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/libCEED/examples/solids/problems/
H A Dneo-hookean.c68 units->second = 1; // 1 second in scaled time units in ProcessPhysics_NH()
82 …alar("-units_second", "1 second in scaled time units", NULL, units->second, &units->second, NULL)); in ProcessPhysics_NH()
83 units->second = fabs(units->second); in ProcessPhysics_NH()
99 units->Pascal = units->kilogram / (units->meter * PetscSqr(units->second)); in ProcessPhysics_NH()
H A Dmooney-rivlin.c71 units->second = 1; // 1 second in scaled time units in ProcessPhysics_MR()
91 …alar("-units_second", "1 second in scaled time units", NULL, units->second, &units->second, NULL)); in ProcessPhysics_MR()
92 units->second = fabs(units->second); in ProcessPhysics_MR()
100 units->Pascal = units->kilogram / (units->meter * PetscSqr(units->second)); in ProcessPhysics_MR()
/libCEED/examples/fluids/problems/
H A Dshocktube.c69 PetscScalar second = 1e-2; // 1 second in scaled time units in NS_SHOCKTUBE() local
85 …PetscOptionsScalar("-units_second", "1 second in scaled time units", NULL, second, &second, NULL)); in NS_SHOCKTUBE()
86 second = fabs(second); in NS_SHOCKTUBE()
102 user->units->second = second; in NS_SHOCKTUBE()
H A Deulervortex.c64 PetscScalar second = 1e-2; // 1 second in scaled time units in NS_EULER_VORTEX() local
86 …PetscOptionsScalar("-units_second", "1 second in scaled time units", NULL, second, &second, NULL)); in NS_EULER_VORTEX()
87 second = fabs(second); in NS_EULER_VORTEX()
103 user->units->second = second; in NS_EULER_VORTEX()
112 mean_velocity[i] *= (meter / second); in NS_EULER_VORTEX()
H A Dadvection.c156 PetscScalar second = 1e-2; // 1 second in scaled time units in NS_ADVECTION() local
193 …PetscOptionsScalar("-units_second", "1 second in scaled time units", NULL, second, &second, NULL)); in NS_ADVECTION()
194 second = fabs(second); in NS_ADVECTION()
216 Joule = kilogram * PetscSqr(meter) / PetscSqr(second); in NS_ADVECTION()
220 user->units->second = second; in NS_ADVECTION()
230 wind[i] *= (meter / second); in NS_ADVECTION()
H A Dnewtonian.c112 const CeedScalar kg = units->kilogram, m = units->meter, sec = units->second, K = units->Kelvin; in UnitTests_Newtonian()
268 PetscScalar second = 1; // 1 second in scaled time units in NS_NEWTONIAN_IG() local
354 …PetscOptionsScalar("-units_second", "1 second in scaled time units", NULL, second, &second, NULL)); in NS_NEWTONIAN_IG()
355 second = fabs(second); in NS_NEWTONIAN_IG()
380 Pascal = kilogram / (meter * PetscSqr(second)); in NS_NEWTONIAN_IG()
381 J_per_kg_K = PetscSqr(meter) / (PetscSqr(second) * Kelvin); in NS_NEWTONIAN_IG()
382 m_per_squared_s = meter / PetscSqr(second); in NS_NEWTONIAN_IG()
383 W_per_m_K = kilogram * meter / (pow(second, 3) * Kelvin); in NS_NEWTONIAN_IG()
387 user->units->second = second; in NS_NEWTONIAN_IG()
400 mu *= Pascal * second; in NS_NEWTONIAN_IG()
[all …]
H A Ddensitycurrent.c76 PetscScalar second = user->units->second; in NS_DENSITY_CURRENT() local
83 N *= (1. / second); in NS_DENSITY_CURRENT()
H A Dchannel.c56 PetscScalar second = user->units->second; in NS_CHANNEL() local
62 umax *= meter / second; in NS_CHANNEL()
H A Dblasius.c304 PetscScalar second = user->units->second; in NS_BLASIUS() local
311 U_inf *= meter / second; in NS_BLASIUS()
H A Dbc_freestream.c31 PetscScalar second = user->units->second; in FreestreamBCSetup() local
39 for (int i = 0; i < 3; i++) Y_inf.velocity[i] = reference->velocity[i] * second / meter; in FreestreamBCSetup()
102 for (int i = 0; i < 3; i++) Y_inf.velocity[i] *= meter / second; in FreestreamBCSetup()
/libCEED/examples/fluids/src/
H A Dsetupts.c233 time /= user->units->second; // Dimensionalize time back in WriteOutput()
322 PetscCall(TSSetMaxTime(*ts, 500. * user->units->second)); in TSSolve_NS()
325 PetscCall(TSSetTimeStep(*ts, 1.e-2 * user->units->second)); in TSSolve_NS()
327 PetscCall(TSAdaptSetStepLimits(adapt, 1.e-12 * user->units->second, 1.e2 * user->units->second)); in TSSolve_NS()
355 PetscCall(TSSetTime(*ts, app_ctx->cont_time * user->units->second)); in TSSolve_NS()
366 CeedScalar previous_time = app_ctx->cont_time * user->units->second; in TSSolve_NS()
/libCEED/backends/sycl/
H A Donline_compiler.sycl.cpp188 …on = std::to_string(OutputFormatVersion.first) + ", " + std::to_string(OutputFormatVersion.second); in compile()
199 …on = std::to_string(OutputFormatVersion.first) + ", " + std::to_string(OutputFormatVersion.second); in compile()
/libCEED/julia/LibCEED.jl/docs/src/
H A DMisc.md15 dispatch. An object `D = CeedDim(dim)` can be created, and passed as a second
H A DUserQFunctions.md46 function evaluated at each quadrature point. The second input array is `qdata`,
82 [`Ceed`](@ref) object where the Q-function will be created, and the second
92 the name of the array, and the second entry is either `:in` or `:out`, according
/libCEED/examples/solids/include/
H A Dstructs.h36 PetscScalar second; member
/libCEED/examples/deal.II/
H A Dbps-cpu.h179 for (unsigned cell = range.first; cell < range.second; ++cell) in do_cell_integral_range()
/libCEED/examples/fluids/
H A DREADME.md325 - 1 second in scaled time units
445 - 1 second in scaled time units
489 - 1 second in scaled time units
528 - 1 second in scaled time units
593 - Stokes hypothesis second viscosity coefficient
H A Dnavierstokes.h196 PetscScalar second; member
H A Dindex.md160 …ta t$, so small time steps result in the Jacobian being dominated by the second term, which is a s…
224 …X} = \nabla_{\bm x}\bm X \cdot \bm u$, with units of reference length (non-dimensional) per second.
420 To get second-order statistics from these terms, simply use the identity:
500 It is currently assumed that the second component of the filter width tensor is in the wall-normal …
515 … normal kernel to our differential kernel, we attempt to have them match second order moments with…
/libCEED/examples/solids/
H A Dindex.md16 …gime, while $\bm S$ and $\bm E$ are their finite-strain generalizations (second Piola-Kirchoff ten…
123 For notational convenience, we express the symmetric second order tensors $\bm \sigma$ and $\bm \ep…
248 where $\bm S$ is the *second Piola-Kirchhoff stress* tensor, a symmetric tensor defined entirely in…
328 We differentiate $\Phi$ as in the Neo-Hookean case {eq}`neo-hookean-stress` to yield the second Pio…
467 Moving from Neo-Hookean to Mooney-Rivlin modifies the second term and adds the third.
509 … 3$ matrix products as in {eq}`eq-neo-hookean-incremental-stress` or the second line of {eq}`eq-ne…
H A DREADME.md193 - 1 second in scaled time units
/libCEED/doc/sphinx/source/
H A DlibCEEDapi.md257 The second argument is an expected vector length.
H A Dreleasenotes.md459 libCEED v0.4 was made again publicly available in the second full CEED software