| /honee/qfunctions/ |
| H A D | blasius.h | 70 CeedScalar mu = blasius->newt_ctx.gas.mu; in BlasiusSolution() local
72 CeedScalar nu = mu / rho_infty; in BlasiusSolution()
82 *t12 = mu * U_infty * f[2] * sqrt(U_infty / (nu * (x0 + x[0] - x_inflow))); in BlasiusSolution()
102 const CeedScalar mu = context->newt_ctx.gas.mu; in ICsBlasius() local
110 const CeedScalar x0 = U_infty * S_infty.U.density / (mu * 25 / Square(delta0)); in ICsBlasius()
136 …const CeedScalar x0 = U_infty * rho_0 / (gas.mu * 25 / Square(context->delta0)… in Blasius_Inflow()
191 …const CeedScalar x0 = U_infty * rho_0 / (gas.mu * 25 / Square(context->delta0)… in Blasius_Inflow_Jacobian()
|
| H A D | monitor_totalkineticenergy.h | 30 v[1][i] = wdetJ * -2 * gas.mu * DotN((CeedScalar *)strain_rate, (CeedScalar *)strain_rate, 9); in MonitorTotalKineticEnergy()
31 v[2][i] = wdetJ * -gas.lambda * gas.mu * Square(div_u); in MonitorTotalKineticEnergy()
35 v[4][i] = wdetJ * gas.mu * Dot3(vorticity, vorticity); in MonitorTotalKineticEnergy()
|
| H A D | stabilization.h | 75 const CeedScalar mu = gas.mu; in Tau_diagPrim() local
93 …tau = Square(rho) * (4. * Square(dts) + velocity_term) + Ctau_v * Square(mu) * DotN((CeedScalar *)… in Tau_diagPrim()
|
| H A D | stg_shur14.h | 250 const CeedScalar mu = stg_ctx->newt_ctx.gas.mu; in StgShur14Preprocess() local
255 const CeedScalar nu = mu / rho; in StgShur14Preprocess()
297 const CeedScalar nu = gas.mu / rho; in ICsStg()
347 const CeedScalar mu = gas.mu; in StgShur14Inflow() local
369 CalcSpectrum(X[1][i], eps, lt, h_node_sep, mu / rho, qn, stg_ctx); in StgShur14Inflow()
488 const CeedScalar nu = gas.mu / rho; in StgShur14InflowStrongQF()
|
| H A D | channel.h | 33 const CeedScalar mu = gas.mu; in Exact_Channel() local
42 const CeedScalar Pr = mu / (cp * k); in Exact_Channel()
|
| H A D | newtonian_types.h | 22 CeedScalar mu; member
|
| H A D | sgs_dd_training.h | 48 …ComputeSgsDDInputs(grad_velo_aniso, km_A_ij, delta, gas.mu / s.U.density, eigenvectors, inputs, &g… in ComputeSGS_DDAnisotropicTrainingDataNodal()
|
| H A D | sgs_dd_model.h | 90 ComputeSgsDD_Fused(grad_velo_aniso, km_A_ij, delta, gas.mu / s.U.density, km_sgs, sgsdd_ctx); in ComputeSgsDDNodal_Fused()
134 …ComputeSgsDDInputs(grad_velo_aniso, km_A_ij, delta, gas.mu / s.U.density, eigenvectors, model_inpu… in ComputeSgsDDNodal_Sequential_Inputs()
|
| H A D | newtonian_state.h | 46 CEED_QFUNCTION_HELPER CeedScalar Prandtl(NewtonianIGProperties gas) { return gas.cp * gas.mu / gas.… in Prandtl()
556 stress[i] = gas.mu * (2 * strain_rate[i] + gas.lambda * div_u * (i < 3)); in NewtonianStress()
|
| /honee/problems/ |
| H A D | newtonian.c | 394 .mu = 1.8e-5, in NS_NEWTONIAN_IG()
421 …r dynamic viscosity coefficient", NULL, newtonian_ig_ctx->gas.mu, &newtonian_ig_ctx->gas.mu, NULL)… in NS_NEWTONIAN_IG()
479 newtonian_ig_ctx->gas.mu *= units->Pascal * units->second; in NS_NEWTONIAN_IG()
|
| H A D | channel.c | 92 channel_ctx->B = body_force_scale * 2 * umax * newtonian_ig_ctx->gas.mu / (H * H); in NS_CHANNEL()
|
| /honee/src/spanstats/ |
| H A D | cflpe.c | 95 collect_ctx->diffusion_coeff = newtonian_ig_ctx->gas.mu; in CreateStatisticCollectionOperator()
|
| /honee/doc/ |
| H A D | theory.md | 19 …{\sigma} = \mu(\nabla \bm{u} + (\nabla \bm{u})^T + \lambda (\nabla \cdot \bm{u})\bm{I}_3)$ is the …
281 + C_v \mu^2 \Vert \bm g \Vert_F ^2}
|
| H A D | runtime_options.md | 468 * - `-mu`
|
| H A D | examples.md | 177 … 2000,125,1000 -dm_plex_dim 3 -rc 400. -bc_wall 1,2,5,6 -wall_comps 1,2,3 -bc_symmetry_y 3,4 -mu 75
189 …$ is the center velocity, $T_w$ is the temperature at the wall, $Pr=\frac{\mu}{c_p \kappa}$ is the…
|