=5×105πrE=0.05\pi r\left( {{10}^{-3}} \right)\\\ \Rightarrow E =5\times {{10}^{-5}}\pi r.
Now, substitute r=2cm=0.02mr=2cm=0.02m in the above equation.
E=105π(0.02) E=106π E=πμVE={{10}^{-5}}\pi (0.02)\\\ \Rightarrow E ={{10}^{-6}}\pi \\\ \therefore E =\pi \mu V.
This means that the emf induced in the loop when the radius of the loop is 2 cm is πμV\pi \mu V.

Hence, the correct option is B.

Note: In some books you find that the emf induced in a loop due to the varying magnetic flux is equal to E=dϕdtE=-\dfrac{d\phi }{dt}.
Here, the negative sign only indicates that the emf is induced in such a way that it opposes the change in current in the loop. It is advisable not to use the negative sign as it may confuse things.