The Navier-Stokes equations with the discontinuous Galerkin method and upwinding – class body.
The Navier-Stokes equations with the discontinuous Galerkin method and upwinding – class body
Float Re1,
const geo& omega,
string approx)
mrh[0] = a*xh[0] +
b.trans_mult(xh[1]) -
lh;
mrh[1] =
b*xh[0] -
c*xh[1] -
kh;
return mrh;
}
trial du (
Xh); test v (
Xh);
}
field lh(Float epsilon, Float t, const test &v)
see the Float page for the full documentation
see the geo page for the full documentation
see the test page for the full documentation
see the test page for the full documentation
form inertia(W w, U u, V v, integrate_option iopt=integrate_option())
The inertia term of the Navier-Stokes equation with the discontinuous Galerkin method – upwinding var...
form d_inertia_upw(field w, trial dw, field u, test v, integrate_option iopt=integrate_option())
form inertia_upw(field w, trial u, test v, integrate_option iopt=integrate_option())
navier_stokes_upw_dg(Float Re, const geo &omega, string approx)
value_type residue(const value_type &uh) const
void update_derivative(const value_type &uh) const
navier_stokes_dg::value_type value_type