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/libCEED/examples/nek/boxes/
H A Db1e.rea130 F IFHEAT
132 T T F F F F F F F F F IFNAV & IFADVC (convection in P.S. fields)
133 F F T T T T T T T T T T IFTMSH (IF mesh for this field is T mesh)
134 F IFAXIS
135 F IFSTRS
136 F IFSPLIT
137 F IFMGRID
138 F IFMODEL
139 F IFKEPS
140 F IFMVBD
[all …]
/libCEED/examples/solids/
H A Dindex.md245 \bm{P} = \bm{F} \, \bm{S},
248 … a symmetric tensor defined entirely in the initial configuration, and $\bm{F} = \bm I_3 + \nabla_…
256 \bm C = \bm F^T \bm F
282 where $J = \lvert \bm F \rvert = \sqrt{\lvert \bm C \rvert}$ is the determinant of deformation (i.e…
308 To sketch this idea, suppose we have the $2\times 2$ non-symmetric matrix $\bm{F} = \left( \begin{s…
417 …m E)$, as well as geometric nonlinearities through $\bm P = \bm F\, \bm S$, $\bm E(\bm F)$, and th…
426 \diff \bm P = \frac{\partial \bm P}{\partial \bm F} \!:\! \diff \bm F = \diff \bm F\, \bm S + \bm F…
432 … \frac{\partial \bm E}{\partial \bm F} \!:\! \diff \bm F = \frac 1 2 \Big( \diff \bm F^T \bm F + \…
435 and $\diff\bm F = \nabla_X\diff\bm u$.
475 \diff \bm P &= \diff \bm F\, \bm S
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H A Delasticity.c55 Vec R, R_loc, F, F_loc; // g: global, loc: local in main() local
205 PetscCall(VecDuplicate(U_g[fine_level], &F)); in main()
289 PetscCall(VecZeroEntries(F)); in main()
294 PetscCall(DMLocalToGlobal(level_dms[fine_level], F_loc, ADD_VALUES, F)); in main()
614 PetscCall(VecScale(F, scalingFactor)); in main()
618 PetscCall(SNESSolve(snes, F, U)); in main()
851 PetscCall(VecDestroy(&F)); in main()
/libCEED/examples/solids/qfunctions/
H A Dfinite-strain-neo-hookean.h207 const CeedScalar F[3][3] = { in ElasFSResidual_NH() local
234 for (CeedInt m = 0; m < 3; m++) P[j][k] += F[j][m] * S[m][k]; in ElasFSResidual_NH()
303 const CeedScalar F[3][3] = { in ElasFSJacobian_NH() local
323 …for (CeedInt n = 0; n < 3; n++) deltaEwork[m] += (graddeltau[n][indj[m]] * F[n][indk[m]] + F[n][in… in ElasFSJacobian_NH()
379 …for (CeedInt m = 0; m < 3; m++) deltaP[j][k] += graddeltau[j][m] * S[m][k] + F[j][m] * deltaS[m][k… in ElasFSJacobian_NH()
H A Dfinite-strain-mooney-rivlin.h209 const CeedScalar F[3][3] = { in ElasFSResidual_MR() local
237 for (CeedInt m = 0; m < 3; m++) P[j][k] += F[j][m] * S[m][k]; in ElasFSResidual_MR()
302 const CeedScalar F[3][3] = { in ElasFSJacobian_MR() local
323 …for (CeedInt n = 0; n < 3; n++) dEwork[m] += (graddeltau[n][indj[m]] * F[n][indk[m]] + F[n][indj[m… in ElasFSJacobian_MR()
400 for (CeedInt m = 0; m < 3; m++) dP[j][k] += graddeltau[j][m] * S[m][k] + F[j][m] * dS[m][k]; in ElasFSJacobian_MR()
/libCEED/doc/papers/joss/
H A Dpaper.bib294 author = {Satish Balay and Shrirang Abhyankar and Mark~F. Adams and Jed Brown and Peter Brune
298 and Barry~F. Smith and Stefano Zampini and Hong Zhang and Hong Zhang},
337 author={Deville, Michel O and Fischer, Paul F and Mund, Ernest H},
352 author = {Benjamin S. Kirk and John W. Peterson and Roy H. Stogner and Graham F. Carey},
422 author={Lottes, J.W. and Fischer, P.F.},
434 …w and Marin, Oana and Mills, Richard Tran and Munson, Todd and Smith, Barry F and Zampini, Stefano…
H A Dpaper.md87 $$ v^T F(u) := \int_\Omega v \cdot f_0(u, \nabla u) + \nabla v \!:\! f_1(u, \nabla u) = 0 \quad \fo…
92 $$ F(u) = \sum_e \mathcal E_e^T B_e^T W_e f(B_e \mathcal E_e u), $$
/libCEED/examples/fluids/
H A Dindex.md39 \frac{\partial \bm{q}}{\partial t} + \nabla \cdot \bm{F}(\bm{q}) -S(\bm{q}) = 0 \, ,
52 \bm{F}(\bm{q}) &=
86 \int_{\Omega} \bm v \cdot \left(\frac{\partial \bm{q}_N}{\partial t} + \nabla \cdot \bm{F}(\bm{q}_N…
96 - \int_{\Omega} \nabla \bm v \!:\! \bm{F}(\bm{q}_N)\,dV & \\
97 + \int_{\partial \Omega} \bm v \cdot \bm{F}(\bm q_N) \cdot \widehat{\bm{n}} \,dS
102 where $\bm{F}(\bm q_N) \cdot \widehat{\bm{n}}$ is typically replaced with a boundary condition.
105 …F$ represents contraction over both fields and spatial dimensions while a single dot represents co…
134 f(t^n, \bm{q}_N^n) = - [\nabla \cdot \bm{F}(\bm{q}_N)]^n + [S(\bm{q}_N)]^n \, .
180 - \int_{\Omega} \nabla \bm v \!:\! \bm{F}(\bm{q}_N)\,dV & \\
181 + \int_{\partial \Omega} \bm v \cdot \bm{F}(\bm{q}_N) \cdot \widehat{\bm{n}} \,dS & \\
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/libCEED/rust/libceed/src/
H A Dlib.rs165 pub(crate) fn check_error<F>(ceed_ptr: F, ierr: i32) -> Result<i32> in check_error() argument
167 F: FnOnce() -> bind_ceed::Ceed, in check_error()
/libCEED/doc/sphinx/source/
H A Dreferences.bib32 author = {Giraldo, F. X. and Restelli, M. and Läuter, M.},
141 author = {Bower, Allan F},
161 author = {Toro, Eleuterio F.},
H A DlibCEEDapi.md14 We start by considering the discrete residual $F(u)=0$ formulation in weak form.
/libCEED/julia/LibCEED.jl/src/
H A DUserQFunction.jl1 struct UserQFunction{F,K} argument
2 f::F
/libCEED/examples/fluids/qfunctions/
H A Driemann_solver.h64 StateConservative F = { in Flux_HLL() local
69 return F; in Flux_HLL()
/libCEED/
H A DMakefile690 …$(call quiet,LINK.F) -DSOURCE_DIR='"$(abspath $(<D))/"' $(CEED_LDFLAGS) -o $@ $(abspath $<) $(CEED…
696 …$(call quiet,LINK.F) -DSOURCE_DIR='"$(abspath $(<D))/"' $(CEED_LDFLAGS) -o $@ $(abspath $<) $(CEED…
739 PETSC_DIR="$(abspath $(PETSC_DIR))" OPT="$(OPT)" $(basename $(@F))
H A DDoxyfile1474 # ad/0/A/9/0A939EF6-E31C-430F-A3DF-DFAE7960D564/htmlhelp.exe).
/libCEED/rust/libceed-sys/c-src/
H A DMakefile690 …$(call quiet,LINK.F) -DSOURCE_DIR='"$(abspath $(<D))/"' $(CEED_LDFLAGS) -o $@ $(abspath $<) $(CEED…
696 …$(call quiet,LINK.F) -DSOURCE_DIR='"$(abspath $(<D))/"' $(CEED_LDFLAGS) -o $@ $(abspath $<) $(CEED…
739 PETSC_DIR="$(abspath $(PETSC_DIR))" OPT="$(OPT)" $(basename $(@F))