F (reference) in projects: libCEED - OpenGrok search results

Searched refs:F (Results 1 – 16 of 16) sorted by relevance

/libCEED/examples/nek/boxes/
H A D	b1e.rea	`130 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 D	index.md	245 \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 [all …]
H A D	elasticity.c	`55 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 D	finite-strain-neo-hookean.h	`207 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 D	finite-strain-mooney-rivlin.h	`209 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 D	paper.bib	`294 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 D	paper.md	`87 $$ v^T F(u) := \int_\Omega v \cdot f_0(u, \nabla u) + \nabla v \!:\! f_1(u, \nabla u) = 0 \quad \fo… 92 $$ 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 D	index.md	39 \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 & \\ [all …]
/libCEED/rust/libceed/src/
H A D	lib.rs	`165 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 D	references.bib	`32 author = {Giraldo, F. X. and Restelli, M. and Läuter, M.}, 141 author = {Bower, Allan F}, 161 author = {Toro, Eleuterio F.},`
H A D	libCEEDapi.md	`14 We start by considering the discrete residual $F(u)=0$ formulation in weak form.`
/libCEED/julia/LibCEED.jl/src/
H A D	UserQFunction.jl	`1 struct UserQFunction{F,K} argument 2 f::F`
/libCEED/examples/fluids/qfunctions/
H A D	riemann_solver.h	`64 StateConservative F = { in Flux_HLL() local 69 return F; in Flux_HLL()`
/libCEED/
H A D	Makefile	`690 …$(call quiet,LINK.F) -DSOURCE_DIR='"$(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 $(@F))`
H A D	Doxyfile	`1474 # ad/0/A/9/0A939EF6-E31C-430F-A3DF-DFAE7960D564/htmlhelp.exe).`
/libCEED/rust/libceed-sys/c-src/
H A D	Makefile	`690 …$(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))`

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