For complex loading (like a point load), you would wrap the solution in a for loop to sum the Fourier series (e.g., 5. Conclusion
% Composite Plate Bending Analysis (FSDT) clear; clc; % 1. Material Properties (e.g., Carbon/Epoxy) E1 = 175e9; % Pa E2 = 7e9; % Pa G12 = 3.5e9; % Pa nu12 = 0.25; nu21 = nu12 * E2 / E1; % 2. Plate Geometry and Mesh a = 1.0; % Length (m) b = 1.0; % Width (m) h = 0.01; % Total Thickness (m) q0 = -10000; % Applied Load (N/m^2) % 3. Layup Sequence (Angles in degrees) layup = [0, 90, 90, 0]; n_layers = length(layup); t_layer = h / n_layers; z = -h/2 : t_layer : h/2; % Z-coordinates of layer interfaces % 4. Initialize ABD Matrices A = zeros(3,3); B = zeros(3,3); D = zeros(3,3); % Reduced Stiffness Matrix (Q) for orthotropic ply Q_bar = zeros(3,3); Q11 = E1 / (1 - nu12*nu21); Q12 = nu12 * E2 / (1 - nu12*nu21); Q22 = E2 / (1 - nu12*nu21); Q66 = G12; Q = [Q11, Q12, 0; Q12, Q22, 0; 0, 0, Q66]; % 5. Build ABD Matrix for i = 1:n_layers theta = deg2rad(layup(i)); T = [cos(theta)^2, sin(theta)^2, 2*sin(theta)*cos(theta); sin(theta)^2, cos(theta)^2, -2*sin(theta)*cos(theta); -sin(theta)*cos(theta), sin(theta)*cos(theta), cos(theta)^2-sin(theta)^2]; Q_layer = inv(T) * Q * (T'); % Transformed stiffness A = A + Q_layer * (z(i+1) - z(i)); B = B + 0.5 * Q_layer * (z(i+1)^2 - z(i)^2); D = D + (1/3) * Q_layer * (z(i+1)^3 - z(i)^3); end % 6. Navier Solution (Simplified for m=1, n=1) m = 1; n = 1; alpha = m * pi / a; beta = n * pi / b; % Bending Stiffness Component (D11 for a simple case) % For a symmetric cross-ply, w_max calculation: D11 = D(1,1); D12 = D(1,2); D22 = D(2,2); D66 = D(3,3); w_center = q0 / (pi^4 * (D11*(m/a)^4 + 2*(D12 + 2*D66)*(m/a)^2*(n/b)^2 + D22*(n/b)^4)); fprintf('Max Central Deflection: %.6f mm\n', w_center * 1000); Use code with caution. 4. Interpreting Results
Laminated composite plates are staples in aerospace, automotive, and marine engineering due to their high strength-to-weight ratios. Unlike isotropic materials (like steel), composites are orthotropic; their properties depend on the orientation of the fibers. Analyzing their bending behavior requires accounting for coupling effects between stretching, twisting, and bending. 1. Theoretical Framework: FSDT Composite Plate Bending Analysis With Matlab Code
The constitutive relationship for a laminate is defined by the :
Relates in-plane strains to in-plane forces. For complex loading (like a point load), you
If your B matrix is non-zero, the plate will experience "warping" even under pure tension.
Relates curvatures to bending moments. 2. The Solution Strategy To solve for displacement ( Plate Geometry and Mesh a = 1
This article provides a comprehensive overview of the static analysis of laminated composite plates using First-Order Shear Deformation Theory (FSDT) and provides a functional MATLAB script to calculate deflections. Composite Plate Bending Analysis With MATLAB Code
MATLAB is an ideal tool for this analysis because it handles the matrix inversions and transformations of orthotropic properties seamlessly. This script serves as a foundation; for more complex geometries or boundary conditions, one would transition to the .