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1 COMBINATION RESISTANCE


          1.1  General concepts

             Combination resistance occurs when  in the cross-sections of
          the rod at least two internal power factors simultaneously operate
          (the exception is direct cross-ply, which is referred to simply rod
          resistance, as in practical calculations the influence of shear force
          is usually neglected).
                                              In      calculating      the
                                           combination    resistance   the
                                           principle  of  superposition  is
                                           used.  It  should  be  mentioned
                                           that  in  the  general  case  in  the
                                           cross-  sections  of  the  rod  load
                                           can  occur  six  internal  force
                                           factors  (fig. 1.1).  Longitudinal

                                           force    N      and    bending
                                                      x
                    Figure 1.1
                                           moments     M ,    M   cause
                                                         y      z
                                           normal  stresses  in  the  cross
          section.  Shear  forces  Q ,  Q ,  and  bending  moment M   cause
                                  y    z                          x
          tangent stress.
             All kinds of combination resistance can be divided into three
          groups:
                1. Combination resistance where at any section point there
             may  occur  only  normal  stresses   ,      ,     ,  acting
                                                   N  x  M  y  M  z
             lengthways of one straight line (linear stress state) and can be
             calculated by the algebraic summation
                                           .
                                   N     M     M
                                    x     y     z
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