The circuit element ‘X’ where the current leads the voltage by \( \frac{\pi}{2} \) is the capacitor. In capacitive circuits, the charging current for the capacitor leads the voltage across the capacitor.
The reactance \( X_C \) of a capacitor is given by:
\[ X_C = \frac{1}{\omega C} \]
where \( \omega \) is the angular frequency (\( \omega = 2 \pi f \), with \( f \) being the frequency of the AC supply), and \( C \) is the capacitance in farads.
The capacitive reactance \( X_C \), for a capacitor in an AC circuit is defined 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 shows that \( X_C \) is inversely proportional to the frequency \( f \).
To illustrate the relationship graphically:
In an AC circuit, a capacitor impedes the flow of the current depending on the frequency of the AC supply. Higher frequencies reduce the reactance, allowing more current to pass through, demonstrating a characteristic called capacitive reactance.
In a DC circuit, a capacitor initially conducts as it charges, but once fully charged, it acts as an open circuit. Thus, after the initial charge period, no current flows through the capacitor in a steady-state DC circuit.
The correct IUPAC name of \([ \text{Pt}(\text{NH}_3)_2\text{Cl}_2 ]^{2+} \) is: