Step 1: Understanding the Question:
A multi-turn conducting coil ($N = 600$, $A = 0.06\text{ m}^2$) is initially positioned perpendicular to a uniform magnetic field ($B = 5 \times 10^{-5}\text{ Wb/m}^2$).
The coil is then rotated by $90^\circ$ over a time interval of $\Delta t = 0.2\text{ s}$. We need to compute the magnitude of the average electromotive force (e.m.f.) induced across the coil terminals.
Step 2: Key Formula or Approach:
According to Faraday's Law of Electromagnetic Induction, the average induced e.m.f. ($e$) corresponds to the time rate of change of the linked magnetic flux:
$$|e| = N \frac{|\Delta \phi|}{\Delta t} = N \frac{|\phi_2 - \phi_1|}{\Delta t}$$
The magnetic flux linked through a single loop depends on its orientation: $\phi = BA \cos\theta$.
Initially, the coil faces the flux directly ($\theta_1 = 0^\circ$), and it rotates to a parallel orientation ($\theta_2 = 90^\circ$).
Step 3: Detailed Explanation:
Let's evaluate the initial ($\phi_1$) and final ($\phi_2$) magnetic flux states:
$$\phi_1 = BA \cos(0^\circ) = BA(1) = BA$$
$$\phi_2 = BA \cos(90^\circ) = BA(0) = 0$$
The net change in magnetic flux per turn is:
$$|\Delta \phi| = |\phi_2 - \phi_1| = |0 - BA| = BA$$
Now, substitute this flux difference into Faraday's equation along with the system variables:
$$|e| = \frac{N \cdot B \cdot A}{\Delta t}$$
Substitute the given values ($N = 600$, $B = 5 \times 10^{-5}$, $A = 0.06$, $\Delta t = 0.2$):
$$|e| = \frac{600 \times (5 \times 10^{-5}) \times 0.06}{0.2}$$
Simplify the numerical multiplication in the numerator:
$$600 \times 0.06 = 36$$
$$36 \times 5 \times 10^{-5} = 180 \times 10^{-5} = 1.8 \times 10^{-3}$$
Now divide by the time denominator:
$$|e| = \frac{1.8 \times 10^{-3}}{0.2} = 9 \times 10^{-3}\text{ V}$$
Step 4: Final Answer:
The magnitude of the average induced e.m.f. is $9 \times 10^{-3}\text{ V}$, which corresponds to option (B).