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Mallard 0.8.0
Unstructured, GPU accelerated, high-order finite volume CFD solver
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Viscous (diffusive) flux functor for the Navier-Stokes equations. More...
Go to the source code of this file.
Classes | |
| struct | ViscousFluxFunctor |
| Integrates the viscous stress and heat flux over every face (one-point rule) and adds them to face_flux (see ConvectiveFluxFunctor). More... | |
Functions | |
| KOKKOS_INLINE_FUNCTION void | viscous_traction (const rtype mu, const rtype g[][N_DIM], const rtype *n, rtype *tau_n, const rtype hoop_divergence=0.0_r) |
| Viscous traction tau . n of a Newtonian fluid under Stokes' hypothesis, tau = mu (grad u + grad u^T - 2/3 div u I), with g[k][i] = d u_k / d x_i. Axisymmetric flows add the hoop part u_r / r of the divergence. | |
| KOKKOS_INLINE_FUNCTION rtype | hoop_divergence (const rtype r, const rtype *u, const rtype g[][N_DIM]) |
| u_r / r at radius r for velocity u and gradient g (g[k][i] = d u_k / d x_i), with r = y: its limit d u_r / d r on the axis. | |
| KOKKOS_INLINE_FUNCTION rtype | variance_jump (const Kokkos::View< rtype *[3]> &covariance, const int32_t c0, const int32_t c1, const rtype *d) |
| Axisymmetric meshes: jump from cell c0 to c1 of the cells' r-weighted variance along d (Mesh::cell_covariance), divided by |d|^2. | |
| KOKKOS_INLINE_FUNCTION rtype | mean_offset (const rtype *g0, const rtype *g1, const rtype *d, const rtype dvar) |
| Part of the jump of two cell averages that comes from the cells' different spreads (variance jump dvar along d, see variance_jump): an average exceeds the value at the center by q_ss var / 2, with the second derivative q_ss along d from the cell gradients g0, g1. | |
| KOKKOS_INLINE_FUNCTION rtype | face_fraction (const Kokkos::View< rtype *[N_DIM]> &face_coords, const Kokkos::View< rtype *[N_DIM]> &cell_coords, const uint32_t f, const int32_t c0, const rtype *d) |
| Fraction along d (from the center of cell c0 to that of its neighbor) of the projection of face f's center. | |
Viscous (diffusive) flux functor for the Navier-Stokes equations.
| KOKKOS_INLINE_FUNCTION rtype face_fraction | ( | const Kokkos::View< rtype *[N_DIM]> & | face_coords, |
| const Kokkos::View< rtype *[N_DIM]> & | cell_coords, | ||
| const uint32_t | f, | ||
| const int32_t | c0, | ||
| const rtype * | d | ||
| ) |
Fraction along d (from the center of cell c0 to that of its neighbor) of the projection of face f's center.
| KOKKOS_INLINE_FUNCTION rtype hoop_divergence | ( | const rtype | r, |
| const rtype * | u, | ||
| const rtype | g[][N_DIM] | ||
| ) |
u_r / r at radius r for velocity u and gradient g (g[k][i] = d u_k / d x_i), with r = y: its limit d u_r / d r on the axis.
| KOKKOS_INLINE_FUNCTION rtype mean_offset | ( | const rtype * | g0, |
| const rtype * | g1, | ||
| const rtype * | d, | ||
| const rtype | dvar | ||
| ) |
Part of the jump of two cell averages that comes from the cells' different spreads (variance jump dvar along d, see variance_jump): an average exceeds the value at the center by q_ss var / 2, with the second derivative q_ss along d from the cell gradients g0, g1.
| KOKKOS_INLINE_FUNCTION rtype variance_jump | ( | const Kokkos::View< rtype *[3]> & | covariance, |
| const int32_t | c0, | ||
| const int32_t | c1, | ||
| const rtype * | d | ||
| ) |
Axisymmetric meshes: jump from cell c0 to c1 of the cells' r-weighted variance along d (Mesh::cell_covariance), divided by |d|^2.
| KOKKOS_INLINE_FUNCTION void viscous_traction | ( | const rtype | mu, |
| const rtype | g[][N_DIM], | ||
| const rtype * | n, | ||
| rtype * | tau_n, | ||
| const rtype | hoop_divergence = 0.0_r |
||
| ) |
Viscous traction tau . n of a Newtonian fluid under Stokes' hypothesis, tau = mu (grad u + grad u^T - 2/3 div u I), with g[k][i] = d u_k / d x_i. Axisymmetric flows add the hoop part u_r / r of the divergence.