Solution to Exact Differential Equation

Theorem
The first order ordinary differential equation‎:
 * $F = M \left({x, y}\right) + N \left({x, y}\right) \dfrac {\mathrm d y} {\mathrm d x} = 0$

is an exact differential equation‎ :
 * $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$

The general solution of such an equation‎ is:
 * $f \left({x, y}\right) = C$

where:
 * $\dfrac {\partial f} {\partial x} = M, \dfrac {\partial f} {\partial y} = N$

Necessary Condition
Let $F$ be exact.

Then by definition there exists a function whose second partial derivatives of $f$ exist and are continuous:
 * $f \left({x, y}\right)$

where:
 * $\dfrac {\partial f} {\partial x} = M, \dfrac {\partial f} {\partial y} = N$

Differentiating $M$ and $N$ partially WRT $y$ and $x$ respectively:


 * $\dfrac {\partial M} {\partial y} = \dfrac {\partial^2 f} {\partial x \partial y}, \dfrac {\partial N} {\partial x} = \dfrac {\partial^2 f} {\partial y \partial x}$

From Mixed Second Partial Derivatives are Equal:
 * $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$

Sufficient Condition
Let $F$ be such that:
 * $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$

Take the equation:
 * $\dfrac {\partial f} {\partial x} = M$

and integrate it WRT $x$:
 * $\displaystyle (1): \quad f = \int M \ \mathrm d x + g \left({y}\right)$

Note that the arbitrary constant here is an arbitrary function of $y$, since when differentiating partially WRT $x$ it disappears.

So, now we need to find such a $g \left({y}\right)$ so as to make $f$ as defined in $(1)$ satisfy $\dfrac {\partial f} {\partial y} = N$.

Differentiating $(1)$ WRT $y$ and equating it to $N$:
 * $\displaystyle \frac {\partial} {\partial y} \int M \ \mathrm d x + g' \left({y}\right) = N$

So:
 * $\displaystyle g' \left({y}\right) = N - \frac {\partial} {\partial y} \int M \ \mathrm d x$

which can be integrated WRT $y$ thus:
 * $\displaystyle g \left({y}\right) = \int \left({N - \frac {\partial} {\partial y} \int M \ \mathrm d x}\right) \ \mathrm d y$

which works as long as the integrand is a function of $y$ only.

This will happen if its derivative WRT $x$ is equal to zero.

We need to make sure of that, so we try it out:

This is our initial condition.

The Solution
Then $F$ can be written in the form:
 * $\dfrac {\partial f} {\partial x} \ \mathrm d x + \dfrac {\partial f} {\partial y} \ \mathrm d y = 0$

and the solution follows.