The formula for current in a capacitor within an AC circuit is:
\[ I = V \frac{\omega C}{\sqrt{1 + (\omega C)^2}} \]
The parameters are defined as follows:
In a capacitor, the displacement current is equivalent to the conduction current. The current flowing through the capacitor is determined by:
\[ I = V \frac{\omega C}{X_C} \]
Here, \(X_C = \frac{1}{\omega C}\) signifies the capacitive reactance.
The calculation proceeds as follows:
\[ I = \frac{230 \times 300 \times 200 \times 10^{-12}}{X_C} = 13.8 \mu\text{A} \]
Consequently, the RMS current, comprising both conduction and displacement current, is 13.8 $\mu\text{A}$.
A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit. 
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.