Talha's Physics Academy
AC Through Parallel RC, RL, RLC Circuits and Parallel Resonance
Video Lecture
Watch the complete video lecture below to understand alternating current flowing through parallel RC and RL circuits, parallel RLC circuits, and parallel resonance.
Describe the Flow of AC Through RC and RL Parallel Circuits
1. Parallel RL Circuit
In a parallel RL circuit, a resistor ($R$) and an inductor ($L$) are connected in parallel across an alternating voltage source. The applied voltage $V$ is common across both parallel branches. Because the branch currents ($I_R$ and $I_L$) are out of phase—with the inductive current lagging behind the resistive current—phasor addition must be employed to determine the total supply current.
Using the phasor diagram and Pythagoras' theorem, the total current $I$ is given by:
$$I = \sqrt{I_R^2 + I_L^2}$$
The reciprocal of impedance ($Z$) for a parallel RL circuit is expressed as:
$$\frac{1}{Z^2} = \frac{1}{R^2} + \frac{1}{X_L^2}$$
2. Parallel RC Circuit
In a parallel RC circuit, a resistor ($R$) and a capacitor ($C$) are connected in parallel across an alternating voltage source. The applied voltage $V$ is common across both branches. The current flowing through the capacitor ($I_C$) leads the resistive current ($I_R$) by $\frac{\pi}{2}$ radians.
Using phasor addition, the total current is:
$$I = \sqrt{I_R^2 + I_C^2}$$
The reciprocal of impedance ($Z$) for a parallel RC circuit is expressed as:
$$\frac{1}{Z^2} = \frac{1}{R^2} + \frac{1}{X_C^2}$$

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