deepmodeling / jax-fem

Differentiable Finite Element Method with JAX
GNU General Public License v3.0
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differentiable-programming finite-element-methods jax topology-optimization

A GPU-accelerated differentiable finite element analysis package based on JAX. Used to be part of the suite of open-source python packages for Additive Manufacturing (AM) research, JAX-AM.

Finite Element Method (FEM)

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FEM is a powerful tool, where we support the following features

Updates (Dec 11, 2023):

Thermal profile in direct energy deposition.

Linear static analysis of a bracket.

Crystal plasticity: grain structure (left) and stress-xx (right).

Stokes flow: velocity (left) and pressure(right).

Topology optimization with differentiable simulation.

Installation

Create a conda environment from the given environment.yml file and activate it:

conda env create -f environment.yml
conda activate jax-fem-env

Install JAX

Then there are two options to continue:

Option 1

Clone the repository:

git clone https://github.com/deepmodeling/jax-fem.git
cd jax-fem

and install the package locally:


pip install -e .

Quick tests: You can check demos/ for a variety of FEM cases. For example, run

python -m demos.hyperelasticity.example

for hyperelasticity.

Also,

python -m tests.benchmarks

will execute a set of test cases.

Option 2

Install the package from the PyPI release directly:

pip install jax-fem

Quick tests: You can create an example.py file and run it:

python example.py
import jax
import jax.numpy as np
import os

from jax_fem.problem import Problem
from jax_fem.solver import solver
from jax_fem.utils import save_sol
from jax_fem.generate_mesh import get_meshio_cell_type, Mesh, rectangle_mesh

class Poisson(Problem):
    def get_tensor_map(self):
        return lambda x: x

    def get_mass_map(self):
        def mass_map(u, x):
            val = -np.array([10*np.exp(-(np.power(x[0] - 0.5, 2) + np.power(x[1] - 0.5, 2)) / 0.02)])
            return val
        return mass_map

ele_type = 'QUAD4'
cell_type = get_meshio_cell_type(ele_type)
Lx, Ly = 1., 1.
meshio_mesh = rectangle_mesh(Nx=32, Ny=32, domain_x=Lx, domain_y=Ly)
mesh = Mesh(meshio_mesh.points, meshio_mesh.cells_dict[cell_type])

def left(point):
    return np.isclose(point[0], 0., atol=1e-5)

def right(point):
    return np.isclose(point[0], Lx, atol=1e-5)

def bottom(point):
    return np.isclose(point[1], 0., atol=1e-5)

def top(point):
    return np.isclose(point[1], Ly, atol=1e-5)

def dirichlet_val(point):
    return 0.

location_fns = [left, right, bottom, top]
value_fns = [dirichlet_val]*4
vecs = [0]*4
dirichlet_bc_info = [location_fns, vecs, value_fns]

problem = Poisson(mesh=mesh, vec=1, dim=2, ele_type=ele_type, dirichlet_bc_info=dirichlet_bc_info)
sol = solver(problem, linear=True, use_petsc=True)

data_dir = os.path.join(os.path.dirname(__file__), 'data')
vtk_path = os.path.join(data_dir, f'vtk/u.vtu')
save_sol(problem.fes[0], sol[0], vtk_path)

By running the code above and use Paraview for visualization, you should see the following solution

Solution to the Poisson's equation due to a source term.

License

This project is licensed under the GNU General Public License v3 - see the LICENSE for details.

Citations

If you found this library useful in academic or industry work, we appreciate your support if you consider 1) starring the project on Github, and 2) citing relevant papers:

@article{xue2023jax,
  title={JAX-FEM: A differentiable GPU-accelerated 3D finite element solver for automatic inverse design and mechanistic data science},
  author={Xue, Tianju and Liao, Shuheng and Gan, Zhengtao and Park, Chanwook and Xie, Xiaoyu and Liu, Wing Kam and Cao, Jian},
  journal={Computer Physics Communications},
  pages={108802},
  year={2023},
  publisher={Elsevier}
}