Step 1: Understanding the Question:
The problem requires finding the analytical expression for the coefficient of self-induction ($L$) of a flat, closely-wound circular coil containing a total of $N$ turns and a cross-sectional radius $R$.
Step 2: Key Formula or Approach:
1. The magnetic field ($B$) at the geometric center of a circular coil carrying a current $I$ is given by:
$$B = \frac{\mu_0 N I}{2R}$$
2. The total magnetic flux linkage ($\Phi$) passing through all $N$ loops of the coil area $A = \pi R^2$ is:
$$\Phi = N \cdot (B \cdot A)$$
3. The self-inductance ($L$) is defined by the fundamental relationship matching total flux per unit current:
$$\Phi = L \cdot I \implies L = \frac{\Phi}{I}$$
Step 3: Detailed Explanation:
Let's first compute the total magnetic flux linked across the entire multi-turn coil assembly.
Substitute the magnetic field expression $B$ and area $A = \pi R^2$ into the flux linkage equation:
$$\Phi = N \cdot \left( \frac{\mu_0 N I}{2R} \right) \cdot \left( \pi R^2 \right)$$
Combine the terms together:
$$\Phi = \frac{\mu_0 N^2 \pi R^2 I}{2R}$$
One factor of the radius $R$ cancels out between the numerator and denominator:
$$\Phi = \frac{\mu_0 N^2 \pi R I}{2}$$
Now, to find the self-inductance coefficient $L$, divide the total flux linkage expression by the current variable $I$:
$$L = \frac{\Phi}{I} = \frac{\mu_0 N^2 \pi R}{2}$$
Step 4: Final Answer:
The coefficient of self-induction equals $\frac{\mu_0 N^2 \pi R}{2}$, which matches option (C).