1.5 The inverse temperature as an integrating factor

The phrase ”integrating factor” origins from the theory for solving differential equations. The factor 1T is called an integrating factor for δQ, since dS = δQT 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

dydx = -2yx.

(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 1T a total differential is found

dS = δQT.

(1.10)