forked from precice/tutorials
-
Notifications
You must be signed in to change notification settings - Fork 0
Commit
This commit does not belong to any branch on this repository, and may belong to a fork outside of the repository.
Add nutils solid participant to perpendicular flap (precice#431)
* add nutils solid participant * Add new nutils solver to README list --------- Co-authored-by: Benjamin Uekermann <[email protected]>
- Loading branch information
1 parent
5a5c695
commit 1828d10
Showing
4 changed files
with
114 additions
and
0 deletions.
There are no files selected for viewing
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,6 @@ | ||
#!/bin/sh | ||
set -e -u | ||
|
||
. ../../tools/cleaning-tools.sh | ||
|
||
clean_nutils . |
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,4 @@ | ||
#!/bin/sh | ||
set -e -u | ||
|
||
python3 solid.py richoutput=no |
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,102 @@ | ||
#! /usr/bin/env python3 | ||
|
||
from nutils import mesh, function, solver, export, cli | ||
from nutils.expression_v2 import Namespace | ||
import numpy | ||
import treelog | ||
import precice | ||
|
||
|
||
def main(young=4e6, density=3e3, poisson=.3, nelems=2, timestepsize=0.01, npoints_per_elem=3): | ||
|
||
topo, geom = mesh.rectilinear([numpy.linspace(-.05, .05, nelems+1), numpy.linspace(0, 1, 10*nelems+1)]) | ||
wall = topo.boundary['left,top,right'].sample('uniform', npoints_per_elem) | ||
|
||
ns = Namespace() | ||
ns.X = geom | ||
ns.δ = function.eye(2) | ||
ns.define_for('X', gradient='∇', normal='n', jacobians=('dV', 'dS')) | ||
ns.add_field('dt') | ||
ns.add_field(('u', 'u0', 'testu', 'v', 'v0', 'testv'), topo.basis('std', degree=1), shape=(2,)) | ||
ns.add_field('F', wall.basis(), shape=(2,)) | ||
ns.qw = 1 / npoints_per_elem # quadrature weight | ||
ns.t_i = 'F_i / qw dS' | ||
ns.dudt_i = '(u_i - u0_i) / dt' | ||
ns.dvdt_i = '(v_i - v0_i) / dt' | ||
ns.ρ = density | ||
ns.λ = young * poisson / ((1 + poisson) * (1 - 2 * poisson)) | ||
ns.μ = young / (2 * (1 + poisson)) | ||
ns.σ_ij = 'λ ∇_k(u_k) δ_ij + μ (∇_j(u_i) + ∇_i(u_j))' | ||
|
||
# make sure we correctly scale point forces to tractions | ||
testforce = numpy.random.normal(size=(wall.npoints, 2)) | ||
numpy.testing.assert_almost_equal( | ||
actual=wall.integrate('t_i dS' @ ns, F=testforce), | ||
desired=testforce.sum(0), | ||
decimal=10, | ||
err_msg='nutils error: failed to recover net force') | ||
|
||
# continuum equations: ρ v' = ∇·σ + F, u' = v | ||
res = topo.integral('testv_i (dudt_i - v_i) dV' @ ns, degree=2) | ||
res += topo.integral('(testu_i ρ dvdt_i + ∇_j(testu_i) σ_ij) dV' @ ns, degree=2) | ||
res -= wall.integral('testu_i t_i dS' @ ns) | ||
|
||
# boundary conditions: fully constrained at y=0 | ||
sqr = topo.boundary['bottom'].integral('u_k u_k' @ ns, degree=2) | ||
cons = solver.optimize('u,', sqr, droptol=1e-10) | ||
|
||
# initial conditions: undeformed and unmoving | ||
sqr = topo.integral('u_k u_k + v_k v_k' @ ns, degree=2) | ||
arguments = solver.optimize('u,v', sqr, constrain=cons) | ||
|
||
# preCICE setup | ||
solverProcessIndex = 0 | ||
solverProcessSize = 1 | ||
interface = precice.Interface("Solid", "../precice-config.xml", solverProcessIndex, solverProcessSize) | ||
meshID = interface.get_mesh_id("Solid-Mesh") | ||
dataIndices = interface.set_mesh_vertices(meshID, wall.eval(ns.X)) | ||
writedataID = interface.get_data_id("Displacement", meshID) | ||
readdataID = interface.get_data_id("Force", meshID) | ||
|
||
# initialize preCICE | ||
precice_dt = interface.initialize() | ||
|
||
timestep = 0 | ||
force = numpy.zeros((wall.npoints, 2)) | ||
|
||
while interface.is_coupling_ongoing(): | ||
with treelog.context(f'timestep {timestep}'): | ||
|
||
# read displacements from interface | ||
if interface.is_read_data_available(): | ||
force = interface.read_block_vector_data(readdataID, dataIndices) | ||
|
||
# save checkpoint | ||
if interface.is_action_required(precice.action_write_iteration_checkpoint()): | ||
checkpoint = timestep, arguments | ||
interface.mark_action_fulfilled(precice.action_write_iteration_checkpoint()) | ||
|
||
# advance variables | ||
timestep += 1 | ||
dt = min(precice_dt, timestepsize) | ||
arguments = dict(dt=dt, u0=arguments['u'], v0=arguments['v'], F=force) | ||
arguments = solver.solve_linear('u:testu,v:testv', res, arguments=arguments, constrain=cons) | ||
|
||
# write forces to interface | ||
if interface.is_write_data_required(dt): | ||
writedata = wall.eval(ns.u, **arguments) | ||
interface.write_block_vector_data(writedataID, dataIndices, writedata) | ||
|
||
# do the coupling | ||
precice_dt = interface.advance(dt) | ||
|
||
# read checkpoint if required | ||
if interface.is_action_required(precice.action_read_iteration_checkpoint()): | ||
timestep, arguments = checkpoint | ||
interface.mark_action_fulfilled(precice.action_read_iteration_checkpoint()) | ||
|
||
interface.finalize() | ||
|
||
|
||
if __name__ == '__main__': | ||
cli.run(main) |