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9.9  Effect of idealization  331
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            9.9  Efl  'ect of idealization on the analysis of open
                 an  d closed section beams
         The addition of direct stress carrying booms to open and closed section beams will
         clearly  modify  the  analyses  presented  in  the  earlier  part  of  this  chapter.  Before
         considering individual cases we shall discuss the implications  of structural idealiza-
         tion.  Generally,  in  any  idealization,  different  loading  conditions  require  different
         idealizations of  the  same  structure.  In  Example  9.11, the  loading  is  applied  in  a
         vertical plane.  If,  however, the loading has been  applied in  a horizontal  plane the
         assumed  stress distribution  in  the panels  of the section would  have  been different,
         resulting in different values of boom area.
           Suppose that  an open  or closed  section beam  is  subjected  to given  bending  or
         shear  loads  and  that  the  required  idealization  has  been  completed.  The  analysis
         of  such  sections  usually  involves  the  determination  of  the  neutral  axis  position
         and  the  calculation  of  sectional  properties.  The  position  of  the  neutral  axis  is
         derived  from  the  condition  that  the  resultant  load  on  the  beam  cross-section  is
         zero,  i.e.


                                  a, dA  = 0  (see Section 9.1)


         The area A in this expression is clearly the direct stress carrying area. It follows that
         the centroid of the cross-section is the centroid of the direct stress carrying area of the
         section, depending on the degree and method  of idealization. The sectional proper-
         ties, Zy,y etc., must also refer to the direct stress carrying area.



         9.9.1  Bending of open and closed section beams


         The analysis  presented  in  Section 9.1  applies  and  the  direct  stress  distribution  is
         given by any of Eqs (9.6), (9.7) or (9.9), depending on the beam section being inves-
         tigated. In these equations the coordinates (x,y) of points  in  the cross-section  are
         referred to axes having their origin at the centroid of the direct stress carrying area.
         Furthermore,  the  section  properties  I,,,  IFF and  Zyy  are calculated  for  the  direct
         stress carrying area only.
           In the case where the beam cross-section has been completely idealized into direct
         stress carrying  booms  and shear  stress  only  carrying panels,  the  direct  stress dis-
         tribution  consists  of a  series of direct  stresses concentrated  at the centroids of  the
         booms.


         Example 9.12
         The fuselage section shown in Fig. 9.49 is subjected to a bending moment of 100 kN m
         applied in the vertical plane of symmetry. If the section has been completely idealized
         into  a combination  of  direct  stress carrying booms  and shear stress only carrying
         panels, determine the direct stress in each boom.
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