Table of partial differential equations#
Name |
Equation |
Classification(s) |
|---|---|---|
Poisson |
\(\nabla\cdot(\mathsf{D}\cdot\nabla u) = f\) |
elliptic, second-order in space |
diffusion |
\(\frac{\partial u}{\partial t} = \nabla\cdot(\mathsf{D}\cdot\nabla u)\) |
parabolic, second-order in space, first-order in time |
advection |
\(\frac{\partial u}{\partial t}+\textbf{a}\cdot\nabla u = 0\) |
hyperbolic, first-order in space, first-order in time |
advection-diffusion |
\(\frac{\partial u}{\partial t}+\textbf{a}\cdot\nabla u = \nabla\cdot(\mathsf{D}\cdot\nabla u)\) |
parabolic, second-order in space, first-order in time |
advection-diffusion-reaction (nonlinear) |
\(\frac{\partial u}{\partial t}+\textbf{a}\cdot\nabla u = \nabla\cdot(\mathsf{D}\cdot\nabla u) + \Sigma(u)\) |
parabolic, second-order in space, first-order in time |
advection-diffusion-reaction (linear) |
\(\frac{\partial u}{\partial t}+\textbf{a}\cdot\nabla u = \nabla\cdot(\mathsf{D}\cdot\nabla u) + Ru + J\) |
parabolic, second-order in space, first-order in time |
steady advection-diffusion-reaction |
\(\textbf{a}\cdot\nabla u = \nabla\cdot(\mathsf{D}\cdot\nabla u) + Ru + J\) |
parabolic, second-order in space |
steady diffusion-reaction |
\(0 = \nabla\cdot(\mathsf{D}\cdot\nabla u) + Ru + J\) |
parabolic, second-order in space |
steady advection-reaction |
\(\textbf{a}\cdot\nabla u = Ru + J\) |
hyperbolic, first-order in space |
Helmholtz |
\(\nabla\cdot(\mathsf{D}\cdot\nabla u) + k^2 u = f\) |
elliptic, second-order in space |
wave |
\(\frac{\partial^2u}{\partial t^2} = \nabla\cdot(\mathsf{D}\cdot\nabla u)\) |
hyperbolic, second-order in space, second-order in time |
Darcy |
\(\begin{matrix}\nabla\cdot\textbf{u} = 0\\ \textbf{u} = -\frac{\mathsf{K}}{\mu}\cdot(\nabla p - \textbf{f}\,)\end{matrix}\) |
mixed, first-order in space |
Darcy streamfunction |
\(\nabla\cdot\left(\frac{\mu\mathsf{K}^{\mathsf{T}}\cdot\nabla\psi}{\text{det}(\mathsf{K})}\right)=-\frac{\partial(f_y)}{\partial x} + \frac{\partial(f_x)}{\partial y}\) |
elliptic, second-order in space |
Darcy pressure |
\(\nabla\cdot\left(\frac{\mathsf{K}}{\mu}\cdot\nabla p\right)=\nabla\cdot\left(\frac{\mathsf{K}}{\mu}\cdot\textbf{f}\right)\) |
elliptic, second-order in space |
Stokes |
\(\begin{matrix}\nabla\cdot\textbf{u} = 0\\ \textbf{0}=-\nabla p + \nabla\cdot\tau + \textbf{f}\end{matrix}\) |
mixed, second-order in space |
Navier-Stokes |
\(\begin{matrix}\nabla\cdot\textbf{u} = 0\\ \rho \left(\frac{\partial\textbf{u}}{\partial t}+\textbf{u}\cdot\nabla\textbf{u}\right)=-\nabla p + \nabla\cdot\tau + \textbf{f}\end{matrix}\) |
mixed, second-order in space, first-order in time |