When proving that $$\int^{\infty}_{-\infty}\frac{1}{\sqrt{2\pi}\sigma}{e^{-\frac{1}{2}({\frac{x-\mu}{\sigma})}^2}}dx=1$$
and I faced a problem, $$A^2=\frac{1}{2\pi}\int^\infty_{-\infty}\int^\infty_{-\infty}e^{-\frac{y^2+z^2}{2}}dydz$$is $$\frac{1}{2\pi}\int^{2\pi}_{0}\int^\infty_{0}e^{-\frac{r^2}{2}}rdrd{\theta}$$
by putting $y=r\sin{\theta},z=r\cos{\theta}$
Can I have some additional explanations about this?
The integral is much easier to calculate, if the cartesian coordinates are transformed in polar coordinates. A point is given there by the radius r (distance from the point 0/0) and the angle phi. The resulting double integral quickly brings the desired result.