According to Elementary Differential Geometry by A N Pressley, a parameterization for Mobius strip is :
$\textit{Example 4.9}$
The Möbius band is the surface obtained by rotating a straight line segment $\cal L$ around its midpoint $P$ at the same time as $P$ moves around a circle $\cal C$, in such a way that as $P$ moves once around $\cal C$, $\cal L$ makes a half-turn about $P$. If we take $\cal C$ to be the circle $x^2+y^2=1$ in the $xy$-plane, and $\cal L$ to be a segment of length $1$ that is initially parallel to the $z$-axis with its midpoint $P$ at $(1,0,0)$, then after $P$ has rotated by an angle $\theta$ around the $z$-axis, $\cal L$ should have rotated by $\theta/2$ around $P$ in the plane containing $P$ and the $z$-axis. The point of $\cal L$ initially at $(1,0,t)$ is then at the point $$\boldsymbol\sigma(t,\theta)=\left(\left(1-t\sin\dfrac\theta2\right)\cos\theta,\left(1-t\sin\dfrac\theta2\right)\sin\theta,t\cos\dfrac\theta2\right).$$ We take the domain of definition of $\boldsymbol\sigma$ to be $$U=\{(t,\theta)\in\mathbf R^2\mid-1/2<t<1/2,\ 0<\theta<2\pi\}.$$
And according to Wiki another parameterization is
$x(u,v)= \left(1+\frac{v}{2} \cos \frac{u}{2}\right)\cos u\\ y(u,v)= \left(1+\frac{v}{2} \cos\frac{u}{2}\right)\sin u\\ z(u,v)= \frac{v}{2}\sin \frac{u}{2}.$
My questions are:
1- how these two 'different' parameterizations can be transformed to each other? Supposing the domains remain same ($0 ≤ u < 2π$ and $−1 ≤ v ≤ 1$) is it not possible by changing variables to do the reparameterizations (esp. $x$ and $y$ in $(x,y,z)$).
2- How (at least one of) the mentioned parameterizations be derived? Wiki and the book mentioning with no proof.
Thank you.