This function calculates the rms value of a sinusoidal voltage with superimposed DC voltage.
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The picture shows a sine wave voltage with a peak value of ± 60 volts which is superimposed by a DC voltage (offset) of 20 volts.
The rms value is defined as a DC voltage value with the same thermal effect as the specified AC voltage. With sinusoidal alternating current it is without offset:
\(\displaystyle U_{rms}=\frac{U_p}{\sqrt{2}}\)
In order to calculate the effective value of a superimposed sinusoidal voltage, the value of the voltage difference between the maximum and minimum voltage (Upp) must first be determined.
\(\displaystyle U_{pp}=U_{max}-U_{min}\)
The peak value can be derived from this
\(\displaystyle U_p=\frac{ U_{pp} } {2} =\frac{U_{max}-U_{min}}{2}\)
The formula for the rms value of the sinusoidal voltage without DC voltage component is therefore:
\(\displaystyle U_{rms}=\frac{U_p}{\sqrt{2}}=\frac{ U_{pp} } {2 · \sqrt{2}} =\frac{U_{max}-U_{min}}{2 · \sqrt{2}}\)
To calculate the rms value with offset, the rms value of the sinusoidal voltage is added to the square of the value of the direct voltage. The formula is
\(\displaystyle U2_{rms}=\sqrt{U_{rms}^2 + U_{off}^2}\)
The mean value of the pure sine voltage is always 0V. If the voltage is superimposed on a DC voltage, the average value is identical to the superimposed DC voltage.
\(\displaystyle U_p\)
Peak voltage
\(\displaystyle U_{pp}\)
Peak-to-peak voltage
\(\displaystyle U_{rms}\)
RMS value of the AC voltage
\(\displaystyle U2_{rms}\)
Rms AC voltage with superimposed DC
\(\displaystyle U_{off}\)
Superimposed DC voltage (offset)
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