| /honee/examples/ |
| H A D | STGRand_flatplate_STG.dat | 2 …633363958E-01 6.835806560233085E-01 5.085799333171893E-01 9.293046644173316E-01 -8.520184178061596…
3 …967224327E-02 -6.300442772473570E-01 7.731249829460483E-01 9.238430871512343E-01 4.496034590721042…
4 …989669561E-01 -1.886013683924178E-01 -1.621731519981648E-01 8.669199738947448E-01 2.48733367296705…
5 …02644478E-01 -4.767349679302436E-01 -1.750288349882919E-01 4.320268588685827E+00 5.075442565700029…
6 …096851644E-01 -5.816049922517896E-01 7.923817785451968E-01 1.079492607600402E+00 -6.02670396662472…
7 …42053982E-01 5.900173099831675E-01 -2.289865814689692E-01 4.574666416301042E+00 5.812147393758103E…
8 …761517107E-02 6.378138301804963E-02 9.976608244450238E-01 1.639930833954775E+00 2.102479764311849E…
9 …67798926E-01 -5.686143231379204E-02 -9.595455533415366E-01 3.897938125188386E+00 9.365809084700991…
10 …133240252E-01 6.244520259556716E-01 -7.705181768617595E-01 4.050914108554178E-01 9.637531433064010…
11 …425341763E-01 4.123730553223061E-01 5.728063156454518E-01 6.184182280633475E+00 -5.985052230890442…
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| H A D | STGInflow_flatplate_STG.dat | 2 …E+00 0.000000000000E+00 0.000000000000E+00 0.000000000000E+00 7.179008029304E-31 7.179008029304E-3…
3 …E-05 3.859880951139E-03 1.022205052658E-09 0.000000000000E+00 2.934407604273E-09 2.934407604273E-0…
4 …E-05 1.293994531398E-02 1.139636601650E-08 0.000000000000E+00 1.130013883590E-07 1.130013883590E-0…
5 …E-04 2.721100002367E-02 5.045959894221E-08 0.000000000000E+00 1.082086442189E-06 1.082086442189E-0…
6 …E-04 4.666441482957E-02 1.489340379839E-07 0.000000000000E+00 5.628400074474E-06 5.628400074474E-0…
7 …E-04 7.126275358731E-02 3.485106033744E-07 0.000000000000E+00 2.055754308391E-05 2.055754308391E-0…
8 …E-04 1.008849013915E-01 7.021767233631E-07 0.000000000000E+00 5.896074901976E-05 5.896074901976E-0…
9 …E-04 1.352353775508E-01 1.270071883928E-06 0.000000000000E+00 1.404470843706E-04 1.404470843706E-0…
10 …E-04 1.737287577352E-01 2.113446008549E-06 0.000000000000E+00 2.870184227390E-04 2.870184227390E-0…
11 …E-03 2.154124333813E-01 3.286504269223E-06 0.000000000000E+00 5.147709417387E-04 5.147709417387E-0…
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| H A D | STGRand.dat | 2 1.0E0 0.0E0 0.0E0 1.4E0 0.0E0 7.071067811865475E-1 7.071067811865475E…
3 0.0E0 7.071067811865475E-1 7.071067811865475E-1 2.4E0 1.0E0 0.0E0 0.0E0
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| H A D | conv_plot.py | 49 E = data['rel_error']
50 H = amin(E) * (h / amin(h))**p
51 ax.loglog(h, E, 'o', color=colors[i])
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| /honee/qfunctions/ |
| H A D | eulervortex.h | 81 CeedScalar rho, P, T, E, u[3] = {0.}; in Exact_Euler() local
104 E = 2.; in Exact_Euler()
111 q[4] = E; in Exact_Euler()
115 E = 2.; in Exact_Euler()
124 q[4] = E; in Exact_Euler()
176 …bian_Euler(CeedScalar dF[3][5][5], const CeedScalar rho, const CeedScalar u[3], const CeedScalar E, in ConvectiveFluxJacobian_Euler() argument
185 …dF[i][4][k + 1] = ((i == k) ? (E * gamma / rho - (gamma - 1.) * u_sq / 2.) : 0.) - (gamma - 1.… in ConvectiveFluxJacobian_Euler()
189 dF[i][4][0] = u[i] * ((gamma - 1.) * u_sq - E * gamma / rho); in ConvectiveFluxJacobian_Euler()
279 const CeedScalar E = q[4][i]; in Euler() local
305 …alar E_kinetic = 0.5 * rho * (u[0] * u[0] + u[1] * u[1] + u[2] * u[2]), E_internal = E - E_kinetic, in Euler()
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| H A D | shocktube.h | 109 …bian_Euler(CeedScalar dF[3][5][5], const CeedScalar rho, const CeedScalar u[3], const CeedScalar E, in ConvectiveFluxJacobian_Euler() argument
118 …dF[i][4][k + 1] = ((i == k) ? (E * gamma / rho - (gamma - 1.) * u_sq / 2.) : 0.) - (gamma - 1.… in ConvectiveFluxJacobian_Euler()
122 dF[i][4][0] = u[i] * ((gamma - 1.) * u_sq - E * gamma / rho); in ConvectiveFluxJacobian_Euler()
228 const CeedScalar E = q[4][i]; in EulerShockTube() local
256 …alar E_kinetic = 0.5 * rho * (u[0] * u[0] + u[1] * u[1] + u[2] * u[2]), E_internal = E - E_kinetic, in EulerShockTube()
279 …for (CeedInt j = 0; j < 3; j++) dv[j][4][i] += wdetJ * (E + P) * (u[0] * dXdx[j][0] + u[1] * dXdx[… in EulerShockTube()
317 ConvectiveFluxJacobian_Euler(jacob_F_conv, rho, u, E, gamma); in EulerShockTube()
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| H A D | channel.h | 116 const CeedScalar E = rho_in * e_internal + E_kinetic; in Channel_Inflow() local
132 v[4][i] -= wdetJb * u_normal * (E + P); in Channel_Inflow()
155 const CeedScalar E = q[4][i]; in Channel_Outflow() local
172 v[4][i] -= wdetJb * u_normal * (E + P); in Channel_Outflow()
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| H A D | stg_shur14.h | 387 const CeedScalar E = E_internal + E_kinetic; in StgShur14Inflow() local
404 v[4][i] -= wdetJb * u_normal * (E + P); in StgShur14Inflow()
406 const CeedScalar U[] = {rho, u[0], u[1], u[2], E}, kmstress[6] = {0.}; in StgShur14Inflow()
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| H A D | advection.h | 509 const CeedScalar E = q[4][i]; in Advection_InOutFlowGeneric() local
523 v[4][i] = -(1 - strong_form) * wdetJb * E * u_normal; in Advection_InOutFlowGeneric()
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| /honee/doc/ |
| H A D | references.bib | 25 author = {Hughes, Thomas J R and Scovazzi, Guglielmo and Tezduyar, Tayfun E},
101 author = {Whiting, Christian H and Jansen, Kenneth E and Dey, Saikat},
127 author = {Tezduyar, Tayfun E and Senga, Masayoshi},
206 author = {Prakash, Aviral and Jansen, Kenneth E. and Evans, John A.},
217 author = {Prakash, Aviral and Jansen, Kenneth E. and Evans, John A.},
250 author = {Van Driest, E. R.},
264 author = {Jansen, Kenneth E. and Collis, S. Scott and Whiting, Christian and Shakib, Farzin},
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| H A D | examples.md | 14 E &= \frac{p_\infty}{\gamma -1}\left(1+A\exp\left(\frac{-(\bar{x}^2 + \bar{y}^2)}{2\sigma^2}\right)…
186 $$T = T_w \left [ 1 + \frac{Pr \hat{E}c}{3} \left \{1 - \left(\frac{x_2}{H}\right)^4 \right \} \ri…
272 - `5.9E-4`
425 \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} \right) &= 0 \, , \\
545 …nsity $\rho$ and momentum density $\rho \bm u$ constant while advecting "total energy density" $E$.
549 \frac{\partial E}{\partial t} + \nabla \cdot (\bm{u} E ) - \kappa \nabla E = 0 \, ,
560 …We have solved {eq}`eq-advection` applying zero energy density $E$, and no-flux for $\bm{u}$ on th…
607 For the outflow boundary conditions, we have used the current values of $E$, following {cite}`papan…
611 …_N) \cdot \widehat{\bm{n}} \,dS = \int_{\partial \Omega_{outflow}} \bm v \, E \, \bm u \cdot \wide…
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| H A D | theory.md | 15 \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} -\bm{u} \cdot \bm{\s…
20 …bm{u}$, where $\bm{u}$ is the vector velocity field), $E$ the total energy density (defined as $E …
23 P = \left( {c_p}/{c_v} -1\right) \left( E - {\bm{U}\cdot\bm{U}}/{(2 \rho)} \right) \, ,
41 E \equiv \rho e
58 {(E + P)\bm{U}}/{\rho}
220 (E + P)\diff\bm U/\rho + (\diff E + \diff P)\bm U/\rho - (E + P) \bm U/\rho^2 \diff\rho
540 The wavemode amplitudes $q^n$ are defined by a model energy spectrum $E(\kappa)$:
543 q^n = \frac{E(\kappa^n) \Delta \kappa^n}{\sum^N_{n=1} E(\kappa^n)\Delta \kappa^n} \ ,\quad \Delta \…
546 $$ E(\kappa) = \frac{(\kappa/\kappa_e)^4}{[1 + 2.4(\kappa/\kappa_e)^2]^{17/6}} f_\eta f_{\mathrm{cu…
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| H A D | runtime_options.md | 155 - `1E-11`
|