:0.35 A
Capacitive Reactance
$$ X_C = \frac{1}{\omega C} = \frac{1}{2 \pi f C} $$
$$ X_C = \frac{1}{2 \times 3.14 \times 50 \times 10 \times 10^{-6}} = \frac{1000}{3.14} $$
$$ V_{rms} = 210 \ V $$
$$ i_{rms} = \frac{V_{rms}}{X_c} = \frac{210}{X_c} $$
Peak current \( = \sqrt{2} i_{rms} \)
$$ = \sqrt{2} \times \frac{210}{1000} \times 3.14 = 0.932 \simeq 0.93 \ A $$
The capacitive reactance is given by:
$$ X_C = \frac{1}{2\pi f C} $$
Given values:
$$ X_C = \frac{1}{2\pi (50) (10 \times 10^{-6})} $$
Solving:
$$ X_C = \frac{1}{3.14 \times 10^{-3}} $$
$$ X_C \approx 318.47 \, \Omega $$
The peak current is given by:
$$ I_0 = \frac{V_0}{X_C} $$
Where:
$$ V_0 = \sqrt{2} V_{\text{rms}} = \sqrt{2} (210) $$
$$ V_0 \approx 296.98 \text{ V} $$
Substituting values:
$$ I_0 = \frac{296.98}{318.47} $$
$$ I_0 \approx 0.93 \text{ A} $$
The peak current is approximately 0.93 A.
What are the charges stored in the \( 1\,\mu\text{F} \) and \( 2\,\mu\text{F} \) capacitors in the circuit once current becomes steady? 

Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity) 