Step 1: Understanding the Concept:
For a flat spiral coil, the radius of the turns varies linearly from the inner radius $r_1$ to the outer radius $r_2$. The magnetic moment of a single loop is $I \times A$. For a spiral, we must integrate the moments of all infinitesimal turns across the radius.
Step 2: Key Formula or Approach:
1. Number of turns per unit radial length $n = \frac{N}{r_2 - r_1}$.
2. Magnetic moment of a small element $dr$: $dm = (n \, dr) I (\pi r^2)$.
3. Total magnetic moment $M = \int_{r_1}^{r_2} n I \pi r^2 \, dr$.
Step 3: Detailed Explanation:
1. Substitute the constants:
\[ M = \frac{N I \pi}{r_2 - r_1} \int_{r_1}^{r_2} r^2 \, dr = \frac{N I \pi}{r_2 - r_1} \left[ \frac{r^3}{3} \right]_{r_1}^{r_2} \]
2. Simplify the expression using $r_2^3 - r_1^3 = (r_2 - r_1)(r_2^2 + r_1^2 + r_1 r_2)$:
\[ M = \frac{N I \pi}{3} (r_2^2 + r_1^2 + r_1 r_2) \]
3. Plug in the values ($N=200, I=0.02, r_1=0.03, r_2=0.06$):
\[ M = \frac{200 \times 0.02 \times 3.14}{3} (0.0036 + 0.0009 + 0.0018) \]
\[ M = \frac{12.56}{3} (0.0063) = 12.56 \times 0.0021 = 0.026376 \text{ A.m}^2 \]
4. Converting to $\alpha \times 10^{-2}$: $M \approx 2.64 \times 10^{-2}$. So, $\alpha = 2.64$.
Step 4: Final Answer:
The value of $\alpha$ is 2.64.