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ryujin 2.1.1 revision ee5cbcbf2346c1299c942d0e1f13b46449973c18
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#include <source/euler_aeos/hyperbolic_system.h>
Public Member Functions | |
Constructor and setup | |
| HyperbolicSystemView (const HyperbolicSystem &hyperbolic_system) | |
Access to runtime parameters | |
| DEAL_II_ALWAYS_INLINE const std::string & | equation_of_state () const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | reference_density () const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | vacuum_state_relaxation_small () const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | vacuum_state_relaxation_large () const |
| DEAL_II_ALWAYS_INLINE bool | compute_strict_bounds () const |
Low-level access to the selected equation of state | |
| DEAL_II_ALWAYS_INLINE Number | eos_pressure (const Number &rho, const Number &e) const |
| DEAL_II_ALWAYS_INLINE Number | eos_specific_internal_energy (const Number &rho, const Number &p) const |
| DEAL_II_ALWAYS_INLINE Number | eos_specific_entropy (const Number &rho, const Number &e) const |
| DEAL_II_ALWAYS_INLINE Number | eos_cold_curve_bound (const Number &rho) const |
| DEAL_II_ALWAYS_INLINE Number | eos_temperature (const Number &rho, const Number &e) const |
| DEAL_II_ALWAYS_INLINE Number | eos_speed_of_sound (const Number &rho, const Number &e) const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | eos_covolume_constant () const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | eos_interpolation_pinfty () const |
| DEAL_II_ALWAYS_INLINE ScalarNumber | eos_interpolation_q () const |
Surrogate functions for computing various interpolatory | |
physical quantities that are needed for Riemann solver, indicator and limiter. | |
| Number | surrogate_specific_entropy (const state_type &U, const Number &gamma_min) const |
| Number | surrogate_harten_entropy (const state_type &U, const Number &gamma_min) const |
| state_type | surrogate_harten_entropy_derivative (const state_type &U, const Number &eta, const Number &gamma_min) const |
| Number | surrogate_gamma (const state_type &U, const Number &p) const |
| Number | surrogate_pressure (const state_type &U, const Number &gamma) const |
| Number | surrogate_speed_of_sound (const state_type &U, const Number &gamma) const |
| bool | is_admissible (const state_type &U) const |
Special functions for boundary states | |
| template<int component> | |
| state_type | prescribe_riemann_characteristic (const state_type &U, const Number &p, const state_type &U_bar, const Number &p_bar, const dealii::Tensor< 1, dim, Number > &normal) const |
| template<typename Lambda > | |
| state_type | apply_boundary_conditions (const dealii::types::boundary_id id, const state_type &U, const dealii::Tensor< 1, dim, Number > &normal, const Lambda &get_dirichlet_data) const |
State transformations | |
| template<typename ST > | |
| state_type | expand_state (const ST &state) const |
| template<typename ST > | |
| state_type | from_initial_state (const ST &initial_state) const |
| state_type | from_primitive_state (const state_type &primitive_state) const |
| state_type | to_primitive_state (const state_type &state) const |
| template<typename Lambda > | |
| state_type | apply_galilei_transform (const state_type &state, const Lambda &lambda) const |
Static Public Attributes | |
Constexpr booleans used in the EulerInitialStates namespace | |
| static constexpr bool | have_gamma = false |
| static constexpr bool | have_covolume_constant = true |
| static constexpr bool | have_energy_equation = true |
Flux computations | |
| static constexpr bool | have_high_order_flux = false |
| flux_type | f (const state_type &U, const Number &p) const |
| flux_contribution_type | flux_contribution (const PrecomputedVectorView &pv, const InitialPrecomputedVectorView &piv, const unsigned int i, const state_type &U_i) const |
| flux_contribution_type | flux_contribution (const PrecomputedVectorView &pv, const InitialPrecomputedVectorView &piv, const unsigned int *js, const state_type &U_j) const |
| state_type | flux_divergence (const flux_contribution_type &flux_i, const flux_contribution_type &flux_j, const dealii::Tensor< 1, dim, Number > &c_ij) const |
| state_type | high_order_flux_divergence (const flux_contribution_type &flux_i, const flux_contribution_type &flux_j, const dealii::Tensor< 1, dim, Number > &c_ij) const =delete |
Computing stencil source terms | |
| static constexpr bool | have_source_terms = false |
| state_type | nodal_source (const PrecomputedVectorView &pv, const unsigned int i, const state_type &U_i, const ScalarNumber tau) const =delete |
| state_type | nodal_source (const PrecomputedVectorView &pv, const unsigned int *js, const state_type &U_j, const ScalarNumber tau) const =delete |
Computing derived physical quantities | |
| Number | filter_vacuum_density (const Number &rho) const |
| static Number | density (const state_type &U) |
| static dealii::Tensor< 1, dim, Number > | momentum (const state_type &U) |
| static Number | total_energy (const state_type &U) |
| static Number | internal_energy (const state_type &U) |
| static state_type | internal_energy_derivative (const state_type &U) |
A view of the HyperbolicSystem that makes methods available for a given dimension dim and choice of number type Number (which can be a scalar float, or double, as well as a VectorizedArray holding packed scalars.
Intended usage:
Definition at line 164 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::ScalarNumber = typename get_value_type<Number>::type |
The underlying scalar number type.
Definition at line 175 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::state_type = dealii::Tensor<1, problem_dimension, Number> |
Storage type for a (conserved) state vector \(\boldsymbol U\).
Definition at line 185 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::flux_type = dealii::Tensor<1, problem_dimension, dealii::Tensor<1, dim, Number> > |
Storage type for the flux \(\mathbf{f}\).
Definition at line 190 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::flux_contribution_type = flux_type |
The storage type used for flux contributions.
Definition at line 196 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::precomputed_type = std::array<Number, n_precomputed_values> |
Array type used for precomputed values.
Definition at line 236 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::initial_precomputed_type = std::array<Number, n_initial_precomputed_values> |
Array type used for precomputed initial values.
Definition at line 256 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::StateVector = Vectors:: StateVector<ScalarNumber, problem_dimension, n_precomputed_values> |
A compound state vector.
Definition at line 268 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::HyperbolicVector = Vectors::MultiComponentVector<ScalarNumber, problem_dimension> |
MulticomponentVector for storing the hyperbolic state vector:
Definition at line 274 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::PrecomputedVector = Vectors::MultiComponentVector<ScalarNumber, n_precomputed_values> |
MulticomponentVector for storing a vector of precomputed states:
Definition at line 280 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::PrecomputedVectorView = Vectors::MultiComponentVectorView< ScalarNumber, n_precomputed_values, dealii::VectorizedArray<ScalarNumber>::size(), dealii::MemorySpace::Host, false> |
MulticomponentVectorView for accessing a vector of precomputed states:
Definition at line 287 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::InitialPrecomputedVector = Vectors::MultiComponentVector<ScalarNumber, n_initial_precomputed_values> |
MulticomponentVector for storing a vector of precomputed initial states:
Definition at line 298 of file hyperbolic_system.h.
| using ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::InitialPrecomputedVectorView = Vectors::MultiComponentVectorView< ScalarNumber, n_initial_precomputed_values, dealii::VectorizedArray<ScalarNumber>::size(), dealii::MemorySpace::Host, false> |
MulticomponentVectorView for accessing a vector of precomputed initial states:
Definition at line 306 of file hyperbolic_system.h.
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Constructor taking a reference to the underlying HyperbolicSystem
Definition at line 323 of file hyperbolic_system.h.
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Definition at line 334 of file hyperbolic_system.h.
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Definition at line 339 of file hyperbolic_system.h.
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Definition at line 345 of file hyperbolic_system.h.
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Definition at line 351 of file hyperbolic_system.h.
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Definition at line 356 of file hyperbolic_system.h.
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For a given density \(\rho\) and specific internal energy \(e\) return the pressure \(p\).
Definition at line 371 of file hyperbolic_system.h.
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For a given density \(\rho\) and pressure \(p\) return the specific internal energy \(e\).
Definition at line 392 of file hyperbolic_system.h.
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For a given density \(\rho\) and specific internal energy \(e\) return the specific entropy \(s\).
Definition at line 412 of file hyperbolic_system.h.
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For a given density \(\rho\) return the cold curve bound \(e\ge e_{s_0}(\rho)\).
Definition at line 432 of file hyperbolic_system.h.
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For a given density \(\rho\) and specific internal energy \(e\) return the temperature \(T\).
Definition at line 451 of file hyperbolic_system.h.
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For a given density \(\rho\) and specific internal energy \(e\) return the sound speed \(a\).
Definition at line 472 of file hyperbolic_system.h.
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Return the interpolatory covolume \(b_{\text{interp}}\).
Definition at line 490 of file hyperbolic_system.h.
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Return the interpolatory reference pressure \(p_{\infty}\).
Definition at line 499 of file hyperbolic_system.h.
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Return the interpolatory reference specific internal energy \(q\).
Definition at line 509 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, return the density U[0]
Definition at line 1029 of file hyperbolic_system.h.
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Given a density rho this function returns 0 if the magniatude of rho is smaller or equal than relaxation_large * rho_cutoff. Otherwise rho is returned unmodified. Here, rho_cutoff is the reference density multiplied by eps.
Definition at line 1037 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, return the momentum vector [U[1], ..., U[1+dim]].
Definition at line 1051 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, return the total energy U[1+dim]
Definition at line 1062 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, compute and return the internal energy \(\varepsilon = (\rho e)\).
Definition at line 1070 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, compute and return the derivative of the internal energy \(\varepsilon = (\rho e)\).
Definition at line 1084 of file hyperbolic_system.h.
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For a given (2+dim dimensional) state vector U, compute and return a (scaled) surrogate specific entropy
\[ e^{(\gamma_{\text{min}} - 1)s} = \frac{\rho\,(e-q)-p_{\infty}(1-b\rho)}{\rho^\gamma_{\text{min}}} (1 - b\,\rho)^{\gamma_{\text{min}} -1}. \]
Definition at line 1111 of file hyperbolic_system.h.
References ryujin::pow().
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For a given (2+dim dimensional) state vector U, compute and return a surrogate Harten-type entropy
\[ \eta = (1-b\,\rho)^{\frac{\gamma_{\text{min}-1}}{\gamma_{\text{min}}+1}} \big(\rho^2 (e-q) - \rho p_{\infty}(1-b\,\rho)\big) ^{1/(\gamma_{\text{min}}+1)} \]
Definition at line 1131 of file hyperbolic_system.h.
References ryujin::positive_part(), and ryujin::pow().
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For a given (2+dim dimensional) state vector U, compute and return the derivative \(\eta'\) of the Harten-type entropy
\[ \eta = (1-b\,\rho)^{\frac{\gamma_{\text{min}-1}}{\gamma_{\text{min}}+1}} \big(\rho^2 (e-q) - \rho p_{\infty}(1-b\,\rho)\big) ^{1/(\gamma_{\text{min}}+1)} \]
Definition at line 1158 of file hyperbolic_system.h.
References ryujin::pow(), and ryujin::EulerAEOS::safe_division().
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For a given (2+dim dimensional) state vector U and pressure p, compute a surrogate gamma:
\[ \gamma(\rho, e, p) = 1 + \frac{(p + p_{\infty})(1 - b \rho)} {\rho (e-q) - p_{\infty}(1-b \rho)} \]
This function is used in various places to create interpolations of the pressure.
Definition at line 1214 of file hyperbolic_system.h.
References ryujin::EulerAEOS::safe_division().
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For a given (2+dim dimensional) state vector U and gamma gamma, compute a surrogate pressure:
\[ p(\rho, e, \gamma) = (\gamma - 1) \frac{\rho (e - q)}{1 - b \rho} -\gamma\,p_{\infty} \]
This function is the complementary function to surrogate_gamma(), meaning the following property holds true:
Definition at line 1233 of file hyperbolic_system.h.
References ryujin::positive_part(), and ryujin::EulerAEOS::safe_division().
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For a given (2+dim dimensional) state vector U and gamma gamma, compute a surrogate speed of sound:
\begin{align} c^2(\rho, e, \gamma) = \frac{\gamma (p + p_\infty)}{\rho X} = \frac{\gamma (\gamma -1)[\rho (e - q) - p_\infty X]}{\rho X^2} \end{align}
Definition at line 1252 of file hyperbolic_system.h.
References ryujin::positive_part().
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Returns whether the state U is admissible. If U is a vectorized state then U is admissible if all vectorized values are admissible.
Definition at line 1272 of file hyperbolic_system.h.
| state_type ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::prescribe_riemann_characteristic | ( | const state_type & | U, |
| const Number & | p, | ||
| const state_type & | U_bar, | ||
| const Number & | p_bar, | ||
| const dealii::Tensor< 1, dim, Number > & | normal | ||
| ) | const |
Decomposes a given state U into Riemann invariants and then replaces the first or second Riemann characteristic from the one taken from U_bar state. Note that the U_bar state is just the prescribed dirichlet values.
| state_type ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::apply_boundary_conditions | ( | const dealii::types::boundary_id | id, |
| const state_type & | U, | ||
| const dealii::Tensor< 1, dim, Number > & | normal, | ||
| const Lambda & | get_dirichlet_data | ||
| ) | const |
Apply boundary conditions.
For the compressible Euler equations we have:
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Given a state U and a pressure p compute the flux
\[ \begin{pmatrix} \textbf m \\ \textbf v\otimes \textbf m + p\mathbb{I}_d \\ \textbf v(E+p) \end{pmatrix}, \]
Definition at line 1577 of file hyperbolic_system.h.
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Given a state U_i and an index i compute flux contributions.
Intended usage:
For the Euler equations we simply compute f(U_i).
Definition at line 1599 of file hyperbolic_system.h.
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Definition at line 1613 of file hyperbolic_system.h.
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Given flux contributions flux_i and flux_j compute the flux (-f(U_i) - f(U_j)
Definition at line 1627 of file hyperbolic_system.h.
References ryujin::add(), and ryujin::contract().
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| state_type ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::expand_state | ( | const ST & | state | ) | const |
Given a state vector associated with a different spatial dimensions than the current one, return an "expanded" version of the state vector associated with dim spatial dimensions where the momentum vector of the conserved state state is expaned with zeros to a total length of dim entries.
| state_type ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::from_initial_state | ( | const ST & | initial_state | ) | const |
Given an initial state [rho, u_1, ..., u_d, p] return a conserved state [rho, m_1, ..., m_d, E]. Most notably, the specific equation of state oracle is queried to convert the pressure value into a specific internal energy.
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Given a primitive state [rho, u_1, ..., u_d, e] return a conserved state.
Definition at line 1679 of file hyperbolic_system.h.
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Given a conserved state return a primitive state [rho, u_1, ..., u_d, e]
Definition at line 1702 of file hyperbolic_system.h.
| state_type ryujin::EulerAEOS::HyperbolicSystemView< dim, Number >::apply_galilei_transform | ( | const state_type & | state, |
| const Lambda & | lambda | ||
| ) | const |
Transform the current state according to a given operator lambda acting on a dim dimensional momentum (or velocity) vector.
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The dimension of the state space.
Definition at line 180 of file hyperbolic_system.h.
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An array holding all component names of the conserved state as a string.
Definition at line 202 of file hyperbolic_system.h.
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An array holding all component names of the primitive state as a string.
Definition at line 217 of file hyperbolic_system.h.
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The number of precomputed values.
Definition at line 231 of file hyperbolic_system.h.
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An array holding all component names of the precomputed values.
Definition at line 241 of file hyperbolic_system.h.
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The number of precomputed initial values.
Definition at line 251 of file hyperbolic_system.h.
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An array holding all component names of the precomputed values.
Definition at line 262 of file hyperbolic_system.h.
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Definition at line 521 of file hyperbolic_system.h.
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Definition at line 522 of file hyperbolic_system.h.
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Definition at line 523 of file hyperbolic_system.h.
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The low-order and high-order fluxes are the same:
Definition at line 772 of file hyperbolic_system.h.
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We do not have source terms
Definition at line 786 of file hyperbolic_system.h.