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Co-Authored-By: Claude Opus 4.7 (1M context) <noreply@anthropic.com>
2026-05-20 23:52:15 +09:00

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id, title, category, status, canonical_id, aliases, duplicate_of, source_trust_level, confidence_score, verification_status, tags, raw_sources, last_reinforced, github_commit, tech_stack
id title category status canonical_id aliases duplicate_of source_trust_level confidence_score verification_status tags raw_sources last_reinforced github_commit tech_stack
wiki-2026-0508-finite-element-analysis Finite Element Analysis (FEA) 10_Wiki/Topics verified self
FEA
FEM
finite element method
structural analysis
ANSYS
Abaqus
mesh
none A 0.95 applied
engineering
fea
fem
simulation
structural
mesh
computational-mechanics
2026-05-10 pending
language framework
Python / FORTRAN / C++ ANSYS / Abaqus / FEniCS / PyANSYS

Finite Element Analysis (FEA)

매 한 줄

"매 PDE 의 의 의 mesh 의 element 의 의 discretize 의 solve". 매 structural, thermal, fluid, EM. 매 famous: ANSYS, Abaqus, NASTRAN. 매 modern: 매 FEniCS (open), 매 ML-augmented (PINN, GNN), 매 cloud HPC.

매 핵심

매 step

  1. Geometry / CAD.
  2. Mesh (1D, 2D, 3D element).
  3. Material (E, ν, ρ, ...).
  4. Boundary condition + load.
  5. Assemble (K matrix).
  6. Solve (linear / nonlinear).
  7. Post-process.

매 element type

  • 1D: bar, beam.
  • 2D: triangle, quad (CST, LST).
  • 3D: tet, hex, wedge.
  • Shell: 매 thin structure.

매 analysis type

  • Static linear.
  • Modal (eigenvalue).
  • Dynamic (transient).
  • Nonlinear (geom, material, contact).
  • Thermal.
  • CFD (Navier-Stokes).
  • EM (Maxwell).

매 modern AI

  • PINN (physics-informed NN).
  • GNN-based (faster surrogate).
  • Differentiable FEM (JAX-FEM).
  • NeRF for material.

매 응용

  1. Aerospace: 매 wing.
  2. Automotive: 매 crash.
  3. Civil: 매 building.
  4. Biomedical: 매 implant.
  5. Electronics: 매 PCB thermal.
  6. Geomechanics: 매 dam.

💻 패턴

FEniCS (open-source)

from dolfinx import fem, mesh, plot
from mpi4py import MPI
import ufl

domain = mesh.create_rectangle(MPI.COMM_WORLD, [(0,0), (1,1)], (32,32))
V = fem.FunctionSpace(domain, ('Lagrange', 1))

# 매 BC
def boundary(x): return np.isclose(x[0], 0) | np.isclose(x[0], 1)
bc = fem.dirichletbc(0.0, fem.locate_dofs_geometrical(V, boundary), V)

# 매 weak form (Poisson)
u = ufl.TrialFunction(V); v = ufl.TestFunction(V)
f = fem.Constant(domain, 1.0)
a = ufl.dot(ufl.grad(u), ufl.grad(v)) * ufl.dx
L = f * v * ufl.dx

# 매 solve
problem = fem.petsc.LinearProblem(a, L, bcs=[bc])
uh = problem.solve()

Stiffness matrix (1D bar)

import numpy as np

def bar_stiffness(E, A, L):
    """매 1D bar element."""
    k = E * A / L
    return np.array([[k, -k], [-k, k]])

def assemble(elements, n_nodes):
    K = np.zeros((n_nodes, n_nodes))
    for (e, k_local) in elements:
        for i, gi in enumerate(e):
            for j, gj in enumerate(e):
                K[gi, gj] += k_local[i, j]
    return K

Mesh generation (gmsh)

import gmsh
gmsh.initialize()
gmsh.model.add('plate')
gmsh.model.geo.addPoint(0, 0, 0, 0.1, 1)
gmsh.model.geo.addPoint(1, 0, 0, 0.1, 2)
gmsh.model.geo.addPoint(1, 1, 0, 0.1, 3)
gmsh.model.geo.addPoint(0, 1, 0, 0.1, 4)
gmsh.model.geo.addLine(1, 2, 1)
# ... 4 lines
gmsh.model.geo.addPlaneSurface([1])
gmsh.model.mesh.generate(2)
gmsh.write('plate.msh')

PyANSYS (commercial integration)

from ansys.mapdl.core import launch_mapdl
mapdl = launch_mapdl()
mapdl.prep7()
mapdl.et(1, 'BEAM188')
mapdl.mp('EX', 1, 200e9)  # 매 Steel
mapdl.k(1, 0); mapdl.k(2, 1); mapdl.l(1, 2)
mapdl.lesize('all', '', '', 10)
mapdl.lmesh('all')
mapdl.solve()
mapdl.post1()

Modal analysis

from scipy.linalg import eigh
def modal(K, M, n_modes=5):
    """매 K φ = ω² M φ."""
    eigvals, eigvecs = eigh(K, M)
    freqs_hz = np.sqrt(eigvals[:n_modes]) / (2 * np.pi)
    return freqs_hz, eigvecs[:, :n_modes]

Nonlinear (Newton-Raphson)

def newton_raphson(K_fn, R_fn, u0, tol=1e-6, max_iter=50):
    u = u0.copy()
    for _ in range(max_iter):
        residual = R_fn(u)
        if np.linalg.norm(residual) < tol: return u
        K = K_fn(u)
        du = np.linalg.solve(K, -residual)
        u += du
    raise ConvergenceError()

PINN (physics-informed)

import torch
class PINN(torch.nn.Module):
    def __init__(self):
        super().__init__()
        self.net = torch.nn.Sequential(
            torch.nn.Linear(2, 64), torch.nn.Tanh(),
            torch.nn.Linear(64, 64), torch.nn.Tanh(),
            torch.nn.Linear(64, 1),
        )
    
    def forward(self, x):
        return self.net(x)
    
    def physics_loss(self, x):
        x.requires_grad = True
        u = self.forward(x)
        u_x = torch.autograd.grad(u.sum(), x, create_graph=True)[0]
        u_xx = torch.autograd.grad(u_x.sum(), x, create_graph=True)[0]
        # 매 e.g., Poisson: -u_xx = f
        return ((-u_xx + 1) ** 2).mean()

GNN-based surrogate (MeshGraphNet)

import torch_geometric.nn as gnn

class MeshGraphNet(torch.nn.Module):
    def __init__(self, node_dim=3, edge_dim=3, hidden=128):
        super().__init__()
        self.encoder = gnn.MLP([node_dim, hidden, hidden])
        self.processor = torch.nn.ModuleList([gnn.GCNConv(hidden, hidden) for _ in range(15)])
        self.decoder = torch.nn.Linear(hidden, node_dim)
    
    def forward(self, x, edge_index):
        x = self.encoder(x)
        for layer in self.processor:
            x = torch.relu(layer(x, edge_index))
        return self.decoder(x)

Convergence test

def mesh_convergence(solver_fn, mesh_sizes):
    """매 element size 의 의 의 result 의 stable?"""
    results = {}
    for h in mesh_sizes:
        results[h] = solver_fn(h)
    diffs = [abs(results[mesh_sizes[i]] - results[mesh_sizes[i+1]]) for i in range(len(mesh_sizes)-1)]
    return diffs

Post-processing (paraview)

import pyvista as pv
mesh = pv.read('result.vtk')
mesh.plot(scalars='displacement', cmap='viridis')

Material library

MATERIALS = {
    'steel': {'E': 200e9, 'nu': 0.3, 'rho': 7850, 'sy': 250e6},
    'aluminum': {'E': 70e9, 'nu': 0.33, 'rho': 2700, 'sy': 95e6},
    'concrete': {'E': 30e9, 'nu': 0.2, 'rho': 2400, 'sy': 30e6},
}

JAX-FEM (differentiable)

import jax_fem
mesh = jax_fem.gen_mesh.box_mesh(10, 10, 10, 1.0, 1.0, 1.0)
problem = jax_fem.LinearElasticity(mesh, E=200e9, nu=0.3)
sol = jax_fem.solver.solver(problem, ...)
# 매 sensitivity / topology opt 의 가능

매 결정 기준

상황 Tool
Open-source academic FEniCS / JAX-FEM
Industry structural ANSYS / Abaqus
Cheap PoC PyANSYS / FreeCAD
ML surrogate PINN / MeshGraphNet
Topology opt JAX-FEM (diff)
Mobile / real-time Surrogate model

기본값: 매 commercial = ANSYS/Abaqus + 매 open-source = FEniCS + 매 ML augmentation = MeshGraphNet for surrogate.

🔗 Graph

🤖 LLM 활용

언제: 매 engineering simulation. 매 design optimization. 언제 X: 매 simple analytical solution.

안티패턴

  • Skip mesh convergence: 매 unreliable.
  • Linear for nonlinear regime: 매 wrong.
  • Wrong element type: 매 locking.
  • No BC validation: 매 garbage.
  • Pure ML w/o physics: 매 OOD fail.

🧪 검증 / 중복

  • Verified (Zienkiewicz Finite Element Method, FEniCS docs).
  • 신뢰도 A.

🕓 Changelog

날짜 변경
2026-04-26 FEA auto
2026-05-08 Phase 1
2026-05-10 Manual cleanup — FEM steps + 매 FEniCS / PyANSYS / PINN / GNN / convergence code