FluxFEM: A weak-form-centric differentiable finite element framework in JAX
Project description
FluxFEM
A weak-form-centric differentiable finite element framework in JAX, where variational forms are treated as first-class, differentiable programs.
Examples and Features
| Example 1: Diffusion | Example 2: Neo Neohookean Hyper Elasticity |
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Features
- Built on JAX, enabling automatic differentiation with grad, jit, vmap, and related transformations.
- Weak-form–centric API that keeps formulations close to code; weak forms are represented as expression trees and compiled into element kernels, enabling automatic differentiation of residuals, tangents, and objectives.
- Two assembly approaches: tensor-based (scikit-fem–style) assembly and weak-form-based assembly.
- Handles both linear and nonlinear analyses with AD in JAX.
Usage
This library provides two assembly approaches.
- A tensor-based assembly, where trial and test functions are represented explicitly as element-level tensors and assembled accordingly (in the style of scikit-fem).
- A weak-form-based assembly, where the variational form is written symbolically and compiled before assembly.
The two approaches are functionally equivalent and share the same element-level execution model,
but they differ in how you author the weak form. The example below mirrors the paper's diffusion
case and makes the distinction explicit with jnp.
Assembly Flow
All expressions are first compiled into an element-level evaluation plan, which operates on quadrature-point–major tensors. This plan is then executed independently for each element during assembly.
As a result, both assembly approaches:
- use the same quadrature-major (q, a, i) data layout,
- perform element-local tensor contractions,
- and are fully compatible with JAX transformations such as
jit,vmap, and automatic differentiation.
kernel-based assembly (explicit JIT units)
If you want to control JIT boundaries explicitly, build a JIT-compiled element kernel
and pass it to space.assemble_*. The kernel must return the integrated element
contribution (not the quadrature integrand).
import fluxfem as ff
import jax
import jax.numpy as jnp
space = ff.make_hex_space(mesh, dim=1, intorder=2)
# bilinear: kernel(ctx) -> (n_ldofs, n_ldofs)
ker_K = ff.make_element_bilinear_kernel(ff.diffusion_form, 1.0, jit=True)
K = space.assemble_bilinear_form(ff.diffusion_form, 1.0, kernel=ker_K)
# linear: kernel(ctx) -> (n_ldofs,)
def linear_kernel(ctx):
integrand = ff.scalar_body_force_form(ctx, 2.0)
wJ = ctx.w * ctx.test.detJ
return (integrand * wJ[:, None]).sum(axis=0)
ker_F = jax.jit(linear_kernel)
F = space.assemble_linear_form(ff.scalar_body_force_form, 2.0, kernel=ker_F)
tensor-based vs weak-form-based (diffusion example)
tensor-based assembly
The tensor-based assembly provides an explicit, low-level formulation with element kernels written using jax.numpy.(jnp).
import fluxfem as ff
import jax.numpy as jnp
def diffusion_form(ctx: ff.FormContext, kappa):
# ctx.test.gradN / ctx.trial.gradN: (n_qp, n_nodes, dim)
# output tensor: (n_qp, n_nodes, n_nodes)
return kappa * jnp.einsum("qia,qja->qij", ctx.test.gradN, ctx.trial.gradN)
space = ff.make_hex_space(mesh, dim=3, intorder=2)
params = ff.Params(kappa=1.0)
K_ts = space.assemble_bilinear_form(diffusion_form, params=params.kappa)
weak-form-based assembly
In the weak-form-based assembly, the variational formulation itself is the primary object. The expression below defines a symbolic computation graph, which is later compiled and executed at the element level.
import fluxfem as ff
import fluxfem.helpers_wf as h_wf
space = ff.make_hex_space(mesh, dim=3, intorder=2)
params = ff.Params(kappa=1.0)
# u, v are symbolic trial/test fields (weak-form DSL objects).
# u.grad / v.grad are symbolic nodes (expression tree), not numeric arrays.
# dOmega() is the integral measure; the whole expression is compiled before assembly.
form_wf = ff.BilinearForm.volume(
lambda u, v, p: p.kappa * (v.grad @ u.grad) * h_wf.dOmega()
).get_compiled()
K_wf = space.assemble_bilinear_form(form_wf, params=params)
Linear Elasticity assembly (weak-form based assembly)
import fluxfem as ff
import fluxfem.helpers_wf as h_wf
space = ff.make_hex_space(mesh, dim=3, intorder=2)
D = ff.isotropic_3d_D(1.0, 0.3)
form_wf = ff.BilinearForm.volume(
lambda u, v, D: h_wf.ddot(v.sym_grad, D @ u.sym_grad) * h_wf.dOmega()
).get_compiled()
K = space.assemble_bilinear_form(form_wf, params=D)
Neo-Hookean residual assembly (weak-form DSL)
Below is a Neo-Hookean hyperelasticity example written in weak form. The residual is expressed symbolically and compiled into element-level kernels executed per element. No manual derivation of tangent operators is required; consistent tangents (Jacobians) for Newton-type solvers are obtained automatically via JAX AD.
def neo_hookean_residual_wf(v, u, params):
mu = params["mu"]
lam = params["lam"]
F = h_wf.I(3) + h_wf.grad(u) # deformation gradient
C = h_wf.matmul(h_wf.transpose(F), F)
C_inv = h_wf.inv(C)
J = h_wf.det(F)
S = mu * (h_wf.I(3) - C_inv) + lam * h_wf.log(J) * C_inv
dE = 0.5 * (h_wf.matmul(h_wf.grad(v), F) + h_wf.transpose(h_wf.matmul(h_wf.grad(v), F)))
return h_wf.ddot(S, dE) * h_wf.dOmega()
autodiff + jit compile
You can differentiate through the solve and JIT compile the hot path. The inverse diffusion tutorial shows this pattern:
def loss_theta(theta):
kappa = jnp.exp(theta)
u = solve_u_jit(kappa, traction_true)
diff = u[obs_idx_j] - u_obs[obs_idx_j]
return 0.5 * jnp.mean(diff * diff)
solve_u_jit = jax.jit(solve_u)
loss_theta_jit = jax.jit(loss_theta)
grad_fn = jax.jit(jax.grad(loss_theta))
Documentation
Full documentation, tutorials, and API reference are hosted at this site.
SetUp
You can install FluxFEM either via pip or Poetry.
Supported Python Versions
FluxFEM supports Python 3.11–3.13:
Choose one of the following methods:
Using pip
pip install fluxfem
Using poetry
poetry add fluxfem
Acknowledgements
I acknowledge the open-source software, libraries, and communities that made this work possible.
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