In the previous paragraph we see : V(t) = V0 sin (2πft)
Correspondingly we can write for the current:
I(t) = I 0 sin (2πft)
I rms = ½ √2 I0
In the previous paragraph we see : V(t) = V0 sin (2πft)
Correspondingly we can write for the current:
I(t) = I 0 sin (2πft)
I rms = ½ √2 I0