sll_c_maxwell_1d_base Type Reference

Inheritance diagram for sll_c_maxwell_1d_base:

Collaboration diagram for sll_c_maxwell_1d_base:

Private Member Functions
procedure(compute_field1_from_field2), deferred	compute_e_from_b
	Solve E and B part of Ampere's law with B constant in time. More...
procedure(compute_field1_from_field2), deferred	compute_b_from_e
	Solve Faraday equation with E constant in time. More...
procedure(signature_compute_field_from_field), deferred	compute_e_from_rho
	Solve E from rho using Poisson. More...
procedure(signature_compute_field_from_field), deferred	compute_rho_from_e
	Compute rho from efield by Gauss law. More...
procedure(signature_compute_E_from_j_1d), deferred	compute_e_from_j
	Solve E from time integrated current (second part of Ampere's law) More...
procedure(signature_compute_phi_from_field), deferred	compute_phi_from_rho
	Solve E from rho using Poisson. More...
procedure(signature_compute_phi_from_field), deferred	compute_phi_from_j
	Solve E from rho using Poisson. More...
procedure(update_dofs_function), deferred	compute_rhs_from_function
	Compute the right-hand-side for a given function f. For Galerkin it is the inner product with the basis functions. For Collocation it is simply a function evaluation at the grid points. More...
procedure(update_dofs_function), deferred	l2projection
	L2 projection. More...
procedure(norm_squared), deferred	l2norm_squared
	Square of the L2norm. More...
procedure(signature_inner_product), deferred	inner_product
	inner product with spline mass matrix More...
procedure(empty), deferred	free
	destructor More...
procedure(signature_mass), deferred	multiply_mass
	product with mass matrix More...
procedure(signature_mass), deferred	invert_mass
	product with inverse mass matrix More...
procedure(multiply_derivative), deferred	multiply_g
	multiplication with gradient matrix More...
procedure(multiply_derivative), deferred	multiply_gt
	multiplication with divergence matrix More...
procedure	compute_curl_part
	Solve source-free Maxwell's equations. More...
procedure	transform_dofs
	By default this is just a copy of input to output. More...

Private Attributes
logical	strong_ampere = .false.
	flag to switch between strong and weak Ampere formulation More...

Detailed Description

Definition at line 25 of file sll_m_maxwell_1d_base.F90.

Member Function/Subroutine Documentation

compute_b_from_e()

procedure(compute_field1_from_field2), deferred compute_b_from_e

private

Solve Faraday equation with E constant in time.

Definition at line 42 of file sll_m_maxwell_1d_base.F90.

compute_curl_part()

procedure compute_curl_part

private

Solve source-free Maxwell's equations.

Definition at line 74 of file sll_m_maxwell_1d_base.F90.

compute_e_from_b()

procedure(compute_field1_from_field2), deferred compute_e_from_b

private

Solve E and B part of Ampere's law with B constant in time.

Definition at line 40 of file sll_m_maxwell_1d_base.F90.

compute_e_from_j()

procedure(signature_compute_E_from_j_1d), deferred compute_e_from_j

private

Solve E from time integrated current (second part of Ampere's law)

Definition at line 48 of file sll_m_maxwell_1d_base.F90.

compute_e_from_rho()

procedure(signature_compute_field_from_field), deferred compute_e_from_rho

private

Solve E from rho using Poisson.

Definition at line 44 of file sll_m_maxwell_1d_base.F90.

compute_phi_from_j()

procedure(signature_compute_phi_from_field), deferred compute_phi_from_j

private

Solve E from rho using Poisson.

Definition at line 52 of file sll_m_maxwell_1d_base.F90.

compute_phi_from_rho()

procedure(signature_compute_phi_from_field), deferred compute_phi_from_rho

private

Solve E from rho using Poisson.

Definition at line 50 of file sll_m_maxwell_1d_base.F90.

compute_rho_from_e()

procedure(signature_compute_field_from_field), deferred compute_rho_from_e

private

Compute rho from efield by Gauss law.

Definition at line 46 of file sll_m_maxwell_1d_base.F90.

compute_rhs_from_function()

procedure(update_dofs_function), deferred compute_rhs_from_function

private

Compute the right-hand-side for a given function f. For Galerkin it is the inner product with the basis functions. For Collocation it is simply a function evaluation at the grid points.

Definition at line 56 of file sll_m_maxwell_1d_base.F90.

free()

procedure(empty), deferred free

private

destructor

Definition at line 64 of file sll_m_maxwell_1d_base.F90.

inner_product()

procedure(signature_inner_product), deferred inner_product

private

inner product with spline mass matrix

Definition at line 62 of file sll_m_maxwell_1d_base.F90.

invert_mass()

procedure(signature_mass), deferred invert_mass

private

product with inverse mass matrix

Definition at line 68 of file sll_m_maxwell_1d_base.F90.

l2norm_squared()

procedure(norm_squared), deferred l2norm_squared

private

Square of the L2norm.

Definition at line 60 of file sll_m_maxwell_1d_base.F90.

l2projection()

procedure(update_dofs_function), deferred l2projection

private

L2 projection.

Definition at line 58 of file sll_m_maxwell_1d_base.F90.

multiply_g()

procedure(multiply_derivative), deferred multiply_g

private

multiplication with gradient matrix

Definition at line 70 of file sll_m_maxwell_1d_base.F90.

multiply_gt()

procedure(multiply_derivative), deferred multiply_gt

private

multiplication with divergence matrix

Definition at line 72 of file sll_m_maxwell_1d_base.F90.

multiply_mass()

procedure(signature_mass), deferred multiply_mass

private

product with mass matrix

Definition at line 66 of file sll_m_maxwell_1d_base.F90.

transform_dofs()

procedure transform_dofs

private

By default this is just a copy of input to output.

Definition at line 76 of file sll_m_maxwell_1d_base.F90.

Member Data Documentation

strong_ampere

logical strong_ampere = .false.

private

flag to switch between strong and weak Ampere formulation

tolerance for the field solver

Definition at line 35 of file sll_m_maxwell_1d_base.F90.