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/honee/examples/postprocess/
H A Dvortexshedding.py9 S = np.pi * D * zspan # surface area
10 return 2 * force / (rho * u**2 * S)
/honee/
H A Dcommon.mk8 ansicolor = $(shell echo $(call last_path,$(1)) | cksum | cut -b1-2 | xargs -IS expr 2 \* S + 17)
H A DDoxyfile1835 # search using the keyboard; to jump to the search box use <access key> + S
/honee/doc/
H A Dtheory.md31 \frac{\partial \bm{q}}{\partial t} + \nabla \cdot \bm{F}(\bm{q}) -S(\bm{q}) = 0 \, ,
65 S(\bm{q}) &=
88 …(\frac{\partial \bm{q}_N}{\partial t} + \nabla \cdot \bm{F}(\bm{q}_N) - \bm{S}(\bm{q}_N) \right) \…
97 \int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) \…
107 …ion in just one, which should be clear from context, e.g., $\bm v \cdot \bm S$ contracts over fiel…
138 f(t^n, \bm{q}_N^n) = - [\nabla \cdot \bm{F}(\bm{q}_N)]^n + [S(\bm{q}_N)]^n \, .
183 …\int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) …
187 \nabla \cdot \bm{F} \, (\bm{q}_N) - \bm{S}(\bm{q}_N) \right) \,dV &= 0
200 …\int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) …
394 \frac{\partial \bm{\overline q}}{\partial t} + \nabla \cdot \bm{\overline F}(\bm{\overline q}) -S(\…
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H A Dexamples.md76 Given the force components $\bm F = (F_x, F_y, F_z)$ and surface area $S = \pi D L_z$ where $L_z$ i…
80 C_L &= \frac{2 F_y}{\rho_\infty u_\infty^2 S} \\
81 C_D &= \frac{2 F_x}{\rho_\infty u_\infty^2 S} \\
436 There is no perturbation in the entropy $S=P/\rho^\gamma$ ($\delta S=0)$.
H A Dreferences.bib264 author = {Jansen, Kenneth E. and Collis, S. Scott and Whiting, Christian and Shakib, Farzin},
/honee/problems/
H A Dbc_freestream.c183 static inline CeedScalar RelativeError(CeedScalar S, CeedScalar A, CeedScalar B, CeedScalar thresho… in RelativeError() argument
184 return (A - B) / (fabs(S) > threshold ? S : 1); in RelativeError()