Abstract

A weighted integration route with robust one-point integration (hourglass-controlled) is proposed as efficient, time saving alternative to Gauss quadrature for stiffness matrix of bilinear quadrilaterals. One-point rule relies on sampling at the center of the element to linearize the geometric transformation and average the material property over it. This enables, for a given element, explicit integration of stiffness matrix yielding a first approximation. For a second and better approximation, this procedure is applied independently to each of the four sub-squares of the mapped 2-square of the element and the matrices are assembled. A weighted addition of the two approximations produces a stiffness matrix as accurate as from 3-point Gauss-quadrature (G9P). Whereas, due to explicit integrations, obtaining stiffness matrix in this way demands less than a third of the time needed for 2-point Gauss-quadrature (G4P). On both counts (speed and accuracy) this approach outperforms Gauss-quadrature. Sampling (material and geometry) at 5-points makes this element superior to G4P for Functionally Graded Material (FGM) applications. Bench mark examples by this approach are validated with Gauss quadrature and analytical solutions.

Highlights

  • Even to this day developing stiffness matrices for plane quadrilateral elements keeps enticing researchers (Jeyakarthikeyan et al, 2017)

  • Following a procedure similar to that for triangles the stiffness matrix is conveniently generated in terms of numerical universal matrices for the matching parallelogram

  • Despite the apparently elaborate exercise to find the stiffness matrix, the entire process still requires a third of the time needed for G4P

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Summary

Introduction

Even to this day developing stiffness matrices for plane quadrilateral elements keeps enticing researchers (Jeyakarthikeyan et al, 2017). For a second approximation a cluster of four stable one-point quadrilaterals are carved out of the given quadrilateral and assembled into an (18×18) matrix (in principle) and reduced to (8×8) super element by enforcing the bilinear nature of the displacement description over the element (This procedure is not a static condensation, a procedure associated usually with standard super element formation, but is akin to obtaining transition elements from higher order elements: Zienkiewicz et al (2005; Jeyachandrabose and Kirkhope, 1984)) These two approximations (with h-squared error) are weighted and extrapolated to give a vastly improved stiffness matrix that is as good as employing G9P. Following a procedure similar to that for triangles the stiffness matrix is conveniently generated in terms of numerical universal matrices for the matching parallelogram (as the mid-point rule for a quadrilateral renders the geometric transformation linear). Actual calculations would follow the procedure outlined here to optimize computing effort

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