1.5 The inverse temperature as an integrating factor

The phrase ”integrating factor” origins from the theory for solving differential equations. The factor 1∕T is called an integrating factor for δQ, since dS = δQ∕T is a ”total differential”.
A simple example may illustrate this:
Let

F(x,y) = x2y,

(1.6)

thus

dF(x,y) = 2xydx + x2dy.

(1.7)

We search for solutions F(x,y) = const., but only know the deviation

0 = dF = 2xydx + x2dy,

(1.8)

and after transformation

dy∕dx = -2y∕x.

(1.9)

The four equations are equivalent to some extend, but we lost the factor 1/x in the last equation.
For the solution 0 = 2ydx + xdy it is hard (impossible) to find a function with dG(x,y) = 2ydx + xdy
(try?!?). We first have to multiply with the factor x.
Same as in the above example only after multiplying with the integrating factor 1∕T a total differential is found

dS = δQ∕T.

(1.10)