# -*- coding: utf-8 -*-
"""
This file is part of FElupe.
FElupe is free software: you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation, either version 3 of the License, or
(at your option) any later version.
FElupe is distributed in the hope that it will be useful,
but WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
GNU General Public License for more details.
You should have received a copy of the GNU General Public License
along with FElupe. If not, see <http://www.gnu.org/licenses/>.
"""
import inspect
import warnings
import numpy as np
from ..assembly import IntegralForm
from ..constitution import AreaChange
from ..math import det, dot, transpose
from ..tools._plot import ViewSolid
from ._helpers import Assemble, Evaluate, Results
class Solid:
"Base class for solid bodies which provides methods for visualisations."
def view(self, point_data=None, cell_data=None, cell_type=None, project=None):
"""View the solid with optional given dicts of point- and cell-data items.
Parameters
----------
point_data : dict or None, optional
Additional point-data dict (default is None).
cell_data : dict or None, optional
Additional cell-data dict (default is None).
cell_type : pyvista.CellType or None, optional
Cell-type of PyVista (default is None).
project : callable or None, optional
Project stress at quadrature-points to mesh-points (default is None).
Returns
-------
felupe.ViewSolid
An object which provides visualization methods for solid bodies,
e.g. :class:`felupe.SolidBody`.
See Also
--------
felupe.ViewSolid : Visualization methods for :class:`felupe.SolidBody`.
felupe.project: Project given values at quadrature-points to mesh-points.
felupe.topoints: Shift given values at quadrature-points to mesh-points.
"""
return ViewSolid(
self.field,
solid=self,
point_data=point_data,
cell_data=cell_data,
cell_type=cell_type,
project=project,
)
def plot(self, *args, project=None, **kwargs):
"""Plot the solid body.
See Also
--------
felupe.Scene.plot: Plot method of a scene.
felupe.project: Project given values at quadrature-points to mesh-points.
felupe.topoints: Shift given values at quadrature-points to mesh-points.
"""
return self.view(project=project).plot(*args, **kwargs)
def screenshot(
self,
*args,
filename="solidbody.png",
transparent_background=None,
scale=None,
**kwargs,
):
"""Take a screenshot of the solid body.
See Also
--------
pyvista.Plotter.screenshot: Take a screenshot of a PyVista plotter.
"""
return self.plot(*args, off_screen=True, **kwargs).screenshot(
filename=filename,
transparent_background=transparent_background,
scale=scale,
)
def imshow(self, *args, ax=None, dpi=None, **kwargs):
"""Take a screenshot of the solid body, show the image data in a figure and
return the ax.
"""
if ax is None:
import matplotlib.pyplot as plt
fig, ax = plt.subplots(dpi=dpi)
ax.imshow(self.screenshot(*args, filename=None, **kwargs))
ax.set_axis_off()
return ax
[docs]
class SolidBody(Solid):
r"""A SolidBody with methods for the assembly of sparse vectors/matrices.
Parameters
----------
umat : class
A class which provides methods for evaluating the gradient and the hessian of
the strain energy density function per unit undeformed volume. The function
signatures must be ``dψdF, ζ_new = umat.gradient([F, ζ])`` for
the gradient and ``d2ψdFdF = umat.hessian([F, ζ])`` for the hessian of
the strain energy density function :math:`\psi(\boldsymbol{F})`, where
:math:`\boldsymbol{F}` is the deformation gradient tensor and :math:`\zeta`
holds the array of internal state variables.
field : FieldContainer
A field container with one or more fields.
statevars : ndarray or None, optional
Array of initial internal state variables (default is None).
Notes
-----
The total potential energy of internal forces is given in Eq.
:eq:`solidbody`
.. math::
:label: solidbody
\Pi_{int}(\boldsymbol{F}) = \int_V \psi(\boldsymbol{F})\ dV
with its variation, see Eq. :eq:`solidbody-variation`
.. math::
:label: solidbody-variation
\delta_\boldsymbol{u}(\Pi_{int}) =
\int_V \frac{\partial \psi}{\partial \boldsymbol{F}} \ dV
\longrightarrow \boldsymbol{f}_\boldsymbol{u}
and linearization, see Eq. :eq:`solidbody-linearization`. The right-arrows in
Eq. :eq:`solidbody-variation` and Eq. :eq:`solidbody-linearization`
represent the assembly into system scalars, vectors or matrices.
.. math::
:label: solidbody-linearization
\delta_\boldsymbol{u}\Delta_\boldsymbol{u}(\Pi_{int}) =
\int_V \delta\boldsymbol{F} :
\frac{\partial^2 \psi}{
\partial \boldsymbol{F}\ \partial \boldsymbol{F}
} : \Delta\boldsymbol{F}\ dV
\longrightarrow \boldsymbol{K}_{\boldsymbol{u}\boldsymbol{u}}
The displacement-based formulation leads to a linearized equation system as given in
Eq. :eq:`solidbody-final`.
.. math::
:label: solidbody-final
\boldsymbol{K}_{\boldsymbol{u}\boldsymbol{u}} \cdot \delta \boldsymbol{u} +
\boldsymbol{f}_\boldsymbol{u} = \boldsymbol{0}
.. note::
This class also supports ``umat`` with mixed-field formulations like
:class:`~felupe.NearlyIncompressible` or :class:`~felupe.ThreeFieldVariation`.
Examples
--------
.. pyvista-plot::
>>> import felupe as fem
>>>
>>> mesh = fem.Cube(n=6)
>>> region = fem.RegionHexahedron(mesh)
>>> field = fem.FieldContainer([fem.Field(region, dim=3)])
>>> boundaries, loadcase = fem.dof.uniaxial(field, clamped=True)
>>>
>>> umat = fem.NeoHooke(mu=1, bulk=2)
>>> solid = fem.SolidBody(umat, field)
>>>
>>> table = fem.math.linsteps([0, 1], num=5)
>>> step = fem.Step(
... items=[solid],
... ramp={boundaries["move"]: table},
... boundaries=boundaries,
... )
>>>
>>> job = fem.Job(steps=[step]).evaluate()
>>> solid.plot("Principal Values of Cauchy Stress").show()
See Also
--------
felupe.SolidBodyNearlyIncompressible : A (nearly) incompressible solid body with
methods for the assembly of sparse vectors/matrices.
"""
def __init__(self, umat, field, statevars=None):
self.umat = umat
self.field = field
self.results = Results(stress=True, elasticity=True)
self.results.kinematics = self._extract(self.field)
if statevars is not None:
self.results.statevars = statevars
else:
statevars_shape = (0,)
if hasattr(umat, "x"):
statevars_shape = umat.x[-1].shape
self.results.statevars = np.zeros(
(
*statevars_shape,
field.region.quadrature.npoints,
field.region.mesh.ncells,
)
)
self.assemble = Assemble(vector=self._vector, matrix=self._matrix)
self.evaluate = Evaluate(
gradient=self._gradient,
hessian=self._hessian,
cauchy_stress=self._cauchy_stress,
kirchhoff_stress=self._kirchhoff_stress,
)
self._area_change = AreaChange()
self._form = IntegralForm
def _vector(self, field=None, parallel=False, items=None, args=(), kwargs=None):
if kwargs is None:
kwargs = {}
if field is not None:
self.field = field
self.results.stress = self._gradient(field, args=args, kwargs=kwargs)
self.results.force = self._form(
fun=self.results.stress[slice(items)],
v=self.field,
dV=self.field.region.dV,
).assemble(parallel=parallel)
return self.results.force
def _matrix(self, field=None, parallel=False, items=None, args=(), kwargs=None):
if kwargs is None:
kwargs = {}
if field is not None:
self.field = field
self.results.elasticity = self._hessian(field, args=args, kwargs=kwargs)
form = self._form(
fun=self.results.elasticity[slice(items)],
v=self.field,
u=self.field,
dV=self.field.region.dV,
)
self.results.stiffness_values = form.integrate(
parallel=parallel, out=self.results.stiffness_values
)
self.results.stiffness = form.assemble(values=self.results.stiffness_values)
return self.results.stiffness
def _extract(self, field):
self.field = field
self.results.kinematics = self.field.extract(out=self.results.kinematics)
return self.results.kinematics
def _gradient(self, field=None, args=(), kwargs=None):
if kwargs is None:
kwargs = {}
if field is not None:
self.field = field
self.results.kinematics = self._extract(self.field)
if "out" in inspect.signature(self.umat.gradient).parameters:
kwargs["out"] = self.results.gradient
gradient = self.umat.gradient(
[*self.results.kinematics, self.results.statevars], *args, **kwargs
)
self.results.gradient = gradient[0]
self.results.stress, self.results._statevars = gradient[:-1], gradient[-1]
return self.results.stress
def _hessian(self, field=None, args=(), kwargs=None):
if kwargs is None:
kwargs = {}
if field is not None:
self.field = field
self.results.kinematics = self._extract(self.field)
if "out" in inspect.signature(self.umat.hessian).parameters:
kwargs["out"] = self.results.hessian
self.results.elasticity = self.umat.hessian(
[*self.results.kinematics, self.results.statevars], *args, **kwargs
)
self.results.hessian = self.results.elasticity[0]
return self.results.elasticity
def _kirchhoff_stress(self, field=None):
self._gradient(field)
P = self.results.stress[0]
F = self.results.kinematics[0]
return dot(P, transpose(F))
def _cauchy_stress(self, field=None):
self._gradient(field)
P = self.results.stress[0]
F = self.results.kinematics[0]
if P.shape[:2] == (2, 2):
warnings.warn(
"\n".join(
[
"Cauchy stress tensor can't be evaluated on a 2d-Field.",
"Falling-back to the Kirchhoff stress tensor.",
]
)
)
J = 1
else:
J = det(F)
return dot(P, transpose(F)) / J
