| /honee/ |
| H A D | conf.py | 162 latex_macros = r"""
199 'preamble': r"""
207 'fontpkg': r"""
218 latexauthorslist = r' \and '.join(authorlist)
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| H A D | pytorch_pkgconfig.py | 38 regex_ABI = re.compile(r'"(\S*GLIBCXX_USE_CXX11_ABI\S*)"')
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| /honee/problems/ |
| H A D | blasius.c | 20 PetscScalar *r, f[4], h[4]; in CompressibleBlasiusResidual() local
31 PetscCall(VecGetArray(R, &r)); in CompressibleBlasiusResidual()
35 r[0] = f[0]; in CompressibleBlasiusResidual()
36 r[1] = f[1]; in CompressibleBlasiusResidual()
40 r[2] = f[1] - 1.; in CompressibleBlasiusResidual()
55 r[3 + i] = 2 * (mu_rho_tilde[0] * f[3] + mu_rho_tilde[1] * f[2]) + f[2] * f[0]; in CompressibleBlasiusResidual()
56 …r[N + 2 + i] = (mu_rho_tilde[0] * h[2] + mu_rho_tilde[1] * h[1]) + Pr * f[0] * h[1] + Pr * (gamma … in CompressibleBlasiusResidual()
61 r[N] = h[0] - blasius->T_wall / S_infty.Y.temperature; in CompressibleBlasiusResidual()
65 r[N + 1] = h[0] - 1.; in CompressibleBlasiusResidual()
69 PetscCall(VecRestoreArray(R, &r)); in CompressibleBlasiusResidual()
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| /honee/qfunctions/ |
| H A D | riemann_solver.h | 43 …_HELPER CeedScalar RoeAverage(RoeWeights r, CeedScalar q_left, CeedScalar q_right) { return r.left… in RoeAverage() argument
45 CEED_QFUNCTION_HELPER CeedScalar RoeAverage_fwd(RoeWeights r, RoeWeights dr, CeedScalar q_left, Cee… in RoeAverage_fwd() argument
47 return q_right * dr.right + q_left * dr.left + r.right * dq_right + r.left * dq_left; in RoeAverage_fwd()
101 RoeWeights r = RoeSetup(left.U.density, right.U.density); in ComputeHLLSpeeds_Roe() local
105 CeedScalar u_roe = RoeAverage(r, u_left, u_right); in ComputeHLLSpeeds_Roe()
109 CeedScalar H_roe = RoeAverage(r, H_left, H_right); in ComputeHLLSpeeds_Roe()
122 RoeWeights r = RoeSetup(left.U.density, right.U.density); in ComputeHLLSpeeds_Roe_fwd() local
127 CeedScalar u_roe = RoeAverage(r, u_left, u_right); in ComputeHLLSpeeds_Roe_fwd()
128 CeedScalar du_roe = RoeAverage_fwd(r, dr, u_left, u_right, du_left, du_right); in ComputeHLLSpeeds_Roe_fwd()
135 CeedScalar H_roe = RoeAverage(r, H_left, H_right); in ComputeHLLSpeeds_Roe_fwd()
[all …]
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| H A D | densitycurrent.h | 105 const CeedScalar r = Norm3(rr); in Exact_DC() local
106 const CeedScalar delta_theta = r <= rc ? thetaC * (1. + cos(M_PI * r / rc)) / 2. : 0.; in Exact_DC()
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| H A D | advection.h | 102 CeedScalar r = sqrt(Square(x - x0[0]) + Square(y - x0[1]) + Square(z - x0[2])); in Exact_AdvectionGeneric() local
106 q[4] = r <= rc ? (1. - r / rc) : 0.; in Exact_AdvectionGeneric()
110 q[4] = ((r <= rc) && (y < center[1])) ? (1. - r / rc) : 0.; in Exact_AdvectionGeneric()
114 … q[4] = ((r <= rc) && (y < center[1])) ? (1. - r / rc) * fmin(1.0, (center[1] - y) / 1.25) : 0.; in Exact_AdvectionGeneric()
117 q[4] = r <= rc ? .5 + .5 * cos(r * M_PI / rc) : 0; in Exact_AdvectionGeneric()
124 CeedScalar r = sqrt(Square(x - center[0]) + Square(y - center[1])); in Exact_AdvectionGeneric() local
126 q[4] = r > half_width ? 0. : cos(2 * M_PI * r / half_width + M_PI) + 1.; in Exact_AdvectionGeneric()
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| H A D | eulervortex.h | 76 const CeedScalar r = sqrt(Square(x0) + Square(y0)); in Exact_Euler() local
77 const CeedScalar C = vortex_strength * exp((1. - r * r) / 2.) / (2. * M_PI); in Exact_Euler()
78 …const CeedScalar delta_T = -(gamma - 1.) * vortex_strength * vortex_strength * exp(1 - r * r) / (… in Exact_Euler()
130 T = 1. - S_bubble * exp(1. - r * r); in Exact_Euler()
143 T = 1. - S_bubble * exp(1. - r * r); in Exact_Euler()
157 T = 1. - (r < 1. ? S_bubble : 0.); in Exact_Euler()
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| /honee/examples/ |
| H A D | stdoutParsing.py | 10 …r".*(?:^Degree of FEM Space: (\d+)).*(?:^Global FEM nodes: (\d{2,})).*(?:^dm_plex_box_faces: (\S+)…
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| /honee/src/ |
| H A D | setupts.c | 96 const StateConservative *r; in Surface_Forces_NS() local
99 PetscCall(DMPlexPointLocalRead(dm, p, g_array, &r)); in Surface_Forces_NS()
103 reaction_force[w * dim + j] -= r[node].momentum[j]; in Surface_Forces_NS()
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| /honee/tests/ |
| H A D | junit_common.py | 329 keyvalues_pattern = re.compile(r'''
363 args_pattern = re.compile(r'''
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| /honee/doc/ |
| H A D | auxiliary.md | 198 B(\Delta; \bm{r}) =
200 1 & \Vert \bm{r} \Vert \leq \Delta/2 \\
201 0 & \Vert \bm{r} \Vert > \Delta/2
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| H A D | theory.md | 211 … ansatz for subgrid state fluctuations $\tilde{\bm q} = -\bm\tau \bm r$ where $\bm r$ is a strong …
390 This filtering operation results in an extra stress-like term, $\bm{\tau}^r$, representing the effe…
404 \bm{\tau}^r \\
405 \bm{u} \cdot \bm{\tau}^r
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| H A D | examples.md | 432 … \pi} \, e^{0.5(1-r^2)} \, (-\bar{y}, \, \bar{x}) \, , \\ \delta T &= - \frac{(\gamma-1) \, \epsil…
435 …= (x-x_c, \, y-y_c)$, $(x_c, \, y_c)$ represents the center of the domain, $r^2=\bar{x}^2 + \bar{y…
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