The equation for the voltage across a capacitor is:
\[
V = V_{\text{max}} \sin(\omega t)
\]
where \( V_{\text{max}} = 100 \sqrt{2} \) V is the maximum voltage, and \( \omega \) is the angular frequency.
For an AC circuit with a capacitor, the RMS (Root Mean Square) current is related to the voltage by:
\[
I_{\text{rms}} = \frac{V_{\text{rms}}}{X_C}
\]
where:
- \( V_{\text{rms}} \) is the RMS voltage,
- \( X_C = \frac{1}{\omega C} \) is the reactance of the capacitor.
First, calculate the RMS voltage:
\[
V_{\text{rms}} = \frac{V_{\text{max}}}{\sqrt{2}} = \frac{100 \sqrt{2}}{\sqrt{2}} = 100 \, \text{V}
\]
Now, calculate the reactance \( X_C \). The reactance \( X_C \) is given by:
\[
X_C = \frac{1}{\omega C}
\]
Substitute \( C = 2 \, \mu \text{F} = 2 \times 10^{-6} \, \text{F} \) and \( \omega = 2 \pi f \). For a typical mains frequency of \( f = 50 \, \text{Hz} \), we have:
\[
\omega = 2 \pi \times 50 = 314 \, \text{rad/s}
\]
Now, calculate \( X_C \):
\[
X_C = \frac{1}{314 \times 2 \times 10^{-6}} = 1592.5 \, \Omega
\]
Finally, calculate the RMS current:
\[
I_{\text{rms}} = \frac{100}{1592.5} \approx 0.0628 \, \text{A}
\]
However, this current does not match the provided answer choices. Given that the current is usually much larger in real-world problems, there might be a different \( \omega \) or frequency to account for. We might need to consider another approach based on the given details. Please verify the assumptions to confirm the result.