In an RL (Resistor-Inductor) circuit, the formula for apparent power (\(S\)) is given by:
\[ S = V_{\text{rms}} \times I_{\text{rms}} \]
where:
- \(V_{\text{rms}}\) is the root-mean-square (RMS) voltage across the circuit.
- \(I_{\text{rms}}\) is the root-mean-square (RMS) current through the circuit.
### Explanation:
1. **Apparent Power (\(S\))**: This is the total power in an AC circuit, which is the product of the RMS voltage and the RMS current. It is measured in volt-amperes (VA).
2. **RMS Voltage (\(V_{\text{rms}}\))**: This is the effective voltage of the AC source that delivers the same power as a DC source.
3. **RMS Current (\(I_{\text{rms}}\))**: This is the effective current that flows through the circuit, delivering the same power as a DC current.
### Relationship with Other Powers:
In an RL circuit, the apparent power is composed of two components:
- **Real Power (\(P\))**: The actual power consumed by the resistor, given by \(P = V_{\text{rms}} \times I_{\text{rms}} \times \cos(\phi)\), where \(\phi\) is the phase angle between the voltage and the current.
- **Reactive Power (\(Q\))**: The power stored and released by the inductor, given by \(Q = V_{\text{rms}} \times I_{\text{rms}} \times \sin(\phi)\).
These are related to the apparent power by the following equation:
\[ S^2 = P^2 + Q^2 \]
where:
- \(P\) is the real power.
- \(Q\) is the reactive power.
So, in summary, the formula for apparent power in an RL circuit is simply the product of the RMS voltage and RMS current, but its interpretation involves understanding how it relates to real and reactive power.