Power in AC Circuit — Core Principles
Core Principles
Power in an AC circuit is more complex than in a DC circuit due to the sinusoidal variation of voltage and current, and the potential phase difference between them. Instantaneous power, , fluctuates with time and can even be negative.
The crucial quantity for practical applications is the average power, , dissipated over a full cycle. This is given by the formula , where and are the root mean square values of voltage and current, respectively, and is the phase angle between them.
The term is known as the power factor, which indicates the efficiency of power utilization. For purely resistive circuits, and , leading to maximum power dissipation.
For purely inductive or capacitive circuits, and , resulting in zero average power dissipation (wattless current). In LCR series circuits, the power factor is , and at resonance, it becomes 1, maximizing power transfer to the resistance.
Important Differences
vs Power in DC Circuit
| Aspect | This Topic | Power in DC Circuit |
|---|---|---|
| Nature of Voltage/Current | Constant (steady) | Sinusoidally varying with time |
| Formula for Power | $P = VI$ | $P_{avg} = V_{rms}I_{rms}cosphi$ |
| Phase Difference | Not applicable (voltage and current are always in phase) | Exists between voltage and current, denoted by $phi$ |
| Power Factor | Always 1 (implicitly) | Varies between 0 and 1, $cosphi$ |
| Reactive Components (L, C) | No effect on steady power dissipation | Significantly affect power factor and average power (can cause wattless current) |
| Energy Dissipation | Always dissipated in resistance | Only dissipated in resistance; reactive components store/release energy |