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In one rotation, the wire traces out a circle of radius R, i.e., an area A = πR2. Therefore, the rate at which the wire traces out the area is \(\frac{d A}{d t}\) = frequency or rotation × A = fA If the angle between the uniform magnetic field \(\vec{B}\) and the rotation axis is θ, the magnitude of the induced emf is |e|= B\(\frac{d A}{d t}\) cosθ = BfA cosθ = Bf(πR2)cosθ so that the required amplitude is equal to Bf(πR2)
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