def test_partition_of_unity(self):
from sfepy.linalg import combine
from sfepy.discrete import Integral, PolySpace
ok = True
orders = {'2_3' : 5, '2_4' : 5, '3_4' : 5, '3_8' : 5}
bases = (
[ii for ii in combine([['2_4', '3_8'],
['lagrange', 'serendipity', 'bernstein']]
)]
+ [ii for ii in combine([['2_3', '3_4'],
['lagrange', 'bernstein']])]
)
for geom, poly_space_base in bases:
max_order = orders[geom]
for order in range(max_order + 1):
if (poly_space_base == 'serendipity') and not (0 < order < 4):
continue
self.report('geometry: %s, base: %s, order: %d'
% (geom, poly_space_base, order))
integral = Integral('i', order=2 * order)
coors, _ = integral.get_qp(geom)
ps = PolySpace.any_from_args('ps', self.gels[geom], order,
base=poly_space_base)
vals = ps.eval_base(coors)
_ok = nm.allclose(vals.sum(axis=-1), 1, atol=1e-14, rtol=0.0)
self.report('partition of unity:', _ok)
ok = ok and _ok
return ok
def from_conf(conf, options):
from sfepy.discrete import Integral
from sfepy.discrete.fem import Mesh, FEDomain
domains = []
for filename in filename_meshes:
mesh = Mesh.from_file(filename)
domain = FEDomain('domain_%s' % mesh.name.replace(data_dir, ''),
mesh)
domain.create_region('Omega', 'all')
domain.create_region('Gamma', 'vertices of surface', 'facet')
domains.append(domain)
integral = Integral('i', order=3)
qp_coors, qp_weights = integral.get_qp('3_8')
custom_integral = Integral('i',
coors=qp_coors,
weights=qp_weights,
order='custom')
test = Test(domains=domains,
integral=integral,
custom_integral=custom_integral,
conf=conf,
options=options)
return test
def solve_problem(shape, dims, young, poisson, force, transform=None):
domain = make_domain(dims[:2], shape, transform=transform)
omega = domain.regions['Omega']
gamma1 = domain.regions['Gamma1']
gamma2 = domain.regions['Gamma2']
field = Field.from_args('fu', nm.float64, 6, omega, approx_order=1,
poly_space_base='shell10x')
u = FieldVariable('u', 'unknown', field)
v = FieldVariable('v', 'test', field, primary_var_name='u')
thickness = dims[2]
if transform is None:
pload = [[0.0, 0.0, force / shape[1], 0.0, 0.0, 0.0]] * shape[1]
elif transform == 'bend':
pload = [[force / shape[1], 0.0, 0.0, 0.0, 0.0, 0.0]] * shape[1]
elif transform == 'twist':
pload = [[0.0, force / shape[1], 0.0, 0.0, 0.0, 0.0]] * shape[1]
m = Material('m', D=sh.create_elastic_tensor(young=young, poisson=poisson),
values={'.drill' : 1e-7})
load = Material('load', values={'.val' : pload})
aux = Integral('i', order=3)
qp_coors, qp_weights = aux.get_qp('3_8')
qp_coors[:, 2] = thickness * (qp_coors[:, 2] - 0.5)
qp_weights *= thickness
integral = Integral('i', coors=qp_coors, weights=qp_weights, order='custom')
t1 = Term.new('dw_shell10x(m.D, m.drill, v, u)',
integral, omega, m=m, v=v, u=u)
t2 = Term.new('dw_point_load(load.val, v)',
integral, gamma2, load=load, v=v)
eq = Equation('balance', t1 - t2)
eqs = Equations([eq])
fix_u = EssentialBC('fix_u', gamma1, {'u.all' : 0.0})
ls = ScipyDirect({})
nls_status = IndexedStruct()
nls = Newton({}, lin_solver=ls, status=nls_status)
pb = Problem('elasticity with shell10x', equations=eqs)
pb.set_bcs(ebcs=Conditions([fix_u]))
pb.set_solver(nls)
state = pb.solve()
return pb, state, u, gamma2
def test_normals(self):
"""
Check orientations of surface normals on the reference elements.
"""
import sfepy
from sfepy.discrete import Integral
from sfepy.discrete.fem import Mesh, FEDomain
from sfepy.discrete.fem.poly_spaces import PolySpace
from sfepy.discrete.fem.mappings import SurfaceMapping
from sfepy.linalg import normalize_vectors
ok = True
for geom in ['2_3', '2_4', '3_4', '3_8']:
mesh = Mesh.from_file('meshes/elements/%s_1.mesh' % geom,
prefix_dir=sfepy.data_dir)
domain = FEDomain('domain', mesh)
surface = domain.create_region('Surface', 'vertices of surface',
'facet')
domain.create_surface_group(surface)
sd = domain.surface_groups[surface.name]
coors = domain.get_mesh_coors()
gel = domain.geom_els[geom].surface_facet
ps = PolySpace.any_from_args('aux', gel, 1)
mapping = SurfaceMapping(coors, sd.get_connectivity(), ps)
integral = Integral('i', order=1)
vals, weights = integral.get_qp(gel.name)
# Evaluate just in the first quadrature point...
geo = mapping.get_mapping(vals[:1], weights[:1])
expected = expected_normals[geom].copy()
normalize_vectors(expected)
_ok = nm.allclose(expected,
geo.normal[:, 0, :, 0],
rtol=0.0,
atol=1e-14)
self.report('%s: %s' % (geom, _ok))
if not _ok:
self.report('expected:')
self.report(expected)
self.report('actual:')
self.report(geo.normal[:, 0, :, 0])
ok = ok and _ok
return ok
def plot_1D_snr(conf, pb, ana_qp, num_qp, io, order, orders, ir, sol_fig, axs):
"""
Plot 1D solutions and errors
:param conf:
:param io: index of order
:param ir: index of refirement
:param ana_qp:
:param num_qp:
:param order:
:param orders:
:param pb:
:param sol_fig:
:param axs:
:return:
"""
idiff = Integral('idiff', 20)
sol_fig.suptitle("Numerical and exact solutions" +
build_attrs_string(conf, remove_dots=False, sep=", "))
n_cells = pb.domain.shape.n_el
qps = pb.fields["f"].mapping.get_physical_qps(idiff.get_qp("1_2")[0])
fqps = qps.flatten()
coors = pb.domain.mesh.coors
u = pb.fields["f"].unravel_sol(pb.sol.vec)
uu, xx = reconstruct_legendre_dofs(coors, None,
u.swapaxes(0, 1)[:, :, None])
ax = axs[io][ir]
xs = nm.linspace(conf.mstart, conf.mend, 500)[:, None]
ax.set_title("o: {}, h: {}".format(order, n_cells))
ax.plot(xs,
conf.analytic_sol(xs, t=nm.array(1)),
label="exact",
color="grey")
ax.plot(xx[:, 0], uu[:, 0, 0], alpha=.5, label="num-lin")
ax.plot(fqps, ana_qp.flatten(), "--", color="grey", label="exact-qp")
ax.plot(fqps, num_qp.flatten(), label="num-qp")
ax2 = ax.twinx()
ax2.plot(fqps,
nm.abs(num_qp.flatten() - ana_qp.flatten()),
color="red",
label="error-qp")
if io < len(orders) - 1:
ax.set_xticks([])
else:
if ir == 0: # put only one legend
lines, labels = ax.get_legend_handles_labels()
lines2, labels2 = ax2.get_legend_handles_labels()
sol_fig.legend(lines + lines2,
labels + labels2,
loc='center right')
def solve_problem(shape, dims, young, poisson, force, transform=None):
domain = make_domain(dims[:2], shape, transform=transform)
omega = domain.regions['Omega']
gamma1 = domain.regions['Gamma1']
gamma2 = domain.regions['Gamma2']
field = Field.from_args('fu', nm.float64, 6, omega, approx_order=1,
poly_space_base='shell10x')
u = FieldVariable('u', 'unknown', field)
v = FieldVariable('v', 'test', field, primary_var_name='u')
thickness = dims[2]
if transform is None:
pload = [[0.0, 0.0, force / shape[1], 0.0, 0.0, 0.0]] * shape[1]
elif transform == 'bend':
pload = [[force / shape[1], 0.0, 0.0, 0.0, 0.0, 0.0]] * shape[1]
elif transform == 'twist':
pload = [[0.0, force / shape[1], 0.0, 0.0, 0.0, 0.0]] * shape[1]
m = Material('m', D=sh.create_elastic_tensor(young=young, poisson=poisson),
values={'.drill' : 1e-7})
load = Material('load', values={'.val' : pload})
aux = Integral('i', order=3)
qp_coors, qp_weights = aux.get_qp('3_8')
qp_coors[:, 2] = thickness * (qp_coors[:, 2] - 0.5)
qp_weights *= thickness
integral = Integral('i', coors=qp_coors, weights=qp_weights, order='custom')
t1 = Term.new('dw_shell10x(m.D, m.drill, v, u)',
integral, omega, m=m, v=v, u=u)
t2 = Term.new('dw_point_load(load.val, v)',
integral, gamma2, load=load, v=v)
eq = Equation('balance', t1 - t2)
eqs = Equations([eq])
fix_u = EssentialBC('fix_u', gamma1, {'u.all' : 0.0})
ls = ScipyDirect({})
nls_status = IndexedStruct()
nls = Newton({}, lin_solver=ls, status=nls_status)
pb = Problem('elasticity with shell10x', equations=eqs, nls=nls, ls=ls)
pb.time_update(ebcs=Conditions([fix_u]))
state = pb.solve()
return pb, state, u, gamma2
def test_normals(self):
"""
Check orientations of surface normals on the reference elements.
"""
import sfepy
from sfepy.discrete import Integral
from sfepy.discrete.fem import Mesh, FEDomain
from sfepy.discrete.fem.poly_spaces import PolySpace
from sfepy.discrete.fem.mappings import SurfaceMapping
from sfepy.linalg import normalize_vectors
ok = True
for geom in ['2_3', '2_4', '3_4', '3_8']:
mesh = Mesh.from_file('meshes/elements/%s_1.mesh' % geom,
prefix_dir=sfepy.data_dir)
domain = FEDomain('domain', mesh)
surface = domain.create_region('Surface', 'vertices of surface',
'facet')
domain.create_surface_group(surface)
sd = domain.surface_groups[surface.name]
coors = domain.get_mesh_coors()
gel = domain.geom_els[geom].surface_facet
ps = PolySpace.any_from_args('aux', gel, 1)
mapping = SurfaceMapping(coors, sd.get_connectivity(), ps)
integral = Integral('i', order=1)
vals, weights = integral.get_qp(gel.name)
# Evaluate just in the first quadrature point...
geo = mapping.get_mapping(vals[:1], weights[:1])
expected = expected_normals[geom].copy()
normalize_vectors(expected)
_ok = nm.allclose(expected, geo.normal[:, 0, :, 0],
rtol=0.0, atol=1e-14)
self.report('%s: %s' % (geom, _ok))
if not _ok:
self.report('expected:')
self.report(expected)
self.report('actual:')
self.report(geo.normal[:, 0, :, 0])
ok = ok and _ok
return ok
def _get_qp(geometry, order):
from sfepy.discrete import Integral
from sfepy.discrete.fem.geometry_element import GeometryElement
aux = Integral('aux', order=order)
coors, weights = aux.get_qp(geometry)
true_order = aux.qps[geometry].order
output('geometry:', geometry, 'order:', order, 'num. points:',
coors.shape[0], 'true_order:', true_order)
output('min. weight:', weights.min())
output('max. weight:', weights.max())
return GeometryElement(geometry), coors, weights
def _get_qp(geometry, order):
from sfepy.discrete import Integral
from sfepy.discrete.fem.geometry_element import GeometryElement
aux = Integral('aux', order=order)
coors, weights = aux.get_qp(geometry)
true_order = aux.qps[geometry].order
output('geometry:', geometry, 'order:', order, 'num. points:',
coors.shape[0], 'true_order:', true_order)
output('min. weight:', weights.min())
output('max. weight:', weights.max())
return GeometryElement(geometry), coors, weights
def test_hessians(self):
"""
Test the second partial derivatives of basis functions using finite
differences.
"""
from sfepy.linalg import combine
from sfepy.discrete import Integral, PolySpace
ok = True
orders = {'2_3': 3, '2_4': 3, '3_4': 4, '3_8': 3}
bases = ([
ii for ii in combine([['2_3', '2_4', '3_4', '3_8'], ['lagrange']])
])
for geom, poly_space_base in bases:
self.report('geometry: %s, base: %s' % (geom, poly_space_base))
order = orders[geom]
integral = Integral('i', order=order)
coors, _ = integral.get_qp(geom)
ps = PolySpace.any_from_args('ps',
self.gels[geom],
order,
base=poly_space_base)
dim = coors.shape[1]
h1 = nm.zeros((coors.shape[0], dim, dim, ps.n_nod), nm.float64)
eps = 1e-8
for ir in range(dim):
cc = coors.copy()
cc[:, ir] -= eps
aux0 = ps.eval_base(cc, diff=1)
cc[:, ir] += 2 * eps
aux1 = ps.eval_base(cc, diff=1)
h1[:, :, ir, :] = 0.5 * (aux1 - aux0) / eps
h2 = ps.eval_base(coors, diff=2)
_ok = nm.allclose(h1, h2, rtol=0, atol=50 * eps)
self.report('hessians: error: %.2e ok: %s' %
(nm.abs(h1 - h2).max(), _ok))
ok = ok and _ok
return ok
def test_hessians(self):
"""
Test the second partial derivatives of basis functions using finite
differences.
"""
from sfepy.linalg import combine
from sfepy.discrete import Integral
from sfepy.discrete.fem.poly_spaces import PolySpace
ok = True
orders = {'2_3' : 3, '2_4' : 3, '3_4' : 4, '3_8' : 3}
bases = ([ii for ii in combine([['2_3', '2_4', '3_4', '3_8'],
['lagrange']])])
for geom, poly_space_base in bases:
self.report('geometry: %s, base: %s' % (geom, poly_space_base))
order = orders[geom]
integral = Integral('i', order=order)
coors, _ = integral.get_qp(geom)
ps = PolySpace.any_from_args('ps', self.gels[geom], order,
base=poly_space_base)
dim = coors.shape[1]
h1 = nm.zeros((coors.shape[0], dim, dim, ps.n_nod), nm.float64)
eps = 1e-8
for ir in range(dim):
cc = coors.copy()
cc[:, ir] -= eps
aux0 = ps.eval_base(cc, diff=1)
cc[:, ir] += 2 * eps
aux1 = ps.eval_base(cc, diff=1)
h1[:, :, ir, :] = 0.5 * (aux1 - aux0) / eps
h2 = ps.eval_base(coors, diff=2)
_ok = nm.allclose(h1, h2, rtol=0, atol=50*eps)
self.report('hessians: error: %.2e ok: %s'
% (nm.abs(h1 - h2).max(), _ok))
ok = ok and _ok
return ok
def from_conf(conf, options):
from sfepy.discrete import Integral
from sfepy.discrete.fem import Mesh, FEDomain
domains = []
for filename in filename_meshes:
mesh = Mesh.from_file(filename)
domain = FEDomain('domain_%s' % mesh.name.replace(data_dir, ''),
mesh)
domain.create_region('Omega', 'all')
domain.create_region('Gamma', 'vertices of surface', 'facet')
domains.append(domain)
integral = Integral('i', order=3)
qp_coors, qp_weights = integral.get_qp('3_8')
custom_integral = Integral('i', coors=qp_coors, weights=qp_weights,
order='custom')
test = Test(domains=domains, integral=integral,
custom_integral=custom_integral,
conf=conf, options=options)
return test
def main():
parser = ArgumentParser(description=__doc__)
parser.add_argument('--version', action='version', version='%(prog)s')
parser.add_argument('-b',
'--basis',
metavar='name',
action='store',
dest='basis',
default='lagrange',
help=help['basis'])
parser.add_argument('-n',
'--max-order',
metavar='order',
type=int,
action='store',
dest='max_order',
default=10,
help=help['max_order'])
parser.add_argument('-m',
'--matrix',
metavar='type',
action='store',
dest='matrix_type',
default='laplace',
help=help['matrix_type'])
parser.add_argument('-g',
'--geometry',
metavar='name',
action='store',
dest='geometry',
default='2_4',
help=help['geometry'])
options = parser.parse_args()
dim, n_ep = int(options.geometry[0]), int(options.geometry[2])
output('reference element geometry:')
output(' dimension: %d, vertices: %d' % (dim, n_ep))
n_c = {'laplace': 1, 'elasticity': dim}[options.matrix_type]
output('matrix type:', options.matrix_type)
output('number of variable components:', n_c)
output('polynomial space:', options.basis)
output('max. order:', options.max_order)
mesh = Mesh.from_file(data_dir +
'/meshes/elements/%s_1.mesh' % options.geometry)
domain = FEDomain('domain', mesh)
omega = domain.create_region('Omega', 'all')
orders = nm.arange(1, options.max_order + 1, dtype=nm.int)
conds = []
order_fix = 0 if options.geometry in ['2_4', '3_8'] else 1
for order in orders:
output('order:', order, '...')
field = Field.from_args('fu',
nm.float64,
n_c,
omega,
approx_order=order,
space='H1',
poly_space_base=options.basis)
to = field.approx_order
quad_order = 2 * (max(to - order_fix, 0))
output('quadrature order:', quad_order)
integral = Integral('i', order=quad_order)
qp, _ = integral.get_qp(options.geometry)
output('number of quadrature points:', qp.shape[0])
u = FieldVariable('u', 'unknown', field)
v = FieldVariable('v', 'test', field, primary_var_name='u')
m = Material('m', D=stiffness_from_lame(dim, 1.0, 1.0), mu=1.0)
if options.matrix_type == 'laplace':
term = Term.new('dw_laplace(m.mu, v, u)',
integral,
omega,
m=m,
v=v,
u=u)
n_zero = 1
else:
assert_(options.matrix_type == 'elasticity')
term = Term.new('dw_lin_elastic(m.D, v, u)',
integral,
omega,
m=m,
v=v,
u=u)
n_zero = (dim + 1) * dim / 2
term.setup()
output('assembling...')
tt = time.clock()
mtx, iels = term.evaluate(mode='weak', diff_var='u')
output('...done in %.2f s' % (time.clock() - tt))
mtx = mtx[0, 0]
try:
assert_(nm.max(nm.abs(mtx - mtx.T)) < 1e-10)
except:
from sfepy.base.base import debug
debug()
output('matrix shape:', mtx.shape)
eigs = eig(mtx, method='eig.sgscipy', eigenvectors=False)
eigs.sort()
# Zero 'true' zeros.
eigs[:n_zero] = 0.0
ii = nm.where(eigs < 0.0)[0]
if len(ii):
output('matrix is not positive semi-definite!')
ii = nm.where(eigs[n_zero:] < 1e-12)[0]
if len(ii):
output('matrix has more than %d zero eigenvalues!' % n_zero)
output('smallest eigs:\n', eigs[:10])
ii = nm.where(eigs > 0.0)[0]
emin, emax = eigs[ii[[0, -1]]]
output('min:', emin, 'max:', emax)
cond = emax / emin
conds.append(cond)
output('condition number:', cond)
output('...done')
plt.figure(1)
plt.semilogy(orders, conds)
plt.xticks(orders, orders)
plt.xlabel('polynomial order')
plt.ylabel('condition number')
plt.grid()
plt.figure(2)
plt.loglog(orders, conds)
plt.xticks(orders, orders)
plt.xlabel('polynomial order')
plt.ylabel('condition number')
plt.grid()
plt.show()
}
variables = {
'u': ('unknown field', 'fu', 0),
'v': ('test field', 'fu', 'u'),
}
ebcs = {
'fix': ('Gamma1', {
'u.all': 0.0
}),
}
# Custom integral.
aux = Integral('i', order=3)
qp_coors, qp_weights = aux.get_qp('3_8')
qp_coors[:, 2] = thickness * (qp_coors[:, 2] - 0.5)
qp_weights *= thickness
integrals = {
'i': ('custom', qp_coors, qp_weights),
}
equations = {
'elasticity':
"""dw_shell10x.i.Omega(m.D, m.drill, v, u)
= dw_point_load.i.Gamma2(load.val, v)""",
}
solvers = {
'ls': ('ls.scipy_direct', {}),
def main():
parser = ArgumentParser(description=__doc__)
parser.add_argument('--version', action='version', version='%(prog)s')
parser.add_argument('-b',
'--basis',
metavar='name',
action='store',
dest='basis',
default='lagrange',
help=helps['basis'])
parser.add_argument('-n',
'--max-order',
metavar='order',
type=int,
action='store',
dest='max_order',
default=10,
help=helps['max_order'])
parser.add_argument('-m',
'--matrix',
action='store',
dest='matrix_type',
choices=['laplace', 'elasticity', 'smass', 'vmass'],
default='laplace',
help=helps['matrix_type'])
parser.add_argument('-g',
'--geometry',
metavar='name',
action='store',
dest='geometry',
default='2_4',
help=helps['geometry'])
parser.add_argument('-o',
'--output-dir',
metavar='path',
action='store',
dest='output_dir',
default=None,
help=helps['output_dir'])
parser.add_argument('--no-show',
action='store_false',
dest='show',
default=True,
help=helps['no_show'])
options = parser.parse_args()
dim, n_ep = int(options.geometry[0]), int(options.geometry[2])
output('reference element geometry:')
output(' dimension: %d, vertices: %d' % (dim, n_ep))
n_c = {
'laplace': 1,
'elasticity': dim,
'smass': 1,
'vmass': dim
}[options.matrix_type]
output('matrix type:', options.matrix_type)
output('number of variable components:', n_c)
output('polynomial space:', options.basis)
output('max. order:', options.max_order)
mesh = Mesh.from_file(data_dir +
'/meshes/elements/%s_1.mesh' % options.geometry)
domain = FEDomain('domain', mesh)
omega = domain.create_region('Omega', 'all')
orders = nm.arange(1, options.max_order + 1, dtype=nm.int32)
conds = []
for order in orders:
output('order:', order, '...')
field = Field.from_args('fu',
nm.float64,
n_c,
omega,
approx_order=order,
space='H1',
poly_space_base=options.basis)
quad_order = 2 * field.approx_order
output('quadrature order:', quad_order)
integral = Integral('i', order=quad_order)
qp, _ = integral.get_qp(options.geometry)
output('number of quadrature points:', qp.shape[0])
u = FieldVariable('u', 'unknown', field)
v = FieldVariable('v', 'test', field, primary_var_name='u')
m = Material('m', D=stiffness_from_lame(dim, 1.0, 1.0))
if options.matrix_type == 'laplace':
term = Term.new('dw_laplace(v, u)', integral, omega, v=v, u=u)
n_zero = 1
elif options.matrix_type == 'elasticity':
term = Term.new('dw_lin_elastic(m.D, v, u)',
integral,
omega,
m=m,
v=v,
u=u)
n_zero = (dim + 1) * dim // 2
elif options.matrix_type in ('smass', 'vmass'):
term = Term.new('dw_dot(v, u)', integral, omega, v=v, u=u)
n_zero = 0
term.setup()
output('assembling...')
timer = Timer(start=True)
mtx, iels = term.evaluate(mode='weak', diff_var='u')
output('...done in %.2f s' % timer.stop())
mtx = mtx[0, 0]
try:
assert_(nm.max(nm.abs(mtx - mtx.T)) < 1e-10)
except:
from sfepy.base.base import debug
debug()
output('matrix shape:', mtx.shape)
eigs = eig(mtx, method='eig.sgscipy', eigenvectors=False)
eigs.sort()
# Zero 'true' zeros.
eigs[:n_zero] = 0.0
ii = nm.where(eigs < 0.0)[0]
if len(ii):
output('matrix is not positive semi-definite!')
ii = nm.where(eigs[n_zero:] < 1e-12)[0]
if len(ii):
output('matrix has more than %d zero eigenvalues!' % n_zero)
output('smallest eigs:\n', eigs[:10])
ii = nm.where(eigs > 0.0)[0]
emin, emax = eigs[ii[[0, -1]]]
output('min:', emin, 'max:', emax)
cond = emax / emin
conds.append(cond)
output('condition number:', cond)
output('...done')
if options.output_dir is not None:
indir = partial(op.join, options.output_dir)
else:
indir = None
plt.rcParams['font.size'] = 12
plt.rcParams['lines.linewidth'] = 3
fig, ax = plt.subplots()
ax.semilogy(orders, conds)
ax.set_xticks(orders)
ax.set_xticklabels(orders)
ax.set_xlabel('polynomial order')
ax.set_ylabel('condition number')
ax.set_title(f'{options.basis.capitalize()} basis')
ax.grid()
plt.tight_layout()
if indir is not None:
fig.savefig(indir(f'{options.basis}-{options.matrix_type}-'
f'{options.geometry}-{options.max_order}-xlin.png'),
bbox_inches='tight')
fig, ax = plt.subplots()
ax.loglog(orders, conds)
ax.set_xticks(orders)
ax.set_xticklabels(orders)
ax.set_xlabel('polynomial order')
ax.set_ylabel('condition number')
ax.set_title(f'{options.basis.capitalize()} basis')
ax.grid()
plt.tight_layout()
if indir is not None:
fig.savefig(indir(f'{options.basis}-{options.matrix_type}-'
f'{options.geometry}-{options.max_order}-xlog.png'),
bbox_inches='tight')
if options.show:
plt.show()
class DGField(FEField):
"""Class for usage with DG terms, provides functionality for Discontinous
Galerkin method like neighbour look up, projection to discontinuous basis
and correct DOF treatment.
"""
family_name = 'volume_DG_legendre_discontinuous'
is_surface = False
def __init__(self,
name,
dtype,
shape,
region,
space="H1",
poly_space_base="legendre",
approx_order=1,
integral=None):
"""
Creates DGField, with Legendre polyspace and default integral
corresponding to 2 * approx_order.
Parameters
----------
name : string
dtype : type
shape : string
'vector', 'scalar' or something else
region : sfepy.discrete.common.region.Region
space : string
default "H1"
poly_space_base : PolySpace
optionally force polyspace
approx_order : 0 for FVM, default 1
integral : Integral
if None integral of order 2*approx_order is created
"""
shape = parse_shape(shape, region.domain.shape.dim)
Struct.__init__(self,
name=name,
dtype=dtype,
shape=shape,
region=region)
if isinstance(approx_order, tuple):
self.approx_order = approx_order[0]
else:
self.approx_order = approx_order
# geometry
self.domain = region.domain
self.region = region
self.dim = region.tdim
self._setup_geometry()
self._setup_connectivity()
# TODO treat domains embedded into higher dimensional spaces?
self.n_el_facets = self.dim + 1 if self.gel.is_simplex else 2**self.dim
# approximation space
self.space = space
self.poly_space_base = poly_space_base
self.force_bubble = False
self._create_interpolant()
# DOFs
self._setup_shape()
self._setup_all_dofs()
self.ravel_sol = get_raveler(self.n_el_nod, self.n_cell)
self.unravel_sol = get_unraveler(self.n_el_nod, self.n_cell)
# integral
self.clear_qp_base()
self.clear_facet_qp_base()
if integral is None:
self.integral = Integral("dg_fi", order=2 * self.approx_order)
else:
self.integral = integral
self.ori = None
self.basis_transform = None
# mapping
self.mappings = {}
self.mapping = self.create_mapping(self.region,
self.integral,
"volume",
return_mapping=True)[1]
self.mappings0 = {}
# neighbour facet mapping and data caches
# TODO use lru cache or different method?
self.clear_facet_neighbour_idx_cache()
self.clear_normals_cache()
self.clear_facet_vols_cache()
self.boundary_facet_local_idx = {}
def _create_interpolant(self):
name = self.gel.name + '_DG_legendre'
ps = PolySpace.any_from_args(name,
self.gel,
self.approx_order,
base=self.poly_space_base,
force_bubble=False)
self.poly_space = ps
# 'legendre_simplex' is created for '1_2'.
if self.gel.name in ["2_4", "3_8"]:
self.extended = True
else:
self.extended = False
def _setup_all_dofs(self):
"""Sets up all the differet kinds of DOFs, for DG only bubble DOFs"""
self.n_el_nod = self.poly_space.n_nod
self.n_vertex_dof = 0 # in DG we will propably never need vertex DOFs
self.n_edge_dof = 0 # use facets DOFS for AFS methods
self.n_face_dof = 0 # use facet DOF for AFS methods
(self.n_bubble_dof, self.bubble_remap,
self.bubble_dofs) = self._setup_bubble_dofs()
self.n_nod = self.n_vertex_dof + self.n_edge_dof \
+ self.n_face_dof + self.n_bubble_dof
def _setup_bubble_dofs(self):
"""Creates DOF information for so called element, cell or bubble DOFs
- the only DOFs used in DG
n_dof = n_cells * n_el_nod
remap optional remapping between cells
dofs is mapping between dofs and cells
Returns
-------
n_dof : int
remap : ndarray
dofs : ndarray
"""
self.n_cell = self.region.get_n_cells(self.is_surface)
n_dof = self.n_cell * self.n_el_nod
dofs = nm.arange(n_dof, dtype=nm.int32)\
.reshape(self.n_cell, self.n_el_nod)
remap = nm.arange(self.n_cell)
self.econn = dofs
self.dofs2cells = nm.repeat(nm.arange(self.n_cell), self.n_el_nod)
return n_dof, remap, dofs
def _setup_shape(self):
"""What is shape used for and what it really means.
Does it represent shape of the problem?
"""
self.n_components = nm.prod(self.shape)
self.val_shape = self.shape
def _setup_geometry(self):
"""Setup the field region geometry."""
# get_gel extracts the highest dimension geometry from self.region
self.gel = get_gel(self.region)
def _setup_connectivity(self):
"""Forces self.domain.mesh to build necessary conductivities
so they are available in self.get_nbrhd_dofs
"""
self.region.domain.mesh.cmesh.setup_connectivity(self.dim, self.dim)
self.region.domain.mesh.cmesh.setup_connectivity(
self.dim - 1, self.dim)
self.region.domain.mesh.cmesh.setup_connectivity(
self.dim, self.dim - 1)
def get_coor(self, nods=None):
"""Returns coors for matching nodes
# TODO revise DG_EPBC and EPBC matching?
Parameters
----------
nods :
if None use all nodes (Default value = None)
Returns
-------
coors : ndarray
coors on surface
"""
if nods is None:
nods = self.bubble_dofs
cells = self.dofs2cells[nods]
coors = self.domain.mesh.cmesh.get_centroids(self.dim)[cells]
eps = min(self.domain.cmesh.get_volumes(
self.dim)) / (self.n_el_nod + 2)
if self.dim == 1:
extended_coors = nm.zeros(nm.shape(coors)[:-1] + (2, ))
extended_coors[:, 0] = coors[:, 0]
coors = extended_coors
# shift centroid coors to lie within cells but be different for each dof
# use coors of facet QPs?
coors += eps * nm.repeat(nm.arange(self.n_el_nod), len(
nm.unique(cells)))[:, None]
return coors
def clear_facet_qp_base(self):
"""Clears facet_qp_base cache"""
self.facet_bf = {}
self.facet_qp = None
self.facet_whs = None
def _transform_qps_to_facets(self, qps, geo_name):
"""Transforms points given in qps to all facets of the reference element
with geometry geo_name.
Parameters
----------
qps :
qps corresponding to facet dimension to be transformed
geo_name :
element type
Returns
-------
tqps : ndarray
tqps is of shape shape(qps) + (n_el_facets, geo dim)
"""
if geo_name == "1_2":
tqps = nm.zeros(nm.shape(qps) + (
2,
1,
))
tqps[..., 0, 0] = 0.
tqps[..., 1, 0] = 1.
elif geo_name == "2_3":
tqps = nm.zeros(nm.shape(qps) + (
3,
2,
))
# 0.
tqps[..., 0, 0] = qps # x = 0 + t
tqps[..., 0, 1] = 0. # y = 0
# 1.
tqps[..., 1, 0] = 1 - qps # x = 1 - t
tqps[..., 1, 1] = qps # y = t
# 2.
tqps[..., 2, 0] = 0 # x = 0
tqps[..., 2, 1] = 1 - qps # y = 1 - t
elif geo_name == "2_4":
tqps = nm.zeros(nm.shape(qps) + (
4,
2,
))
# 0.
tqps[..., 0, 0] = qps # x = t
tqps[..., 0, 1] = 0. # y = 0
# 1.
tqps[..., 1, 0] = 1 # x = 1
tqps[..., 1, 1] = qps # y = t
# 2.
tqps[..., 2, 0] = 1 - qps # x = 1 -t
tqps[..., 2, 1] = 1 # y = 1
# 3.
tqps[..., 3, 0] = 0 # x = 0
tqps[..., 3, 1] = 1 - qps # y = 1 - t
elif geo_name == "3_4":
# tqps = nm.zeros(nm.shape(qps) + (4, 3,))
raise NotImplementedError(
"Geometry {} not supported, yet".format(geo_name))
elif geo_name == "3_8":
# tqps = nm.zeros(nm.shape(qps) + (8, 3,))
raise NotImplementedError(
"Geometry {} not supported, yet".format(geo_name))
else:
raise NotImplementedError(
"Geometry {} not supported, yet".format(geo_name))
return tqps
def get_facet_qp(self):
"""Returns quadrature points on all facets of the reference element in
array of shape (n_qp, 1 , n_el_facets, dim)
Returns
-------
qps : ndarray
quadrature points
weights : ndarray
Still needs to be transformed to actual facets!
"""
if self.dim == 1:
facet_qps = self._transform_qps_to_facets(nm.zeros((1, 1)), "1_2")
weights = nm.ones((1, 1, 1))
else:
qps, weights = self.integral.get_qp(
cell_facet_gel_name[self.gel.name])
weights = weights[None, :, None]
facet_qps = self._transform_qps_to_facets(qps, self.gel.name)
return facet_qps, weights
def get_facet_base(self, derivative=False, base_only=False):
"""
Returns values of base in facets quadrature points, data shape is a bit
crazy right now:
(number of qps, 1, n_el_facets, 1, n_el_nod)
end for derivatine:
(1, number of qps, (dim,) * derivative, n_el_facets, 1, n_el_nod)
Parameters
----------
derivative: truthy or integer
base_only: do not return weights
Returns
-------
facet_bf : ndarray
values of basis functions in facet qps
weights : ndarray, optionally
weights of qps
"""
if derivative:
diff = int(derivative)
else:
diff = 0
if diff in self.facet_bf:
facet_bf = self.facet_bf[diff]
whs = self.facet_whs
else:
qps, whs = self.get_facet_qp()
ps = self.poly_space
self.facet_qp = qps
self.facet_whs = whs
if derivative:
facet_bf = nm.zeros((1, ) + nm.shape(qps)[:-1] +
(self.dim, ) * diff + (self.n_el_nod, ))
else:
facet_bf = nm.zeros(nm.shape(qps)[:-1] + (
1,
self.n_el_nod,
))
for i in range(self.n_el_facets):
facet_bf[..., i, :, :] = \
ps.eval_base(qps[..., i, :], diff=diff,
transform=self.basis_transform)
self.facet_bf[diff] = facet_bf
if base_only:
return facet_bf
else:
return facet_bf, whs
def clear_facet_neighbour_idx_cache(self, region=None):
"""
If region is None clear all!
Parameters
----------
region : sfepy.discrete.common.region.Region
If None clear all.
"""
if region is None:
self.facet_neighbour_index = {}
else:
self.facet_neighbour_index.pop(region.name)
def get_facet_neighbor_idx(self, region=None, eq_map=None):
"""
Returns index of cell neighbours sharing facet, along with local index
of the facet within neighbour, also treats periodic boundary conditions
i.e. plugs correct neighbours for cell on periodic boundary.
Where there are no neighbours specified puts -1 instead of neighbour
and facet id
Cashes neighbour index in self.facet_neighbours
Parameters
----------
region : sfepy.discrete.common.region.Region
Main region, must contain cells.
eq_map :
eq_map from state variable containing information on
EPBC and DG EPBC. (Default value = None)
Returns
-------
facet_neighbours : ndarray
Shape is
(n_cell, n_el_facet, 2),
first value is index of the neighbouring cell,
the second is index of the facet in said nb. cell.
"""
if region is None or eq_map is None:
# HOTFIX enabling limiter to obtain connectivity data without
# knowing eq_map or region
if self.region.name in self.facet_neighbour_index:
return self.facet_neighbour_index[self.region.name]
else:
raise ValueError("No facet neighbour mapping for main " +
"region {}".format(self.region.name) +
" cached yet, call with region and " +
"eq_map first.")
if region.name in self.facet_neighbour_index:
return self.facet_neighbour_index[region.name]
dim, n_cell, n_el_facets = self.get_region_info(region)
cmesh = region.domain.mesh.cmesh
cells = region.cells
facet_neighbours = nm.zeros((n_cell, n_el_facets, 2), dtype=nm.int32)
c2fi, c2fo = cmesh.get_incident(dim - 1, cells, dim, ret_offsets=True)
for ic, o1 in enumerate(c2fo[:-1]): # loop over cells
o2 = c2fo[ic + 1]
# get neighbours per facet of the cell
c2ci, c2co = cmesh.get_incident(dim,
c2fi[o1:o2],
dim - 1,
ret_offsets=True)
ii = cmesh.get_local_ids(c2fi[o1:o2], dim - 1, c2ci, c2co, dim)
fis = nm.c_[c2ci, ii]
nbrs = []
for ifa, of1 in enumerate(c2co[:-1]): # loop over facets
of2 = c2co[ifa + 1]
if of2 == (of1 + 1): # facet has only one cell
# Surface facet.
nbrs.append([-1, -1]) # c2ci[of1]) # append no neighbours
else:
if c2ci[of1] == cells[ic]: # do not append the cell itself
nbrs.append(fis[of2 - 1])
else:
nbrs.append(fis[of1])
facet_neighbours[ic, :, :] = nbrs
facet_neighbours = \
self._set_fem_periodic_facet_neighbours(facet_neighbours, eq_map)
facet_neighbours = \
self._set_dg_periodic_facet_neighbours(facet_neighbours, eq_map)
# cache results
self.facet_neighbour_index[region.name] = facet_neighbours
return facet_neighbours
def _set_dg_periodic_facet_neighbours(self, facet_neighbours, eq_map):
"""
Parameters
----------
facet_neighbours : array_like
Shape is
(n_cell, n_el_facet, 2),
first value is index of the neighbouring cell
the second is index of the facet in said nb. cell.
eq_map :
must contain dg_ep_bc a List with pairs of slave and master boundary
cell boundary facet mapping
Returns
-------
facet_neighbours : ndarray
Updated incidence array.
"""
# if eq_map.
# treat DG EPBC - these are definitely preferred
if eq_map.n_dg_epbc > 0 and self.gel.name not in ["1_2", "2_4", "3_6"]:
raise ValueError("Periodic boundary conditions not supported " +
"for geometry {} elements.".format(self.gel.name))
dg_epbc = eq_map.dg_epbc
for master_bc2bfi, slave_bc2bfi in dg_epbc:
# set neighbours of periodic cells to one another
facet_neighbours[master_bc2bfi[:, 0], master_bc2bfi[:, 1], 0] = \
slave_bc2bfi[:, 0]
facet_neighbours[slave_bc2bfi[:, 0], slave_bc2bfi[:, 1], 0] = \
master_bc2bfi[:, 0]
# set neighbours facets
facet_neighbours[slave_bc2bfi[:, 0], slave_bc2bfi[:, 1], 1] = \
master_bc2bfi[:, 1]
facet_neighbours[master_bc2bfi[:, 0], master_bc2bfi[:, 1], 1] =\
slave_bc2bfi[:, 1]
return facet_neighbours
def _set_fem_periodic_facet_neighbours(self, facet_neighbours, eq_map):
"""Maybe remove after DG EPBC revision in self.get_coor
Parameters
----------
facet_neighbours : array_like
Shape is (n_cell, n_el_facet, 2), first value is index of the
neighbouring cell the second is index of the facet in said nb. cell.
eq_map :
eq_map from state variable containing information on
EPBC and DG EPBC.
Returns
-------
facet_neighbours : ndarray
Updated incidence array.
"""
# treat classical FEM EPBCs - we need to correct neighbours
if eq_map.n_epbc > 0:
# set neighbours of periodic cells to one another
mcells = nm.unique(self.dofs2cells[eq_map.master])
scells = nm.unique(self.dofs2cells[eq_map.slave])
mcells_facets = nm.array(
nm.where(facet_neighbours[mcells] == -1))[1,
0] # facets mcells
scells_facets = nm.array(
nm.where(facet_neighbours[scells] == -1))[1,
0] # facets scells
# [1, 0] above, first we need second axis to get axis on which
# facet indices are stored, second we drop axis with neighbour
# local facet index,
#
# for multiple s/mcells this will have to be
# something like 1 + 2*nm.arange(len(mcells)) - to skip double
# entries for -1 tags in neighbours and neighbour local facet idx
# set neighbours of mcells to scells
facet_neighbours[mcells, mcells_facets, 0] = scells
# set neighbour facets to facets of scell missing neighbour
facet_neighbours[mcells, mcells_facets, 1] = scells_facets
# we do not need to distinguish EBC and EPBC cells, EBC overwrite
# EPBC, we only need to fix shapes
# set neighbours of scells to mcells
facet_neighbours[scells, scells_facets, 0] = mcells
# set neighbour facets to facets of mcell missing neighbour0
facet_neighbours[scells, scells_facets, 1] = mcells_facets
return facet_neighbours
@staticmethod
def get_region_info(region):
"""
Extracts information about region needed in various methods of DGField
Parameters
----------
region : sfepy.discrete.common.region.Region
Returns
-------
dim, n_cell, n_el_facets
"""
if not region.has_cells():
raise ValueError("Region {} has no cells".format(region.name))
n_cell = region.get_n_cells()
dim = region.tdim
gel = get_gel(region)
n_el_facets = dim + 1 if gel.is_simplex else 2**dim
return dim, n_cell, n_el_facets
def get_both_facet_state_vals(self,
state,
region,
derivative=None,
reduce_nod=True):
"""Computes values of the variable represented by dofs in
quadrature points located at facets, returns both values -
inner and outer, along with weights.
Parameters
----------
state : state variable containing BC info
region : sfepy.discrete.common.region.Region
derivative : compute derivative if truthy,
compute n-th derivative if a number (Default value = None)
reduce_nod : if False DOES NOT sum nodes into values at QPs
(Default value = True)
Returns
-------
inner_facet_values (n_cell, n_el_facets, n_qp),
outer facet values (n_cell, n_el_facets, n_qp),
weights,
if derivative is True:
inner_facet_values (n_cell, n_el_facets, dim, n_qp),
outer_facet values (n_cell, n_el_facets, dim, n_qp)
"""
if derivative:
diff = int(derivative)
else:
diff = 0
unreduce_nod = int(not reduce_nod)
inner_base_vals, outer_base_vals, whs = \
self.get_both_facet_base_vals(state, region, derivative=derivative)
dofs = self.unravel_sol(state.data[0])
n_qp = whs.shape[-1]
outputs_shape = (self.n_cell, self.n_el_facets) + \
(self.n_el_nod,) * unreduce_nod + \
(self.dim,) * diff + \
(n_qp,)
inner_facet_vals = nm.zeros(outputs_shape)
if unreduce_nod:
inner_facet_vals[:] = nm.einsum('id...,idf...->ifd...', dofs,
inner_base_vals)
else:
inner_facet_vals[:] = nm.einsum('id...,id...->i...', dofs,
inner_base_vals)
per_facet_neighbours = self.get_facet_neighbor_idx(
region, state.eq_map)
outer_facet_vals = nm.zeros(outputs_shape)
for facet_n in range(self.n_el_facets):
if unreduce_nod:
outer_facet_vals[:, facet_n, :] = \
nm.einsum('id...,id...->id...',
dofs[per_facet_neighbours[:, facet_n, 0]],
outer_base_vals[:, :, facet_n])
else:
outer_facet_vals[:, facet_n, :] = \
nm.einsum('id...,id...->i...',
dofs[per_facet_neighbours[:, facet_n, 0]],
outer_base_vals[:, :, facet_n])
boundary_cells = nm.array(
nm.where(per_facet_neighbours[:, :, 0] < 0)).T
outer_facet_vals[boundary_cells[:, 0], boundary_cells[:, 1]] = 0.0
# TODO detect and print boundary cells without defined BCs?
for ebc, ebc_vals in zip(state.eq_map.dg_ebc.get(diff, []),
state.eq_map.dg_ebc_val.get(diff, [])):
if unreduce_nod:
raise NotImplementedError(
"Unreduced DOFs are not available for boundary " +
"outerfacets")
outer_facet_vals[ebc[:, 0], ebc[:, 1], :] = \
nm.einsum("id,id...->id...",
ebc_vals, inner_base_vals[0, :, ebc[:, 1]])
else:
# fix flipping qp order to accomodate for
# opposite facet orientation of neighbours
outer_facet_vals[ebc[:, 0], ebc[:, 1], :] = ebc_vals[:, ::-1]
# flip outer_facet_vals moved to get_both_facet_base_vals
return inner_facet_vals, outer_facet_vals, whs
def get_both_facet_base_vals(self, state, region, derivative=None):
"""Returns values of the basis function in quadrature points on facets
broadcasted to all cells inner to the element as well as outer ones
along with weights for the qps broadcasted and transformed to elements.
Contains quick fix to flip facet QPs for right integration order.
Parameters
----------
state : used to get EPBC info
region : sfepy.discrete.common.region.Region for connectivity
derivative : if u need derivative
(Default value = None)
Returns
-------
outer_facet_base_vals:
inner_facet_base_vals:
shape (n_cell, n_el_nod, n_el_facet, n_qp) or
(n_cell, n_el_nod, n_el_facet, dim, n_qp)
when derivative is True or 1
whs: shape (n_cell, n_el_facet, n_qp)
"""
if derivative:
diff = int(derivative)
else:
diff = 0
facet_bf, whs = self.get_facet_base(derivative=derivative)
n_qp = nm.shape(whs)[1]
facet_vols = self.get_facet_vols(region)
whs = facet_vols * whs[None, :, :, 0]
base_shape = (self.n_cell, self.n_el_nod, self.n_el_facets) + \
(self.dim,) * diff + \
(n_qp,)
inner_facet_base_vals = nm.zeros(base_shape)
outer_facet_base_vals = nm.zeros(base_shape)
if derivative:
inner_facet_base_vals[:] = facet_bf[0, :, 0, :, :, :]\
.swapaxes(-2, -3).T
else:
inner_facet_base_vals[:] = facet_bf[:, 0, :, 0, :].T
per_facet_neighbours = self.get_facet_neighbor_idx(
region, state.eq_map)
# numpy prepends shape resulting from multiple
# indexing before remaining shape
if derivative:
outer_facet_base_vals[:] = \
inner_facet_base_vals[0, :, per_facet_neighbours[:, :, 1]]\
.swapaxes(-3, -4)
else:
outer_facet_base_vals[:] = \
inner_facet_base_vals[0, :, per_facet_neighbours[:, :, 1]]\
.swapaxes(-2, -3)
# fix to flip facet QPs for right integration order
return inner_facet_base_vals, outer_facet_base_vals[..., ::-1], whs
def clear_normals_cache(self, region=None):
"""Clears normals cache for given region or all regions.
Parameters
----------
region : sfepy.discrete.common.region.Region
region to clear cache or None to clear all
"""
if region is None:
self.normals_cache = {}
else:
if isinstance(region, str):
self.normals_cache.pop(region)
else:
self.normals_cache.pop(region.name)
def get_cell_normals_per_facet(self, region):
"""Caches results, use clear_normals_cache to clear the cache.
Parameters
----------
region: sfepy.discrete.common.region.Region
Main region, must contain cells.
Returns
-------
normals: ndarray
normals of facets in array of shape (n_cell, n_el_facets, dim)
"""
if region.name in self.normals_cache:
return self.normals_cache[region.name]
dim, n_cell, n_el_facets = self.get_region_info(region)
cmesh = region.domain.mesh.cmesh
normals = cmesh.get_facet_normals()
normals_out = nm.zeros((n_cell, n_el_facets, dim))
c2f = cmesh.get_conn(dim, dim - 1)
for ic, o1 in enumerate(c2f.offsets[:-1]):
o2 = c2f.offsets[ic + 1]
for ifal, ifa in enumerate(c2f.indices[o1:o2]):
normals_out[ic, ifal] = normals[o1 + ifal]
self.normals_cache[region.name] = normals_out
return normals_out
def clear_facet_vols_cache(self, region=None):
"""Clears facet volume cache for given region or all regions.
Parameters
----------
region : sfepy.discrete.common.region.Region
region to clear cache or None to clear all
"""
if region is None:
self.facet_vols_cache = {}
else:
if isinstance(region, str):
self.facet_vols_cache.pop(region)
else:
self.facet_vols_cache.pop(region.name)
def get_facet_vols(self, region):
"""Caches results, use clear_facet_vols_cache to clear the cache
Parameters
----------
region : sfepy.discrete.common.region.Region
Returns
-------
vols_out: ndarray
volumes of the facets by cells shape (n_cell, n_el_facets, 1)
"""
if region.name in self.facet_vols_cache:
return self.facet_vols_cache[region.name]
dim, n_cell, n_el_facets = self.get_region_info(region)
cmesh = region.domain.mesh.cmesh
if dim == 1:
vols = nm.ones((cmesh.num[0], 1))
else:
vols = cmesh.get_volumes(dim - 1)[:, None]
vols_out = nm.zeros((n_cell, n_el_facets, 1))
c2f = cmesh.get_conn(dim, dim - 1)
for ic, o1 in enumerate(c2f.offsets[:-1]):
o2 = c2f.offsets[ic + 1]
for ifal, ifa in enumerate(c2f.indices[o1:o2]):
vols_out[ic, ifal] = vols[ifa]
self.facet_vols_cache[region.name] = vols_out
return vols_out
def get_data_shape(self, integral, integration='volume', region_name=None):
"""Returns data shape
(n_nod, n_qp, self.gel.dim, self.n_el_nod)
Parameters
----------
integral : integral used
integration :
'volume' is only supported value (Default value = 'volume')
region_name : not used
(Default value = None)
Returns
-------
data_shape : tuple
"""
if integration in ('volume', ):
# from FEField.get_data_shape()
_, weights = integral.get_qp(self.gel.name)
n_qp = weights.shape[0]
data_shape = (self.n_cell, n_qp, self.gel.dim, self.n_el_nod)
# econn.shape[1] == n_el_nod i.e. number nod in element
else:
raise NotImplementedError('unsupported integration! (%s)' %
integration)
return data_shape
def get_econn(self, conn_type, region, is_trace=False, integration=None):
"""Getter for econn
Parameters
----------
conn_type : string or Struct
'volume' is only supported
region : sfepy.discrete.common.region.Region
is_trace : ignored
(Default value = False)
integration : ignored
(Default value = None)
Returns
-------
econn : ndarray
connectivity information
"""
ct = conn_type.type if isinstance(conn_type, Struct) else conn_type
if ct == 'volume':
if region.name == self.region.name:
conn = self.econn
else:
raise ValueError("Bad region for the field")
else:
raise ValueError('unknown connectivity type! (%s)' % ct)
return conn
def setup_extra_data(self, geometry, info, is_trace):
"""This is called in create_adof_conns(conn_info, var_indx=None,
active_only=True, verbose=True)
for each variable but has no effect.
Parameters
----------
geometry :
ignored
info :
set to self.info
is_trace :
set to self.trace
"""
# placeholder, what is this used for?
# dct = info.dc_type.type
self.info = info
self.is_trace = is_trace
def get_dofs_in_region(self, region, merge=True):
"""Return indices of DOFs that belong to the given region.
Not Used in BC treatment
Parameters
----------
region : sfepy.discrete.common.region.Region
merge : bool
merge dof tuple into one numpy array, default True
Returns
-------
dofs : ndarray
"""
dofs = []
if region.has_cells(): # main region or its part
els = nm.ravel(self.bubble_remap[region.cells])
eldofs = self.bubble_dofs[els[els >= 0]]
dofs.append(eldofs)
else:
# return indices of cells adjacent to boundary facets
dim = self.dim
cmesh = region.domain.mesh.cmesh
bc_cells = cmesh.get_incident(dim, region.facets, dim - 1)
bc_dofs = self.bubble_dofs[bc_cells]
dofs.append(bc_dofs)
if merge:
dofs = nm.concatenate(dofs)
return dofs
def get_bc_facet_idx(self, region):
"""Caches results in self.boundary_facet_local_idx
Parameters
----------
region : sfepy.discrete.common.region.Region
surface region defining BCs
Returns
-------
bc2bfi : ndarray
index of cells on boundary along with corresponding facets
"""
if region.name in self.boundary_facet_local_idx:
return self.boundary_facet_local_idx[region.name]
bc2bfi = region.get_facet_indices()
self.boundary_facet_local_idx[region.name] = bc2bfi
return bc2bfi
def create_mapping(self,
region,
integral,
integration,
return_mapping=True):
"""Creates and returns mapping
Parameters
----------
region : sfepy.discrete.common.region.Region
integral : Integral
integration : str
'volume' is only accepted option
return_mapping : default True
(Default value = True)
Returns
-------
mapping : VolumeMapping
"""
domain = self.domain
coors = domain.get_mesh_coors(actual=True)
dconn = domain.get_conn()
# from FEField
if integration == 'volume':
qp = self.get_qp('v', integral)
# qp = self.integral.get_qp(self.gel.name)
iels = region.get_cells()
geo_ps = self.gel.poly_space
ps = self.poly_space
bf = self.get_base('v', 0, integral, iels=iels)
conn = nm.take(dconn, iels.astype(nm.int32), axis=0)
mapping = VolumeMapping(coors, conn, poly_space=geo_ps)
vg = mapping.get_mapping(qp.vals,
qp.weights,
poly_space=ps,
ori=self.ori,
transform=self.basis_transform)
out = vg
else:
raise ValueError('unsupported integration geometry type: %s' %
integration)
if out is not None:
# Store the integral used.
out.integral = integral
out.qp = qp
out.ps = ps
# Update base.
out.bf[:] = bf
if return_mapping:
out = (out, mapping)
return out
def set_dofs(self, fun=0.0, region=None, dpn=None, warn=None):
"""Compute projection of fun into the basis, alternatively set DOFs
directly to provided value or values either in main volume region
or in boundary region.
Parameters
----------
fun : callable, scalar or array corresponding to dofs
(Default value = 0.0)
region : sfepy.discrete.common.region.Region
region to set DOFs on (Default value = None)
dpn : number of dofs per element
(Default value = None)
warn :
(Default value = None)
Returns
-------
nods : ndarray
vals : ndarray
"""
if region is None:
region = self.region
return self.set_cell_dofs(fun, region, dpn, warn)
elif region.has_cells():
return self.set_cell_dofs(fun, region, dpn, warn)
elif region.kind_tdim == self.dim - 1:
nods, vals = self.set_facet_dofs(fun, region, dpn, warn)
return nods, vals
def set_cell_dofs(self, fun=0.0, region=None, dpn=None, warn=None):
"""
Compute projection of fun onto the basis, in main region, alternatively
set DOFs directly to provided value or values
Parameters
----------
fun : callable, scallar or array corresponding to dofs
(Default value = 0.0)
region : sfepy.discrete.common.region.Region
region to set DOFs on (Default value = None)
dpn : number of dofs per element
(Default value = None)
warn : not used
(Default value = None)
Returns
-------
nods : ndarray
vals : ndarray
"""
aux = self.get_dofs_in_region(region)
nods = nm.unique(nm.hstack(aux))
if nm.isscalar(fun):
vals = nm.zeros(aux.shape)
vals[:, 0] = fun
vals = nm.hstack(vals)
elif isinstance(fun, nm.ndarray):
# useful for testing, allows to pass complete array of dofs as IC
if nm.shape(fun) == nm.shape(nods):
vals = fun
elif callable(fun):
qp, weights = self.integral.get_qp(self.gel.name)
coors = self.mapping.get_physical_qps(qp)
base_vals_qp = self.poly_space.eval_base(qp)[:, 0, :]
# this drops redundant axis that is returned by eval_base due to
# consistency with derivatives
# left hand, so far only orthogonal basis
# for legendre base this can be calculated exactly
# in 1D it is: 1 / (2 * nm.arange(self.n_el_nod) + 1)
lhs_diag = nm.einsum("q,q...->...", weights, base_vals_qp**2)
rhs_vec = nm.einsum("q,q...,iq...->i...", weights, base_vals_qp,
fun(coors))
vals = (rhs_vec / lhs_diag)
# plot for 1D
# from utils.visualizer import plot1D_legendre_dofs, reconstruct
# _legendre_dofs
# import matplotlib.pyplot as plt
# plot1D_legendre_dofs(self.domain.mesh.coors, (vals,), fun)
# ww, xx = reconstruct_legendre_dofs(self.domain.mesh.coors, 1,
# vals.T[..., None, None])
# plt.plot(xx, ww[:, 0], label="reconstructed dofs")
# plt.show()
return nods, vals
def set_facet_dofs(self, fun, region, dpn, warn):
"""Compute projection of fun onto the basis on facets, alternatively
set DOFs directly to provided value or values
Parameters
----------
fun : callable, scalar or array corresponding to dofs
region : sfepy.discrete.common.region.Region
region to set DOFs on
dpn : int
number of dofs per element
warn :
not used
Returns
-------
nods : ndarray
vals : ndarray
"""
raise NotImplementedError(
"Setting facet DOFs is not supported with DGField, " +
"use values at qp directly. " +
"This is usually result of using ebc instead of dgebc")
aux = self.get_dofs_in_region(region)
nods = nm.unique(nm.hstack(aux))
if nm.isscalar(fun):
vals = nm.zeros(aux.shape)
vals[:, 0] = fun
vals = nm.hstack(vals)
elif isinstance(fun, nm.ndarray):
assert_(len(fun) == dpn)
vals = nm.zeros(aux.shape)
vals[:, 0] = nm.repeat(fun, vals.shape[0])
elif callable(fun):
vals = nm.zeros(aux.shape)
# set zero DOF to value fun, set other DOFs to zero
# get facets QPs
qp, weights = self.get_facet_qp()
weights = weights[0, :, 0]
qp = qp[:, 0, :, :]
# get facets weights ?
# get coors
bc2bfi = self.get_bc_facet_idx(region)
coors = self.mapping.get_physical_qps(qp)
# get_physical_qps returns data in strange format, swapping
# some axis and flipping qps order
bcoors = coors[bc2bfi[:, 1], ::-1, bc2bfi[:, 0], :]
# get facet basis vals
base_vals_qp = self.poly_space.eval_base(qp)[:, 0, 0, :]
# solve for boundary cell DOFs
bc_val = fun(bcoors)
# this returns singular matrix - projection on the boundary should
# be into facet dim space
#lhs = nm.einsum("q,qd,qc->dc", weights, base_vals_qp, base_vals_qp)
# inv_lhs = nm.linalg.inv(lhs)
# rhs_vec = nm.einsum("q,q...,iq...->i...",
# weights, base_vals_qp, bc_val)
return nods, vals
def get_bc_facet_values(self, fun, region, ret_coors=False, diff=0):
"""Returns values of fun in facet QPs of the region
Parameters
----------
diff: derivative 0 or 1 supported
fun: Function value or values to set qps values to
region : sfepy.discrete.common.region.Region
boundary region
ret_coors: default False,
Return physical coors of qps in shape (n_cell, n_qp, dim).
Returns
-------
vals : ndarray
In shape (n_cell,) + (self.dim,) * diff + (n_qp,)
"""
if region.has_cells():
raise NotImplementedError(
"Region {} has cells and can't be used as boundary region".
format(region))
# get facets QPs
qp, weights = self.get_facet_qp()
weights = weights[0, :, 0]
qp = qp[:, 0, :, :]
n_qp = qp.shape[0]
# get facets weights ?
# get physical coors
bc2bfi = self.get_bc_facet_idx(region)
n_cell = bc2bfi.shape[0]
coors = self.mapping.get_physical_qps(qp)
# get_physical_qps returns data in strange format,
# swapping some axis and flipping qps order
# to get coors in shape (n_facet, n_qp, n_cell, dim)
if len(coors.shape) == 3:
coors = coors[:, None, :, :] # add axis for qps when it is missing
coors = coors.swapaxes(0, 2)
bcoors = coors[bc2bfi[:, 1], ::-1, bc2bfi[:, 0], :]
diff_shape = (self.dim, ) * diff
output_shape = (n_cell, ) + diff_shape + (n_qp, )
vals = nm.zeros(output_shape)
# we do not need last axis of coors, values are scalars
if nm.isscalar(fun):
if sum(diff_shape) > 1:
output(("Warning: Setting gradient of shape {} "
"in region {} with scalar value {}").format(
diff_shape, region.name, fun))
vals[:] = fun
elif isinstance(fun, nm.ndarray):
try:
vals[:] = fun[:, None]
except ValueError:
raise ValueError(("Provided values of shape {} could not" +
" be used to set BC qps of shape {} in " +
"region {}").format(fun.shape, vals.shape,
region.name))
elif callable(fun):
# get boundary values
vals[:] = fun(bcoors)
if ret_coors:
return bcoors, vals
return vals
def get_nodal_values(self, dofs, region, ref_nodes=None):
"""Computes nodal representation of the DOFs
Parameters
---------
dofs : array_like
dofs to transform to nodes
region : ignored
ref_nodes:
reference node to use instead of default qps
Parameters
----------
dofs : array_like
region : Region
ref_nodes : array_like
(Default value = None)
Returns
-------
nodes : ndarray
nodal_vals : ndarray
"""
if ref_nodes is None:
# poly_space could provide special nodes
ref_nodes = self.get_qp('v', self.integral).vals
base_vals_node = self.poly_space.eval_base(ref_nodes)[:, 0, :]
dofs = self.unravel_sol(dofs[:, 0])
nodal_vals = nm.sum(dofs * base_vals_node.T, axis=1)
nodes = self.mapping.get_physical_qps(ref_nodes)
# import matplotlib.pyplot as plt
# plt.plot(nodes[:, 0], nodal_vals)
# plt.show()
return nodes, nodal_vals
def create_output(self,
dofs,
var_name,
dof_names=None,
key=None,
extend=True,
fill_value=None,
linearization=None):
"""Converts the DOFs corresponding to the field to a dictionary of
output data usable by Mesh.write().
For 1D puts DOFs into vairables u_modal{0} ... u_modal{n}, where
n = approx_order and marks them for writing as cell data.
For 2+D puts dofs into name_cell_nodes and creates sturct with:
mode = "cell_nodes", data and iterpolation scheme.
Also get node values and adds them to dictionary as cell_nodes
Parameters
----------
dofs : ndarray, shape (n_nod, n_component)
The array of DOFs reshaped so that each column corresponds
to one component.
var_name : str
The variable name corresponding to `dofs`.
dof_names : tuple of str
The names of DOF components. (Default value = None)
key : str, optional
The key to be used in the output dictionary instead of the
variable name. (Default value = None)
extend : bool, not used
Extend the DOF values to cover the whole domain.
(Default value = True)
fill_value : float or complex, not used
The value used to fill the missing DOF values if `extend` is True.
(Default value = None)
linearization : Struct or None, not used
The linearization configuration for higher order approximations.
(Default value = None)
Returns
-------
out : dict
"""
out = {}
udofs = self.unravel_sol(dofs)
name = var_name if key is None else key
if self.dim == 1:
for i in range(self.n_el_nod):
out[name + "_modal{}".format(i)] = \
Struct(mode="cell", data=udofs[:, i, None, None])
else:
interpolation_scheme = self.poly_space.get_interpol_scheme()
unravel = get_unraveler(self.n_el_nod, self.n_cell)
out[name + "_cell_nodes"] = Struct(mode="cell_nodes",
data=unravel(dofs)[..., 0],
scheme=interpolation_scheme)
return out
def _gen_common_data(orders, gels, report):
import sfepy
from sfepy.base.base import Struct
from sfepy.linalg import combine
from sfepy.discrete import FieldVariable, Integral
from sfepy.discrete.fem import Mesh, FEDomain, Field
from sfepy.discrete.common.global_interp import get_ref_coors
bases = ([ii
for ii in combine([['2_4', '3_8'], ['lagrange', 'lobatto']])] +
[ii for ii in combine([['2_3', '3_4'], ['lagrange']])])
for geom, poly_space_base in bases:
report('geometry: %s, base: %s' % (geom, poly_space_base))
order = orders[geom]
integral = Integral('i', order=order)
aux = '' if geom in ['2_4', '3_8'] else 'z'
mesh0 = Mesh.from_file('meshes/elements/%s_2%s.mesh' % (geom, aux),
prefix_dir=sfepy.data_dir)
gel = gels[geom]
perms = gel.get_conn_permutations()
qps, qp_weights = integral.get_qp(gel.surface_facet.name)
zz = nm.zeros_like(qps[:, :1])
qps = nm.hstack(([qps] + [zz]))
shift = shifts[geom]
rcoors = nm.ascontiguousarray(qps + shift[:1, :] - shift[1:, :])
ccoors = nm.ascontiguousarray(qps + shift[:1, :] + shift[1:, :])
for ir, pr in enumerate(perms):
for ic, pc in enumerate(perms):
report('ir: %d, ic: %d' % (ir, ic))
report('pr: %s, pc: %s' % (pr, pc))
mesh = mesh0.copy()
conn = mesh.cmesh.get_conn(mesh0.cmesh.tdim, 0).indices
conn = conn.reshape((mesh0.n_el, -1))
conn[0, :] = conn[0, pr]
conn[1, :] = conn[1, pc]
conn2 = mesh.get_conn(gel.name)
assert_((conn == conn2).all())
cache = Struct(mesh=mesh)
domain = FEDomain('domain', mesh)
omega = domain.create_region('Omega', 'all')
region = domain.create_region('Facet', rsels[geom], 'facet')
field = Field.from_args('f',
nm.float64,
shape=1,
region=omega,
approx_order=order,
poly_space_base=poly_space_base)
var = FieldVariable('u', 'unknown', field)
report('# dofs: %d' % var.n_dof)
vec = nm.empty(var.n_dof, dtype=var.dtype)
ps = field.poly_space
dofs = field.get_dofs_in_region(region, merge=False)
edofs, fdofs = nm.unique(dofs[1]), nm.unique(dofs[2])
rrc, rcells, rstatus = get_ref_coors(field,
rcoors,
cache=cache)
crc, ccells, cstatus = get_ref_coors(field,
ccoors,
cache=cache)
assert_((rstatus == 0).all() and (cstatus == 0).all())
yield (geom, poly_space_base, qp_weights, mesh, ir, ic, field,
ps, rrc, rcells[0], crc, ccells[0], vec, edofs, fdofs)
fields = {
'fu': ('real', 6, 'Omega', 1, 'H1', 'shell10x'),
}
variables = {
'u' : ('unknown field', 'fu', 0),
'v' : ('test field', 'fu', 'u'),
}
ebcs = {
'fix' : ('Gamma1', {'u.all' : 0.0}),
}
# Custom integral.
aux = Integral('i', order=3)
qp_coors, qp_weights = aux.get_qp('3_8')
qp_coors[:, 2] = thickness * (qp_coors[:, 2] - 0.5)
qp_weights *= thickness
integrals = {
'i' : ('custom', qp_coors, qp_weights),
}
equations = {
'elasticity' :
"""dw_shell10x.i.Omega(m.D, m.drill, v, u)
= dw_point_load.i.Gamma2(load.val, v)""",
}
solvers = {
'ls' : ('ls.scipy_direct', {}),
def main():
parser = OptionParser(usage=usage, version='%prog')
parser.add_option('-b', '--basis', metavar='name',
action='store', dest='basis',
default='lagrange', help=help['basis'])
parser.add_option('-n', '--max-order', metavar='order', type=int,
action='store', dest='max_order',
default=10, help=help['max_order'])
parser.add_option('-m', '--matrix', metavar='type',
action='store', dest='matrix_type',
default='laplace', help=help['matrix_type'])
parser.add_option('-g', '--geometry', metavar='name',
action='store', dest='geometry',
default='2_4', help=help['geometry'])
options, args = parser.parse_args()
dim, n_ep = int(options.geometry[0]), int(options.geometry[2])
output('reference element geometry:')
output(' dimension: %d, vertices: %d' % (dim, n_ep))
n_c = {'laplace' : 1, 'elasticity' : dim}[options.matrix_type]
output('matrix type:', options.matrix_type)
output('number of variable components:', n_c)
output('polynomial space:', options.basis)
output('max. order:', options.max_order)
mesh = Mesh.from_file(data_dir + '/meshes/elements/%s_1.mesh'
% options.geometry)
domain = FEDomain('domain', mesh)
omega = domain.create_region('Omega', 'all')
orders = nm.arange(1, options.max_order + 1, dtype=nm.int)
conds = []
order_fix = 0 if options.geometry in ['2_4', '3_8'] else 1
for order in orders:
output('order:', order, '...')
field = Field.from_args('fu', nm.float64, n_c, omega,
approx_order=order,
space='H1', poly_space_base=options.basis)
to = field.approx_order
quad_order = 2 * (max(to - order_fix, 0))
output('quadrature order:', quad_order)
integral = Integral('i', order=quad_order)
qp, _ = integral.get_qp(options.geometry)
output('number of quadrature points:', qp.shape[0])
u = FieldVariable('u', 'unknown', field)
v = FieldVariable('v', 'test', field, primary_var_name='u')
m = Material('m', lam=1.0, mu=1.0)
if options.matrix_type == 'laplace':
term = Term.new('dw_laplace(m.mu, v, u)',
integral, omega, m=m, v=v, u=u)
n_zero = 1
else:
assert_(options.matrix_type == 'elasticity')
term = Term.new('dw_lin_elastic_iso(m.lam, m.mu, v, u)',
integral, omega, m=m, v=v, u=u)
n_zero = (dim + 1) * dim / 2
term.setup()
output('assembling...')
tt = time.clock()
mtx, iels = term.evaluate(mode='weak', diff_var='u')
output('...done in %.2f s' % (time.clock() - tt))
mtx = mtx[0][0, 0]
try:
assert_(nm.max(nm.abs(mtx - mtx.T)) < 1e-10)
except:
from sfepy.base.base import debug; debug()
output('matrix shape:', mtx.shape)
eigs = eig(mtx, method='eig.sgscipy', eigenvectors=False)
eigs.sort()
# Zero 'true' zeros.
eigs[:n_zero] = 0.0
ii = nm.where(eigs < 0.0)[0]
if len(ii):
output('matrix is not positive semi-definite!')
ii = nm.where(eigs[n_zero:] < 1e-12)[0]
if len(ii):
output('matrix has more than %d zero eigenvalues!' % n_zero)
output('smallest eigs:\n', eigs[:10])
ii = nm.where(eigs > 0.0)[0]
emin, emax = eigs[ii[[0, -1]]]
output('min:', emin, 'max:', emax)
cond = emax / emin
conds.append(cond)
output('condition number:', cond)
output('...done')
plt.figure(1)
plt.semilogy(orders, conds)
plt.xticks(orders, orders)
plt.xlabel('polynomial order')
plt.ylabel('condition number')
plt.grid()
plt.figure(2)
plt.loglog(orders, conds)
plt.xticks(orders, orders)
plt.xlabel('polynomial order')
plt.ylabel('condition number')
plt.grid()
plt.show()
def _gen_common_data(orders, gels, report):
import sfepy
from sfepy.base.base import Struct
from sfepy.linalg import combine
from sfepy.discrete import FieldVariable, Integral
from sfepy.discrete.fem import Mesh, FEDomain, Field
from sfepy.discrete.common.global_interp import get_ref_coors
bases = ([ii for ii in combine([['2_4', '3_8'],
['lagrange', 'lobatto']])]
+ [ii for ii in combine([['2_3', '3_4'],
['lagrange']])])
for geom, poly_space_base in bases:
report('geometry: %s, base: %s' % (geom, poly_space_base))
order = orders[geom]
integral = Integral('i', order=order)
aux = '' if geom in ['2_4', '3_8'] else 'z'
mesh0 = Mesh.from_file('meshes/elements/%s_2%s.mesh' % (geom, aux),
prefix_dir=sfepy.data_dir)
gel = gels[geom]
perms = gel.get_conn_permutations()
qps, qp_weights = integral.get_qp(gel.surface_facet.name)
zz = nm.zeros_like(qps[:, :1])
qps = nm.hstack(([qps] + [zz]))
shift = shifts[geom]
rcoors = nm.ascontiguousarray(qps
+ shift[:1, :] - shift[1:, :])
ccoors = nm.ascontiguousarray(qps
+ shift[:1, :] + shift[1:, :])
for ir, pr in enumerate(perms):
for ic, pc in enumerate(perms):
report('ir: %d, ic: %d' % (ir, ic))
report('pr: %s, pc: %s' % (pr, pc))
mesh = mesh0.copy()
conn = mesh.get_conn(gel.name)
conn[0, :] = conn[0, pr]
conn[1, :] = conn[1, pc]
cache = Struct(mesh=mesh)
domain = FEDomain('domain', mesh)
omega = domain.create_region('Omega', 'all')
region = domain.create_region('Facet', rsels[geom], 'facet')
field = Field.from_args('f', nm.float64, shape=1,
region=omega, approx_order=order,
poly_space_base=poly_space_base)
var = FieldVariable('u', 'unknown', field)
report('# dofs: %d' % var.n_dof)
vec = nm.empty(var.n_dof, dtype=var.dtype)
ap = field.ap
ps = ap.interp.poly_spaces['v']
dofs = field.get_dofs_in_region(region, merge=False)
edofs, fdofs = nm.unique(dofs[1]), nm.unique(dofs[2])
rrc, rcells, rstatus = get_ref_coors(field, rcoors,
cache=cache)
crc, ccells, cstatus = get_ref_coors(field, ccoors,
cache=cache)
assert_((rstatus == 0).all() and (cstatus == 0).all())
yield (geom, poly_space_base, qp_weights, mesh, ir, ic,
ap, ps, rrc, rcells[0], crc, ccells[0],
vec, edofs, fdofs)
