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| Rusanov (const Rusanov &)=default |
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Rusanov & | operator= (const Rusanov &)=default |
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| Rusanov (Rusanov &&)=default |
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Rusanov & | operator= (Rusanov &&)=default |
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void | pup (PUP::er &p) override |
| std::unique_ptr< BoundaryCorrection > | get_clone () const override |
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double | dg_package_data (gsl::not_null< Scalar< DataVector > * > packaged_mass_density, gsl::not_null< tnsr::I< DataVector, Dim, Frame::Inertial > * > packaged_momentum_density, gsl::not_null< Scalar< DataVector > * > packaged_energy_density, gsl::not_null< Scalar< DataVector > * > packaged_normal_dot_flux_mass_density, gsl::not_null< tnsr::I< DataVector, Dim, Frame::Inertial > * > packaged_normal_dot_flux_momentum_density, gsl::not_null< Scalar< DataVector > * > packaged_normal_dot_flux_energy_density, gsl::not_null< Scalar< DataVector > * > packaged_abs_char_speed, const Scalar< DataVector > &mass_density, const tnsr::I< DataVector, Dim, Frame::Inertial > &momentum_density, const Scalar< DataVector > &energy_density, const tnsr::I< DataVector, Dim, Frame::Inertial > &flux_mass_density, const tnsr::IJ< DataVector, Dim, Frame::Inertial > &flux_momentum_density, const tnsr::I< DataVector, Dim, Frame::Inertial > &flux_energy_density, const tnsr::I< DataVector, Dim, Frame::Inertial > &velocity, const Scalar< DataVector > &specific_internal_energy, const tnsr::i< DataVector, Dim, Frame::Inertial > &normal_covector, const std::optional< tnsr::I< DataVector, Dim, Frame::Inertial > > &, const std::optional< Scalar< DataVector > > &normal_dot_mesh_velocity, const EquationsOfState::EquationOfState< false, 2 > &equation_of_state) const |
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void | dg_boundary_terms (gsl::not_null< Scalar< DataVector > * > boundary_correction_mass_density, gsl::not_null< tnsr::I< DataVector, Dim, Frame::Inertial > * > boundary_correction_momentum_density, gsl::not_null< Scalar< DataVector > * > boundary_correction_energy_density, const Scalar< DataVector > &mass_density_int, const tnsr::I< DataVector, Dim, Frame::Inertial > &momentum_density_int, const Scalar< DataVector > &energy_density_int, const Scalar< DataVector > &normal_dot_flux_mass_density_int, const tnsr::I< DataVector, Dim, Frame::Inertial > &normal_dot_flux_momentum_density_int, const Scalar< DataVector > &normal_dot_flux_energy_density_int, const Scalar< DataVector > &abs_char_speed_int, const Scalar< DataVector > &mass_density_ext, const tnsr::I< DataVector, Dim, Frame::Inertial > &momentum_density_ext, const Scalar< DataVector > &energy_density_ext, const Scalar< DataVector > &normal_dot_flux_mass_density_ext, const tnsr::I< DataVector, Dim, Frame::Inertial > &normal_dot_flux_momentum_density_ext, const Scalar< DataVector > &normal_dot_flux_energy_density_ext, const Scalar< DataVector > &abs_char_speed_ext, dg::Formulation dg_formulation) const |
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| BoundaryCorrection (const BoundaryCorrection &)=default |
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BoundaryCorrection & | operator= (const BoundaryCorrection &)=default |
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| BoundaryCorrection (BoundaryCorrection &&)=default |
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BoundaryCorrection & | operator= (BoundaryCorrection &&)=default |
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| BoundaryCorrection (CkMigrateMessage *msg) |
template<size_t Dim>
class NewtonianEuler::BoundaryCorrections::Rusanov< Dim >
A Rusanov/local Lax-Friedrichs Riemann solver.
Let \(U\) be the state vector of evolved variables, \(F^i\) the corresponding fluxes, and \(n_i\) be the outward directed unit normal to the interface. Denoting \(F := n_i F^i\), the Rusanov boundary correction is
\begin{align*}G_\text{Rusanov} = \frac{F_\text{int} - F_\text{ext}}{2} -
\frac{\text{max}\left(\{|\lambda_\text{int}|\},
\{|\lambda_\text{ext}|\}\right)}{2} \left(U_\text{ext} - U_\text{int}\right),
\end{align*}
where "int" and "ext" stand for interior and exterior, and \(\{|\lambda|\}\) is the set of characteristic/signal speeds. The minus sign in front of the \(F_{\text{ext}}\) is necessary because the outward directed normal of the neighboring element has the opposite sign, i.e. \(n_i^{\text{ext}}=-n_i^{\text{int}}\). The characteristic/signal speeds are given by:
\begin{align*}\lambda_{\pm}&=v^i n_i \pm c_s, \\
\lambda_v&=v^i n_i
\end{align*}
where \(v^i\) is the spatial velocity and \(c_s\) the sound speed.
- Note
- In the strong form the dg_boundary_terms function returns \(G - F_\text{int}\)