The emf induced in a rotating rod placed in a magnetic field is given by the formula:
\[
\mathcal{E} = B \omega l^2
\]
Where:
- \( \mathcal{E} \) is the induced emf,
- \( B \) is the magnetic field strength,
- \( \omega \) is the angular velocity,
- \( l \) is the length of the rod.
The angular velocity \( \omega \) is related to the frequency \( f \) by:
\[
\omega = 2\pi f
\]
Now, given:
- \( B = 2 \, \text{T} \),
- \( f = 100 \, \text{Hz} \),
- \( l = 2 \, \text{m} \),
First, calculate the angular velocity:
\[
\omega = 2 \pi \times 100 = 200\pi \, \text{rad/s}
\]
Now substitute the values into the formula for emf:
\[
\mathcal{E} = 2 \times 200\pi \times 2^2 = 2 \times 200\pi \times 4 = 1600 \pi \, \text{volt}
\]
Thus, the emf developed across the ends of the rod is \( 1600 \pi \) volts.