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396  Stress analysis of aircraft components













                   Fig. 10.30  Shear flows giving G(dB/dz)  = I  for the separated cells of a two-cell wing section.


                   that each cell acts independently and that cell I is subjected to a constant shear flow qI
                   such that G(dB/dz) for cell I is equal to unity. From Eqs (9.49) and (9.52)




                   where


                                                  s  -  ds/t
                                                  1-11
                   Hence
                                                       24
                                                   41  = -
                                                        61
                   Similarly, for G(dB/dz) to be unity for cell I1




                   We now have the situation shown in Fig. 10.30 where the two cells are separate and




                   Imagine now that the two cells are rejoined with the interior web as a common part of
                   both cells. The action of qII is to reduce the rate of twist in cell I by applying, in effect,
                   a clockwise torque to cell I opposing the anticlockwise torque corresponding to qI.
                   Thus,  G(de/dz)I  is  not  now  equal  to  G(dB/dz)II so  that  the  assumption  of  an
                   undistorted cross-section is invalidated and the shear flows qr and qII are therefore
                   not the true shear flows.
                     To correct this situation we  again suppose that the cells are separated and apply
                   constant  shear flows qf  and  qfI around  cells  I  and  I1  respectively to  counteract
                   the effect of  qII (shown dotted)  on cell  I  and qI on cell 11.  The total  shear flows
                   now  acting on each cell are  shown in Fig.  10.31. Note  that  the effect of  a shear
                   flow acting on one wall  of  a cell, e.g.  qII applied to  the internal web  and  acting
                   on cell I, is counteracted by a constant shear flow applied around the complete cell.
                   Thus
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