Buckling Analysis of a Square Plate
Let us consider a square plate with a side a and thickness h (see figure).
The thickness of plate h is much smaller than the length of its side a.
The plate is uniformly compressed in a transversal direction.
Consider the case when the loaded edges of plate are simply-supported; non-loaded edges are clamped.
Let us use the following data: plate side length a = 500 mm, thickness of plate h = 3 mm , applied distributed force P = 1 Pa.
Material characteristics assume default values: Young's modulus E = 2.1E+011 Pа, Poisson's ratio ν = 0.28.
The finite element model with applied loads and restraints |
Analytical solution for this problem is given by:
σcritical = K π2 D / a2 h ,
where E – Young’s modulus, D = E h3 / 12 (1-ν2) – cylindrical stiffness of plate, K – coefficient whose value depends on the type of the supports of the plate edges (in this case K = 7.69).
Thus, σcritical = K π2 D / a2 h = 0.5188E+008 Pa.
After carrying out calculation with the help of AutoFEM, the following results are obtained:
Table 1. Parameters of finite element mesh
Finite Element Type |
Number of nodes |
Number of finite elements |
quadratic tetrahedron |
5202 |
15000 |
Table 2. Result "Critical load"*
Numerical solution |
Analytical solution |
Error δ = 100%*|σ*critical-σcritical| / |σcritical| |
0.5277E+008 |
0.5188E+008 |
1.72 |
Conclusions:
The relative error of the numerical solution compared with the analytical solution not exceed 1.72% for quadratic finite elements.
*The results of numerical tests depend on the finite element mesh and may differ slightly from those given in the table.
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