This is taken from Saff&Snider
Q1: I know behind the scenes we are trying to perform a change of variable $\theta \to 2\pi - \theta$. But this isn't the "obvious" substitution I would think of. I would most likely think of $\theta \to \theta/2$ if this was presented to me.
Now this brings my question, is there a reasoning that is missed by me that the author wanted to communicate to me? (Yes I know cosine is even and has period $2\pi$, but that is not what I think being communicated here) because the author didn't outright write we are using an algebraic substitution to solve the integral.
Note I am aware that $\int_{0}^{\pi} \cos dx = \int_{\pi}^{2 \pi} \cos dx$, but is this preserved under $f \to 1/f$ where $f$ is integrand.
Q2: Relating to Q1, how did they know to come up with that substitution
Q3: I found that my substitution $\theta \to \theta/2$ only gets me half of the integral value because I am integrating on a semi-circle $z = e^{i\theta/2}$. My domain $[0,2\pi]$ isn't truly symmetric as oppose to $[-\pi,\pi]$, so I am not sure why multiplying by 2 gets me the real answer.
For those curious, the Residue theorem yields $I = \frac{\pi}{\sqrt{3}}$, but that isn't important to my question(s).

In the half period $[0, \pi], \cos \theta$ takes on every value in its range. So does $\frac {1}{2-\cos\theta}.$ So, in the second half of the period, the function runs through the same values.
This is not true for all periodic functions. It is not true for $f(\theta) = \sin\theta.$
Nonetheless, as it is the case we can say:
$\int_0^\pi \frac{1}{2-\cos\theta}\ d\theta = \frac 12 \int_0^{2\pi} \frac{1}{2-\cos\theta}\ d\theta$
As you note a more formal way to look at it would be to say:
$\int_0^\pi \frac{1}{2-\cos\theta}\ d\theta = \int_{\pi}^{2\pi} \frac{1}{2-\cos\phi}\ d\phi$
by the substitution $\phi = 2\pi - \theta$
or
$\int_0^\pi \frac{1}{2-\cos\theta}\ d\theta = \int_{-\pi}^{0} \frac{1}{2-\cos\theta}\ d\theta$
by the substitution $\phi = -\theta$
Where do these substitutions come from? It is not uncommon to try $u = a+b-x$ as a standard trick in the toolbox. Although this is not what we did, it has a similar feel. The second one might be a little bit more obvious as we are exploiting the fact that $\cos \theta$ is an even function.
As you note, if we use the substitution $\phi = 2\theta$
$\int_0^\pi \frac{1}{2-\cos\theta}\ d\theta$ becomes $\frac 12 \int_0^2\pi \frac{1}{2-\cos\frac \phi 2}\ d\phi$
We still have not cycled a full period for $\cos \frac{\phi}{2}$