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Searched refs:z (Results 1 – 6 of 6) sorted by relevance

/honee/qfunctions/
H A Ddensitycurrent.h99 const CeedScalar z = X[2]; in Exact_DC() local
102 CeedScalar rr[3] = {x - center[0], y - center[1], z - center[2]}; in Exact_DC()
107 const CeedScalar theta = theta0 * exp(Square(N) * z / g) + delta_theta; in Exact_DC()
110 const CeedScalar Pi = 1. + Square(g) * (exp(-Square(N) * z / g) - 1.) / (cp * theta0 * Square(N)); in Exact_DC()
H A Dadvection.h76 const CeedScalar x = X[0], y = X[1], z = dim == 2 ? 0. : X[2]; in Exact_AdvectionGeneric() local
102 CeedScalar r = sqrt(Square(x - x0[0]) + Square(y - x0[1]) + Square(z - x0[2])); in Exact_AdvectionGeneric()
/honee/doc/
H A Dauxiliary.md13 …= \frac{1}{L_z + (T_f - T_0)}\int_0^{L_z} \int_{T_0}^{T_f} \phi(x, y, z, t) \mathrm{d}t \mathrm{d}z
16 where $z$ is the spanwise direction, the domain has size $[0, L_z]$ in the spanwise direction, and …
17 Note that here and in the code, **we assume the spanwise direction to be in the $z$ direction**.
24 Otherwise the negative z face is used.
34 \langle \phi \rangle_z(x,y,t) = \frac{1}{L_z} \int_0^{L_z} \phi(x, y, z, t) \mathrm{d}z
47 …int_0^{L_x} \int_0^{L_y} \left [\frac{1}{L_z} \int_0^{L_z} \phi(x,y,z,t) \mathrm{d}z \right ] \psi…
53 \bm M [\langle \phi \rangle_z]_N = \frac{1}{L_z} \int_\Omega \phi(x,y,z,t) \psi^\mathrm{parent}_N(x…
73 …ngle]_N = \frac{1}{L_z + (T_f - T_0)} \int_\Omega \int_{T_0}^{T_f} \phi(x,y,z,t) \psi^\mathrm{pare…
75 where the integral $\int_{T_0}^{T_f} \phi(x,y,z,t) \mathrm{d}t$ is calculated on a running basis.
H A Druntime_options.md271 - Use symmetry boundary conditions, for the z component, on this list of faces
292 - -z
300 - +z
315 - -z
319 - +z
H A Dexamples.md64 We solve this as a 3D problem with (default) one element in the $z$ direction.
122 …}} \, , \\ e &= c_v \theta(\bm{x},t) \pi(\bm{x},t) + \bm{u}\cdot \bm{u} /2 + g z \, , \end{aligned}
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 …ho_0 V_0^2}{16} \left ( \cos(2 \hat x) + \cos(2 \hat y)\right) \left( \cos(2 \hat z) + 2 \right) \\
394 The coordinate modification is done to transform a given grid onto a domain of $x,y,z \in [0, 2\pi)…
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