| /libCEED/examples/fluids/qfunctions/ |
| H A D | blasius.h | 77 CeedScalar mu = blasius->newtonian_ctx.mu; in BlasiusSolution() local
79 CeedScalar nu = mu / rho_infty; in BlasiusSolution()
89 *t12 = mu * U_infty * f[2] * sqrt(U_infty / (nu * (x0 + x[0] - x_inflow))); in BlasiusSolution()
109 const CeedScalar mu = context->newtonian_ctx.mu; in ICsBlasius() local
117 const CeedScalar x0 = U_infty * S_infty.U.density / (mu * 25 / Square(delta0)); in ICsBlasius()
144 …const CeedScalar x0 = U_infty * rho_0 / (gas->mu * 25 / Square(context->del… in Blasius_Inflow()
201 …const CeedScalar x0 = U_infty * rho_0 / (gas->mu * 25 / Square(context->del… in Blasius_Inflow_Jacobian()
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| H A D | stabilization.h | 80 const CeedScalar mu = gas->mu; in Tau_diagPrim() local
98 …tau = Square(rho) * (4. * Square(dts) + velocity_term) + Ctau_v * Square(mu) * DotN((CeedScalar *)… in Tau_diagPrim()
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| H A D | channel.h | 41 const CeedScalar mu = gas->mu; in Exact_Channel() local
50 const CeedScalar Pr = mu / (cp * k); in Exact_Channel()
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| H A D | stg_shur14.h | 242 const CeedScalar mu = stg_ctx->newtonian_ctx.mu; in StgShur14Preprocess() local
247 const CeedScalar nu = mu / rho; in StgShur14Preprocess()
294 const CeedScalar nu = gas->mu / rho; in ICsStg()
343 const CeedScalar mu = stg_ctx->newtonian_ctx.mu; in StgShur14Inflow() local
365 CalcSpectrum(X[1][i], eps, lt, h_node_sep, mu / rho, qn, stg_ctx); in StgShur14Inflow()
484 const CeedScalar nu = gas->mu / rho; in StgShur14InflowStrongQF()
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| H A D | newtonian_types.h | 25 CeedScalar mu; member
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| H A D | newtonian_state.h | 53 CEED_QFUNCTION_HELPER CeedScalar Prandtl(NewtonianIdealGasContext gas) { return gas->cp * gas->mu /… in Prandtl()
559 stress[i] = gas->mu * (2 * strain_rate[i] + gas->lambda * div_u * (i < 3)); in NewtonianStress()
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| /libCEED/examples/solids/qfunctions/ |
| H A D | finite-strain-neo-hookean.h | 98 CEED_QFUNCTION_HELPER int commonFS(const CeedScalar lambda, const CeedScalar mu, const CeedScalar g… in commonFS() argument
138 for (CeedInt n = 0; n < 3; n++) Swork[m] += mu * C_inv[indj[m]][n] * E2[n][indk[m]]; in commonFS()
161 const CeedScalar mu = TwoMu / 2; in ElasFSResidual_NH() local
220 commonFS(lambda, mu, tempgradu, Swork, Cinvwork, &logJ); in ElasFSResidual_NH()
270 const CeedScalar mu = TwoMu / 2; in ElasFSJacobian_NH() local
316 commonFS(lambda, mu, tempgradu, Swork, Cinvwork, &logJ); in ElasFSJacobian_NH()
371 …) deltaS[j][k] = lambda * Cinv_contract_E * C_inv[j][k] - 2. * (lambda * logJ - mu) * deltaS[j][k]; in ElasFSJacobian_NH()
410 const CeedScalar mu = TwoMu / 2; in ElasFSEnergy_NH() local
458 …energy[i] = (lambda * logJ * logJ / 2. - mu * logJ + mu * (E2[0][0] + E2[1][1] + E2[2][2]) / 2.) *… in ElasFSEnergy_NH()
481 const CeedScalar mu = TwoMu / 2; in ElasFSDiagnostic_NH() local
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| H A D | linear.h | 233 const CeedScalar mu = TwoMu / 2; in ElasEnergy_Linear() local
276 …in_vol * strain_vol / 2. + strain_vol * mu + (e[0][1] * e[0][1] + e[0][2] * e[0][2] + e[1][2] * e[… in ElasEnergy_Linear()
301 const CeedScalar mu = TwoMu / 2; in ElasDiagnostic_Linear() local
359 …in_vol * strain_vol / 2. + strain_vol * mu + (e[0][1] * e[0][1] + e[0][2] * e[0][2] + e[1][2] * e[… in ElasDiagnostic_Linear()
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| /libCEED/examples/solids/ |
| H A D | index.md | 102 \bm{\Phi} = \frac{\lambda}{2} (\operatorname{trace} \bm{\epsilon})^2 + \mu \bm{\epsilon} : \bm{\eps…
108 \bm\sigma = \lambda (\operatorname{trace} \bm\epsilon) \bm I_3 + 2 \mu \bm\epsilon,
114 \begin{aligned} \lambda &= \frac{E \nu}{(1 + \nu)(1 - 2 \nu)} \\ \mu &= \frac{E}{2(1 + \nu)} \end{a…
128 \lambda + 2\mu & \lambda & \lambda & & & \\
129 \lambda & \lambda + 2\mu & \lambda & & & \\
130 \lambda & \lambda & \lambda + 2\mu & & & \\
131 & & & \mu & & \\
132 & & & & \mu & \\
133 & & & & & \mu
147 …{trace} \bm{\epsilon}) (\log(1 + \operatorname{trace} \bm\epsilon) - 1) + \mu \bm{\epsilon} : \bm{…
[all …]
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| H A D | README.md | 257 … - $\frac{\lambda}{2} (\operatorname{trace} \bm{\epsilon})^2 + \mu \bm{\epsilon} : \bm{\epsilon}$
258 …ace} \bm{\epsilon}) (\log(1 + \operatorname{trace} \bm{\epsilon} ) - 1) + \mu \bm{\epsilon} : \bm{…
259 - $\frac{\lambda}{2}(\log J)^2 + \mu \operatorname{trace} \bm{E} - \mu \log J$
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| /libCEED/examples/fluids/problems/ |
| H A D | newtonian.c | 246 CeedScalar mu = 1.8e-5; // Pa s, dynamic viscosity in NS_NEWTONIAN_IG() local
326 PetscCall(PetscOptionsScalar("-mu", "Shear dynamic viscosity coefficient", NULL, mu, &mu, NULL)); in NS_NEWTONIAN_IG()
400 mu *= Pascal * second; in NS_NEWTONIAN_IG()
415 newtonian_ig_ctx->mu = mu; in NS_NEWTONIAN_IG()
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| H A D | channel.c | 84 channel_ctx->B = body_force_scale * 2 * umax * newtonian_ig_ctx->mu / (H * H); in NS_CHANNEL()
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| /libCEED/examples/fluids/ |
| H A D | README.md | 597 * - `-mu`
837 … 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
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| H A D | index.md | 27 …{\sigma} = \mu(\nabla \bm{u} + (\nabla \bm{u})^T + \lambda (\nabla \cdot \bm{u})\bm{I}_3)$ is the …
275 + C_v \mu^2 \Vert \bm g \Vert_F ^2}
682 …$ is the center velocity, $T_w$ is the temperature at the wall, $Pr=\frac{\mu}{c_p \kappa}$ is the…
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| /libCEED/interface/ |
| H A D | ceed-basis.c | 1381 CeedScalar mu = t_nn - t_nnm1 * t_nnm1 / (d + copysign(sqrt(d * d + t_nnm1 * t_nnm1), d)); in CeedSymmetricSchurDecomposition() local
1382 CeedScalar x = mat_T[p + n * p] - mu; in CeedSymmetricSchurDecomposition()
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