Today I half-remembered a wonderful trick to doing thermodynamical partial derivatives, but I neither recall the full set of rules, nor where I got them from! I was hoping someone else knows where they come from or where I can find them written out.
The rules, as far as I remember them, is to define a bracket $[A,B]$ defined on thermodynamical potentials and variables such that:
$[X,X] = 1$,
$[X,Y] = -[Y,X]$,
If $dX = AdB + CdD$, then $[X,Y] = [B,Y][D,Y]$,
and most importantly,
$\left(\frac{\partial X}{\partial Y}\right)_Z = \frac{[X,Z]}{[Y,Z]}$.
As an example of this working (I'm dropping the commas), we have
$$\left(\frac{\partial P}{\partial V}\right)_S = \frac{[PS]}{[VS]}\\ \\ = \frac{[PS]}{[VS]}\cdot \frac{[TP]}{[TP]}\cdot \frac{[TV]}{[TV]} \cdot \frac{[PP]}{[VV]} = \frac{[TP]}{[TV]}\cdot \frac{[HP]}{[TP]}\cdot \frac{[TV]}{[UV]}\\ \\ = \frac{[TP]}{[TV]}\cdot \frac{[HP]}{[TP]} / \frac{[UV]}{[TV]}\\ \\ = \left(\frac{\partial P}{\partial V}\right)_T \cdot \left(\frac{\partial H}{\partial T}\right)_P / \left(\frac{\partial U}{\partial T}\right)_V\\ \\ = \left(\frac{\partial P}{\partial V}\right)_T \cdot \left(\frac{C_p}{C_V}\right)$$
The second equality involves multiplying by 1 several times. The second is based on the third rule.
Edit:
As a user pointed out, the first identity is trivially wrong, and should be
$[X,X] = 0$.
For more details, see the link in the accepted answer.