If you solved simple \(\displaystyle \text{DC}\) circuits, I am sure that you would be familiar with ohm's law:
\(\displaystyle V = I \times R\)
Now even if we have \(\displaystyle \text{AC}\) circuits and combinations of resistors, inductors, and capacitors, the law stays the same, but instead of \(\displaystyle R\), we write \(\displaystyle \bold{Z}\).
where \(\displaystyle \bold{Z}\) is called impedance. The impedance is just the combination of \(\displaystyle R\) and \(\displaystyle L\) (inductor) in our current circuit.
So, we have this formula:
\(\displaystyle \bold{V} = \bold{I}_z \times \bold{Z}\)
This formula will help us solve for \(\displaystyle \bold{I}_z\).
\(\displaystyle \bold{I}_z = \frac{\bold{V}}{\bold{Z}} = \frac{120}{8 + j12} \ \text{A}\)
In the next post, we will try to figure out a way to find the current, \(\displaystyle \bold{I}_v\).