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104               Chapter 6  Three-Dimensional Solid Analysis



                                                                            w
                                                (, , )    
                                               wx  y  z       NN N N   1  2  3  4     
                              where                  v  T      vv v v  
                                                               1
                                                                 2
                                                                      4
                                                                   3
                                                      T
                                                    w
                                                         ww w w  
                                                                  2
                                                               1
                                                                     3
                                                                       4
                              Thus, the element vector of nodal unknowns contains the total of
                              12 unknowns as,
                                                T  u v w u vw u v w u vw   1  1  1  2  2  2  3  3  3  4  4  4  
                                         The  element  vector  containing  the  six  strain  compo-
                              nents can be determined from,
                                                                
                                                               B 
                                                                   
                                                               
                                                      
                                                     (6 1)    (6 12) (12 1)
                                                 B
                              where  the  matrix  is  called  the  strain-displacement  matrix
                              which  relates  the  six  strain  components  with  the  12  nodal
                                                                            K
                              displacements.    The  element  stiffness  matrix     can  then  be
                              determined from,
                                                               T
                                                           V
                                                            B
                                                                 CB
                                                  K
                                                                 
                                                             
                                                   
                                                                     
                                                 (12 12)   (12 6)  (6 6) (6 12)
                              These  element  matrices  are  determined  for  all  elements  before
                              assembling them to become a large stiffness matrix of the system
                              equations.    Boundary  conditions  are  then  applied  and  the  system
                              equations  are  solved  for  all  nodal  displacement  solutions  u   ,v
                                                                                       ,
                                                                                          i
                                                                                      i
                               w .
                                i
                                         Once  all  nodal  solutions  ,u   ,v   w  are  obtained,  the
                                                                   i
                                                                          i
                                                                      i
                              element stresses are determined from,
                                                                 B 
                                                    
                                                                
                                                             C
                                                                     
                                                             
                                                                 
                                                    
                                                   (6 1)    (6 6) (6 12)  (12 1)
                                         The same process is applied for the hexahedral element
                              but  the  number  of  equations  is  larger.    For  example,  the  8-node
                              hexahedral  element  contains  24  equations  while  the  20-node
                              element consists of 60 equations.  Developing a computer program
                              is  thus  a  must  for  solving  a  problem.    We  will  use  the  ANSYS
                              software through its Workbench to analyze three-dimensional solid
                              problems in the following sections.
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