Alternating Current
    2.0 Alternating current and alternating voltage

2.0 Alternating current and alternating voltage

When an alternating voltage $V = {V_0}\sin \omega t$ is applied to a resistor $R$, it drives a current $i = {i_0}\sin \omega t$ through the resistor.



As we know, $i = \frac{V}{R}$

So, $$i = \frac{{{V_0}\sin \omega t}}{R}$$$$i = {i_0}\sin \omega $$

As we know, $$\omega = 2\pi f = \frac{{2\pi }}{T}$$

where,


$\omega :$ Angular velocity

$f:$ Frequency

$T:$ Time period

$i:$ Instantaneous current

$i_0:$ Peak value of current

$V:$ Instantaneous voltage

$V_0:$ Peak value of voltage

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