What my physics book referred to as the paraxial approximation derived to be thus:
$$\frac{1}{s}+\frac{1}{s'}=\frac{2}{R}$$
as a way of showing that in a concave spherical mirror, all reflected rays hit the a single point P. I think it is fair use to show just this diagram, since the book is more than 1000 pages:
It used these equations, and simply removed the $\delta$ term as a simplification for when $$\tan{\alpha}=\frac{h}{s-\delta}\space\space\tan{\beta}=\frac{h}{s'-\delta}\space\space\tan{\phi}=\frac{h}{R-\delta}$$. Using WolframAlpha, I solved for the original Equation:
$$s'=\frac{\delta(s-2R)+Rs}{\delta+R-2s}$$
But this didn't help me understand why exactly all rays converge to P. The book says: "The equation does not contain a single $\alpha.$. It seems, in fact, that since $\theta$ depends on $\alpha$, that in fact the image is somewhat distorted for anything BUT a point.
Changing any single variable in this equation changes all the others! It continues: "All rays from P that make sufficiently small angles with sufficiently small angles with the axis intersect a P' after they are reflected..." but that doesn't make sense to me either.
I guess my question could be summed up as this:
A.) Why is this approximation useful? Would an actual engineer/scientist use it or is it mostly a learning tool?
B.) What is $$\frac{ds'}{d\alpha}$$? Am I correct to infer this value shrinks with the value of $\alpha$?
The book is University Physics by Sears & Zemansky.