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/honee/qfunctions/
H A Driemann_solver.h25 CeedScalar left, right; member
43 …oeAverage(RoeWeights r, CeedScalar q_left, CeedScalar q_right) { return r.left * q_left + r.right … in RoeAverage()
47 return q_right * dr.right + q_left * dr.left + r.right * dq_right + r.left * dq_left; in RoeAverage_fwd()
50 CEED_QFUNCTION_HELPER StateConservative Flux_HLL(State left, State right, StateConservative flux_le… in Flux_HLL() argument
53 UnpackState_U(left.U, U_left); in Flux_HLL()
68 CEED_QFUNCTION_HELPER StateConservative Flux_HLL_fwd(State left, State right, State dleft, State dr… in Flux_HLL_fwd() argument
72 UnpackState_U(left.U, U_l); in Flux_HLL_fwd()
97 CEED_QFUNCTION_HELPER void ComputeHLLSpeeds_Roe(NewtonianIGProperties gas, State left, CeedScalar u… in ComputeHLLSpeeds_Roe() argument
101 RoeWeights r = RoeSetup(left.U.density, right.U.density); in ComputeHLLSpeeds_Roe()
107 CeedScalar H_left = TotalSpecificEnthalpy(gas, left); in ComputeHLLSpeeds_Roe()
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/honee/problems/
H A Dbc_freestream.c485 dR_fd.left = (R1.left - R0.left) / eps; in TestRowSetup_fwd()
494 dR_err.left = RelativeError(dR_fd.left, dR.left, dR_fd.left, divisor_threshold); in TestRowSetup_fwd()
496 …if (fabs(dR_err.left) >= rtol) printf("%s dR.left error %g (expected %.10e, got %.10e)\n", buf, dR… in TestRowSetup_fwd()
/honee/doc/
H A Dtheory.md14 \frac{\partial \bm{U}}{\partial t} + \nabla \cdot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm…
15 \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} -\bm{u} \cdot \bm{\s…
23 P = \left( {c_p}/{c_v} -1\right) \left( E - {\bm{U}\cdot\bm{U}}/{(2 \rho)} \right) \, ,
88 \int_{\Omega} \bm v \cdot \left(\frac{\partial \bm{q}_N}{\partial t} + \nabla \cdot \bm{F}(\bm{q}_N…
97 \int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) \…
131 k_i &= f\left(t^n + c_i \Delta t, \bm{q}_N^n + \Delta t \sum_{j=1}^s a_{ij} k_j \right)\\
183 …\int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) …
186 …+ \int_{\Omega} \nabla\bm v \tcolon\left(\frac{\partial \bm F_{\text{adv}}}{\partial \bm q}\right)…
200 …\int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) …
203 …+ \int_{\Omega} \nabla\bm v \tcolon\left(\frac{\partial \bm F_{\text{adv}}}{\partial \bm q}\right)…
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H A Dexamples.md12 \rho &= \rho_\infty\left(1+A\exp\left(\frac{-(\bar{x}^2 + \bar{y}^2)}{2\sigma^2}\right)\right) \\
14 E &= \frac{p_\infty}{\gamma -1}\left(1+A\exp\left(\frac{-(\bar{x}^2 + \bar{y}^2)}{2\sigma^2}\right)…
67 At time $t=0$, this domain is subjected to freestream boundary conditions at the inflow (left) and …
185 $$ u_1 = u_{\max} \left [ 1 - \left ( \frac{x_2}{H}\right)^2 \right] \quad \quad u_2 = u_3 = 0$$
186 $$T = T_w \left [ 1 + \frac{Pr \hat{E}c}{3} \left \{1 - \left(\frac{x_2}{H}\right)^4 \right \} \ri…
388 p &= p_0 + \frac{\rho_0 V_0^2}{16} \left ( \cos(2 \hat x) + \cos(2 \hat y)\right) \left( \cos(2 \ha…
424 \frac{\partial \bm{U}}{\partial t} + \nabla \cdot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm…
425 \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} \right) &= 0 \, , \\
494 \tau_{SHOCK} = \frac{h_{SHOCK}}{2u_{cha}} \left( \frac{ \,|\, \nabla \rho \,|\, h_{SHOCK}}{\rho_{re…
500 h_{SHOCK} = 2 \left( C_{YZB} \,|\, \bm p \,|\, \right)^{-1}
H A Dauxiliary.md47 \bm M [\langle \phi \rangle_z]_N = \int_0^{L_x} \int_0^{L_y} \left [\frac{1}{L_z} \int_0^{L_z} \phi…
62 To calculate the temporal integral, we do a running average using left-rectangle rule.
64 Periodically, the integral is updated using left-rectangle rule:
115 The terms collected are listed below, with the mathematical definition on the left and the label (p…
182 \int_\Omega \left( v \overline \phi + \beta \nabla v \cdot (\bm{D}\bm{\Delta})^2 \nabla \overline \…
231 \zeta = 1 - \exp\left(-\frac{y^+}{A^+}\right)
/honee/
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