| /honee/qfunctions/ |
| H A D | utils.h | 14 CEED_QFUNCTION_HELPER CeedScalar Max(CeedScalar a, CeedScalar b) { return a < b ? b : a; } in Max() argument
15 CEED_QFUNCTION_HELPER CeedScalar Min(CeedScalar a, CeedScalar b) { return a < b ? a : b; } in Min() argument
17 CEED_QFUNCTION_HELPER void SwapScalar(CeedScalar *a, CeedScalar *b) { in SwapScalar() argument
19 *a = *b; in SwapScalar()
20 *b = temp; in SwapScalar()
82 CeedScalar *b) { in MatVecNM() argument
85 CeedPragmaSIMD for (CeedInt i = 0; i < N; i++) b[i] += DotN(&A[i * M], x, M); in MatVecNM()
88 …CeedInt i = 0; i < M; i++) { CeedPragmaSIMD for (CeedInt j = 0; j < N; j++) b[i] += A[j * M + i] *… in MatVecNM()
94 … CeedScalar A[3][3], const CeedScalar x[3], const CeedTransposeMode transpose_A, CeedScalar b[3]) { in MatVec3()
95 MatVecNM((const CeedScalar *)A, (const CeedScalar *)x, 3, 3, transpose_A, (CeedScalar *)b); in MatVec3()
[all …]
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| H A D | newtonian_state.h | 273 …ive StateConservativeAXPBYPCZ(CeedScalar a, StateConservative X, CeedScalar b, StateConservative Y… in StateConservativeAXPBYPCZ() argument
276 R.density = a * X.density + b * Y.density + c * Z.density; in StateConservativeAXPBYPCZ()
277 …for (int i = 0; i < 3; i++) R.momentum[i] = a * X.momentum[i] + b * Y.momentum[i] + c * Z.momentum… in StateConservativeAXPBYPCZ()
278 R.E_total = a * X.E_total + b * Y.E_total + c * Z.E_total; in StateConservativeAXPBYPCZ()
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| /honee/problems/ |
| H A D | gaussianwave.c | 45 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_GAUSSIAN_WAVE() local
46 BCDefinition bc_def = problem->bc_defs[b]; in NS_GAUSSIAN_WAVE()
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| H A D | stg_shur14.c | 310 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in SetupStg() local
311 BCDefinition bc_def = problem->bc_defs[b]; in SetupStg()
357 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in SetupStrongStg() local
358 BCDefinition bc_def = problem->bc_defs[b]; in SetupStrongStg()
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| H A D | eulervortex.c | 157 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_EULER_VORTEX() local
158 BCDefinition bc_def = problem->bc_defs[b]; in NS_EULER_VORTEX()
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| H A D | channel.c | 112 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_CHANNEL() local
113 BCDefinition bc_def = problem->bc_defs[b]; in NS_CHANNEL()
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| H A D | blasius.c | 227 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_BLASIUS() local
228 BCDefinition bc_def = problem->bc_defs[b]; in NS_BLASIUS()
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| H A D | advection.c | 597 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_ADVECTION() local
598 BCDefinition bc_def = problem->bc_defs[b]; in NS_ADVECTION()
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| H A D | newtonian.c | 611 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in NS_NEWTONIAN_IG() local
612 BCDefinition bc_def = problem->bc_defs[b]; in NS_NEWTONIAN_IG()
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| /honee/src/ |
| H A D | setuplibceed.c | 254 …for (PetscCount b = 0; b < problem->num_bc_defs; b++) PetscCall(BCDefinitionAddOperators(problem->… in SetupLibceed() local
275 …for (PetscCount b = 0; b < problem->num_bc_defs; b++) PetscCall(BCDefinitionAddOperators(problem->… in SetupLibceed() local
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| H A D | strong_boundary_conditions.c | 62 for (PetscCount b = 0; b < problem->num_bc_defs; b++) { in SetupStrongSTG_Ceed() local
63 BCDefinition bc_def_ = problem->bc_defs[b]; in SetupStrongSTG_Ceed()
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| H A D | dm-utils.c | 294 …ormTensorQuadrature(PetscInt dim, PetscInt num_comp, PetscInt num_points, PetscReal a, PetscReal b, in PetscDTUniformTensorQuadrature() argument
317 PetscReal step = (b - a) / num_points; in PetscDTUniformTensorQuadrature()
327 PetscReal step = (b - a) / num_points; in PetscDTUniformTensorQuadrature()
342 PetscReal step = (b - a) / num_points; in PetscDTUniformTensorQuadrature()
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| /honee/ |
| H A D | CONTRIBUTING.md | 39 (b) The contribution is based upon previous work that, to the best of my knowledge, is covered unde…
41 (c) The contribution was provided directly to me by some other person who certified (a), (b) or (c)…
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| H A D | LICENSE-APACHE | 97 (b) You must cause any modified files to carry prominent notices
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| /honee/doc/ |
| H A D | theory.md | 14 …ot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm{I}_3 -\bm\sigma \right) - \rho \bm{b} &= 0 \\
15 …+ P)\bm{U}}{\rho} -\bm{u} \cdot \bm{\sigma} - k \nabla T \right) - \rho \bm{b} \cdot \bm{u} &= 0 \…
20 …ntial energy), $\bm{I}_3$ represents the $3 \times 3$ identity matrix, $\bm{b}$ is a body force ve…
68 \rho \bm{b}\\
69 \rho \bm{b}\cdot \bm{u}
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