The solution to this problem necessitates an understanding of the operational principle of a moving coil galvanometer. In such a device, the deflection is directly proportional to the current passing through it, a phenomenon rooted in the principle that torque on a coil within a magnetic field is proportional to both the current and the coil's number of turns.
The deflection is mathematically represented as:
\(\theta \propto I\)
Given data:
Firstly, convert the given angle from degrees to radians:
\(60^{\circ} = \frac{60 \times \pi}{180} = \frac{\pi}{3} \text{ radians}\)
Utilizing the proportionality, establish equations for both given scenarios:
\(\frac{\pi}{3} \propto 200 \mu A\)
\(\frac{\pi}{10} \propto I_{\text{required}}\)
Since the proportionality constant remains constant, equate the ratios:
\(\frac{200}{I_{\text{required}}} = \frac{\frac{\pi}{3}}{\frac{\pi}{10}}\)
Simplify the right side of the equation:
\(\frac{\pi}{3} \cdot \frac{10}{\pi} = \frac{10}{3}\)
The equation is now:
\(\frac{200}{I_{\text{required}}} = \frac{10}{3}\)
Solve for \(I_{\text{required}}\) by cross-multiplication:
\(I_{\text{required}} = \frac{200 \times 3}{10} = 60 \mu A\)
Consequently, the current necessary to achieve a deflection of \(\frac{\pi}{10}\) radians is 60 \(\mu A\).
The correct option corresponds to 60 \(\mu A\).
Assertion (A): The deflection in a galvanometer is directly proportional to the current passing through it.
Reason (R): The coil of a galvanometer is suspended in a uniform radial magnetic field.