Step 1: Principle involved.
When a conducting loop rotates in a uniform magnetic field, the magnetic flux linked with it changes with time.
According to Faraday’s law, a changing flux induces an alternating emf.
Step 2: Formula for maximum induced emf.
\[
\varepsilon_0 = NBA\omega
\]
Here, \(N = 1\).
Step 3: Calculate required quantities.
Area of the square loop:
\[
A = (0.1)^2 = 0.01 \, \text{m}^2
\]
Magnetic field:
\[
B = 0.2 \, \text{T}
\]
Convert rotational speed into angular velocity:
\[
f = 60 \, \text{rpm} = \frac{60}{60} = 1 \, \text{Hz}
\]
\[
\omega = 2\pi f = 2\pi \times 1 = 2\pi \, \text{rad/s}
\]
Step 4: Determine maximum emf.
\[
\varepsilon_0 = 0.2 \times 0.01 \times 2\pi
\]
\[
\varepsilon_0 = 0.002 \times 2\pi = 0.004\pi \, \text{V}
\]
\[
\varepsilon_0 \approx 0.01256 \, \text{V}
\]
Final Answer:
Maximum induced emf \( = 0.004\pi \, \text{V} \)
or approximately \( 1.26 \times 10^{-2} \, \text{V} \)