If you don’t own a copy of the volumes of Feynman’s Lectures on Physics, I would highly recommend one.
He brilliantly introduces complex numbers in Vol. 1, “22-5 Complex Numbers”. But in the next section, “22-6 Imaginary Exponents”, he makes the following famous assertion:
We summarize with this, the most remarkable formula in mathematics:
\begin{equation}
\label{Eq:I:22:9}
e^{i\theta}=\cos\theta+i\sin\theta.
\end{equation}
This is our jewel.
There’s too much to cover here, but I refer you to this lecture where he applies the above formula, with regard to AC circuits: Vol 2. 22 - AC Circuits
An excerpt:
We have already discussed some of the properties of electrical circuits in Chapters 23 and 25 of Vol. I. Now we will cover some of the same material again, but in greater detail. Again we are going to deal only with linear systems and with voltages and currents which all vary sinusoidally; we can then represent all voltages and currents by complex numbers, using the exponential notation described in Chapter 23 of Vol. I. Thus a time-varying voltage V(t) will be written
\begin{equation}
\label{Eq:II:22:1}
V(t)=\hat{V}e^{i\omega t},
\end{equation}
where $$\hat{V}$$
represents a complex number that is independent of t. It is, of course, understood that the actual time-varying voltage V(t) is given by the real part of the complex function on the right-hand side of the equation.
Similarly, all of our other time-varying quantities will be taken to vary sinusoidally at the same frequency ω. So we write
\begin{equation}
\begin{aligned}
I&=\hat{I}\,e^{i\omega t}\quad(\text{current}),\\[3pt]
\xi&=\hat{\xi}\,e^{i\omega t}\quad(\text{emf}),\\[3pt]
E&=\hat{E}\,e^{i\omega t}\quad(\text{electric field}),
\end{aligned}
\label{Eq:II:22:2}
\end{equation} and so on.
Most of the time we will write our equations in terms of V, I, ξ, ...
(instead of in terms of V̂, Î, ξ̂, ...) remembering, though, that the time variations are as given in (22.2).
In our earlier discussion of circuits we assumed that such things as inductances, capacitances, and resistances were familiar to you. We want now to look in a little more detail at what is meant by these idealized circuit elements. We begin with the inductance.
- Note: don’t treat this as an answer, but as supplemental reference