| /libCEED/examples/solids/problems/ |
| H A D | neo-hookean.c | 68 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()
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| H A D | mooney-rivlin.c | 71 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()
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| /libCEED/examples/fluids/problems/ |
| H A D | shocktube.c | 69 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()
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| H A D | eulervortex.c | 64 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()
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| H A D | advection.c | 156 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()
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| H A D | newtonian.c | 112 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 …]
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| H A D | densitycurrent.c | 76 PetscScalar second = user->units->second; in NS_DENSITY_CURRENT() local 83 N *= (1. / second); in NS_DENSITY_CURRENT()
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| H A D | channel.c | 56 PetscScalar second = user->units->second; in NS_CHANNEL() local 62 umax *= meter / second; in NS_CHANNEL()
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| H A D | blasius.c | 304 PetscScalar second = user->units->second; in NS_BLASIUS() local 311 U_inf *= meter / second; in NS_BLASIUS()
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| H A D | bc_freestream.c | 31 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()
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| /libCEED/examples/fluids/src/ |
| H A D | setupts.c | 233 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()
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| /libCEED/backends/sycl/ |
| H A D | online_compiler.sycl.cpp | 188 …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()
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| /libCEED/julia/LibCEED.jl/docs/src/ |
| H A D | Misc.md | 15 dispatch. An object `D = CeedDim(dim)` can be created, and passed as a second
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| H A D | UserQFunctions.md | 46 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
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| /libCEED/examples/solids/include/ |
| H A D | structs.h | 36 PetscScalar second; member
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| /libCEED/examples/deal.II/ |
| H A D | bps-cpu.h | 179 for (unsigned cell = range.first; cell < range.second; ++cell) in do_cell_integral_range()
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| /libCEED/examples/fluids/ |
| H A D | README.md | 325 - 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
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| H A D | navierstokes.h | 196 PetscScalar second; member
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| H A D | index.md | 160 …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…
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| /libCEED/examples/solids/ |
| H A D | index.md | 16 …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…
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| H A D | README.md | 193 - 1 second in scaled time units
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| /libCEED/doc/sphinx/source/ |
| H A D | libCEEDapi.md | 257 The second argument is an expected vector length.
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| H A D | releasenotes.md | 459 libCEED v0.4 was made again publicly available in the second full CEED software
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