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32                    Finite Element Modeling and Simulation with ANSYS Workbench



              That is,


                                                              
                                                              u i
                                                              
                                          E                   
                                                              v i
                                      σ =    −  l  −m  l  m                      (2.35)
                                                            
                                          L                   
                                                              u j
                                                              
                                                              v j
                                                              
            which is a general formula for 2-D bar elements.




            2.5  Examples with Bar Elements
            We now look at examples of using the bar element in the analysis of 1-D stress problems
            and plane truss problems.

                 EXAMPLE 2.1
                                         2A, E         A, E

                                         1               2
                                                    P               x
                                    1           2             3
                                          L             L



                 Problem
                 Find the stresses in the two-bar assembly which is loaded with force P, and constrained
                 at the two ends, as shown in the above figure.

                 Solution
                 Use two 1-D bar elements.
                  For element 1,


                                                     u 1  u 2
                                                    
                                                2 EA 1   − 1
                                             1 k =   −    
                                                 L    1  1  

                  For element 2,

                                                    u 2  u 3
                                                   
                                                EA 1    − 1
                                             2 k =   −   
                                                 L    1  1  

                  Imagine a frictionless pin at node 2, which connects the two elements. We can assem-
                 ble the global FE equation as follows:
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