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newmark.py
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Created
Sat, Nov 16, 20:21
Size
5 KB
Mime Type
text/x-python
Expires
Mon, Nov 18, 20:21 (2 d)
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blob
Format
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Handle
22341637
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rAKA akantu
newmark.py
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#!/usr/bin/python
################################################################
import
akantu
import
numpy
as
np
import
os
,
subprocess
################################################################
class
FixedValue
:
def
__init__
(
self
,
value
,
axis
):
self
.
value
=
value
if
axis
==
'x'
:
axis
=
0
if
axis
==
'y'
:
axis
=
1
self
.
axis
=
axis
def
operator
(
self
,
node
,
flags
,
disp
,
coord
):
# sets the displacement to the desired value in the desired axis
disp
[
self
.
axis
]
=
self
.
value
# sets the blocked dofs vector to true in the desired axis
flags
[
self
.
axis
]
=
True
################################################################
class
LocalElastic
:
def
__init__
(
self
):
## young modulus
self
.
E
=
1
## Poisson coefficient
self
.
nu
=
0.3
## density
self
.
rho
=
1
## First Lame coefficient
self
.
_lambda
=
self
.
nu
*
self
.
E
/
((
1
+
self
.
nu
)
*
(
1
-
2
*
self
.
nu
))
## Second Lame coefficient (shear modulus)
self
.
mu
=
self
.
E
/
(
2
*
(
1
+
self
.
nu
));
## declares all the internals
def
registerInternals
(
self
):
return
[]
## declares all the parameters that could be parsed
def
registerParam
(
self
):
return
[]
## declares all the parameters that are needed
def
getPushWaveSpeed
(
self
):
return
np
.
sqrt
((
self
.
_lambda
+
2
*
self
.
mu
)
/
self
.
rho
);
## constitutive law for a given quadrature point
def
computeStress
(
self
,
grad_u
,
sigma
,
internals
):
lbda
=
1.
mu
=
1.
trace
=
grad_u
.
trace
();
sigma
[:,:]
=
lbda
*
trace
*
np
.
eye
(
2
)
+
mu
*
(
grad_u
+
grad_u
.
T
)
################################################################
def
main
():
spatial_dimension
=
2
Lbar
=
10.
akantu
.
initialize
(
'material.dat'
)
mesh_file
=
'bar.msh'
max_steps
=
250
time_step
=
1e-3
#if mesh was not created the calls gmsh to generate it
if
not
os
.
path
.
isfile
(
mesh_file
):
import
subprocess
ret
=
subprocess
.
call
(
'gmsh -2 bar.geo bar.msh'
,
shell
=
True
)
if
not
ret
==
0
:
raise
Exception
(
'execution of GMSH failed: do you have it installed ?'
)
################################################################
## Initialization
################################################################
mesh
=
akantu
.
Mesh
(
spatial_dimension
)
mesh
.
read
(
mesh_file
)
mesh
.
createGroupsFromStringMeshData
(
"physical_names"
)
model
=
akantu
.
SolidMechanicsModel
(
mesh
)
model
.
initFull
(
akantu
.
SolidMechanicsModelOptions
(
akantu
.
_explicit_lumped_mass
,
True
))
mat
=
LocalElastic
()
model
.
registerNewPythonMaterial
(
mat
,
"local_elastic"
)
model
.
initMaterials
()
model
.
setBaseName
(
"waves"
)
model
.
addDumpFieldVector
(
"displacement"
)
model
.
addDumpFieldVector
(
"acceleration"
)
model
.
addDumpFieldVector
(
"velocity"
)
model
.
addDumpField
(
"blocked_dofs"
)
################################################################
## Boundary conditions
################################################################
residual
=
model
.
getResidual
()
mass
=
model
.
getMass
()
displacement
=
model
.
getDisplacement
()
acceleration
=
model
.
getAcceleration
()
velocity
=
model
.
getVelocity
()
blocked_dofs
=
model
.
getBlockedDOFs
()
################################################################
## boundary conditions
################################################################
model
.
applyDirichletBC
(
FixedValue
(
0
,
'x'
),
"XBlocked"
)
model
.
applyDirichletBC
(
FixedValue
(
0
,
'y'
),
"YBlocked"
)
################################################################
## initial conditions
################################################################
nb_nodes
=
mesh
.
getNbNodes
()
position
=
mesh
.
getNodes
()
pulse_width
=
1
A
=
0.01
for
i
in
range
(
0
,
nb_nodes
):
# Sinus * Gaussian
x
=
position
[
i
,
0
]
-
5.
L
=
pulse_width
k
=
0.1
*
2
*
np
.
pi
*
3
/
L
displacement
[
i
,
0
]
=
A
*
np
.
sin
(
k
*
x
)
*
np
.
exp
(
-
(
k
*
x
)
*
(
k
*
x
)
/
(
L
*
L
))
################################################################
## timestep value computation
################################################################
time_factor
=
0.8
stable_time_step
=
model
.
getStableTimeStep
()
*
time_factor
print
"Stable Time Step = {0}"
.
format
(
stable_time_step
)
print
"Required Time Step = {0}"
.
format
(
time_step
)
time_step
=
stable_time_step
*
time_factor
model
.
setTimeStep
(
time_step
)
################################################################
## loop for evolution of motion dynamics
################################################################
model
.
updateResidual
()
epot
=
model
.
getEnergy
(
'potential'
)
ekin
=
model
.
getEnergy
(
'kinetic'
)
print
"step,step * time_step,epot,ekin,epot + ekin"
for
step
in
range
(
0
,
max_steps
+
1
):
model
.
dump
()
## output energy calculation to screen
print
"{0},{1},{2},{3},{4}"
.
format
(
step
,
step
*
time_step
,
epot
,
ekin
,
(
epot
+
ekin
))
model
.
solveStep
()
akantu
.
finalize
()
return
################################################################
if
__name__
==
"__main__"
:
main
()
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