The circuit element ‘X’ where the current leads the voltage by \( \frac{\pi}{2} \) is a capacitor. In capacitive circuits, the capacitor's charging current precedes the voltage across it.
The reactance \( X_C \) of a capacitor is calculated as:
\[ X_C = \frac{1}{\omega C} \]
Here, \( \omega \) is the angular frequency (\( \omega = 2 \pi f \), with \( f \) being the AC supply frequency), and \( C \) is the capacitance in farads.
The capacitive reactance \( X_C \) for a capacitor in an AC circuit is given by the formula:
\[ X_C = \frac{1}{\omega C} \]
where \( \omega = 2 \pi f \) represents the angular frequency, and \( C \) is the capacitance. This formula indicates that \( X_C \) is inversely proportional to the frequency \( f \).

To illustrate this relationship graphically:
In an AC circuit, a capacitor opposes current flow based on the AC supply frequency. Higher frequencies lead to lower reactance, permitting more current to pass, a property known as capacitive reactance.
In a DC circuit, a capacitor initially conducts during charging. Once fully charged, it acts as an open circuit, halting current flow in a steady-state DC condition.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is: