Given: \(\sqrt{2}=1.4\)
\[ L=\frac{5}{\pi}\;H,\qquad C=\frac{50}{\pi}\times10^{-6}\;F,\qquad R=400\;\Omega \]
From \[ v=140\sin(100\pi t) \]
Peak voltage, \[ V_0=140\;V \]
Angular frequency, \[ \omega=100\pi\;rad\,s^{-1} \]
\[ X_L=\omega L \]
\[ X_L=(100\pi)\times\frac{5}{\pi}=500\;\Omega \]
\[ X_C=\frac{1}{\omega C} \]
\[ X_C=\frac{1}{100\pi\times\frac{50}{\pi}\times10^{-6}} =\frac{1}{5\times10^{-3}} =200\;\Omega \]
Net reactance,
\[ X=X_L-X_C=500-200=300\;\Omega \]
Impedance,
\[ Z=\sqrt{R^2+X^2} \]
\[ Z=\sqrt{400^2+300^2} =\sqrt{160000+90000} =\sqrt{250000} =500\;\Omega \]
Hence,
\[ \boxed{Z=500\;\Omega} \]
RMS voltage,
\[ V_{\rm rms}=\frac{V_0}{\sqrt2} =\frac{140}{1.4}=100\;V \]
Using,
\[ I_{\rm rms}=\frac{V_{\rm rms}}{Z} \]
\[ I_{\rm rms}=\frac{100}{500}=0.2\;A \]
Hence,
\[ \boxed{I_{\rm rms}=0.2\;A} \]