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Question: A rod of length *I* rotates with a uniform angular velocity \(\omega\) about an axis passing through...

A rod of length I rotates with a uniform angular velocity ω\omega about an axis passing through its middle point but normal to its length in a uniform magnetic field of induction B with its direction parallel to the axis of rotation. The induced emf between the two ends of the rod is

A

Bl2ω2\frac{Bl^{2}\omega}{2}

B

Zero

C

(Bl2ω8)\left( \frac{Bl^{2}\omega}{8} \right)

D

2Bl2ω2Bl^{2}\omega

Answer

Zero

Explanation

Solution

Length of the rod between the axis of rotation and one end of the rod =l2= \frac{l}{2}

Area swept out in one rotation =π(l2)2=(πl24)= \pi\left( \frac{l}{2} \right)^{2} = \left( \frac{\pi l^{2}}{4} \right)

Angular velocity =ωrads1= \omega rads^{- 1}

Frequency of revolution =ω2π= \frac{\omega}{2\pi}

Area swept out per second =πl24(ω2π)=l2ω8= \frac{\pi l^{2}}{4}\left( \frac{\omega}{2\pi} \right) = \frac{l^{2}\omega}{8}

Magnetic induction = B

Rate of change of magnetic flux=(Bl2ω8)= \left( \frac{Bl^{2}\omega}{8} \right)

Magnitude of induced emf =Bl2ω8= \frac{Bl^{2}\omega}{8}

Magnitude of induced emf between the axis and the other end is also (Bl2ω8)\left( \frac{Bl^{2}\omega}{8} \right) these two emf’s are in opposite direction hence the potential difference between the two ends of the rod is zero.