Uses of Class
core.math.Vec3

Packages that use Vec3

core.field	This package contains a number of classes used to create and manipulate the images generated for a given animation of an experiment as it evolves.
core.math	This package contains a variety of classes which handle vector manipulations and the evolution of a given experiment as it evolves.
core.postprocessing	This package performs various operations on the images created by a given simulation of an experiment after the images are created by the classes in core.dflic.
core.rendering	This package handles all the code that draws and evolves the DLIC and the experiment.
simulations.experiments	This package contains all the experiments for the various electromagnetic experiments.
simulations.experiments.electrostatics	This package contains all the experiments for the various electrostatic experiments.
simulations.experiments.faradaysLaw	This package contains all the experiments for the various Faraday's Law experiments.
simulations.experiments.fluidFlow
simulations.experiments.magnetostatics	This package contains all the experiments for the various magnetostatic experiments.
simulations.experiments.radiation	This package contains all the experiments for the various radiation experiments.
simulations.objects	This package contains all the various electromagnetic objects that the experiments assemble for a given experiment.

Uses of Vec3 in core.field

Fields in core.field declared as Vec3

private Vec3	EMVec2Field.origin Coordinate system parameters.
private Vec3	EMVec2Field.xgrid Coordinate system parameters.
private Vec3	EMVec2Field.ygrid Coordinate system parameters.
private Vec3	EMVec2Field.xunit Coordinate system parameters.
private Vec3	EMVec2Field.yunit Coordinate system parameters.
private Vec3	EMVec2Field.r
private Vec3	EMVec2Field.v
private Vec3	EMVec2Field.E
private Vec3	EMVec2Field.B

Methods in core.field that return Vec3

abstract Vec3	Vec3Field.get(Vec3 p, Vec2 xpos, Vec3 f) Sets 'f' to the value of the field at 'p'.
Vec3	Vec3Field.get(Vec3 p) Returns: a new Vec3 with the value of the field at 'p'.
abstract Vec3	Vec2Vec3Field.get(Vec2 p, Vec3 f) Sets 'f' to the value of the field at 'p'.
Vec3	Vec2Vec3Field.get(Vec2 p) Returns: a new Vec3 with the value of the field at 'p'.

Methods in core.field with parameters of type Vec3

abstract Vec3	Vec3Field.get(Vec3 p, Vec2 xpos, Vec3 f) Sets 'f' to the value of the field at 'p'.
Vec3	Vec3Field.get(Vec3 p) Returns: a new Vec3 with the value of the field at 'p'.
abstract Vec3	Vec2Vec3Field.get(Vec2 p, Vec3 f) Sets 'f' to the value of the field at 'p'.
Vec2	EMVec2Field.transform(Vec3 x)
Vec2	EMVec2Field.transformV(Vec3 dx)

Constructors in core.field with parameters of type Vec3

EMVec2Field(BaseObject source, Vec3 center, Vec3 xdir, Vec3 ydir, double scale, int FieldOrMotionFieldType)
Constructs a new EMVec2Field that calculates the type of field specified by "FieldOrMotionFieldType" produced by the EMSource "source".

Uses of Vec3 in core.math

Fields in core.math declared as Vec3

static Vec3	Vec3.Zero should not be modified Zero = the zero vector
static Vec3	Vec3.Xhat should not be modified Xhat = the unit x-axis
static Vec3	Vec3.Yhat should not be modified Yhat = the unit x-axis
static Vec3	Vec3.Zhat should not be modified Zhat = the unit x-axis
static Vec3[]	Vec3.Cartesian should not be modified Cartesian array of the cartesian axes
static Vec3	Vec3.Invalid should not be modified Invalid = an invalid Vec3

Methods in core.math that return Vec3

Vec3	Vec3.getNew() Returns a new Vec2 = (0, 0, 0)
Vec3	Vec3.copy() Returns a copy of 'this'
Vec3	Vec3.Set(Vec3 v) Sets the value of 'this' to that of 'v' Returns: resulting 'this'
Vec3	Vec3.Set(double x, double y, double z) Sets 'this' to (x, y, z) Returns: resulting 'this'
Vec3	Vec3.Set(Vec v) Sets 'this' to 'v' Returns: resulting 'this' Requires: 'v' has dimension 3
Vec3	Vec3.SetZero() Sets 'this' to zero Returns: resulting 'this'
Vec3	Vec3.Add(Vec3 v) Adds 'v' to 'this' Returns: resulting 'this'
Vec3	Vec3.Add(double x, double y, double z) Adds (x, y, z) to 'this' Returns: resulting 'this'
Vec3	Vec3.add(Vec3 v) Returns: a new Vec3 that is the sum of 'this' and 'v'
Vec3	Vec3.add(double x, double y, double z) Returns: a new Vec3 that is the sum of 'this' and (x, y, z)
Vec3	Vec3.AddScaled(Vec3 v, double s) Adds 's*v' to 'this' Returns: resulting 'this'
Vec3	Vec3.AddScaled(double x, double y, double z, double s) Adds 's * (x, y, z)' to 'this' Returns: resulting 'this'
Vec3	Vec3.addscaled(Vec3 v, double s) Returns: a new Vec3 that is the sum of 'this' and 's*v'
Vec3	Vec3.addscaled(double x, double y, double z, double s) Returns: a new Vecc3 that is the sum of 'this' and 's * (x, y, z)'
Vec3	Vec3.Sub(Vec3 v) Subtracts 'v' from 'this' Returns: resulting 'this'
Vec3	Vec3.Sub(double x, double y, double z) Subtracts (x, y, z) from 'this' Returns: resulting 'this'
Vec3	Vec3.sub(Vec3 v) Returns: a new Vec3 that is the difference between 'this' and 'v'
Vec3	Vec3.sub(double x, double y, double z) Returns: a new Vec3 that is the difference between 'this' and (x, y, z)
Vec3	Vec3.Neg() Negates 'this' Returns: resulting 'this'
Vec3	Vec3.neg() Returns: a new Vec3 that is the opposite of 'this'
Vec3	Vec3.Scale(double s) Scales 'this' by 's' Returns: resulting 'this'
Vec3	Vec3.scale(double s) Returns: a new Vec3 that is 's*this'
Vec3	Vec3.Scale(Vec3 v) Scales each component of 'this' by the corresponding component of 'v' Returns: resulting 'this'
Vec3	Vec3.scale(Vec3 v) Returns: a new Vec3 that is 'this' with its components scaled by 'v'
Vec3	Vec3.Unit() Rescales 'this' to be of unit magnitude Returns: resulting 'this' Requires: 'this' is not zero
Vec3	Vec3.unit() Returns: a new Vec3 that is 'this' scaled to unit magnitude Requires: 'this' is not zero
Vec3	Vec3.Cross(Vec3 b) Sets 'this' to be the cross product of 'this' and 'b' Returns: resulting 'this'
Vec3	Vec3.Cross(Vec3 a, Vec3 b) Sets 'this' to be the cross product of 'a' and 'b' Returns: resulting 'this'
Vec3	Vec3.cross(Vec3 b) Returns: a new Vec3 that is the cross product of 'this' and 'b'
Vec3	Vec3.Para(Vec3 d) Isolates the component of 'this' parallel to 'd' Returns: resulting 'this' Requires: 'd' is not zero
Vec3	Vec3.para(Vec3 d) Returns: a new Vec3 that is the component of 'this' parallel to 'd' Requires: 'd' is not zero
Vec3	Vec3.ParaUnit(Vec3 d) Isolates the component of 'this' parallel to 'd' Returns: resulting 'this' Requires: 'd' has unit magnitude
Vec3	Vec3.paraunit(Vec3 d) Returns: a new Vec3 that is the component of 'this' parallel to 'd' Requires: 'd' has unit magnitude
Vec3	Vec3.Perp(Vec3 d) Isolates the component of 'this' perpendicular to 'd' Returns: resulting 'this' Requires: 'd' is not zero
Vec3	Vec3.perp(Vec3 d) Returns: a new Vec2 that is the component of 'this' perpendicular to 'd' Requires: 'd' is not zero
Vec3	Vec3.PerpUnit(Vec3 d) Isolates the component of 'this' perpendicular to 'd' Returns: resulting 'this' Requires: 'd' has unit magnitude
Vec3	Vec3.perpunit(Vec3 d) Returns: a new Vec3 that is the component of 'this' perpendicular to 'd' Requires: 'd' has unit magnitude
Vec3	Vec.toVec3() Returns: a new Vec3 that is equal to "this" Requires: "this" is 3-dimensional

Methods in core.math with parameters of type Vec3

Vec3	Vec3.Set(Vec3 v) Sets the value of 'this' to that of 'v' Returns: resulting 'this'
boolean	Vec3.equals(Vec3 v) Returns: true if 'this' equals 'v', false otherwise
Vec3	Vec3.Add(Vec3 v) Adds 'v' to 'this' Returns: resulting 'this'
Vec3	Vec3.add(Vec3 v) Returns: a new Vec3 that is the sum of 'this' and 'v'
Vec3	Vec3.AddScaled(Vec3 v, double s) Adds 's*v' to 'this' Returns: resulting 'this'
Vec3	Vec3.addscaled(Vec3 v, double s) Returns: a new Vec3 that is the sum of 'this' and 's*v'
Vec3	Vec3.Sub(Vec3 v) Subtracts 'v' from 'this' Returns: resulting 'this'
Vec3	Vec3.sub(Vec3 v) Returns: a new Vec3 that is the difference between 'this' and 'v'
double	Vec3.dot(Vec3 v) Returns: the dot product of 'this' and 'v'
Vec3	Vec3.Scale(Vec3 v) Scales each component of 'this' by the corresponding component of 'v' Returns: resulting 'this'
Vec3	Vec3.scale(Vec3 v) Returns: a new Vec3 that is 'this' with its components scaled by 'v'
Vec3	Vec3.Cross(Vec3 b) Sets 'this' to be the cross product of 'this' and 'b' Returns: resulting 'this'
Vec3	Vec3.Cross(Vec3 a, Vec3 b) Sets 'this' to be the cross product of 'a' and 'b' Returns: resulting 'this'
Vec3	Vec3.cross(Vec3 b) Returns: a new Vec3 that is the cross product of 'this' and 'b'
Vec3	Vec3.Para(Vec3 d) Isolates the component of 'this' parallel to 'd' Returns: resulting 'this' Requires: 'd' is not zero
Vec3	Vec3.para(Vec3 d) Returns: a new Vec3 that is the component of 'this' parallel to 'd' Requires: 'd' is not zero
Vec3	Vec3.ParaUnit(Vec3 d) Isolates the component of 'this' parallel to 'd' Returns: resulting 'this' Requires: 'd' has unit magnitude
Vec3	Vec3.paraunit(Vec3 d) Returns: a new Vec3 that is the component of 'this' parallel to 'd' Requires: 'd' has unit magnitude
Vec3	Vec3.Perp(Vec3 d) Isolates the component of 'this' perpendicular to 'd' Returns: resulting 'this' Requires: 'd' is not zero
Vec3	Vec3.perp(Vec3 d) Returns: a new Vec2 that is the component of 'this' perpendicular to 'd' Requires: 'd' is not zero
Vec3	Vec3.PerpUnit(Vec3 d) Isolates the component of 'this' perpendicular to 'd' Returns: resulting 'this' Requires: 'd' has unit magnitude
Vec3	Vec3.perpunit(Vec3 d) Returns: a new Vec3 that is the component of 'this' perpendicular to 'd' Requires: 'd' has unit magnitude

Constructors in core.math with parameters of type Vec3

Vec3(Vec3 v)
Constructs a new Vec2 = 'v'

Uses of Vec3 in core.postprocessing

Fields in core.postprocessing declared as Vec3

Vec3	Colorizer.symVec3 This is the center of the image, used in reconstructing the vector position in space r if we color by region.
Vec3	Colorizer.Xdir This is the X direction in plotting the image, used in reconstructing the vecor position in space r if we color by region.
Vec3	Colorizer.Ydir This is the Y direction in plotting the image, used in reconstructing the vecor position in space r if we color by region.

Methods in core.postprocessing that return Vec3

Vec3	Colorizer.get(Vec3 p, Vec2 xpos, Vec3 f) Takes the input p which codes the x and y field components at this point in the array and the image value, and returns an RGB color f for the pixel at this point in the array.
private Vec3	Colorizer.ConvertToRGB(float Hue, float Saturation, float Value) Converts our HSV values to RGB values.

Methods in core.postprocessing with parameters of type Vec3

Vec3	Colorizer.get(Vec3 p, Vec2 xpos, Vec3 f) Takes the input p which codes the x and y field components at this point in the array and the image value, and returns an RGB color f for the pixel at this point in the array.
private double	Colorizer.Brighten(double fieldMag, Vec3 p) Brightens the image if we are well above the break point.

Constructors in core.postprocessing with parameters of type Vec3

Colorizer(double MyTargetHue, double MyTargetSaturation, double MyTargetValue, double MysaturationPoint, double MyfallOff, boolean MyBrighten, boolean MyflatColor, Vec RegionColor, BaseExperiment experiment, BaseObject emsource, Vec3 symVec3, Vec3 Xdir, Vec3 Ydir, double scale)
This constructor is used when we are coloring by region.

Uses of Vec3 in core.rendering

Fields in core.rendering declared as Vec3

(package private) Vec3	Renderer.Xdir Unit axis for the X-direction of the image
(package private) Vec3	Renderer.Ydir Unit axis for the Y-direction of the image
(package private) Vec3	Renderer.origin The origin for the plot, non-zero and used only when there is no symmerty

Methods in core.rendering that return Vec3

Vec3	Renderer.GetOrigin() GetOrigin() returns the origin of the plot, non-zero only if there is no symmetry.
Vec3	Renderer.GetXdir() Get the X coordinate unit vector of the image.
Vec3	Renderer.GetYdir() Get the Y coordinate unit vector of the image.

Methods in core.rendering with parameters of type Vec3

void	Renderer.SetOrigin(Vec3 Origin) SetOrigin() sets the origin of the plot, non-zero only if there is no symmetry.
void	Renderer.SetXdir(Vec3 myXdir) Set the X coordinate unit vector of the image.
void	Renderer.SetYdir(Vec3 myYdir) Set the Y coordinate unit vector of the image.

Uses of Vec3 in simulations.experiments

Methods in simulations.experiments with parameters of type Vec3

abstract double	BaseExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor)
abstract double	BaseExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow)

Uses of Vec3 in simulations.experiments.electrostatics

Methods in simulations.experiments.electrostatics with parameters of type Vec3

double	TwoChargesExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	TwoChargesExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	ColorTestExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow, Vec RegionParameter)
double	ColorTestExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	ColorTestExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	ChargeInFieldExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	ChargeInFieldExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.

Uses of Vec3 in simulations.experiments.faradaysLaw

Methods in simulations.experiments.faradaysLaw with parameters of type Vec3

double	TwoPlanesExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	TwoPlanesExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	RecedingImageExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	RecedingImageExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	MovingReceedingImageExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	MovingReceedingImageExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	MovingRecedingImagePotentialExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	MovingRecedingImagePotentialExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	FallingRingExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	FallingRingExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	EddyCurrentsMonopoleExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	EddyCurrentsMonopoleExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	EddyCurrentsDipoleExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	EddyCurrentsDipoleExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.

Uses of Vec3 in simulations.experiments.fluidFlow

Fields in simulations.experiments.fluidFlow declared as Vec3

private Vec3

HeliosphereFlowExperiment.Xsun The position of the Sun.

Methods in simulations.experiments.fluidFlow with parameters of type Vec3

double	HeliosphereFlowExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor)
double	HeliosphereFlowExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow)
double	DataInputExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	DataInputExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	CirculatingFlowExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	CirculatingFlowExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.

Constructors in simulations.experiments.fluidFlow with parameters of type Vec3

HeliosphereFlowExperiment(double radiusBowShock, double radiusTerminationShock, Vec3 Xsun)
Constructs the heliosphere using two parameters

Uses of Vec3 in simulations.experiments.magnetostatics

Methods in simulations.experiments.magnetostatics with parameters of type Vec3

double	TeachSpinExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	TeachSpinExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.

Uses of Vec3 in simulations.experiments.radiation

Methods in simulations.experiments.radiation with parameters of type Vec3

double	OscillatingDipoleExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	OscillatingDipoleExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.
double	ElectricAntennaExperiment.getHue(double TargetHue, Vec3 r, Vec RegionColor) Method to find the hue in a given region when we are coloring according to region (Color Mode 4).
double	ElectricAntennaExperiment.getFlowSpeed(Vec3 r, Vec RegionFlow) Method to find the flow speed in a given region when we are determining that speed according to region.

Uses of Vec3 in simulations.objects

Fields in simulations.objects declared as Vec3

Vec3	PointCharge.p the position of the point charge
Vec3	MovingPointCharge.v Velocity of the charge
Vec3	MovingPointCharge.a acceleration of the charge.
private Vec3	MovingMagneticField.B
private Vec3	MovingMagneticField.VelB
Vec3	MagneticMonopole.p The position of the monopole.
Vec3	MagneticMonopole.v The velocity of the charge.
Vec3	MagneticDipoleStatic.p
Vec3	MagneticDipoleStatic.v
Vec3	MagneticDipoleStatic.dipole
Vec3	MagneticDipoleStatic.omega
Vec3	MagneticDipole.p
Vec3	MagneticDipole.v
Vec3	MagneticDipole.m
Vec3	LineMagneticMonopoles.p
Vec3	LineCurrent.p
Vec3	Line3DMagneticDipoles.mdipole the magnetic dipole moment per unit length vector of the line of dipoles
Vec3	Line3DMagneticDipoles.tline A unit vector along the axis of the line of dipoles
Vec3	Line3DMagneticDipoles.p the position of the beginning of the line of dipoles
Vec3	Line3DMagneticDipoles.v Velocity of the line of magnetic dipoles
Vec3	ISMfield.p the position of the sun
Vec3	InfiniteWire.p
Vec3	InfiniteWire.d
Vec3	InfiniteWire.v
Vec3	HelioField.p the position of the sun
(package private) Vec3[]	EMTransform.rot
(package private) Vec3[]	EMTransform.invrot
(package private) Vec3	EMTransform.origin
private Vec3	EMTransform.temp
private Vec3	EMCollection.temp a temporary location for computation of the total electric field and etc.
Vec3	ElectromagneticPlaneWave.k The propagation vector k
Vec3	ElectromagneticPlaneWave.Pol the polarization vector of the electric field
Vec3	ElectricDipoleStatic.p
Vec3	ElectricDipoleStatic.v
Vec3	ElectricDipoleStatic.dipole
Vec3	ElectricDipoleStatic.omega
Vec3	ElectricDipoleRotating.x The position of the dipole.
Vec3	ElectricDipole.x The position of the dipole.
Vec3	ElectricDipole.v The constant velocity of the dipole.
Vec3	ElectricDipole.p The dipole moment of the dipole.
Vec3	ElectricAntenna.x The position of the antenna.
Vec3	CurrentSheet.x
Vec3	CurrentSheet.K
Vec3	CurrentRing.p the observer"s location where we are going to calculate the fields
Vec3	CurrentRing.c center of the ring
Vec3	CurrentRing.d unit vector along the direction of the rings axis, defines the direction of positive current
Vec3	CurrentRing.v the velocity of the ring
Vec3	CurrentRing.omega the angular velocity vector of the ring, omega cross r from center gives the angular speed
private Vec3	CurrentRing.LastX the last calculated location, stored to avoid unnecessary calculations
private Vec3	CurrentRing.LastB the last calculated B field value, stored to avoid unnecessary calculations
private Vec3	CurrentRing.LastE the last calculated E field value, stored to avoid unnecessary calculations
private Vec3	ConstantFields.E
private Vec3	ConstantFields.B
Vec3	ChargeRingFinite.p
Vec3	ChargeRingFinite.d

Methods in simulations.objects that return Vec3

Vec3	TwoPlanes.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the upper half plane
Vec3	TwoPlanes.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
Vec3	PointCharge.Efield(Vec3 x, Vec3 E) the electric field of a stationary point charge
Vec3	PointCharge.Bfield(Vec3 x, Vec3 B) the magnetic field of a stationary point charge (zero)
Vec3	MovingRecedingImagePotentialBelow.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the lower half plane
Vec3	MovingRecedingImagePotentialBelow.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
Vec3	MovingRecedingImagePotentialAbove.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the upper half plane
Vec3	MovingRecedingImagePotentialAbove.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
Vec3	MovingPointCharge.Efield(Vec3 x, Vec3 E) the non-relativistic electric field of a moving point charge
Vec3	MovingPointCharge.Bfield(Vec3 x, Vec3 B) the non-relativistic magnetic field of a moving point charge (v x E )
Vec3	MovingPointCharge.Pfield(Vec3 x, Vec3 P) The Pauli field of a moving point charge.
Vec3	MovingMagneticField.Bfield(Vec3 x, Vec3 B)
Vec3	MovingMagneticField.Efield(Vec3 x, Vec3 E)
Vec3	MagneticMonopole.Bfield(Vec3 x, Vec3 B) Computes the magnetic field of a non-relativistic magnetic monopole.
Vec3	MagneticMonopole.Efield(Vec3 x, Vec3 E) The electric field of a moving monopole.
Vec3	MagneticDipoleStatic.getM(double dt)
Vec3	MagneticDipoleStatic.Bfield(Vec3 x, Vec3 B)
Vec3	MagneticDipoleStatic.Efield(Vec3 x, Vec3 E)
Vec3	MagneticDipoleStatic.Pfield(Vec3 x, Vec3 P)
Vec3	MagneticDipole.Efield(Vec3 x, Vec3 E)
Vec3	MagneticDipole.Bfield(Vec3 x, Vec3 B)
Vec3	LineMagneticMonopoles.Efield(Vec3 x, Vec3 E)
Vec3	LineMagneticMonopoles.Bfield(Vec3 x, Vec3 B)
Vec3	LineCurrent.Efield(Vec3 x, Vec3 E)
Vec3	LineCurrent.Bfield(Vec3 x, Vec3 B)
Vec3	Line3DMagneticDipoles.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic line of moving magnetic dipoles
Vec3	Line3DMagneticDipoles.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole
Vec3	ISMfield.Efield(Vec3 x, Vec3 E) constant electric field except for a sphere centered at p where the field is zero
Vec3	ISMfield.Bfield(Vec3 x, Vec3 B) the magnetic field (zero)
Vec3	InfiniteWire.Efield(Vec3 x, Vec3 E)
Vec3	InfiniteWire.Bfield(Vec3 x, Vec3 B)
Vec3	HelioField.Efield(Vec3 x, Vec3 E) inverse distance squared field
Vec3	HelioField.Bfield(Vec3 x, Vec3 B) the magnetic field (zero)
Vec3	EMTransform.Efield(Vec3 x, Vec3 E)
Vec3	EMTransform.Bfield(Vec3 x, Vec3 B)
Vec3	EMCollection.Efield(Vec3 x, Vec3 E) This method computes the total electric field of all the EM objects in the collection
Vec3	EMCollection.Bfield(Vec3 x, Vec3 B) This method computes the total magnetic field of all the EM objects in the collection
Vec3	EMCollection.Pfield(Vec3 x, Vec3 P) This method computes the total Pauli field of all the EM objects in the collection
Vec3	ElectromagneticPlaneWave.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectromagneticPlaneWave.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricOscillatingDipole.getP(double dt) Returns the dipole moment at a time retarded by dt.
Vec3	ElectricOscillatingDipole.getDP(double dt) Returns the first time derivative of the dipole moment at a time retarded by dt We use the method getT to find out the current time of the dipole
Vec3	ElectricOscillatingDipole.getDDP(double dt) Returns the second time derivative of the dipole moment at a time retarded by dt.
Vec3	ElectricDipoleStatic.getP(double dt)
Vec3	ElectricDipoleStatic.Efield(Vec3 x, Vec3 E)
Vec3	ElectricDipoleStatic.Bfield(Vec3 x, Vec3 B)
Vec3	ElectricDipoleStatic.Pfield(Vec3 x, Vec3 P)
Vec3	ElectricDipoleRotating.getP(double dt) Returns the dipole moment at a time retarded by dt.
Vec3	ElectricDipoleRotating.getDP(double dt) Returns the first time derivative of the dipole moment at a time retarded by dt We use the method getT to find out the current time of the dipole
Vec3	ElectricDipoleRotating.getDDP(double dt) Returns the second time derivative of the dipole moment at a time retarded by dt.
Vec3	ElectricDipoleRotating.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectricDipoleRotating.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricDipole.getP(double dtretarded) Get the dipole moment vector.
Vec3	ElectricDipole.getDP(double dtretarded) Get the time derivative of dipole moment vector of the dipole.
Vec3	ElectricDipole.getDDP(double dtretarded) Get the second time derivative of dipole moment vector of the dipole.
Vec3	ElectricDipole.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectricDipole.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricAntenna.Efield(Vec3 x, Vec3 E) The electric field of the linear antenna.
Vec3	ElectricAntenna.Bfield(Vec3 x, Vec3 B) The magnetic field of the linear antenna.
Vec3	EflowXY.Efield(Vec3 x, Vec3 E)
Vec3	EflowXY.Bfield(Vec3 x, Vec3 B)
Vec3	EddyCurrents.Bfield(Vec3 X, Vec3 B) The eddy current of a moving monopole.
Vec3	EddyCurrents.Efield(Vec3 x, Vec3 E) This "E" field has no meaning for this object, as we are only using this object to calcuate the eddy current in the xy plane and put it in Bfield.
Vec3	DataInputObject.Efield(Vec3 x, Vec3 E) The method that returns the E field.
Vec3	DataInputObject.Bfield(Vec3 x, Vec3 B) The method that returns the input velocity array evalutated at a position x on the screen.
Vec3	CurrentSheet.getK(double dt)
Vec3	CurrentSheet.Efield(Vec3 xobs, Vec3 E)
Vec3	CurrentSheet.Bfield(Vec3 x, Vec3 B)
Vec3	CurrentRing.Efield(Vec3 x, Vec3 E) Sets "E" to the value of the electric field at "x".
Vec3	CurrentRing.Bfield(Vec3 x, Vec3 B) Sets "B" to the value of the magnetic field at "x".
Vec3	ConstantFields.Efield(Vec3 x, Vec3 E)
Vec3	ConstantFields.Bfield(Vec3 x, Vec3 B)
Vec3	ColorTestField.Efield(Vec3 x, Vec3 E) the electric field of our color test field
Vec3	ColorTestField.Bfield(Vec3 x, Vec3 B) the magnetic field of the color test field is zero
Vec3	ChargeRingFinite.Efield(Vec3 x, Vec3 E)
Vec3	ChargeRingFinite.Bfield(Vec3 x, Vec3 B)
abstract Vec3	BaseObject.Efield(Vec3 x, Vec3 E) Sets 'E' to the value of the electric field at 'x'.
abstract Vec3	BaseObject.Bfield(Vec3 x, Vec3 B) Sets 'B' to the value of the magnetic field at 'x'.
Vec3	BaseObject.Pfield(Vec3 x, Vec3 P) Sets 'P' to the value of the Pauli field at 'x'.
Vec3	BaseObject.Efield(Vec3 x) Returns: a new Vec3 with the value of the electric field at 'x'.
Vec3	BaseObject.Pfield(Vec3 x) Returns: a new Vec3 with the value of the Pauli field at 'x'.
Vec3	BaseObject.Bfield(Vec3 x) Returns: a new Vec3 with the value of the magnetic field at 'x'.

Methods in simulations.objects with parameters of type Vec3

Vec3	TwoPlanes.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the upper half plane
Vec3	TwoPlanes.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
double	TwoPlanes.Potential1(Vec3 x, double potential) the potential in the first quadrant x>0, z>0
double	TwoPlanes.Potential2(Vec3 x, double potential) the potential in the second quadrant x<0, z>0
double	TwoPlanes.Potential3(Vec3 x, double potential) the potential in the third quadrant x<0, z<0
double	TwoPlanes.Potential4(Vec3 x, double potential) the potential in the fourth quadrant x>0, z<0
Vec3	PointCharge.Efield(Vec3 x, Vec3 E) the electric field of a stationary point charge
Vec3	PointCharge.Bfield(Vec3 x, Vec3 B) the magnetic field of a stationary point charge (zero)
Vec3	MovingRecedingImagePotentialBelow.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the lower half plane
Vec3	MovingRecedingImagePotentialBelow.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
double	MovingRecedingImagePotentialBelow.Potential(Vec3 x, double potential) the potential of a moving monopole in the upper halfplane
Vec3	MovingRecedingImagePotentialAbove.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic moving magnetic monopole in the upper half plane
Vec3	MovingRecedingImagePotentialAbove.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole, which currently we set to zero
double	MovingRecedingImagePotentialAbove.Potential(Vec3 x, double potential) the potential of a moving monopole in the upper halfplane
void	MovingPointCharge.Acceleration(Vec3 a) Sets the acceleration
Vec3	MovingPointCharge.Efield(Vec3 x, Vec3 E) the non-relativistic electric field of a moving point charge
Vec3	MovingPointCharge.Bfield(Vec3 x, Vec3 B) the non-relativistic magnetic field of a moving point charge (v x E )
Vec3	MovingPointCharge.Pfield(Vec3 x, Vec3 P) The Pauli field of a moving point charge.
Vec3	MovingMagneticField.Bfield(Vec3 x, Vec3 B)
Vec3	MovingMagneticField.Efield(Vec3 x, Vec3 E)
Vec3	MagneticMonopole.Bfield(Vec3 x, Vec3 B) Computes the magnetic field of a non-relativistic magnetic monopole.
Vec3	MagneticMonopole.Efield(Vec3 x, Vec3 E) The electric field of a moving monopole.
Vec3	MagneticDipoleStatic.Bfield(Vec3 x, Vec3 B)
Vec3	MagneticDipoleStatic.Efield(Vec3 x, Vec3 E)
Vec3	MagneticDipoleStatic.Pfield(Vec3 x, Vec3 P)
Vec3	MagneticDipole.Efield(Vec3 x, Vec3 E)
Vec3	MagneticDipole.Bfield(Vec3 x, Vec3 B)
Vec3	LineMagneticMonopoles.Efield(Vec3 x, Vec3 E)
Vec3	LineMagneticMonopoles.Bfield(Vec3 x, Vec3 B)
Vec3	LineCurrent.Efield(Vec3 x, Vec3 E)
Vec3	LineCurrent.Bfield(Vec3 x, Vec3 B)
Vec3	Line3DMagneticDipoles.Bfield(Vec3 x, Vec3 B) the magnetic field of a non-relativistic line of moving magnetic dipoles
Vec3	Line3DMagneticDipoles.Efield(Vec3 x, Vec3 E) the electric field of a moving monopole
Vec3	ISMfield.Efield(Vec3 x, Vec3 E) constant electric field except for a sphere centered at p where the field is zero
Vec3	ISMfield.Bfield(Vec3 x, Vec3 B) the magnetic field (zero)
Vec3	InfiniteWire.Efield(Vec3 x, Vec3 E)
Vec3	InfiniteWire.Bfield(Vec3 x, Vec3 B)
Vec3	HelioField.Efield(Vec3 x, Vec3 E) inverse distance squared field
Vec3	HelioField.Bfield(Vec3 x, Vec3 B) the magnetic field (zero)
void	EMTransform.Translation(Vec3 trans)
void	EMTransform.Rotation(Vec3 axis, double angle)
void	EMTransform.RigidTransform(Vec3 axis, double angle, Vec3 trans)
Vec3	EMTransform.Efield(Vec3 x, Vec3 E)
Vec3	EMTransform.Bfield(Vec3 x, Vec3 B)
Vec3	EMCollection.Efield(Vec3 x, Vec3 E) This method computes the total electric field of all the EM objects in the collection
Vec3	EMCollection.Bfield(Vec3 x, Vec3 B) This method computes the total magnetic field of all the EM objects in the collection
Vec3	EMCollection.Pfield(Vec3 x, Vec3 P) This method computes the total Pauli field of all the EM objects in the collection
Vec3	ElectromagneticPlaneWave.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectromagneticPlaneWave.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricDipoleStatic.Efield(Vec3 x, Vec3 E)
Vec3	ElectricDipoleStatic.Bfield(Vec3 x, Vec3 B)
Vec3	ElectricDipoleStatic.Pfield(Vec3 x, Vec3 P)
Vec3	ElectricDipoleRotating.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectricDipoleRotating.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricDipole.Efield(Vec3 x, Vec3 E) Compute the electric field at position x and time t
Vec3	ElectricDipole.Bfield(Vec3 x, Vec3 B) Compute the magnetic field at position x and time t
Vec3	ElectricAntenna.Efield(Vec3 x, Vec3 E) The electric field of the linear antenna.
Vec3	ElectricAntenna.Bfield(Vec3 x, Vec3 B) The magnetic field of the linear antenna.
Vec3	EflowXY.Efield(Vec3 x, Vec3 E)
Vec3	EflowXY.Bfield(Vec3 x, Vec3 B)
Vec3	EddyCurrents.Bfield(Vec3 X, Vec3 B) The eddy current of a moving monopole.
Vec3	EddyCurrents.Efield(Vec3 x, Vec3 E) This "E" field has no meaning for this object, as we are only using this object to calcuate the eddy current in the xy plane and put it in Bfield.
Vec3	DataInputObject.Efield(Vec3 x, Vec3 E) The method that returns the E field.
Vec3	DataInputObject.Bfield(Vec3 x, Vec3 B) The method that returns the input velocity array evalutated at a position x on the screen.
Vec3	CurrentSheet.Efield(Vec3 xobs, Vec3 E)
Vec3	CurrentSheet.Bfield(Vec3 x, Vec3 B)
private void	CurrentRing.CalculateFields(Vec3 x) Computes both the electric and magnetic fields at the observer"s position.
Vec3	CurrentRing.Efield(Vec3 x, Vec3 E) Sets "E" to the value of the electric field at "x".
Vec3	CurrentRing.Bfield(Vec3 x, Vec3 B) Sets "B" to the value of the magnetic field at "x".
Vec3	ConstantFields.Efield(Vec3 x, Vec3 E)
Vec3	ConstantFields.Bfield(Vec3 x, Vec3 B)
Vec3	ColorTestField.Efield(Vec3 x, Vec3 E) the electric field of our color test field
Vec3	ColorTestField.Bfield(Vec3 x, Vec3 B) the magnetic field of the color test field is zero
Vec3	ChargeRingFinite.Efield(Vec3 x, Vec3 E)
Vec3	ChargeRingFinite.Bfield(Vec3 x, Vec3 B)
abstract Vec3	BaseObject.Efield(Vec3 x, Vec3 E) Sets 'E' to the value of the electric field at 'x'.
abstract Vec3	BaseObject.Bfield(Vec3 x, Vec3 B) Sets 'B' to the value of the magnetic field at 'x'.
Vec3	BaseObject.Pfield(Vec3 x, Vec3 P) Sets 'P' to the value of the Pauli field at 'x'.
Vec3	BaseObject.Efield(Vec3 x) Returns: a new Vec3 with the value of the electric field at 'x'.
Vec3	BaseObject.Pfield(Vec3 x) Returns: a new Vec3 with the value of the Pauli field at 'x'.
Vec3	BaseObject.Bfield(Vec3 x) Returns: a new Vec3 with the value of the magnetic field at 'x'.

Constructors in simulations.objects with parameters of type Vec3

PointCharge(double q, Vec3 p, double radius)
constructor for the point charge setting Pauli radius

PointCharge(double q, Vec3 p)
constructor for the point charge with radius set to 5.

MovingPointCharge(double q, Vec3 p, double radius)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, double radius, double power)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, double radius, Vec3 v)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, double radius, double power, Vec3 v)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, double radius, double power, Vec3 v, Vec3 a)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, Vec3 v)
Constructor for the moving point charge.

MovingPointCharge(double q, Vec3 p, Vec3 v, Vec3 a)
Constructor for the moving point charge.

MovingMagneticField(Vec3 B, Vec3 VelB)

MagneticMonopole(double q, Vec3 p, Vec3 v, double zplane, int image, double radius)
Constructor for the monopole.

MagneticDipoleStatic(Vec3 p, Vec3 dipole, Vec3 omega, double radius)

MagneticDipoleStatic(Vec3 p, Vec3 v, Vec3 dipole, Vec3 omega, double radius)

MagneticDipole(Vec3 p, Vec3 m)

MagneticDipole(Vec3 p, Vec3 v, Vec3 m)

LineMagneticMonopoles(double lambda, Vec3 p, double radius)

LineMagneticMonopoles(double lambda, Vec3 p)

LineCurrent(double i, Vec3 p, double radius)

LineCurrent(double i, Vec3 p)

Line3DMagneticDipoles(Vec3 mdipole, Vec3 tline, Vec3 p, Vec3 v, double zplane, int image)
constructor for the line of dipoles

ISMfield(double radius, Vec3 p)
constructor

InfiniteWire(double I, Vec3 p, Vec3 d)

InfiniteWire(double I, double dIdt, Vec3 p, Vec3 d)

InfiniteWire(double I, Vec3 p, Vec3 d, Vec3 v)

InfiniteWire(double I, double dIdt, Vec3 p, Vec3 d, Vec3 v)

HelioField(double radius, Vec3 p)
constructor

ElectromagneticPlaneWave(Vec3 k, double omega, double E0, Vec3 Pol, double phase)
Create an electromagnetic plane wave

ElectricOscillatingDipole(Vec3 x, Vec3 p, double p0, double p1, double omega, double phase)
Constructs an ElectricOscillatingDipole centered at "x" at t = 0.

ElectricDipoleStatic(Vec3 p, Vec3 dipole, Vec3 omega, double radius)

ElectricDipoleStatic(Vec3 p, Vec3 v, Vec3 dipole, Vec3 omega, double radius)

ElectricDipoleRotating(Vec3 x, double p0, double omega, double theta)
Create an electric dipole

ElectricDipole(Vec3 x, Vec3 p)
Create an electric dipole with zero velocity at t = 0.

ElectricDipole(Vec3 x, Vec3 v, Vec3 p)
Create an electric dipole with non-zero velocity at t = 0.

ElectricAntenna(Vec3 x, double k, double ak, double w, double ta)
constructor for the linear antenna

CurrentSheet(Vec3 x, Vec3 K, double Econstant)

CurrentRing(Vec3 p, Vec3 d, double R, double I)
Constructs a new Current ring.

CurrentRing(Vec3 p, Vec3 d, double R, double I, Vec3 v)
Constructs a new Current ring.

CurrentRing(Vec3 p, Vec3 d, double R, double I, double dIdt)
Constructs a new Current ring.

CurrentRing(Vec3 p, Vec3 d, double R, double I, Vec3 v, Vec3 omega)
Constructs a new Current ring.

ConstantFields(Vec3 E, Vec3 B)

ChargeRingFinite(Vec3 p, Vec3 d, double R, int Ncharges, double q)