To find the net induced emf in the rotating disc, we must first understand the concept of motional emf in a magnetic field.
Here, the disc rotates in a uniform magnetic field. The induced emf (\(E\)) can be calculated using the formula for motional emf in a rotating disc:
\(E = \frac{1}{2} B \omega R^2\)
where:
First, we need to convert the frequency from revolutions per second (rev/s) to angular speed (rad/s):
\(\omega = 2\pi \times \text{frequency}\)
Substituting the frequency in the given formula:
\(\omega = 2\pi \times 10 = 20\pi \text{ rad/s}\)
Now we can substitute these values into the formula for the emf:
\(E = \frac{1}{2} \times 0.1 \times 20\pi \times (0.1)^2\)
This simplifies to:
\(E = \frac{1}{2} \times 0.1 \times 20\pi \times 0.01\)
\(E = 0.01\pi \text{ V}\)
Therefore, the correct induced emf is \(\pi \times 10^{-2} \text{ V}\), which matches the option "
$\pi\times10^{-2}V$