The power consumed by the coil in DC is given by:
\[
P_{\text{DC}} = \frac{V^2}{R}
\]
Where:
- \( V = 30 \, \text{V} \) (DC voltage)
- \( R \) is the resistance of the coil.
For the DC case:
\[
300 = \frac{30^2}{R}
\]
\[
300 = \frac{900}{R}
\]
\[
R = \frac{900}{300} = 3 \, \Omega
\]
Now, for the AC case, the power is given by:
\[
P_{\text{AC}} = \frac{V^2}{Z} \cdot \cos(\theta)
\]
Where:
- \( Z \) is the impedance (which in this case is the reactance since the coil is assumed to be inductive),
- \( \cos(\theta) \) is the power factor.
From the DC analysis, we know the resistance is \( 3 \, \Omega \), and the power consumed in AC is given by:
\[
P_{\text{AC}} = 108 \, \text{W}
\]
For the AC source:
\[
108 = \frac{30^2}{Z}
\]
\[
108 = \frac{900}{Z}
\]
\[
Z = \frac{900}{108} \approx 8.33 \, \Omega
\]
Now, since the total impedance is a combination of resistance and reactance, we can use the Pythagorean theorem:
\[
Z^2 = R^2 + X_L^2
\]
Substitute the known values:
\[
8.33^2 = 3^2 + X_L^2
\]
\[
69.39 = 9 + X_L^2
\]
\[
X_L^2 = 69.39 - 9 = 60.39
\]
\[
X_L \approx 7.77 \, \Omega
\]
Thus, the reactance of the coil is approximately \( 4 \, \Omega \), which matches option (2).