def __init__(self, datafile):
test_data = pickle.load(datafile)
self.desired_dofnos = test_data['dofnos']
self.desired_rhs_contribs = test_data['rhs_contribs']
self.discretisation_order = test_data['order']
self.mesh = get_centred_cube(
test_data['domain_size'], test_data['max_edge_len'])
self.discretisation_space = dolfin.FunctionSpace(
self.mesh, "Nedelec 1st kind H(curl)", self.discretisation_order)
self.no_integration_points = test_data['no_integration_points']
self.I = test_data['I']
self.source_endpoints = test_data['source_endpoints']
def __init__(self, datafile):
test_data = pickle.load(datafile)
ff_result_data = test_data['ff_result_data']
nf_input_data = test_data['nf_input_data']
self.desired_E_ff = ff_result_data['E_ff']
self.desired_E_theta = self.desired_E_ff[:,0]
self.desired_E_phi = self.desired_E_ff[:,1]
self.theta_coords = ff_result_data['theta_deg']
self.phi_coords = ff_result_data['phi_deg']
self.discretisation_order = nf_input_data['order']
self.mesh = get_centred_cube(
nf_input_data['domain_size'], nf_input_data['max_edge_len'])
self.discretisation_space = dolfin.FunctionSpace(
self.mesh, "Nedelec 1st kind H(curl)", self.discretisation_order)
self.discretisation_dofs = nf_input_data['x']
self.frequency = nf_input_data['freq']
def __init__(self):
### Problem parameters
self.freq = 1.0e+9 # Frequency
self.lam = c0/self.freq
self.l = self.lam/10 # Dipole length
self.I = 1.0 # Dipole current
self.source_direction = np.array([0,0,1.]) # Source orientation
self.source_centre = np.array([0,0,0.]) # Position of the source
self.source_endpoints = np.array(
[-self.source_direction*self.l/2, self.source_direction*self.l/2]) \
+ self.source_centre
### Discretisation settings
self.order = 2
self.domain_size = np.array([self.lam]*3)*0.5
self.max_edge_len = self.lam/6
self.mesh = get_centred_cube(self.domain_size, self.max_edge_len)
## Set up materials function with all free-space
material_mesh_func = dolfin.MeshFunction('uint', self.mesh, 3)
material_mesh_func.set_all(0)
materials = {0:dict(eps_r=1, mu_r=1),}
## Set up 1st-order analytical ABC
abc = sucemfem.BoundaryConditions.ABC.ABCBoundaryCondition()
abc.set_region_number(1)
bcs = sucemfem.BoundaryConditions.container.BoundaryConditions()
bcs.add_boundary_condition(abc)
## Set up high level problem class
dp = sucemfem.ProblemConfigurations.EMDrivenProblem.DrivenProblemABC()
dp.set_mesh(self.mesh)
dp.set_basis_order(self.order)
dp.set_material_regions(materials)
dp.set_region_meshfunction(material_mesh_func)
dp.set_boundary_conditions(bcs)
## Set up current fillament source
current_sources = sucemfem.Sources.current_source.CurrentSources()
fillament_source = sucemfem.Sources.fillament_current_source.FillamentCurrentSource()
fillament_source.set_source_endpoints(self.source_endpoints)
fillament_source.set_value(self.I)
current_sources.add_source(fillament_source)
## Set source in problem container
dp.set_sources(current_sources)
self.problem = dp
self.function_space = dp.function_space
def test_ff_error(self):
sucemfem.Utilities.Optimization.set_dolfin_optimisation(True)
### Postprocessing requests
theta_deg = N.linspace(10, 170, 161)
no_ff_pts = len(theta_deg)
phi_deg = N.zeros(no_ff_pts)
### Problem parameters
freq = 1.0e+9 # Frequency
lam = c0/freq
l = lam/4 # Dipole length
I = 1.0 # Dipole current
source_direction_z = N.array([0,0,1.]) # Source orientation
source_direction_x = N.array([1.,0,0]) # Source orientation
source_direction_y = N.array([0,1,0.]) # Source orientation
source_centre = N.array([0,0,0.]) # Position of the source
source_endpoints_z = N.array(
[-source_direction_z*l/2, source_direction_z*l/2]) + source_centre
source_endpoints_x = N.array(
[-source_direction_x*l/2, source_direction_x*l/2]) + source_centre
source_endpoints_y = N.array(
[-source_direction_y*l/2, source_direction_y*l/2]) + source_centre
### Discretisation settings
order = 2
domain_size = N.array([lam]*3)*1
max_edge_len = lam/6
mesh = get_centred_cube(domain_size, max_edge_len)
### Implementation
#
## Set up materials function with all free-space
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {0:dict(eps_r=1, mu_r=1),}
## Set up 1st-order analytical ABC
abc = ABCBoundaryCondition()
abc.set_region_number(1)
bcs = BoundaryConditions()
bcs.add_boundary_condition(abc)
## Set up high level problem class
dp = DrivenProblemABC()
dp.set_mesh(mesh)
dp.set_basis_order(order)
dp.set_material_regions(materials)
dp.set_region_meshfunction(material_mesh_func)
dp.set_boundary_conditions(bcs)
## Set up current fillament source
current_sources = sucemfem.Sources.current_source.CurrentSources()
fillament_source = FillamentCurrentSource()
fillament_source.no_integration_points = 1000
fillament_source.set_source_endpoints(source_endpoints_z)
fillament_source.set_value(I)
current_sources.add_source(fillament_source)
## Set source in problem container
dp.set_sources(current_sources)
dp.init_problem()
dp.set_frequency(freq)
## Get sytem LHS matrix and RHS Vector
A = dp.get_LHS_matrix()
b_z = dp.get_RHS()
fillament_source.set_source_endpoints(source_endpoints_x)
b_x = dp.get_RHS()
fillament_source.set_source_endpoints(source_endpoints_y)
b_y = dp.get_RHS()
#import pdb ; pdb.set_trace()
A
print 'solve using UMFPack'
umf_solver = sucemfem.Utilities.LinalgSolvers.UMFPACKSolver(A)
x_z = umf_solver.solve(b_z)
x_x = umf_solver.solve(b_x)
x_y = umf_solver.solve(b_y)
## Post-process solution to obtain far-field
print 'calculating far field'
surf_ntff = surface_ntff.NTFF(dp.function_space)
surf_ntff.set_dofs(x_z)
surf_ntff.set_frequency(freq)
surf_E_ff_z = N.array([surf_ntff.calc_pt(th_deg, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)])
surf_E_theta_z = surf_E_ff_z[:,0]
surf_E_phi_z = surf_E_ff_z[:,1]
surf_ntff.set_dofs(x_x)
surf_E_ff_x = N.array([surf_ntff.calc_pt(th_deg+90, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)])
surf_E_theta_x = surf_E_ff_x[:,0]
surf_E_phi_x = surf_E_ff_x[:,1]
surf_ntff.set_dofs(x_y)
surf_E_ff_y = N.array([surf_ntff.calc_pt(th_deg+90, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)])
surf_E_theta_y = surf_E_ff_y[:,0]
surf_E_phi_y = surf_E_ff_y[:,1]
## Calculate some errors relative to the analytical solution
an_E_theta = [current_fillament_farfield.eval_E_theta(freq, l, I, th)
for th in N.deg2rad(theta_deg)]
err_z = normalised_RMS(
surf_E_theta_z, an_E_theta, surf_E_phi_z)
err_theta_z = normalised_RMS(surf_E_theta_z, an_E_theta)
err_abs_theta_z = normalised_RMS(N.abs(surf_E_theta_z),
N.abs(an_E_theta))
err_x = normalised_RMS(
surf_E_theta_x, an_E_theta, surf_E_phi_x)
err_theta_x = normalised_RMS(surf_E_theta_x, an_E_theta)
err_abs_theta_x = normalised_RMS(N.abs(surf_E_theta_x),
N.abs(an_E_theta))
err_y = normalised_RMS(
surf_E_theta_y, an_E_theta, surf_E_phi_y)
err_theta_y = normalised_RMS(surf_E_theta_y, an_E_theta)
err_abs_theta_y = normalised_RMS(N.abs(surf_E_theta_y),
N.abs(an_E_theta))
print 'Far-field RMS error: ', err_z, err_x, err_y
# Expected error for lam/6 mesh, 2nd order discretisation,
# lam/4 current fillament source is ~4.685%
self.assertTrue(err_z < 4.7)
self.assertTrue(err_x < 4.7)
self.assertTrue(err_z < 4.7)
def test_ff_error(self):
sucemfem.Utilities.Optimization.set_dolfin_optimisation(True)
### Postprocessing requests
theta_deg = N.linspace(10, 170, 161)
no_ff_pts = len(theta_deg)
phi_deg = N.zeros(no_ff_pts)
### Problem parameters
freq = 1.0e+9 # Frequency
lam = c0 / freq
l = lam / 4 # Dipole length
I = 1.0 # Dipole current
source_direction_z = N.array([0, 0, 1.]) # Source orientation
source_direction_x = N.array([1., 0, 0]) # Source orientation
source_direction_y = N.array([0, 1, 0.]) # Source orientation
source_centre = N.array([0, 0, 0.]) # Position of the source
source_endpoints_z = N.array([
-source_direction_z * l / 2, source_direction_z * l / 2
]) + source_centre
source_endpoints_x = N.array([
-source_direction_x * l / 2, source_direction_x * l / 2
]) + source_centre
source_endpoints_y = N.array([
-source_direction_y * l / 2, source_direction_y * l / 2
]) + source_centre
### Discretisation settings
order = 2
domain_size = N.array([lam] * 3) * 1
max_edge_len = lam / 6
mesh = get_centred_cube(domain_size, max_edge_len)
### Implementation
#
## Set up materials function with all free-space
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {
0: dict(eps_r=1, mu_r=1),
}
## Set up 1st-order analytical ABC
abc = ABCBoundaryCondition()
abc.set_region_number(1)
bcs = BoundaryConditions()
bcs.add_boundary_condition(abc)
## Set up high level problem class
dp = DrivenProblemABC()
dp.set_mesh(mesh)
dp.set_basis_order(order)
dp.set_material_regions(materials)
dp.set_region_meshfunction(material_mesh_func)
dp.set_boundary_conditions(bcs)
## Set up current fillament source
current_sources = sucemfem.Sources.current_source.CurrentSources()
fillament_source = FillamentCurrentSource()
fillament_source.no_integration_points = 1000
fillament_source.set_source_endpoints(source_endpoints_z)
fillament_source.set_value(I)
current_sources.add_source(fillament_source)
## Set source in problem container
dp.set_sources(current_sources)
dp.init_problem()
dp.set_frequency(freq)
## Get sytem LHS matrix and RHS Vector
A = dp.get_LHS_matrix()
b_z = dp.get_RHS()
fillament_source.set_source_endpoints(source_endpoints_x)
b_x = dp.get_RHS()
fillament_source.set_source_endpoints(source_endpoints_y)
b_y = dp.get_RHS()
#import pdb ; pdb.set_trace()
A
print 'solve using UMFPack'
umf_solver = sucemfem.Utilities.LinalgSolvers.UMFPACKSolver(A)
x_z = umf_solver.solve(b_z)
x_x = umf_solver.solve(b_x)
x_y = umf_solver.solve(b_y)
## Post-process solution to obtain far-field
print 'calculating far field'
surf_ntff = surface_ntff.NTFF(dp.function_space)
surf_ntff.set_dofs(x_z)
surf_ntff.set_frequency(freq)
surf_E_ff_z = N.array([
surf_ntff.calc_pt(th_deg, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)
])
surf_E_theta_z = surf_E_ff_z[:, 0]
surf_E_phi_z = surf_E_ff_z[:, 1]
surf_ntff.set_dofs(x_x)
surf_E_ff_x = N.array([
surf_ntff.calc_pt(th_deg + 90, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)
])
surf_E_theta_x = surf_E_ff_x[:, 0]
surf_E_phi_x = surf_E_ff_x[:, 1]
surf_ntff.set_dofs(x_y)
surf_E_ff_y = N.array([
surf_ntff.calc_pt(th_deg + 90, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)
])
surf_E_theta_y = surf_E_ff_y[:, 0]
surf_E_phi_y = surf_E_ff_y[:, 1]
## Calculate some errors relative to the analytical solution
an_E_theta = [
current_fillament_farfield.eval_E_theta(freq, l, I, th)
for th in N.deg2rad(theta_deg)
]
err_z = normalised_RMS(surf_E_theta_z, an_E_theta, surf_E_phi_z)
err_theta_z = normalised_RMS(surf_E_theta_z, an_E_theta)
err_abs_theta_z = normalised_RMS(N.abs(surf_E_theta_z),
N.abs(an_E_theta))
err_x = normalised_RMS(surf_E_theta_x, an_E_theta, surf_E_phi_x)
err_theta_x = normalised_RMS(surf_E_theta_x, an_E_theta)
err_abs_theta_x = normalised_RMS(N.abs(surf_E_theta_x),
N.abs(an_E_theta))
err_y = normalised_RMS(surf_E_theta_y, an_E_theta, surf_E_phi_y)
err_theta_y = normalised_RMS(surf_E_theta_y, an_E_theta)
err_abs_theta_y = normalised_RMS(N.abs(surf_E_theta_y),
N.abs(an_E_theta))
print 'Far-field RMS error: ', err_z, err_x, err_y
# Expected error for lam/6 mesh, 2nd order discretisation,
# lam/4 current fillament source is ~4.685%
self.assertTrue(err_z < 4.7)
self.assertTrue(err_x < 4.7)
self.assertTrue(err_z < 4.7)
from sucemfem.PostProcessing import surface_ntff, variational_ntff
# Enable dolfin's form optimizations
sucemfem.Utilities.Optimization.set_dolfin_optimisation()
# Near-field of an infintesimal dipole
fname = 'reference_dofs-2-0.149896229-0.0499654096667.pickle'
theta_deg = N.linspace(0, 180, 181)
no_ff_pts = len(theta_deg)
phi_deg = N.zeros(no_ff_pts)
data = pickle.load(open(fname))
print data
lam = c0/data['freq']
k0 = data['freq']*2*N.pi/c0
mesh = get_centred_cube(data['domain_size'], data['max_edge_len'])
#plot(mesh,interactive=True)
V = dolfin.FunctionSpace(mesh, "Nedelec 1st kind H(curl)", data['order'])
#------------------------------
# Calculate using the standard surface integral NTFF
surf_ntff = surface_ntff.NTFF(V)
surf_ntff.set_dofs(data['x'])
surf_ntff.set_frequency(data['freq'])
surf_E_ff = N.array([surf_ntff.calc_pt(th_deg, ph_deg)
for th_deg, ph_deg in zip(theta_deg, phi_deg)])
surf_E_theta = surf_E_ff[:,0]
surf_E_phi = surf_E_ff[:,1]
#------------------------------
# Calculate using the variational integral NTFF
var_ntff = variational_ntff.NTFF(V)
import pickle
sys.path.append('../../../')
## Problem parameters
freq = 1e9
lam = c0/freq
I = 1. # Dipole current
l = lam/1000 # Dipole length
source_value = N.array([0,0,1.])*I*l
source_coord = N.array([0,0,0.])
## Discretisation settings
order = 2
domain_size = N.array([lam]*3)*0.5
max_edge_len = lam/6
mesh = get_centred_cube(domain_size, max_edge_len, source_coord)
# Request information:
field_pts = N.array(
[N.max(domain_size)/2-max_edge_len/2,0,0]
)*(N.arange(88)/100+1/10)[:, N.newaxis]
## Implementation
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {0:dict(eps_r=1, mu_r=1),}
abc = ABCBoundaryCondition()
abc.set_region_number(1)
bcs = sucemfem.BoundaryConditions.container.BoundaryConditions()
bcs.add_boundary_condition(abc)
dp = DrivenProblemABC()
dp.set_mesh(mesh)
### Problem parameters
freq = 1.0e+9 # Frequency
lam = c0 / freq
l = lam / 10 # Dipole length
I = 1.0 # Dipole current
source_direction = N.array([0, 0, 1.]) # Source orientation
source_centre = N.array([0, 0, 0.]) # Position of the source
source_endpoints = N.array(
[-source_direction * l / 2, source_direction * l / 2]) + source_centre
### Discretisation settings
order = 2
domain_size = N.array([lam] * 3) * 0.25
max_edge_len = lam / 6
mesh = get_centred_cube(domain_size, max_edge_len)
fname = 'power_flux_reference_dofs_f-%f_o-%d_s-%f_l-%f_h-%f' % (
freq, order, domain_size[0], l / lam, max_edge_len / lam)
meshfilename = fname + '_mesh.xml'
materialsfilename = fname + '_materials.xml'
print fname
### Implementation
#
## Set up materials function with all free-space
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {
0: dict(eps_r=1, mu_r=1),
}
## Set up 1st-order analytical ABC
from pylab import *
from blog_example import analytical_pts, analytical_result
## Problem parameters
I = problem_data['I'] # Dipole current
l = problem_data['l'] # Dipole length
source_value = N.array([0, 0, 1.]) * I * l
freq = problem_data['f']
lam = c0 / freq
source_coord = N.array([0, 0, 0.])
## Discretisation settings
order = 1
domain_size = N.array([2 * lam] * 3)
max_edge_len = lam / 6
mesh = get_centred_cube(domain_size, max_edge_len, source_coord)
# Request information:
field_pts = N.array([lam, 0, 0]) * (N.arange(88) / 100 + 1 / 10)[:, N.newaxis]
## Implementation
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {
0: dict(eps_r=1, mu_r=1),
}
abc = ABCBoundaryCondition()
abc.set_region_number(1)
bcs = BoundaryConditions()
bcs.add_boundary_condition(abc)
dp = DrivenProblemABC()
dp.set_mesh(mesh)
### Problem parameters
freq = 1.0e+9 # Frequency
lam = c0/freq
l = lam/4 # Dipole length
I = 1.0 # Dipole current
source_direction = N.array([0,0,1.]) # Source orientation
source_centre = N.array([0,0,0.]) # Position of the source
source_endpoints = N.array(
[-source_direction*l/2, source_direction*l/2]) + source_centre
### Discretisation settings
order = 2
domain_size = N.array([lam]*3)*1
max_edge_len = lam/6
mesh = get_centred_cube(domain_size, max_edge_len)
### Implementation
#
## Set up materials function with all free-space
material_mesh_func = dolfin.MeshFunction('uint', mesh, 3)
material_mesh_func.set_all(0)
materials = {0:dict(eps_r=1, mu_r=1),}
## Set up 1st-order analytical ABC
abc = ABCBoundaryCondition()
abc.set_region_number(1)
bcs = BoundaryConditions()
bcs.add_boundary_condition(abc)
## Set up high level problem class
dp = DrivenProblemABC()
dp.set_mesh(mesh)
