Second-order
linear
Linearity is the property of a mathematical relationship ('' function'') that can be graphically represented as a straight line. Linearity is closely related to '' proportionality''. Examples in physics include rectilinear motion, the linear ...
partial differential equations (PDEs) are classified as either elliptic,
hyperbolic, or
parabolic. Any second-order linear PDE in two variables can be written in the form
:
where , , , , , , and are functions of and and where
,
and similarly for
. A PDE written in this form is elliptic if
:
with this naming convention inspired by the equation for a
planar ellipse.
The simplest examples of elliptic PDE's are the
Laplace equation
In mathematics and physics, Laplace's equation is a second-order partial differential equation named after Pierre-Simon Laplace, who first studied its properties. This is often written as
\nabla^2\! f = 0 or \Delta f = 0,
where \Delta = \n ...
,
, and the
Poisson equation
Poisson's equation is an elliptic partial differential equation of broad utility in theoretical physics. For example, the solution to Poisson's equation is the potential field caused by a given electric charge or mass density distribution; with ...
,
In a sense, any other elliptic PDE in two variables can be considered to be a generalization of one of these equations, as it can always be put into the canonical form
:
through a change of variables.
Qualitative behavior
Elliptic equations have no real
characteristic curves, curves along which it is not possible to eliminate at least one second derivative of
from the conditions of the
Cauchy problem.
Since characteristic curves are the only curves along which solutions to partial differential equations with smooth parameters can have discontinuous derivatives, solutions to elliptic equations cannot have discontinuous derivatives anywhere. This means elliptic equations are well suited to describe equilibrium states, where any discontinuities have already been smoothed out. For instance, we can obtain Laplace's equation from the
heat equation by setting
. This means that Laplace's equation describes a steady state of the heat equation.
In parabolic and hyperbolic equations, characteristics describe lines along which information about the initial data travels. Since elliptic equations have no real characteristic curves, there is no meaningful sense of information propagation for elliptic equations. This makes elliptic equations better suited to describe static, rather than dynamic, processes.
Derivation of canonical form
We derive the canonical form for elliptic equations in two variables,
.
:
and
.
If