In the mathematical theory of partial differential equations, a Monge equation,[1] named after Gaspard Monge, is a first-order partial differential equation for an unknown function u in the independent variables x1,...,xn
F\left(u,x1,x2,...,x
,..., | |||||
|
\partialu | |
\partialxn |
\right)=0
that is a polynomial in the partial derivatives of u. Any Monge equation has a Monge cone.
Classically, putting u = x0, a Monge equation of degree k is written in the form
\sum | |
i0+ … +in=k |
P | |
i0...in |
(x0,x1,...,xk)
i0 | |
dx | |
0 |
i1 | |
dx | |
1 |
…
in | |
dx | |
n |
=0
and expresses a relation between the differentials dxk. The Monge cone at a given point (x0, ..., xn) is the zero locus of the equation in the tangent space at the point.
The Monge equation is unrelated to the (second-order) Monge–Ampère equation.