Introduction
A lot of PDE(s) can be writen in a generic form, and depends mainly on the definition of coefficients. The generic form that we use is describe by the next equation :
with \(u\) the unknown and \(\Omega \in \mathbb{R}^n\) the computation domain . We call this generic form by Coefficient Form PDE and the coefficients are
-
\(d\) : damping or mass coefficient
-
\(c\) : diffusion coefficient
-
\(\alpha\) : conservative flux convection coefficient
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\(\gamma\) : conservative flux source term
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\(\beta\) : convection coefficient
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\(a\) : absorption or reaction coefficient
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\(f\) : source term
Many problems are multiphysics (i.e. several unknowns) and the generic form can be extended naturally into a system of generic PDE.
Coefficients of each equation can be defined by an expression that depends of the current unknown or unknowns of other equations. |
The unknown of each PDEs can be defined as a scalar function (\(u:\mathbb{R}^n \longrightarrow \mathbb{R}\)) or a vectorial function (\(u:\mathbb{R}^n \longrightarrow \mathbb{R}^n\)). We need also to respect some constraint on the coefficient shape as described in the next table.
Coefficient | Scalar Unknown | Vectorial Unknown |
---|---|---|
\(d\) |
scalar |
scalar |
\(c\) |
scalar or matrix |
scalar or matrix |
\(\alpha\) |
vectorial |
x |
\(\gamma\) |
vectorial |
x |
\(\beta\) |
vectorial |
vectorial |
\(a\) |
scalar |
scalar |
\(f\) |
scalar |
vectorial |
2. Boundary Conditions
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Dirichlet :
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Neumann : generic version which can depend on the unknowns
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Robin :
5. Stabilized finite element
Given a cfpdes
equation named eq
, SUPG and GaLS can be used as stabilisation methods.
To enable them use, in the command-line or .cfg
file, the option cfpdes.eq.stabilitsation=1
and define the stabilisation type cfpdes.eq.stabilitsation.type=gls #supg#unusual-gls #gls
type | |
---|---|
|
default option |
|
|
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Examples are available here