I've seen it done a few times, it's always roughly apparent that "oh yeah, okay, they've dropped this, pulled this there, yeah, okay, kind of convincing" - but I've never why or how to do it for myself.
I probably don't understand it enough to be searching in the right way, but I'm unable to find anything useful by Googling.
There's a really nice mathmo derivation that I barely understand a word of here.
And a thoroughly unhelpful Physicist "thus it is this" non-explanation here.
But how about a nice not-mathematically-proper-but-it-works method for Engineers?
To be clear, I want to know how to go from:
$$ \lim_{\Delta\omega\rightarrow0} \sum_{n=-\infty}^{\infty} \dfrac{G(n\cdot\Delta\omega)\cdot\Delta\omega}{2\pi} \cdot e^{jn\cdot\Delta\omega\cdot t} $$
to:
$$ \dfrac{1}{2\pi} \int_{-\infty}^{\infty}G(\omega) e^{j\omega t} \cdot d\omega $$
and vice versa, and know how to do this for other problems, since as I said, I can sort of see that we've kept the limits, integrated wrt the limit, and removed the summation variable \$n\$. But if I did that on another problem, I wouldn't know I was 'doing it right' - and going in the other direction, how do we know where to put the \$n\$ back in?