| /honee/problems/ |
| H A D | bc_freestream.c | 220 const CeedScalar T = 200; in TestRiemannHLL_fwd() local 222 const CeedScalar p = (HeatCapacityRatio(gas) - 1) * rho * gas.cv * T; in TestRiemannHLL_fwd() 225 const CeedScalar Y0_left[5] = {p, u[0], u[1], u[2], T}; in TestRiemannHLL_fwd() 226 const CeedScalar Y0_right[5] = {1.2 * p, 1.2 * u[0], 1.2 * u[1], 1.2 * u[2], 1.2 * T}; in TestRiemannHLL_fwd() 282 const CeedScalar T = 200; in TestRiemannHLLC_fwd() local 284 const CeedScalar p = (HeatCapacityRatio(gas) - 1) * rho * gas.cv * T; in TestRiemannHLLC_fwd() 287 const CeedScalar Y0_left[5] = {p, u[0], u[1], u[2], T}; in TestRiemannHLLC_fwd() 288 const CeedScalar Y0_right[5] = {1.2 * p, 1.2 * u[0], 1.2 * u[1], 1.2 * u[2], 1.2 * T}; in TestRiemannHLLC_fwd() 344 const CeedScalar T = 200; in TestComputeHLLSpeeds_Roe_fwd() local 346 const CeedScalar p = (HeatCapacityRatio(gas) - 1) * rho * gas.cv * T; in TestComputeHLLSpeeds_Roe_fwd() [all …]
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| H A D | newtonian.c | 739 const CeedScalar T = 200 * K; in UnitTests_Newtonian() local 741 const CeedScalar P = (HeatCapacityRatio(gas) - 1) * rho * gas.cv * T; in UnitTests_Newtonian() 745 const CeedScalar e_internal = gas.cv * T; in UnitTests_Newtonian() 750 const CeedScalar Y0[5] = {P, u[0], u[1], u[2], T}; in UnitTests_Newtonian()
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| /honee/qfunctions/ |
| H A D | eulervortex.h | 81 CeedScalar rho, P, T, E, u[3] = {0.}; in Exact_Euler() local 86 T = 1 + delta_T; in Exact_Euler() 90 rho = pow(T / S_vortex, 1 / (gamma - 1.)); in Exact_Euler() 91 P = rho * T; in Exact_Euler() 130 T = 1. - S_bubble * exp(1. - r * r); in Exact_Euler() 131 rho = P / (R * T); in Exact_Euler() 138 q[4] = rho * (cv * T + (u[0] * u[0] + u[1] * u[1]) / 2.); in Exact_Euler() 143 T = 1. - S_bubble * exp(1. - r * r); in Exact_Euler() 144 rho = P / (R * T); in Exact_Euler() 153 q[4] = rho * (cv * T + (u[0] * u[0] + u[1] * u[1]) / 2.); in Exact_Euler() [all …]
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| H A D | newtonian_state.h | 48 …undSpeed(NewtonianIGProperties gas, CeedScalar T) { return sqrt(gas.cp * (HeatCapacityRatio(gas) -… in SoundSpeed() argument 50 …eedScalar Mach(NewtonianIGProperties gas, CeedScalar T, CeedScalar u) { return u / SoundSpeed(gas,… in Mach() argument
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| /honee/tests/createPyTorchModel/ |
| H A D | update_weights.py | 12 weights.append(np.loadtxt(new_parameters_Path / 'w1.dat', skiprows=1).reshape(6, 20).T) 13 weights.append(np.loadtxt(new_parameters_Path / 'w2.dat', skiprows=1).reshape(20, 6).T)
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| /honee/doc/ |
| H A D | theory.md | 15 …cdot \left( \frac{(E + P)\bm{U}}{\rho} -\bm{u} \cdot \bm{\sigma} - k \nabla T \right) - \rho \bm{b… 19 where $\bm{\sigma} = \mu(\nabla \bm{u} + (\nabla \bm{u})^T + \lambda (\nabla \cdot \bm{u})\bm{I}_3)… 20 …r (e.g., gravity vector $\bm{g}$), $k$ the thermal conductivity constant, $T$ represents the temp… 63 - \bm{u} \cdot \bm{\sigma} - k \nabla T 232 …it vector $\hat{\bm n}$ is given by $\lVert \bigl(\nabla_{\bm X} \bm x\bigr)^T \hat{\bm n} \rVert$. 284 where $\bm g = \nabla_{\bm x} \bm{X}^T \cdot \nabla_{\bm x} \bm{X}$ is the metric tensor and $\Vert… 342 This term requires a second derivative to evaluate; first to evaluate $\bm \sigma$ and $\nabla T$ f… 521 \bm{\hat{x}}^n &= \left[(x - U_0 t)\max(2\kappa_{\min}/\kappa^n, 0.1) , y, z \right]^T 525 …osition of the Reynolds stress tensor $\bm{C}$ (such that $\bm{R} = \bm{CC}^T$ ), bulk velocity $U… 722 where $\bm{Y}' = [P - P_\mathrm{ref}, \bm{0}, 0]^T$, and $\sigma(\bm{x})$ is a linear ramp starting…
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| H A D | auxiliary.md | 66 $$\overline{\phi}_\mathrm{new} = \overline{\phi}_{\mathrm{old}} + \phi(t_\mathrm{new}) \Delta T$$ 67 where $\phi(t_\mathrm{new})$ is the statistic at the current time and $\Delta T$ is the time since … 123 | $\mean{\rho T}$ | MeanDensityTemperature | 124 | $\mean{\rho T u_i}$ | MeanDensityTemperatureFlux[$i$] |
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| H A D | runtime_options.md | 479 …}, \rho e$), `primitive` ($P, \bm{u}, T$), or `entropy` ($\frac{\gamma - s}{\gamma - 1} - \frac{\r…
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| H A D | examples.md | 186 $$T = T_w \left [ 1 + \frac{Pr \hat{E}c}{3} \left \{1 - \left(\frac{x_2}{H}\right)^4 \right \} \ri… 429 …=1$, $P=1$, $T=P/\rho= 1$ (Specific Gas Constant, $R$, is 1), and $\bm{u}=(u_1,u_2,0)$ while the p… 432 …\epsilon}{2 \pi} \, e^{0.5(1-r^2)} \, (-\bar{y}, \, \bar{x}) \, , \\ \delta T &= - \frac{(\gamma-1…
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| /honee/src/ |
| H A D | dm-utils.c | 618 …(*interp)[q * P + p_ceed] = tabulation->T[0][((face * Q + q) * P * num_comp + p_petsc) * num_comp … in ComputeFieldTabulationP2C() 620 …(*grad)[(d * Q + q) * P + p_ceed] = tabulation->T[1][(((face * Q + q) * P * num_comp + p_petsc) * … in ComputeFieldTabulationP2C()
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| /honee/ |
| H A D | Doxyfile | 2441 # https://www.graphviz.org/), a graph visualization toolkit from AT&T and Lucent 2750 # files in one run (i.e. multiple -o and -T options on the command line). This 2781 # specifying prog as the value, doxygen will call the tool as prog -T
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