How do I calculate the peak-to-peak voltage of a sine wave given RMS voltage?


The short answer:

\begin{equation} \frac{V_{p-p}}{V_{rms}} = 2\sqrt{2} \end{equation}

The long answer, or how to derive the above:

As noted on the Wikipedia page for root mean square, the RMS of a sine wave is equal to its amplitude divided by the square root of two. (You can also derive this by doing the integral over a sine wave yourself.)

\begin{equation} V_{rms} = \frac{a}{\sqrt{2}} \end{equation}

The peak-to-peak voltage is twice the amplitude of the wave, since it's measuring from the tip of a peak to the tip of a trough.

\begin{equation} V_{p-p} = 2a \end{equation}

We can rearrange these two equations:

\begin{equation} V_{rms} \cdot \sqrt{2} = a \end{equation} \begin{equation} V_{p-p} = 2 \cdot (V_{rms} \cdot \sqrt{2}) \end{equation} \begin{equation} V_{p-p} = V_{rms} \cdot 2\sqrt{2} \end{equation}

Thus, we multiply the RMS voltage by twice the square root of two - a factor of about 2.828 or so:

\begin{equation} 2\sqrt{2} = 2.8284271247.... \end{equation}

Of course, the process also works in reverse - if you can measure the peak-to-peak voltage, dividing that by the same factor will give you the RMS voltage assuming a perfect sine wave.

  • $\begingroup$ I hope we get LaTeX equation support here - this would be a great use case for it! $\endgroup$
    – Dan
    Oct 24 '13 at 0:11
  • $\begingroup$ @Dan yep, hoping it gets turned on soon. $\endgroup$
    – Amber
    Oct 24 '13 at 0:28
  • $\begingroup$ Can you explain a little more? I'm still not entirely following. $\endgroup$
    – Dan
    Oct 28 '13 at 20:17

In a pure sine wave $V_{RMS} \times 1.414$ will give you peak. $V_{Peak} \times .707$ will give you RMS.

  • $\begingroup$ Note, however, that "peak" and "peak to peak" are not the same thing. $\endgroup$
    – Amber
    Oct 29 '13 at 22:37
  • $\begingroup$ That formula will work for "peak "or "peak to peak" depending on what you feed it. Of course peak × 2 also works for" p to p. $\endgroup$ Oct 29 '13 at 23:57

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