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332  Open and closed, thin-walled beams





                                                                      - 1


                       600
                                        4                      I
                      600                v
                                                  6tt- I
                                                                                 -
                                                                            I200 mm
                                                                      I I40
                               C.'                                                   X
                                                                                 -
                      640 640                                                    Y
                          0          .) 144
                                      3
                         850
                             640  9-8

                 Fig. 9.49  Idealized fuselage section of Example 9.12.
                   The  section  has  Cy as  an  axis  of  symmetry  and  resists  a  bending  moment
                 M, = 100 kN m. Equation (9.6) therefore reduces to




                 The origin of axes Cxy coincides with the position of the centroid of the direct stress
                 carrying area which, in this case, is the centroid of  the boom areas. Thus, taking
                 moments of area about boom 9
                    (6 x 640 + 6 x 600 f2 x 620 + 2 x 850)J = 640 x  1200 + 2 x 600 x  1140
                                                          +2 x 600 x 960+2 x 600 x 768
                                                          +2x620~565+2~640~336

                                                           +2 x 640 x  144+2 x 850 x 38
                 which gives
                                                J  = 540mm

                  The solution is now completed in Table 9.1.
                    From column @
                                            I,,  = 1854 x  106mm4
                  and column 0 is completed using Eq. (i).



                  9.9.2  Shear of open section beams
                 -III-lll*-,-,-*---X.-~~-~-~~"~-"--~--~I-1II.L.-I*~X
                  The derivation of Eq. (9.34) for the shear flow distribution in the cross-section of an
                  open section beam is based on the equilibrium equation (9.22). The thickness r in this
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