Given the problem statement, the inductive reactance at \( 50 \, \mathrm{Hz} \) is \( X_L = 20 \, \Omega \). The formula for inductive reactance is \( X_L = 2\pi f L \). Substituting the known values, \( 2\pi \times 50 \times L = 20 \). Solving for inductance \( L \), we get \( L = \frac{20}{2\pi \times 50} = \frac{1}{5\pi} \, \mathrm{H} \). When the frequency is increased to \( 100 \, \mathrm{Hz} \), the new inductive reactance is calculated using \( X_L = 2\pi f L \). Substituting \( f = 100 \, \mathrm{Hz} \) and \( L = \frac{1}{5\pi} \, \mathrm{H} \), we find \( X_L = 2\pi \times 100 \times \frac{1}{5\pi} = 40 \, \Omega \). The circuit impedance \( Z \) is determined by the formula \( Z = \sqrt{R^2 + X_L^2} \). With \( R = 30 \, \Omega \) and \( X_L = 40 \, \Omega \), the impedance is \( Z = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500} = 50 \, \Omega \). Ohm's Law, \( I = \frac{V}{Z} \), is used to find the current. Substituting \( V = 200 \, \mathrm{V} \) and \( Z = 50 \, \Omega \), the current is \( I = \frac{200}{50} = 4 \, \mathrm{A} \). Therefore, the current flowing through the coil is \( I = 4 \, \mathrm{A} \).