A conducting square frame of side a and a long straight wire carrying current I are located in the same plane as shown in the figure. The frame moves to the right with a constant velocity V. The emf induced in the frame will be proportional to
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Answer:
The answer will be (2x-a) -2/(2x+a)
Explanation:
According to figure we can say that as the frame is a square therefore the sides are equal and the side = a
The current located at the similar plane is given as I
and the velocity of the frame is given as v
B1 and B2 are the magnetic fields
let the induced emf of the frame is e
Therefore e = B1(PQ)v -B2(RS)v
= μ0I x av/2π(x-a)/2 - μ0I x av/2π(x+a)/2
= μ0I av/2π (2/(2x-a) -2/(2x+a))
= μ0I av/2π x 2 (2a/(2x-a) -(2x+a))
Therefore we can see that emf e varies with the term of (2x-a) -(2x+a)
Therefore we can say that emf e ∝ 1/ (2x-a) -(2x+a)
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