The magnetic moment (\(M\)) of a circular coil is given by the formula \( M = nIA \), where n is the number of turns, I is the current, and A is the area of the coil.
The area of a circular coil with radius r is \( A = \pi r^2 \).
So, the magnetic moment is \( M = nI(\pi r^2) \).
Let's write down the information given for coil A and coil B.
For coil A: \( n_A = 300 \), \( M_A \), \( I_A \), \( r_A \).
For coil B: \( n_B = 200 \), \( M_B \), \( I_B \), \( r_B \).
We are given that the currents are equal: \( I_A = I_B = I \).
We are given the ratio of their magnetic moments: \( \frac{M_A}{M_B} = \frac{1}{2} \).
Now, let's write the ratio of the magnetic moments using the formula.
\( \frac{M_A}{M_B} = \frac{n_A I_A (\pi r_A^2)}{n_B I_B (\pi r_B^2)} \).
Since \(I_A = I_B\) and \(\pi\) is a constant, they cancel out.
\( \frac{M_A}{M_B} = \frac{n_A r_A^2}{n_B r_B^2} \).
We are given this ratio is 1/2. Substitute the known values.
\( \frac{1}{2} = \frac{300 \cdot r_A^2}{200 \cdot r_B^2} = \frac{3}{2} \left( \frac{r_A}{r_B} \right)^2 \).
Now, we need to solve for the ratio of the radii, \( \frac{r_A}{r_B} \).
\( \left( \frac{r_A}{r_B} \right)^2 = \frac{1}{2} \times \frac{2}{3} = \frac{1}{3} \).
Taking the square root of both sides:
\( \frac{r_A}{r_B} = \sqrt{\frac{1}{3}} = \frac{1}{\sqrt{3}} \).
The ratio of the radii of coils A and B is \( 1:\sqrt{3} \).