Three-dimensional finite element analysis in cylindrical coordinates for nonlinear solid mechanics problems

Abstract A formulation for three-dimensional nonlinear finite element analysis in cylindrical coordinates in presented. The elements are isoparametric with the same interpolation functions used to represent the geometry and the physical displacement components. The elements can be used for general three-dimensional analysis, but they are most effective for cases when the geometry and the response are best described in cylindrical coordinates. In contrast to formulations in Cartesian coordinates, the foregoing formulation allows the exact representation of a circular shape. For structures with circular geometries, the improved accuracy of the elements can provide better finite element predictions and reduce the number of elements needed in the circumferential direction. The reduction in the number of elements can result in a significant recuction in computer resources needed for large three-dimensional analyses, particularly in the presence of nonlinearities. Whereas the elements may, for some problems, be less efficient than semianalytic elements, the generality of the interpolation provides greater flexibility in modeling different shapes and responses. The mathematical formulation of the three-dimensional finite element equations in cylindrical coordinates is first described for finite strain and deformation. The advantages and additional complexities associated with the cylindrical coordinate formulation are discussed, and the implementation into finite element codes is described. Numerical studies are then presented for two static nonlinear three-dimensional problems: a pneumatic tire in contact with a rigid pavement and the skew bending of a stiffened annular plate. The finite element predictions of the cylindrical coordinate formulation are compared to experimental data and to the predictions from a commercial code using isoparametric finite elements developed in Cartesian coordinates.

[1]  J. Barlow,et al.  Optimal stress locations in finite element models , 1976 .

[2]  Z.-S. Tian,et al.  A study of stress concentrations in solids with circular holes by three-dimensional special hybrid stress finite elements , 1990 .

[3]  H. D. Hibbit Some follower forces and load stiffness , 1979 .

[4]  C. Truesdell,et al.  The Classical Field Theories , 1960 .

[5]  Ahmed K. Noor,et al.  Computational strategies for tire modeling and analysis , 1996 .

[6]  S. K. Clark,et al.  MECHANICS OF PNEUMATIC TIRES , 1971 .

[7]  K. T. Danielson,et al.  Finite Elements Developed in Cylindrical Coordinates for Three‐Dimensional Tire Analysis , 1997 .

[8]  J. S. Chen,et al.  Consistent finite element procedures for nonlinear rubber elasticity with a higher order strain energy function , 1994 .

[9]  J. A. Stricklin,et al.  Rigid-body displacements of curved elements in the analysis of shells by the matrix- displacement method. , 1967 .

[10]  M. G. Pottinger,et al.  The Three‐Dimensional Contact Patch Stress Field of Solid and Pneumatic Tires , 1992 .

[11]  Y. Fung Foundations of solid mechanics , 1965 .

[12]  J. Volakis,et al.  A collection of edge-based elements , 1992 .

[13]  L. E. Malvern Introduction to the mechanics of a continuous medium , 1969 .

[14]  R. Cook,et al.  Concepts and Applications of Finite Element Analysis , 1974 .

[15]  Ahmed K. Noor,et al.  Exploiting symmetries in the modeling and analysis of tires , 1987 .

[16]  John S. Campbell,et al.  Local and global smoothing of discontinuous finite element functions using a least squares method , 1974 .

[17]  J. Barlow More on optimal stress points—reduced integration, element distortions and error estimation , 1989 .

[18]  Duc T. Nguyen,et al.  Computational Mechanics Analysis Tools for Parallel-Vector Supercomputers , 1993 .

[19]  Klaus-Jürgen Bathe,et al.  Some recent advances for practical finite element analysis , 1993 .

[20]  A. Elwi,et al.  Large displacement axisymmetric element for nonaxisymmetric deformation , 1993 .

[21]  G. Cantin,et al.  Rigid body motions in curved finite elements , 1970 .

[22]  A nonlinear axisymmetric finite element for modelling nonaxisymmetric behaviour , 1993 .

[23]  J. Z. Zhu,et al.  The superconvergent patch recovery and a posteriori error estimates. Part 1: The recovery technique , 1992 .

[24]  J. C. Simo,et al.  Penalty function formulations for incompressible nonlinear elastostatics , 1982 .

[25]  Thomas J. R. Hughes,et al.  Solution algorithms for nonlinear transient heat conduction analysis employing element-by-element iterative strategies , 1985 .

[26]  K. Danielson,et al.  Fourier continuum finite elements for large deformation problems , 1993 .

[27]  H. Rothert,et al.  On the Three‐Dimensional Computation of Steel‐Belted Tires , 1986 .

[28]  K. Satyamurthy,et al.  An Efficient Approach for the Three‐Dimensional Finite Element Analysis of Tires , 1988 .

[29]  G.R. Buchanan,et al.  Vibration of infinite piezoelectric cylinders with anisotropic properties using cylindrical finite elements , 1991, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[30]  Body-oriented coordinates applied to the finite-element method , 1988 .

[31]  J. A. Stricklin,et al.  Implicit rigid body motion in curved finite elements , 1971 .

[32]  D. R. Strome,et al.  Direct stiffness method analysis of shells of revolution utilizing curved elements. , 1966 .

[33]  Ray W. Clough,et al.  Explicit addition of rigid-body motions in curved finite elements. , 1973 .

[34]  M. J. Trinko Ply and Rubber Stresses and Contact Forces for a Loaded Radial Tire , 1983 .

[35]  H. Saunders,et al.  Finite element procedures in engineering analysis , 1982 .