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/honee/qfunctions/
H A Dadvection.h76 const CeedScalar x = X[0], y = X[1], z = dim == 2 ? 0. : X[2]; in Exact_AdvectionGeneric() local
81 q[1] = -(y - center[1]); in Exact_AdvectionGeneric()
93 q[1] = y / ly; in Exact_AdvectionGeneric()
102 CeedScalar r = sqrt(Square(x - x0[0]) + Square(y - x0[1]) + Square(z - x0[2])); 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()
124 CeedScalar r = sqrt(Square(x - center[0]) + Square(y - center[1])); in Exact_AdvectionGeneric()
131 CeedScalar inflow_to_point[3] = {x - context->lx / 2, y, 0}; in Exact_AdvectionGeneric()
138 …(y < boundary_threshold && wind[1] < boundary_threshold) || // outflow at -y bounda… in Exact_AdvectionGeneric()
140 …(y > context->ly - boundary_threshold && wind[1] > boundary_threshold) // outflow at +y bounda… in Exact_AdvectionGeneric()
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H A Ddensitycurrent.h98 const CeedScalar y = X[1]; in Exact_DC() local
102 CeedScalar rr[3] = {x - center[0], y - center[1], z - center[2]}; in Exact_DC()
H A Dutils.h37 …d CopyN(const CeedScalar *x, CeedScalar *y, const CeedInt N) { CeedPragmaSIMD for (CeedInt i = 0; … in CopyN() argument
50 CEED_QFUNCTION_HELPER void AXPY(CeedScalar alpha, const CeedScalar *x, CeedScalar *y, CeedInt N) { in AXPY() argument
51 CeedPragmaSIMD for (CeedInt i = 0; i < N; i++) y[i] += alpha * x[i]; in AXPY()
H A Deulervortex.h69 const CeedScalar x = X[0], y = X[1]; // Coordinates in Exact_Euler() local
75 const CeedScalar y0 = y - yc; in Exact_Euler()
/honee/doc/
H A Dauxiliary.md13 \langle \phi \rangle(x,y) = \frac{1}{L_z + (T_f - T_0)}\int_0^{L_z} \int_{T_0}^{T_f} \phi(x, y, z, …
22 The function $\langle \phi \rangle (x,y)$ is represented on a 2-D finite element grid, taken from t…
34 \langle \phi \rangle_z(x,y,t) = \frac{1}{L_z} \int_0^{L_z} \phi(x, y, z, t) \mathrm{d}z
41 \bm M u_N = \int_0^{L_x} \int_0^{L_y} u \psi^\mathrm{parent}_N \mathrm{d}y \mathrm{d}x
47 …} \left [\frac{1}{L_z} \int_0^{L_z} \phi(x,y,z,t) \mathrm{d}z \right ] \psi^\mathrm{parent}_N(x,y)…
53 …langle \phi \rangle_z]_N = \frac{1}{L_z} \int_\Omega \phi(x,y,z,t) \psi^\mathrm{parent}_N(x,y) \ma…
58 This assumption means quadrature points in the full domain have the same $(x,y)$ coordinate locatio…
73 \bm M [\langle \phi \rangle]_N = \frac{1}{L_z + (T_f - T_0)} \int_\Omega \int_{T_0}^{T_f} \phi(x,y,…
75 where the integral $\int_{T_0}^{T_f} \phi(x,y,z,t) \mathrm{d}t$ is calculated on a running basis.
231 \zeta = 1 - \exp\left(-\frac{y^+}{A^+}\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)…
18 …ude and width of the perturbation, respectively, and $(\bar{x}, \bar{y}) = (x-x_e, y-y_e)$ is the …
21 The boundary conditions are freestream in the x and y directions. When using an HLL (Harten, Lax, v…
63 …$ is centered at $(0,0)$ in a computational domain $-4.5 \leq x \leq 15.5$, $-4.5 \leq y \leq 4.5$.
68 A symmetry (adiabatic free slip) condition is imposed at the top and bottom boundaries $(y = \pm 4.…
291 - Path to file with y node locations. If empty, will use mesh warping instead.
385 u &= V'_x + V \sin(\hat x) \cos(\hat y) \sin(\hat z) \\
386 v &= V'_y - V \cos(\hat x) \sin(\hat y) \sin(\hat z) \\
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…
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H A Druntime_options.md268 - Use symmetry boundary conditions, for the y component, on this list of faces
323 - -y
327 - +y
H A Dtheory.md521 \bm{\hat{x}}^n &= \left[(x - U_0 t)\max(2\kappa_{\min}/\kappa^n, 0.1) , y, z \right]^T
568 y
588 y --Calc-->ke
591 yC[y]
601 y --Copy--> yC;
/honee/examples/postprocess/
H A Dvortexshedding.py33 y="Drag Coefficient",
39 y="Lift Coefficient",