DIFFUSION EQUATION

The 'diffusion equation' is a partial differential equation which describes density fluctuations in a material undergoing diffusion. It is also used to describe processes exhibiting diffusive-like behaviour, for instance the 'diffusion' of alleles in a population in population genetics.
The equation is usually written as:
:
abla cdot igg( D(phi,ec{r}) ,
ablaphi(ec{r},t) igg),
where $,\; phi$ is the density of the diffusing material, $,\; t$ is time, $,\; D$ is the collective diffusion coefficient, is the spatial coordinate and the nabla symbol $,$
abla represents the vector differential operator del. If the diffusion coefficient depends on the density then the equation is nonlinear, otherwise it is linear. If $,\; D$ is constant, then the equation reduces to the following linear equation:
:
abla^2phi(ec{r},t),
also called the heat equation. More generally, when ''D'' is a symmetric positive definite matrix, the equation describes anisotropic diffusion.

Contents

Derivation

See also

Derivation

The diffusion equation can be derived in a straightforward way from the continuity equation, which states that a change in density in any part of the system is due to inflow and outflow of material into and out of that part of the system. Effectively, no material is created or destroyed:
:
ablacdotec{j}=0,
where is the flux of the diffusing material. The diffusion equation can be obtained easily from this when combined with the phenomenological Fick's first law, which assumes that the flux of the diffusing material in any part of the system is proportional to the local density gradient:
:
abla,phi,(,ec{r},t,).

See also

★ Diffusion

★ Heat equation

★ Fick's Second Law