Ok, let's see. Pick coordinates $x=(x_1,...,x_n)$ on $M$, then you get coordinates on $T^{\ast}M$ coming from $x_1,...,x_n$ in the base and picking out the coefficients relative to the basis $dx_1,...,dx_n$ in the fibers. In these charts, $df\colon M\rightarrow T^{\ast}M$ looks as follows: take a point $p$ in Euclidean space, map it to $x^{-1}(p)$, take this to $df\vert_{x^{-1}(p)}$, the first $n$ coordinate of this are just $p$ again, but $df\vert_{x^{-1}(p)}=\sum_{i=1}^n\frac{\partial f}{\partial x_i}\Big\vert_{x^{-1}(p)}dx_i\vert_{x^{-1}(p)}$, so the last $n$ coordinates are just $\frac{…