100817-1253 EST
There are many viewers of this forum that have a rather incomplete understanding of electrical instruments, devices, circuits, and the use of equations to solve problems with respect to these areas.
Using terms correctly, having an understanding of the words, and being flexible in understanding different perspectives is important in effective communication.
Having an understanding of the meaning of RMS, how it evolved, and how it can be effectively used is important to obtaining reasonably correct answers to some problems.
I can not find a precise trail on the evolution of the use of RMS measurements in the electrical field.
I believe the trail on the concept of RMS starts in the field of statistics with Francis Galton conceiving the standard deviation function in the 1860s. This certainly predates electrical usage. See section "Statistics, standard deviation, regression and correlation" at
http://en.wikipedia.org/wiki/Francis_Galton. There are many other search results that fill in some of the holes.
At some point the name RMS became associated with standard deviation. Then at some other point the correlation of an RMS calculation with the calculation of power in a pure resistance like, Pave = summation from time 1 to time 2 of v^2 / R divided by (time 2 - time1), produced a result of Vrms^2 / R. So the sq-root of (Vrms^2) or just Vrms of any wave shape and a pure resistance could predict the power dissipated in that resistance.
Note: R = Vrms^2 / P and R = P / Irms^2. Combining these produces Vrms^2 / P = P / Irms^2 and rearranging results in Vrms^2 * Irms^2 = P^2 or Vrms * Irms = P. But this equation only applies in certain special cases, albeit, these may be quite common circuits.
The important point of this whole thread is that the user must understand their instruments, equations, and circuits or they may get an incorrect answer.
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