How and WHY does the RMS of current gve us the equivalent DC?
I've been though this answer here:-root mean square for dc but it doesn't answer my question.
How and WHY does the RMS of current gve us the equivalent DC?
I've been though this answer here:-root mean square for dc but it doesn't answer my question.
It's an arguably limited equivalence, but a convenient one. The power dissipation in a linear resistor R due to an alternating current $I\cdot\sin(\omega t)$ is the same as the power dissipation in the same resistor due to a direct current with the corresponding r.m.s. value, which is $I/\sqrt 2$.
To see why, just consider the instantaneous power dissipation rate in the alternating case, that is $I^2\cdot R\cdot \sin^2(\omega t)$ . With the math equivalence $\sin^2(\omega t) = (1 - \cos(2 \omega t))/2$ , of which the mean value is of course just $1/2$, the mean power dissipation rate is $(I^2/2).R$, i.e. the same as what would be produced by a direct current $I/\sqrt 2$. I hope that helps.