Rheolef
7.2
an efficient C++ finite element environment
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The class characteristic implements the Lagrange-Galerkin method. It is the extension of the method of characteristic from the finite difference to the finite element context.
Note that the Lagrange-Galerkin method applies to diffusion-convection problems when the convection term is not dominant. For more serious problems, please refer to the discontinuous Galerkin method in the Rheolef library.
Consider the bilinear form lh
defined by
/ | lh(x) = | uh(x+dh(x)) v(x) dx | / Omega
where dh
is a deformation vector field. The characteristic is defined by X(x)=x+dh(x)
for any x in Omega, and the previous integral writes equivalently:
/ | lh(x) = | uh(X(x)) v(x) dx | / Omega
For instance, in Lagrange-Galerkin methods, the deformation field dh(x)=-dt*uh(x)
where uh
is the advection field and dt
a time step. The following code implements the computation of lh
:
field dh = ...; field uh = ...; characteristic X (dh); test v (Xh); field lh = integrate (compose(uh, X)*v, qopt);
The Gauss-Lobatto quadrature formula is recommended for the computation of integrals involving the characteristic X
of the Lagrange-Galerkin method. The order equal to the polynomial order of Xh
(order 1: trapeze, order 2: simpson, etc). Recall that this choice of quadrature formula guaranties inconditionnal stability at any polynomial order. Alternative quadrature formulae or order can be used by using the additional integrate_option
argument to the integrate
function.
This documentation has been generated from file main/lib/characteristic.h
The characteristic
class is simply an alias to the characteristic_basic
class
The characteristic_basic
class provides an interface, via the smart_pointer
class family, to a data container: