r.m.s. Values & Power
r.m.s. Values & Power
- An alternating current averages to zero — yet it lights lamps. The average that matters is the average of the square, and it brings a factor of √2.
Root-mean-square
- The of an alternating current is the steady (direct) current that delivers the same average power to a resistive load. It is the honest “effective” value — mains “230 V” is an r.m.s. figure.
Symbols
- = root-mean-square values (sinusoidal a.c. only) (A, V)
- Where √2 comes from: power goes as , and the figure shows averaging to exactly . Square root of the mean of the square: .
- Both conversion directions are live: 2024 gave the peak 3.5 A and wanted r.m.s. 2.5 A (divide) (9702/42/O/N/24 Q8(b)(iii)); 2025 gave r.m.s. 6.0 V and wanted the peak 8.5 V (multiply) (9702/42/M/J/25 Q8(a)(ii)). Decide which way before touching √2.
- With r.m.s. values, every d.c. power formula works unchanged: . Use peaks instead and the answer doubles — in fact mean power is exactly half the peak power, a show-that in 2024: peak W against mean W (9702/42/O/N/24 Q8(c)).
- Power–time sketches are rubric-marked: a sinusoidal curve (at twice the supply frequency) whose troughs sit on the time axis — power never goes negative — with peaks placed and labelled (9702/41/M/J/24 Q7(b)(ii)).
When √2 is banned: non-sinusoidal a.c.
A 2023 square-wave current ran at for half each cycle and (reversed) for the other half. The only safe route is first principles: power is then , mean , so . Writing scored zero — belongs to sine waves only (9702/41/O/N/23 Q7).