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Lambert Theisen
fenicsR13
Commits
03c3fccb
Commit
03c3fccb
authored
Aug 02, 2019
by
Lambert Theisen
Browse files
Add two case to coupled system
parent
82159bb6
Changes
2
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tests/coupled/inputs/01_coeffs_sources_rot.yml
→
tests/coupled/inputs/01_coeffs_sources_rot
_p1p1p1p1p1_stab
.yml
View file @
03c3fccb
File moved
tests/coupled/inputs/01_coeffs_sources_rot_p2p2p2p2p2_stab.yml
0 → 100644
View file @
03c3fccb
# Case name, used as output folder
case_name
:
01_source_rot_p1p1p1_stab
# Meshes
# ======
# Input files in h5 format.
# List containing one or more meshes to perform simulation on.
meshes
:
-
../mesh/ring0.h5
-
../mesh/ring1.h5
-
../mesh/ring2.h5
-
../mesh/ring3.h5
-
../mesh/ring4.h5
# - ../mesh/ring5.h5
# - ../mesh/ring6.h5 # fails on Macbook 8GB
# - ../mesh/ring7.h5 # fails on iMac 24GB, works on iMac 48GB
# - ../mesh/ring6.h5
elements
:
"
theta"
:
"
shape"
:
"
Lagrange"
"
degree"
:
2
"
s"
:
"
shape"
:
"
Lagrange"
"
degree"
:
2
"
p"
:
"
shape"
:
"
Lagrange"
"
degree"
:
2
"
u"
:
"
shape"
:
"
Lagrange"
"
degree"
:
2
"
sigma"
:
"
shape"
:
"
Lagrange"
"
degree"
:
2
# Stabilization
# =============
# - continous interior penalty (cip) with three parameters delta_i
stabilization
:
cip
:
enable
:
True
delta_1
:
1.0
delta_2
:
1.0
delta_3
:
0.01
# Formulation Parameters
# ======================
# Number of spatial dimensions, currently only two-dimensional.
nsd
:
2
# heat, stress, coupled
mode
:
"
coupled"
# Coefficients as in westerkamp2019 or without as in torrilhon2017
use_coeffs
:
True
# Knudsen number
tau
:
1.0
# Refaction coefficient
xi_tilde
:
1.0
# xi_tilde: 0.7978845608 # sqrt(2/pi)
bcs
:
3000
:
"
name"
:
"
inner"
"
theta_w"
:
1.0
"
v_t"
:
-10.0
3100
:
"
name"
:
"
outer"
"
theta_w"
:
0.5
"
v_t"
:
0.0
# heat source
heat_source
:
"
0"
# mass source
mass_source
:
"
1.0
*
(1.0
-
(5.0*pow(R,2))/(18.0*pow(tau,2)))
*
cos(phi)"
# Perform convergence study on given set of meshes with exact solution
convergence_study
:
enable
:
True
exact_solution
:
esols/01_coeffs_sources_rot.cpp
plot
:
True
write_systemmatrix
:
False
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