The emf induced in a rotating rod in a magnetic field is given by the formula:
\[
\text{emf} = \frac{1}{2} B \omega L^2
\]
where:
- \( B \) is the magnetic field strength,
- \( \omega \) is the angular velocity of the rod,
- \( L \) is the length of the ro(D)
First, let's calculate the angular velocity \( \omega \):
- The frequency of rotation is \( f = 100 \, \text{rev/s} \),
- The angular velocity is \( \omega = 2 \pi f = 2 \pi \times 100 = 200 \pi \, \text{rad/s} \).
The length of the rod is \( L = 10 \, \text{cm} = 0.1 \, \text{m} \), and the magnetic field strength is \( B = 1 \, \text{T} \).
Now, substitute these values into the formula for emf:
\[
\text{emf} = \frac{1}{2} \times 1 \times 200 \pi \times (0.1)^2
\]
\[
\text{emf} = \frac{1}{2} \times 200 \pi \times 0.01
\]
\[
\text{emf} = 3.14 \, \text{V}
\]
Thus, the induced emf across the ends of the rod is \( 3.14 \, \text{V} \).