| /libCEED/examples/fluids/qfunctions/ |
| H A D | riemann_solver.h | 105 RoeWeights r = RoeSetup(left.U.density, right.U.density); in ComputeHLLSpeeds_Roe() 126 RoeWeights r = RoeSetup(left.U.density, right.U.density); in ComputeHLLSpeeds_Roe_fwd() 127 RoeWeights dr = RoeSetup_fwd(left.U.density, right.U.density, dleft.U.density, dright.U.density); in ComputeHLLSpeeds_Roe_fwd() 221 CeedScalar fact = side.U.density * (s_side - u_side) / (s_side - s_star); in RiemannFlux_HLLC_Star() 222 CeedScalar denom = side.U.density * (s_side - u_side); in RiemannFlux_HLLC_Star() 231 side.U.E_total / side.U.density // in RiemannFlux_HLLC_Star() 241 CeedScalar fact = side.U.density * (s_side - u_side) / (s_side - s_star); in RiemannFlux_HLLC_Star_fwd() 242 …CeedScalar dfact = (side.U.density * (ds_side - du_side) + dside.U.density * (s_side - u_side)) / … in RiemannFlux_HLLC_Star_fwd() 244 CeedScalar denom = side.U.density * (s_side - u_side); in RiemannFlux_HLLC_Star_fwd() 245 CeedScalar ddenom = side.U.density * (ds_side - du_side) + dside.U.density * (s_side - u_side); in RiemannFlux_HLLC_Star_fwd() [all …]
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| H A D | newtonian_state.h | 21 CeedScalar density; member 32 U[0] = s.density; in UnpackState_U() 62 return e_internal + e_kinetic + s.Y.pressure / s.U.density; in TotalSpecificEnthalpy() 68 …de_internal + de_kinetic + ds.Y.pressure / s.U.density - s.Y.pressure / Square(s.U.density) * ds.U… in TotalSpecificEnthalpy_fwd() 73 for (CeedInt i = 0; i < 3; i++) Y.velocity[i] = U.momentum[i] / U.density; in StatePrimitiveFromConservative() 75 CeedScalar e_total = U.E_total / U.density; in StatePrimitiveFromConservative() 78 Y.pressure = (HeatCapacityRatio(gas) - 1) * U.density * e_internal; in StatePrimitiveFromConservative() 85 dY.velocity[i] = (dU.momentum[i] - s.Y.velocity[i] * dU.density) / s.U.density; in StatePrimitiveFromConservative_fwd() 89 CeedScalar e_total = s.U.E_total / s.U.density; in StatePrimitiveFromConservative_fwd() 90 CeedScalar de_total = (dU.E_total - e_total * dU.density) / s.U.density; in StatePrimitiveFromConservative_fwd() [all …]
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| H A D | turb_spanstats.h | 28 v[TURB_MEAN_DENSITY][i] = wdetJ * s.U.density; in ChildStatsCollection() 34 v[TURB_MEAN_DENSITY_TEMPERATURE][i] = wdetJ * s.U.density * s.Y.temperature; in ChildStatsCollection() 35 …v[TURB_MEAN_DENSITY_TEMPERATURE_FLUX_X][i] = wdetJ * s.U.density * s.Y.temperature * s.Y.velocity[… in ChildStatsCollection() 36 …v[TURB_MEAN_DENSITY_TEMPERATURE_FLUX_Y][i] = wdetJ * s.U.density * s.Y.temperature * s.Y.velocity[… in ChildStatsCollection() 37 …v[TURB_MEAN_DENSITY_TEMPERATURE_FLUX_Z][i] = wdetJ * s.U.density * s.Y.temperature * s.Y.velocity[… in ChildStatsCollection()
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| H A D | blasius.h | 117 const CeedScalar x0 = U_infty * S_infty.U.density / (mu * 25 / Square(delta0)); in ICsBlasius() 121 State s = BlasiusSolution(context, x, x0, x_inflow, S_infty.U.density, &t12); in ICsBlasius() 142 const CeedScalar rho_0 = S_infty.U.density; in Blasius_Inflow() 162 s.U.density = s_int.U.density; in Blasius_Inflow() 199 const CeedScalar rho_0 = S_infty.U.density; in Blasius_Inflow_Jacobian()
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| H A D | gaussianwave.h | 48 …const CeedScalar e_kinetic = 0.5 * S_infty.U.density * Dot3(S_infty.Y.velocity, S_infty.Y.velocity… in IC_GaussianWave() 52 U[0] = S_infty.U.density * perturbation; in IC_GaussianWave()
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| H A D | newtonian.h | 189 …const CeedScalar body_force[5] = {0, s.U.density * g[0], s.U.density * g[1], s.U.density * g[2], D… in RHSFunction_Newtonian() 262 …const CeedScalar body_force[5] = {0, s.U.density * g[0], s.U.density * g[1], s.U.density * g[2], D… in IFunction_Newtonian() 355 …const CeedScalar dbody_force[5] = {0, ds.U.density * g[0], ds.U.density * g[1], ds.U.density * g[2… in IJacobian_Newtonian()
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| H A D | stabilization.h | 81 const CeedScalar rho = s.U.density; in Tau_diagPrim()
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| /libCEED/examples/fluids/ |
| H A D | README.md | 8 The state variables are mass density, momentum density, and energy density. 302 … pure advection, which holds density $\rho$ and momentum density $\rho \bm u$ constant while advec… 804 - Axis of density current cylindrical anomaly, or `(0,0,0)` for spherically symmetric
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| H A D | index.md | 28 …mass density, $U$ the momentum density (defined as $\bm{U}=\rho \bm{u}$, where $\bm{u}$ is the vec… 45 …row\textrm{ volume mass density}\\ \leftarrow\textrm{ momentum density}\\ \l… 318 …he exact solution to the Euler equations, and the so called {ref}`problem-density-current` problem. 534 …We have solved {eq}`eq-advection` applying zero energy density $E$, and no-flux for $\bm{u}$ on th… 588 …s taken to be the acoustic speed while the reference density $\rho_{ref}$ is just the local densit… 600 …ortional to the element length in the direction of the density gradient unit vector. This density … 614 (problem-density-current)= 659 where $\rho_\infty, u_\infty$ are the freestream (inflow) density and velocity respectively. 694 the velocity is prescribed by the Blasius soution profile, density is set 695 constant, and temperature is allowed to float. Using `weakT: true`, density is [all …]
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| /libCEED/examples/solids/ |
| H A D | index.md | 83 Here, we define a strain energy density functional $\Phi(\bm \epsilon) \in \mathbb R$ and obtain th… 90 The strain energy density functional cannot be an arbitrary function $\Phi(\bm \epsilon)$; it can o… 99 For the linear elasticity model, the strain energy density is given by 144 However, the strain energy density differs and is given by 239 $\rho_0$ is known as the *initial* mass density. 268 Recall that the strain energy density functional can only depend upon invariants. 322 A coupled Mooney-Rivlin strain energy density (cf. Neo-Hookean {eq}`neo-hookean-energy`) is {cite}`…
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| H A D | README.md | 225 …name{trace} \bm{E}$, $\operatorname{trace} \bm{E}^2$, $\lvert J \rvert$, and strain energy density.
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| /libCEED/julia/LibCEED.jl/examples/ |
| H A D | ex2-surface.jl | 8 # map [0,1] to [0,1] varying the mesh density
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| H A D | ex1-volume.jl | 9 # map [0,1] to [0,1] varying the mesh density
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| H A D | ex3-volume.jl | 9 # map [0,1] to [0,1] varying the mesh density
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| H A D | ex1-volume-c.jl | 192 # map [0,1] to [0,1] varying the mesh density
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| /libCEED/doc/papers/joss/ |
| H A D | paper.md | 156 …ime integration; \autoref{fig:NSvortices} shows vortices arising in the "density current" [@straka… 161 ![Strain energy density in a twisted Neo-Hookean beam.\label{fig:Solids}](img/SolidTwistExample.jpe…
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| H A D | paper.bib | 324 title={Numerical solutions of a non-linear density current: A benchmark solution and comparisons},
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| /libCEED/doc/sphinx/source/ |
| H A D | references.bib | 92 …title = {Numerical solutions of a non-linear density current: A benchmark solution and compari…
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