#include <field.h>

Inheritance diagram for Field:

Collaboration diagram for Field:

Public Member Functions
	Field ()=default
	Field (int I_total, int J_total, int K_total)
void	allocate ()
void	zero ()
void	allocate_and_zero ()
void	normalise_volume ()
	Normalises the field entries by dividing by the angular norm.
void	set_phasors (SplitField &F, int n, double omega, double dt, int Nt)
void	add_to_angular_norm (int n, int Nt, SimulationParameters &params)
	Compute the phasor_norm of the current field and add it to the current norm-value.
std::complex< double >	phasor_norm (double f, int n, double omega, double dt, int Nt)
virtual double	phase (int n, double omega, double dt)=0
virtual std::complex< double >	interpolate_to_centre_of (AxialDirection d, CellCoordinate cell)=0
	Interpolates a Field component to the centre of a Yee cell.
void	interpolate_over_range (mxArray x_out, mxArray y_out, mxArray *z_out, int i_lower, int i_upper, int j_lower, int j_upper, int k_lower, int k_upper, Dimension mode=Dimension::THREE)
	Interpolates the Field over the range provided.
void	interpolate_over_range (mxArray x_out, mxArray y_out, mxArray *z_out, Dimension mode=Dimension::THREE)
	Interpolates the Field over the range provided.
virtual void	interpolate_transverse_electric_components (CellCoordinate cell, std::complex< double > x_at_centre, std::complex< double > y_at_centre, std::complex< double > *z_at_centre)=0
	Interpolates the Field's transverse electric components to the centre of Yee cell i,j,k.
virtual void	interpolate_transverse_magnetic_components (CellCoordinate cell, std::complex< double > x_at_centre, std::complex< double > y_at_centre, std::complex< double > *z_at_centre)=0
	Interpolates the Field's transverse magnetic components to the centre of Yee cell i,j,k.
void	set_values_from (Field &other)
double	normalised_difference (Field &other)
	Computes the maximum pointwise absolute difference of the other field to this one, divided by the largest absolute value of this field's components.
Public Member Functions inherited from Grid
int	max_IJK_tot () const
void	set_preferred_interpolation_methods (tdms_flags::InterpolationMethod im)
	Set the preferred interpolation methods.

Public Attributes
double	ft = 0.
std::complex< double >	angular_norm = 0.
XYZTensor3D< double >	real
XYZTensor3D< double >	imag
int	il = 0
int	iu = 0
int	jl = 0
int	ju = 0
int	kl = 0
int	ku = 0
Public Attributes inherited from Grid
IJKDimensions	tot = {0, 0, 0}

Additional Inherited Members
Protected Attributes inherited from Grid
tdms_flags::InterpolationMethod	interpolation_method

Detailed Description

A complex field defined over a grid. Has real and imaginary components at each (x, y, z) grid point

Constructor & Destructor Documentation

◆ Field() [1/2]

Field::Field ( )

default

Default no arguments constructor

◆ Field() [2/2]

Field::Field	(	int	I_total,
		int	J_total,
		int	K_total )

Constructor of the field with a defined size in the x, y, z Cartesian dimensions

Member Function Documentation

◆ add_to_angular_norm()

void Field::add_to_angular_norm	(	int	n,
		int	Nt,
		SimulationParameters &	params )

Compute the phasor_norm of the current field and add it to the current norm-value.

Note that the calls: add_to_angular_norm(n, Nt, params), and add_to_angular_norm(n % Nt, Nt, params),

are equivalent up to numerical precision when using n = tind, and Nt = Nsteps as set in the main simulation.

Parameters

n	The number of timesteps INTO the current sinusoidal period
Nt	The number of timesteps in a sinusoidal period
params	The simulation parameters

◆ allocate()

void Field::allocate ( )

Allocate the memory appropriate for all the 3D tensors associated with this split field

◆ allocate_and_zero()

void Field::allocate_and_zero ( )

inline

Allocate and set to zero all components of the field

◆ interpolate_over_range() [1/2]

void Field::interpolate_over_range	(	mxArray *	x_out,
		mxArray *	y_out,
		mxArray *	z_out,
		Dimension	mode = Dimension::THREE )

Interpolates the Field over the range provided.

Default range is to interpolate to the midpoint of all consecutive points.

Parameters

[out]	x_out,y_out,z_out	Output arrays for interpolated values
	i_lower,j_lower,k_lower	Lower index for interpolation in the i,j,k directions, respectively
	i_upper,j_upper,k_upper	Upper index for interpolation in the i,j,k directions, respectively
	mode	Determines which field components to compute, based on the simulation Dimension

◆ interpolate_over_range() [2/2]

void Field::interpolate_over_range	(	mxArray *	x_out,
		mxArray *	y_out,
		mxArray *	z_out,
		int	i_lower,
		int	i_upper,
		int	j_lower,
		int	j_upper,
		int	k_lower,
		int	k_upper,
		Dimension	mode = Dimension::THREE )

Interpolates the Field over the range provided.

Default range is to interpolate to the midpoint of all consecutive points.

Parameters

[out]	x_out,y_out,z_out	Output arrays for interpolated values
	i_lower,j_lower,k_lower	Lower index for interpolation in the i,j,k directions, respectively
	i_upper,j_upper,k_upper	Upper index for interpolation in the i,j,k directions, respectively
	mode	Determines which field components to compute, based on the simulation Dimension

◆ interpolate_to_centre_of()

virtual std::complex< double > Field::interpolate_to_centre_of	(	AxialDirection	d,
		CellCoordinate	cell )

pure virtual

Interpolates a Field component to the centre of a Yee cell.

Parameters

d	Field component to interpolate
cell	Index (i,j,k) of the Yee cell to interpolate to the centre of

Returns: std::complex<double> The interpolated field value

Implemented in ElectricField, and MagneticField.

◆ interpolate_transverse_electric_components()

virtual void Field::interpolate_transverse_electric_components	(	CellCoordinate	cell,
		std::complex< double > *	x_at_centre,
		std::complex< double > *	y_at_centre,
		std::complex< double > *	z_at_centre )

pure virtual

Interpolates the Field's transverse electric components to the centre of Yee cell i,j,k.

Parameters

[in]	cell	Yee cell index
[out]	x_at_centre,y_at_centre,z_at_centre	Addresses to write interpolated values for the x,y,z components (respectively)

Implemented in ElectricField, and MagneticField.

◆ interpolate_transverse_magnetic_components()

virtual void Field::interpolate_transverse_magnetic_components	(	CellCoordinate	cell,
		std::complex< double > *	x_at_centre,
		std::complex< double > *	y_at_centre,
		std::complex< double > *	z_at_centre )

pure virtual

Interpolates the Field's transverse magnetic components to the centre of Yee cell i,j,k.

Parameters

[in]	cell	Yee cell index
[out]	x_at_centre,y_at_centre,z_at_centre	Addresses to write interpolated values for the x,y,z components (respectively)

Implemented in ElectricField, and MagneticField.

◆ normalise_volume()

void Field::normalise_volume ( )

Normalises the field entries by dividing by the angular norm.

Specifically, real[c][k][j][i] + i imag[c][k][j][i] = ( real[c][k][j][i] + i imag[c][k][j][i] ) / angular_norm

◆ normalised_difference()

double Field::normalised_difference ( Field & other )

Computes the maximum pointwise absolute difference of the other field to this one, divided by the largest absolute value of this field's components.

Specifically, we compute and return the quantity $\frac{ \max_{i,j,k}(this[k][j][i] - other[k][j][i]) }{ \max_{i,j,k}this[k][j][i] }$ This quantity is used to determine convergence of phasors.

The other field must have the same dimensions as this field.

Parameters

other The other field

Returns: double Maximum relative pointwise absolute difference

◆ set_phasors()

void Field::set_phasors	(	SplitField &	F,
		int	n,
		double	omega,
		double	dt,
		int	Nt )

Set the phasors for this field, given a split field. Result gives field according to the exp(-iwt) convention

Parameters

F	The split-field to read values from
n	The current timestep
omega	Angular frequency
dt	Timestep
Nt	Number of timesteps in a sinusoidal period

◆ set_values_from()

void Field::set_values_from ( Field & other )

Set the values of all components in this field from another, equally sized field

◆ zero()

void Field::zero ( )

Set all the values of all components of the field to zero

Member Data Documentation

◆ il

int Field::il = 0

Upper (u) and lower (l) indices in the x,y,z directions. e.g. il is the first non-pml cell in the i direction and iu the last in the corresponding split field grid

The documentation for this class was generated from the following file:

tdms/include/field.h

Public Member Functions

Public Attributes

Additional Inherited Members

Detailed Description

Constructor & Destructor Documentation

◆ Field() [1/2]

◆ Field() [2/2]

Member Function Documentation

◆ add_to_angular_norm()

◆ allocate()

◆ allocate_and_zero()

◆ interpolate_over_range() [1/2]

◆ interpolate_over_range() [2/2]

◆ interpolate_to_centre_of()

◆ interpolate_transverse_electric_components()

◆ interpolate_transverse_magnetic_components()

◆ normalise_volume()

◆ normalised_difference()

◆ set_phasors()

◆ set_values_from()

◆ zero()

Member Data Documentation

◆ il