% Element length L = nodes(n2) - nodes(n1);
% main_bar_assembly.m clear; clc; % ... define nodes, elements, E, A ... K_global = zeros(n_dof); for e = 1:ne n1 = elements(e,1); n2 = elements(e,2); L = nodes(n2) - nodes(n1); ke = bar2e(E, A, L); dof = [n1, n2]; K_global(dof, dof) = K_global(dof, dof) + ke; end % ... apply BCs, solve, post-process ... | Element Type | MATLAB Implementation Key Points | |---------------|----------------------------------| | 2D Quadrilateral (Q4) | Gauss quadrature, shape functions in natural coordinates | | Beam (2D Euler-Bernoulli) | 4 DOF per element (u1, theta1, u2, theta2) | | 3D Tetrahedron (TET4) | Volume coordinates, B matrix size 6x12 | | Heat Transfer (2D) | Same structure, but D becomes thermal conductivity matrix | 8. Conclusion MATLAB M-files provide a transparent, educational, and flexible environment for implementing Finite Element Analysis. The step-by-step approach—pre-processing, assembly, BC application, solving, and post-processing—remains consistent across problem types. While not as efficient as commercial FEA packages for large-scale problems, MATLAB FEA codes are invaluable for learning, prototyping, and research. matlab codes for finite element analysis m files
% Assembly into global matrix dof_list = [n1, n2]; K_global(dof_list, dof_list) = K_global(dof_list, dof_list) + ke; end % Element length L = nodes(n2) - nodes(n1);
% Geometry: nodes and elements nodes = [0; 0.5; 1.0]; % Nodal coordinates (m) elements = [1 2; 2 3]; % Element connectivity apply BCs, solve, post-process
% --- Apply Boundary Conditions --- % Penalty method (or elimination method) penalty = 1e12; K_global(fixed_dof, fixed_dof) = K_global(fixed_dof, fixed_dof) + penalty; F_global(fixed_dof) = penalty * 0; % zero displacement
for e = 1:size(elements, 1) n1 = elements(e, 1); n2 = elements(e, 2);
% Plane stress constitutive matrix D = (E/(1-nu^2)) * [1, nu, 0; nu, 1, 0; 0, 0, (1-nu)/2];