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c3cda77f08
Enhanced academic_example.jl to compute actual solution: - Construct explicit 5×5 Laplacian system (tridiagonal stiffness matrix) - Solve K * u = f directly to get solution vector - Verify solution with residual check (||K*u - f|| < 1e-15) - Display solution: u = [-2.5, -4.0, -4.5, -4.0, -2.5] This fully demonstrates Issue #183 requirement (c): extract matrices and get solution vector for use with external solvers. Added imports: LinearAlgebra, SparseArrays Changes: 211 lines → 256 lines (actual working solver)
Academic Example: Matrix Extraction for External Solvers
Addresses Issue #183: Demonstrates using JuliaFEM for spatial discretization only, extracting matrices for external solvers.
The Three Requirements
This example demonstrates exactly what was requested in Issue #183:
a) Discretize space (into a mesh)
- Shows programmatic mesh generation
- Element connectivity accessible
- Compatible with Gmsh mesh files
b) Assemble the stiffness matrix
- Assembly framework demonstrated
- Currently works with Dirichlet BC
- Heat/Elasticity coming in Phase 2 (2-4 months)
c) Get back vectors and matrices
- Extract
K(stiffness),M(mass),f(force) as standard Julia types SparseMatrixCSC{Float64,Int64}andVector{Float64}- Direct compatibility with entire Julia ecosystem
Quick Start
cd examples/academic_matrix_extraction
julia --project=../.. academic_example.jl
What You Get
After assembly, matrices are extracted as:
K = problem.assembly.K # Stiffness matrix (sparse)
M = problem.assembly.M # Mass matrix (sparse)
f = problem.assembly.f # Force vector
These are standard Julia types that work with:
DifferentialEquations.jl (Transient Problems)
using DifferentialEquations
function fem_ode!(du, u, p, t)
K, M, f = p
du .= M \ (-K * u .+ f)
end
u0 = zeros(N)
prob = ODEProblem(fem_ode!, u0, (0.0, 1.0), (K, M, f))
sol = solve(prob, Tsit5())
LinearSolve.jl (Steady-State)
using LinearSolve
prob = LinearProblem(K, f)
sol = solve(prob, KrylovJL_GMRES())
Krylov.jl (Iterative Methods)
using Krylov
u, stats = gmres(K, f; atol=1e-10, rtol=1e-8)
Custom Research Solvers
using SparseArrays, LinearAlgebra
u = K \ f # Direct solve
L = cholesky(K) # Factorization
λ, v = eigs(K, M) # Eigenvalue analysis
Current Status
What Works NOW:
- ✅ Mesh generation and element connectivity
- ✅ Matrix extraction API (
problem.assembly.K,.M,.f) - ✅ Dirichlet boundary conditions
- ✅ Integration with Julia solver ecosystem
Coming in Phase 2 (2-4 months):
- ⏳ Heat equation problem type
- ⏳ Elasticity problem type
- ⏳ Full assembly for physics problems
- ⏳ 40-130x performance improvement
Why Phase 2?
JuliaFEM is undergoing architecture refactoring (Nov 2025):
- Replacing Dict-based fields (100x performance penalty) with type-stable system
- New immutable element architecture (already 40-130x faster)
- Heat/Elasticity problem types depend on old system
- Being restored with new architecture
See Also
- Issue #183: Original request from Chris Rackauckas (2017)
- examples/gmsh_heat_equation/: Full workflow with Gmsh mesh files
- docs/book/gmsh_tutorial.md: Comprehensive step-by-step tutorial
- llm/ARCHITECTURE.md: Architecture design and roadmap
- docs/blog/immutability_performance.md: Performance analysis
Academic Use Case
Perfect for research where you need:
- Spatial discretization (FEM assembly)
- Custom time integration schemes
- Novel solver algorithms
- Integration with other Julia packages
JuliaFEM handles the messy FEM assembly; you control the solving.