The effective voltage of a sinusoidal signal is commonly referred to as the root mean square (RMS) voltage. For a pure sinusoidal waveform with no DC offset, the RMS voltage is calculated as:
\[
V_{\text{rms}} = \frac{V_{\text{peak}}}{\sqrt{2}}
\]
This value represents the equivalent DC voltage that would deliver the same power to a load as the AC signal.
When a DC offset is applied to a sinusoidal signal, the effective voltage (RMS) is calculated by considering both the AC and DC components. The formula for the RMS voltage in this case is:
\[
V_{\text{rms}} = \sqrt{V_{\text{dc}}^2 + \left(\frac{V_{\text{peak}}}{\sqrt{2}}\right)^2}
\]
Here, \(V_{\text{dc}}\) is the DC offset voltage, and \(V_{\text{peak}}\) is the peak voltage of the AC component.
The two values used to calculate the RMS voltage are the peak voltage (\(V_{\text{peak}}\)) and the DC offset voltage (\(V_{\text{dc}}\)).
- For a signal without a DC offset, the correct value is \(V_{\text{peak}}/\sqrt{2}\).
- For a signal with a DC offset, the correct value is \(\sqrt{V_{\text{dc}}^2 + (V_{\text{peak}}/\sqrt{2})^2}\).
The reason the latter formula is correct for both cases is that it accounts for the presence of a DC component, which affects the total power delivered by the signal.
- The effective voltage of a sinusoidal signal with no DC offset is \(\boxed{V_{\text{rms}} = \frac{V_{\text{peak}}}{\sqrt{2}}}\).
- With a DC offset, the effective voltage is \(\boxed{V_{\text{rms}} = \sqrt{V_{\text{dc}}^2 + \left(\frac{V_{\text{peak}}}{\sqrt{2}}\right)^2}}\).