In mathematics, an exact differential equation or total differential equation is a certain kind of ordinary differential equation which is widely used in physics and engineering.
Definition
Given a simply connected and open subset D of R^{2} and two functions I and J which are continuous on D then an implicit firstorder ordinary differential equation of the form

I(x, y)\, \mathrm{d}x + J(x, y)\, \mathrm{d}y = 0, \,\!
is called an exact differential equation if there exists a continuously differentiable function F, called the potential function, so that

\frac{\partial F}{\partial x}(x, y) = I
and

\frac{\partial F}{\partial y}(x, y) = J.
The nomenclature of "exact differential equation" refers to the exact derivative of a function. For a function F(x_0, x_1,...,x_{n1},x_n), the exact or total derivative with respect to x_0 is given by

\frac{\mathrm{d}F}{\mathrm{d}x_0}=\frac{\partial F}{\partial x_0}+\sum_{i=1}^{n}\frac{\partial F}{\partial x_i}\frac{\mathrm{d}x_i}{\mathrm{d}x_0}.
Example
The function

F(x,y) := \frac{1}{2}(x^2 + y^2)
is a potential function for the differential equation

xdx + ydy = 0.\,
Existence of potential functions
In physical applications the functions I and J are usually not only continuous but even continuously differentiable. Schwarz's Theorem then provides us with a necessary criterion for the existence of a potential function. For differential equations defined on simply connected sets the criterion is even sufficient and we get the following theorem:
Given a differential equation of the form (for example, when F has zero slope in the x and y direction at F(x,y) ):

I(x, y)\, \mathrm{d}x + J(x, y)\, \mathrm{d}y = 0, \,\!
with I and J continuously differentiable on a simply connected and open subset D of R^{2} then a potential function F exists if and only if

\frac{\partial I}{\partial y}(x, y) = \frac{\partial J}{\partial x}(x, y).
Solutions to exact differential equations
Given an exact differential equation defined on some simply connected and open subset D of R^{2} with potential function F then a differentiable function f with (x, f(x)) in D is a solution if and only if there exists real number c so that

F(x, f(x)) = c.\,
For an initial value problem

y(x_0) = y_0\,
we can locally find a potential function by

F(x,y) = \int_{x_0}^x I(t,y_0) \mathrm{d}t + \int_{y_0}^y \left[ J(x,t)  \int_{x_0}^{x} \frac{\partial I}{\partial t}(u, t)\, \mathrm{d}u\,\right]\mathrm{d}t.
Solving

F(x,y) = c\,
for y, where c is a real number, we can then construct all solutions.
See also
References

Boyce, William E.; DiPrima, Richard C. (1986). Elementary Differential Equations (4th ed.). New York: John Wiley & Sons, Inc. ISBN 0471078948
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