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4




            Two-Dimensional Elasticity












            4.1  Introduction
            Many structures that are three-dimensional can be satisfactorily treated as two-dimen-
            sional problems (Figure 4.1). This chapter introduces you to the use of the finite element
            method for deformation and stress analyses of two-dimensional elasticity problems. First,
            the basic equations in plane elasticity theory are reviewed. Then several types of 2-D finite
            elements for plane elasticity analysis are presented. Applications of these elements are
            demonstrated and their accuracies and efficiencies are discussed. This presentation is
                                                                                          ®
            followed by an example illustrating analysis of a 2-D elasticity problem using ANSYS
            Workbench.






            4.2  Review of 2-D Elasticity Theory
            In general, the stresses and strains at any point in a structure consist of six independent
            components, that is (Figure 4.2),


                                          σ x ,  σ y ,  σ z ,  τ xy ,  τ yz ,
                                                           τ zx
            for stresses, and

                                          ε x ,  ε y ,  ε z ,  γ xy ,  γ yz ,
                                                          γ zx
            for strains.
              Under certain conditions, the state of stresses and strains can be simplified. A 3-D stress
            analysis can, therefore, be reduced to a 2-D analysis. There are two general types of models
            involved in this 2-D analysis: plane stress and plane strain.


            4.2.1  Plane Stress
            In the plane stress case, any stress component related to the z direction is zero, that is,

                                                   = 0   ( ε≠ 0)                        (4.1)
                                        z
                                       σ= τ yz  = τ zx     z



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