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Free-Body Diagrams to Three-Dimensional Force Systems
              The first step in solving three-dimensional equilibrium problems,
         as in the case  of  two-dimensions, is to draw a  free-body diagram.
         Before we can do  this, however, it  is first necessary to  discuss the
         types of reactions that can occur at the supports.
              Support Reactions.  The reactive forces and  couple moments
         acting  at  various  types  of  supports  and  connections, when  the
         members are viewed in three dimensions, are listed in Table 1–2. It is
         important to recognize the symbols used to represent each  of these
         supports and to understand  clearly  how the  forces and  couple
         moments are developed. As in the two-dimensional case:
              • A force is developed by a support that restricts the translation
         of its attached member;
              • A couple moment is developed when rotation of the attached
         member is prevented.
              For example, in  Table 1–2, item (4), the  ball-and-socket joint
         prevents any translation of the connecting member; therefore, a force
         must act on the  member at the point of connection.  This force has
         three  components having unknown magnitudes, Fx, Fy, Fz. Provided
         these components are known, one can obtain the magnitude of force,
                 2
          F =  F +  F +  F ,  and the  force’s orientation  defined by its
                      2
                          2
                          z
                     y
                x
         coordinate direction angles  α,  β,  γ,  Eqs. 1-6.  Since the connecting
         member is allowed to rotate freely about any axis, no couple moment
         is resisted by a ball-and-socket joint. It should be noted that the single
         bearing supports in items (5) and (7), the single pin (8), and the single
         hinge  (9)  are  shown  to  resist  both  force  and  couple-moment
         components. If, however, these supports are used in conjunction with
         other bearings, pins, or hinges to hold a rigid body in equilibrium and
         the supports are properly aligned when connected to the body, then
         the force reactions at these supports alone are adequate for supporting
         the body. In other words, the couple moments become redundant and
         are not shown on the free-body diagram. The reason for this should
         become clear after studying the examples which follow.





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