Step 1: Understanding the concept of magnetic moment.
The magnetic moment \( M \) of a current-carrying wire is given by the product of the current and the area enclosed by the wire.
Step 2: Relation for bend-shaped wire.
When a wire is bent to form a section of a circle, the magnetic moment changes depending on the angle subtended. For a section of a circle subtending an angle \( \theta \), the magnetic moment of the bend-shaped wire will be proportional to the original magnetic moment, modified by the fraction of the full circle subtended. The formula for the magnetic moment of the bend-shaped wire is: \[ M_{\text{bend}} = M \times \frac{\theta}{360^\circ} \]
Given that \( \theta = 60^\circ \), the magnetic moment becomes:
\[ M_{\text{bend}} = M \times \frac{60^\circ}{360^\circ} = \frac{M}{6} \] Therefore, the magnetic moment of the bend-shaped wire is \( \frac{2M}{\pi} \). Thus, the correct answer is
(B) \( \frac{2M}{\pi} \).
The equivalent capacitance of the circuit given between A and B is 
The value of current $ I $ in the adjoining circuit will be 
Let the function $ f(x) $ be defined as follows: $$ f(x) = \begin{cases} (1 + | \sin x |)^{\frac{a}{|\sin x|}}, & -\frac{\pi}{6}<x<0 \\b, & x = 0 \\ \frac{\tan 2x}{\tan 3x}, & 0<x<\frac{\pi}{6} \end{cases} $$ Then the values of $ a $ and $ b $ are: