According to the problem, the inductive reactance at \( 50 \, \mathrm{Hz} \) is:
\[
X_L = 20 \, \Omega.
\]
The inductive reactance \( X_L \) is given by:
\[
X_L = 2\pi f L.
\]
Substitute \( f = 50 \, \mathrm{Hz} \) and \( X_L = 20 \, \Omega \):
\[
2\pi \times 50 \times L = 20.
\]
Simplify:
\[
L = \frac{20}{2\pi \times 50} = \frac{1}{5\pi} \, \mathrm{H}.
\]
If the frequency is increased to \( 100 \, \mathrm{Hz} \), the new inductive reactance is:
\[
X_L = 2\pi f L.
\]
Substitute \( f = 100 \, \mathrm{Hz} \) and \( L = \frac{1}{5\pi} \, \mathrm{H} \):
\[
X_L = 2\pi \times 100 \times \frac{1}{5\pi} = 40 \, \Omega.
\]
The impedance \( Z \) of the circuit is given by:
\[
Z = \sqrt{R^2 + X_L^2}.
\]
Substitute \( R = 30 \, \Omega \) and \( X_L = 40 \, \Omega \):
\[
Z = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500}.
\]
Simplify:
\[
Z = 50 \, \Omega.
\]
The current \( I \) is calculated using Ohm's Law:
\[
I = \frac{V}{Z}.
\]
Substitute \( V = 200 \, \mathrm{V} \) and \( Z = 50 \, \Omega \):
\[
I = \frac{200}{50} = 4 \, \mathrm{A}.
\]
Thus, the current flowing through the coil is:
\[
I = 4 \, \mathrm{A}.
\]