(a) At angular frequency $\omega$, the current in $RC$ circuit is given by
$i_{rms} = \frac{V_{rms}}{\sqrt{R^{2} + \left( \frac{1}{\omega C} \right)^{2}}}\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(i)$
Also $\frac{i_{rms}}{2} = \frac{V_{rms}}{\sqrt{R^{2} + \left( \frac{1}{\frac{\omega}{3}}C \right)^{2}}} = \frac{V_{rms}}{\sqrt{R^{2} + \frac{9}{\omega^{2}C^{2}}}}\ \ $ …(ii)
From equation (i) and (ii), we get
$3R^{2} = \frac{5}{\omega^{2}C^{2}} \Rightarrow \frac{\frac{1}{\omega C}}{R} = \sqrt{\frac{3}{5}} \Rightarrow \frac{X_{C}}{R} = \sqrt{\frac{3}{5}}$