Commit bee702af authored by Jeremy BLEYER's avatar Jeremy BLEYER

Some updates of Reissner DG

parent 411bbced
......@@ -10,16 +10,18 @@ Introduction
-------------
This program solves the Reissner-Mindlin plate equations on the unit
square with uniform transverse loading and simply supported boundary conditions.
square with uniform transverse loading and clamped boundary conditions.
The corresponding file can be obtained from :download:`reissner_mindlin_dg.py`.
It uses a Discontinuous Galerkin interpolation for the rotation field to
remove shear-locking issues in the thin plate limit. Details of the formulation
can be found in *P. Hansbo et al., Comput. Methods Appl. Mech. Engrg. 200 (2011) 638–648*,
https://doi.org/10.1016/j.cma.2010.09.009
can be found in [HAN2011]_.
The solution for :math:`w` in this demo will look as follows:
The solution for :math:`\theta_x` on the middle line of equation :math:`y=0.5`
will look as follows for 10 elements and a stabilization parameter :math:`s=1`:
.. image:: dg_rotation_N10_s1.png
:scale: 15%
......@@ -30,6 +32,7 @@ Implementation
Material properties and loading are the same as in :ref:`ReissnerMindlinQuads`::
from __future__ import print_function
from fenics import *
E = Constant(1e3)
......@@ -45,37 +48,37 @@ The unit square mesh is here divided in triangles and we get the facet MeshFunct
mesh = UnitSquareMesh(N, N)
facets = MeshFunction("size_t", mesh, 1)
facets.set_all(0)
ds = Measure("ds")[facets]
ds = Measure("ds", subdomain_data=facets)
Continuous interpolation using of degree 2 is chosen for the deflection :math:`w`
whereas the rotation field :math:`\underline{\theta}` is discretized using discontinuous linear polynomials::
We = FiniteElement("Lagrange", mesh.ufl_cell(), 2)
Te = VectorElement("DG", mesh.ufl_cell(), 1)
V = FunctionSpace(mesh,MixedElement([We,Te]))
V = FunctionSpace(mesh, MixedElement([We, Te]))
Clamped boundary conditions on the lateral boundary are defined as::
def border(x, on_boundary):
return on_boundary
bc = [DirichletBC(V.sub(0),Constant(0.), border)]
bc = [DirichletBC(V.sub(0), Constant(0.), border)]
Standard part of the variational form is the same (without full integration)::
def strain2voigt(eps):
return as_vector([eps[0,0],eps[1,1],2*eps[0,1]])
return as_vector([eps[0, 0], eps[1, 1], 2*eps[0, 1]])
def voigt2stress(S):
return as_tensor([[S[0],S[2]],[S[2],S[1]]])
return as_tensor([[S[0], S[2]], [S[2], S[1]]])
def curv(u):
(w,theta) = split(u)
(w, theta) = split(u)
return sym(grad(theta))
def shear_strain(u):
(w,theta) = split(u)
(w, theta) = split(u)
return theta-grad(w)
def bending_moment(u):
DD = as_tensor([[D,nu*D,0],[nu*D,D,0],[0,0,D*(1-nu)/2.]])
DD = as_tensor([[D, nu*D, 0], [nu*D, D, 0],[0, 0, D*(1-nu)/2.]])
return voigt2stress(dot(DD,strain2voigt(curv(u))))
def shear_force(u):
return F*shear_strain(u)
......@@ -86,7 +89,7 @@ Standard part of the variational form is the same (without full integration)::
L = f*u_[0]*dx
a = inner(bending_moment(u_),curv(du))*dx + dot(shear_force(u_),shear_strain(du))*dx
a = inner(bending_moment(u_), curv(du))*dx + dot(shear_force(u_), shear_strain(du))*dx
We then add the contribution of jumps in rotation across all internal facets plus
......@@ -97,27 +100,27 @@ a stabilization term involing a user-defined parameter :math:`s`::
h_avg = (h('+')+h('-'))/2
stabilization = Constant(10.)
(dw,dtheta) = split(du)
(w_,theta_) = split(u_)
(dw, dtheta) = split(du)
(w_, theta_) = split(u_)
a -= dot(avg(dot(bending_moment(u_),n)),jump(dtheta))*dS + dot(avg(dot(bending_moment(du),n)),jump(theta_))*dS \
- stabilization*D/h_avg*dot(jump(theta_),jump(dtheta))*dS
a -= dot(avg(dot(bending_moment(u_), n)), jump(dtheta))*dS + dot(avg(dot(bending_moment(du), n)), jump(theta_))*dS \
- stabilization*D/h_avg*dot(jump(theta_), jump(dtheta))*dS
Because of the clamped boundary conditions, we also need to add the corresponding
contributions of the external facets (the imposed rotation is zero on the boundary
so that no term arise in the linear functional)::
a -= dot(dot(bending_moment(u_),n),dtheta)*ds + dot(dot(bending_moment(du),n),theta_)*ds \
- 2*stabilization*D/h*dot(theta_,dtheta)*ds
a -= dot(dot(bending_moment(u_), n), dtheta)*ds + dot(dot(bending_moment(du), n), theta_)*ds \
- 2*stabilization*D/h*dot(theta_, dtheta)*ds
We then solve for the solution and export the relevant fields to XDMF files ::
solve(a == L, u, bc)
(w,theta) = split(u)
(w, theta) = split(u)
Vw = FunctionSpace(mesh,We)
Vt = FunctionSpace(mesh,Te)
Vw = FunctionSpace(mesh, We)
Vt = FunctionSpace(mesh, Te)
ww = Function(Vw, name="Deflection")
tt = Function(Vt, name="Rotation")
ww.assign(project(w, Vw))
......@@ -131,5 +134,13 @@ We then solve for the solution and export the relevant fields to XDMF files ::
The solution is compared to the Kirchhoff analytical solution::
print "Kirchhoff deflection:", -1.265319087e-3*float(f/D)
print "Reissner-Mindlin FE deflection:", ww(0.5,0.5)
\ No newline at end of file
print("Kirchhoff deflection:", -1.265319087e-3*float(f/D))
print("Reissner-Mindlin FE deflection:", -ww(0.5, 0.5))
For :math:`h=0.001` and 50 elements per side, one finds :math:`w_{FE} = 1.38322\text{e-5}` against :math:`w_{\text{Kirchhoff}} = 1.38173\text{e-5}` for the thin plate solution.
-----------
References
-----------
.. [HAN2011] Peter Hansbo, David Heintz, Mats G. Larson, A finite element method with discontinuous rotations for the Mindlin-Reissner plate model, *Computer Methods in Applied Mechanics and Engineering*, 200, 5-8, 2011, pp. 638-648, https://doi.org/10.1016/j.cma.2010.09.009.
\ No newline at end of file
......@@ -32,6 +32,7 @@ Implementation
Material parameters for isotropic linear elastic behavior are first defined::
from __future__ import print_function
from fenics import *
E = Constant(1e3)
......@@ -60,31 +61,31 @@ Continuous interpolation using of degree :math:`d=\texttt{deg}` is chosen for bo
deg = 1
We = FiniteElement("Lagrange", mesh.ufl_cell(), deg)
Te = VectorElement("Lagrange", mesh.ufl_cell(), deg)
V = FunctionSpace(mesh,MixedElement([We,Te]))
V = FunctionSpace(mesh, MixedElement([We, Te]))
Clamped boundary conditions on the lateral boundary are defined as::
def border(x, on_boundary):
return on_boundary
bc = [DirichletBC(V,Constant((0.,0.,0.)), border)]
bc = [DirichletBC(V, Constant((0., 0., 0.)), border)]
Some useful functions for implementing generalized constitutive relations are now
defined::
def strain2voigt(eps):
return as_vector([eps[0,0],eps[1,1],2*eps[0,1]])
return as_vector([eps[0, 0], eps[1, 1], 2*eps[0, 1]])
def voigt2stress(S):
return as_tensor([[S[0],S[2]],[S[2],S[1]]])
return as_tensor([[S[0], S[2]], [S[2], S[1]]])
def curv(u):
(w,theta) = split(u)
(w, theta) = split(u)
return sym(grad(theta))
def shear_strain(u):
(w,theta) = split(u)
(w, theta) = split(u)
return theta-grad(w)
def bending_moment(u):
DD = as_tensor([[D,nu*D,0],[nu*D,D,0],[0,0,D*(1-nu)/2.]])
DD = as_tensor([[D, nu*D, 0], [nu*D, D, 0],[0, 0, D*(1-nu)/2.]])
return voigt2stress(dot(DD,strain2voigt(curv(u))))
def shear_force(u):
return F*shear_strain(u)
......@@ -99,20 +100,20 @@ and for quadratic (:math:`d=2`) quadrilaterals, as if it were quadratic (2x2 Gau
u_ = TestFunction(V)
du = TrialFunction(V)
dx_shear = dx(metadata={"quadrature_degree":2*deg-2})
dx_shear = dx(metadata={"quadrature_degree": 2*deg-2})
L = f*u_[0]*dx
a = inner(bending_moment(u_),curv(du))*dx + dot(shear_force(u_),shear_strain(du))*dx_shear
a = inner(bending_moment(u_), curv(du))*dx + dot(shear_force(u_), shear_strain(du))*dx_shear
We then solve for the solution and export the relevant fields to XDMF files ::
solve(a == L, u, bc)
(w,theta) = split(u)
(w, theta) = split(u)
Vw = FunctionSpace(mesh,We)
Vt = FunctionSpace(mesh,Te)
Vw = FunctionSpace(mesh, We)
Vt = FunctionSpace(mesh, Te)
ww = Function(Vw, name="Deflection")
tt = Function(Vt, name="Rotation")
ww.assign(project(w, Vw))
......@@ -126,10 +127,10 @@ We then solve for the solution and export the relevant fields to XDMF files ::
The solution is compared to the Kirchhoff analytical solution::
print "Kirchhoff deflection:", -1.265319087e-3*float(f/D)
print "Reissner-Mindlin FE deflection:", -min(ww.vector().get_local()) # point evaluation for quads
print("Kirchhoff deflection:", -1.265319087e-3*float(f/D))
print("Reissner-Mindlin FE deflection:", -min(ww.vector().get_local())) # point evaluation for quads
# is not implemented in fenics 2017.2
For ``N=50`` quads per side, one finds :math:`w_{FE} = 1.38182\text{e-5}` for linear quads
For :math:`h=0.001` and 50 quads per side, one finds :math:`w_{FE} = 1.38182\text{e-5}` for linear quads
and :math:`w_{FE} = 1.38176\text{e-5}` for quadratic quads against :math:`w_{\text{Kirchhoff}} = 1.38173\text{e-5}` for
the thin plate solution.
\ No newline at end of file
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