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28  •   Using ansys for finite element analysis
                1.5.2  work or energy Methods


                To  develop  the  stiffness  matrix  and  equations  for  two-  and  three-
                dimensional elements, it is much easier to apply a work or energy method.
                These are based on variational calculus. The variational method is appli-
                cable to problems that can be stated by certain integral expressions such
                as the expression for potential energy. The principle of virtual work (using
                virtual displacement),  the principle  of minimum  potential  energy, and
                Castigliano’s theorem are methods frequently used for the purpose of der-
                ivation of element equations. The principle of virtual work is applicable
                for any material behavior, whereas the principle of minimum potential
                energy and Castigliano’s theorem are applicable only to elastic materials.
                    For the purpose of extending, FEM outside the structural stress anal-
                ysis field, a functional (a scalar function of other functions) analogous to
                the one to be used with the principle of minimum potential energy is quite
                useful in deriving the element stiffness matrix and equations.


                1.5.3  Methods of weighted residuals

                Weighted residual methods are particularly suited to problems for which
                differential  equations  are  known,  but  no  variational  statement  or  func-
                tional is available. For stress analysis and some other problem areas, the
                variational method and the most popular weighted residual method (the
                Galerkin method) yield identical finite element formulations.



                1.6   derivation of sPring element
                      eqUations Using direCt method


                To understand the FE formulation, we start with the concept “Everything
                important is simple.” Figure shows a spring element

                              1           k              2
                                                                       x ˆ
                       ˆ
                       ƒ ,d ˆ 1x                        ƒ ,d ˆ 2x
                                                        ˆ
                        1x
                                                         2x
                                           L
                   Two nodes:                            Node 1, node 2
                                                            ˆ
                   Local nodal displacements:            d ˆ 1x    ,d (inch, m, mm)
                                                             2x
                                                            ˆ
                   Local nodal forces:                   ƒ ˆ 1x   2x
                                                           ,f (lb, newton)
                   Spring constant (stiffness)           K (lb/in, N/m, N/mm)
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