Namespaces
namespace	config_tag

Classes
class	FieldList
	the dof list is a struct that contains the dof lists for blocks, sidesets and interfaces More...
class	TMatrix

Enumerations
enum class	Formulation { HPhi , L2PhiH , L2PhiB , L2EdgeH , UNDEFINED }

Functions
const Matrix< real > &	side_connector_edge_function (Calculator *aCalc, const real xi, const real eta, const real zeta)
uint64_t	mesh_config_hash (const string &aText)
	The mesh CONFIGURATION tag: a fingerprint of the settings that decide how a .msh is turned into an enriched mesh – cuts, thin-shell layers, edge-coating walls, periodicity.
string	mesh_config_text (const InputFile &aInputFile)
	The canonical text behind the tag.
uint64_t	mesh_config_tag (const InputFile &aInputFile)
	Convenience: the tag of an input file.
const Matrix< real > &	l2N (Calculator *aCalc, const uint aIndex)
void	background_phi (Calculator aCalc, TimestepMatrices aMatrices)
void	h_picard (Calculator aCalc, TimestepMatrices aMatrices)
	Collapsed h-kernels: all per-point material math is delegated to aCalc->maxwell(), whose constructor-time dispatch covers the bulk/thin-shell, metal/alloy/HTS, defect, and piecewise axes.
void	h_newton_mu0 (Calculator aCalc, TimestepMatrices aMatrices)
void	h_newton_mu (Calculator aCalc, TimestepMatrices aMatrices)
void	h_side_connector (Calculator aCalc, TimestepMatrices aMatrices)
void	h_side_connector_newton (Calculator aCalc, TimestepMatrices aMatrices)
void	h_ghost (Calculator aCalc, TimestepMatrices aMatrices)
	facet-based thin-shell interface / stabilization kernel
void	save_resistivity (Calculator *aCalc, const real aRhoM)
void	save_dotQ (Calculator *aCalc, const real aDotQ)
real	get_resistivity (Calculator *aCalc, const index_t aIndex=BELFEM_UINT_MAX)
void	l2_b2d (Calculator *aCalc, Matrix< real > &aK, Vector< real > &aF)
void	l2_h (Calculator *aCalc, Matrix< real > &aK, Vector< real > &aF)
void	l2_ah_2d (Calculator *aCalc, Matrix< real > &aK, Vector< real > &aF)
void	l2_phi (Calculator *aCalc, Matrix< real > &aK, Vector< real > &aF)
void	l2_phi_ferro (Calculator *aCalc, Matrix< real > &aK, Vector< real > &aF)
void	phi (Calculator aCalc, TimestepMatrices aMatrices)
void	phi_ferro_picard (Calculator aCalc, TimestepMatrices aMatrices)
void	phi_ferro_newton (Calculator aCalc, TimestepMatrices aMatrices)
void	phi_tri3 (Calculator aCalc, TimestepMatrices aMatrices)
void	phi_tet4 (Calculator aCalc, TimestepMatrices aMatrices)
void	phi_tri6_tet10 (Calculator aCalc, TimestepMatrices aMatrices)
void	symmetry_phi_2d (Calculator aCalc, TimestepMatrices aMatrices)
void	symmetry_phi_3d (Calculator aCalc, TimestepMatrices aMatrices)
void	h_symmetry_2d (Calculator aCalc, TimestepMatrices aMatrices)
void	h_symmetry_3d (Calculator aCalc, TimestepMatrices aMatrices)

Enumeration Type Documentation

◆ Formulation

enum class belfem::fem::maxwell::Formulation

strong

Enumerator
HPhi
L2PhiH
L2PhiB
L2EdgeH
UNDEFINED

Function Documentation

◆ background_phi()

void belfem::fem::maxwell::background_phi	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ get_resistivity()

real belfem::fem::maxwell::get_resistivity	(	Calculator *	aCalc,
		const index_t	aIndex = BELFEM_UINT_MAX )

inline

◆ h_ghost()

void belfem::fem::maxwell::h_ghost	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

facet-based thin-shell interface / stabilization kernel

number of dimensions

◆ h_newton_mu()

void belfem::fem::maxwell::h_newton_mu	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ h_newton_mu0()

void belfem::fem::maxwell::h_newton_mu0	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ h_picard()

void belfem::fem::maxwell::h_picard	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

Collapsed h-kernels: all per-point material math is delegated to aCalc->maxwell(), whose constructor-time dispatch covers the bulk/thin-shell, metal/alloy/HTS, defect, and piecewise axes.

Dispatch in IWG_Maxwell::link_to_group() is by solver algorithm and mu constancy only:

Picard -> h_picard Newton, mu constant -> h_newton_mu0 Newton, mu field-dependent -> h_newton_mu

◆ h_side_connector()

void belfem::fem::maxwell::h_side_connector	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ h_side_connector_newton()

void belfem::fem::maxwell::h_side_connector_newton	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ h_symmetry_2d()

void belfem::fem::maxwell::h_symmetry_2d	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ h_symmetry_3d()

void belfem::fem::maxwell::h_symmetry_3d	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ l2_ah_2d()

void belfem::fem::maxwell::l2_ah_2d	(	Calculator *	aCalc,
		Matrix< real > &	aK,
		Vector< real > &	aF )

◆ l2_b2d()

void belfem::fem::maxwell::l2_b2d	(	Calculator *	aCalc,
		Matrix< real > &	aK,
		Vector< real > &	aF )

◆ l2_h()

void belfem::fem::maxwell::l2_h	(	Calculator *	aCalc,
		Matrix< real > &	aK,
		Vector< real > &	aF )

◆ l2_phi()

void belfem::fem::maxwell::l2_phi	(	Calculator *	aCalc,
		Matrix< real > &	aK,
		Vector< real > &	aF )

◆ l2_phi_ferro()

void belfem::fem::maxwell::l2_phi_ferro	(	Calculator *	aCalc,
		Matrix< real > &	aK,
		Vector< real > &	aF )

◆ l2N()

const Matrix< real > & belfem::fem::maxwell::l2N	(	Calculator *	aCalc,
		const uint	aIndex )

inline

◆ mesh_config_hash()

uint64_t belfem::fem::maxwell::mesh_config_hash ( const string & aText )

inline

The mesh CONFIGURATION tag: a fingerprint of the settings that decide how a .msh is turned into an enriched mesh – cuts, thin-shell layers, edge-coating walls, periodicity.

It exists because the .bfm reuse test compares only Mesh::checksum(), which is the identity of the BASE mesh ( node coordinates and element connectivity ). The two answer different questions and both are needed: the checksum catches a changed .msh under an unchanged deck, this tag catches a changed deck under an unchanged .msh.

Deliberately NOT covered, so the user can retune a run against a cached mesh: solver, timestepping, tolerances, output, and boundary-condition amplitudes. Terminal ids ARE covered, because they feed cut construction, and so is the thin-shell ghost switch ( nonlinear magnetic { nitsche ghost penalty { eta } } ), because it decides whether the layer interfaces carry duplicate dofs – a discretization, not a tuning.

Known gap, accepted: a change INSIDE a material definition ( one that adds or removes rho ) can alter thin-shell node duplication while every layer label stays the same. Material labels are covered, definitions are not.

The tag must be reproducible on another machine, because a .bfm travels with its deck and mesh. Hence FNV-1a over fixed-precision TEXT rather than std::hash over raw values: std::hash is unspecified across standard libraries, and raw IEEE bytes would carry endianness plus last-ulp noise ( 100 um and 0.1 mm must give the same tag ). FNV-1a, 64 bit. A defined byte algorithm: identical text yields an identical value on every compiler, library and platform.

◆ mesh_config_tag()

uint64_t belfem::fem::maxwell::mesh_config_tag ( const InputFile & aInputFile )

inline

Convenience: the tag of an input file.

◆ mesh_config_text()

string belfem::fem::maxwell::mesh_config_text ( const InputFile & aInputFile )

inline

The canonical text behind the tag.

Stored in the .bfm next to the tag so a mismatch can show WHICH setting changed instead of only reporting that two numbers differ.

Lines are sorted, so neither the order of sections in the deck nor the iteration order of any container can change the result.

◆ phi()

void belfem::fem::maxwell::phi	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ phi_ferro_newton()

void belfem::fem::maxwell::phi_ferro_newton	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ phi_ferro_picard()

void belfem::fem::maxwell::phi_ferro_picard	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ phi_tet4()

void belfem::fem::maxwell::phi_tet4	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ phi_tri3()

void belfem::fem::maxwell::phi_tri3	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ phi_tri6_tet10()

void belfem::fem::maxwell::phi_tri6_tet10	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ save_dotQ()

void belfem::fem::maxwell::save_dotQ	(	Calculator *	aCalc,
		const real	aDotQ )

inline

◆ save_resistivity()

void belfem::fem::maxwell::save_resistivity	(	Calculator *	aCalc,
		const real	aRhoM )

inline

◆ side_connector_edge_function()

const Matrix< real > & belfem::fem::maxwell::side_connector_edge_function	(	Calculator *	aCalc,
		const real	xi,
		const real	eta,
		const real	zeta )

◆ symmetry_phi_2d()

void belfem::fem::maxwell::symmetry_phi_2d	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

◆ symmetry_phi_3d()

void belfem::fem::maxwell::symmetry_phi_3d	(	Calculator *	aCalc,
		TimestepMatrices *	aMatrices )

Namespaces

Classes

Enumerations

Functions

Enumeration Type Documentation

◆ Formulation

Function Documentation

◆ background_phi()

◆ get_resistivity()

◆ h_ghost()

◆ h_newton_mu()

◆ h_newton_mu0()

◆ h_picard()

◆ h_side_connector()

◆ h_side_connector_newton()

◆ h_symmetry_2d()

◆ h_symmetry_3d()

◆ l2_ah_2d()

◆ l2_b2d()

◆ l2_h()

◆ l2_phi()

◆ l2_phi_ferro()

◆ l2N()

◆ mesh_config_hash()

◆ mesh_config_tag()

◆ mesh_config_text()

◆ phi()

◆ phi_ferro_newton()

◆ phi_ferro_picard()

◆ phi_tet4()

◆ phi_tri3()

◆ phi_tri6_tet10()

◆ save_dotQ()

◆ save_resistivity()

◆ side_connector_edge_function()

◆ symmetry_phi_2d()

◆ symmetry_phi_3d()