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10.2 Fuselages  379

                be checked by calculating the resultant of the shear flow distribution parallel to the Cy
                axis. Thus
                  2[(98.8 + 66.0)145.8 + (86.3 + 53.51123.7 + (63.1 + 30.3)82.5 + (32.8 - 0)29.0]

                      x lop3 = 99.96 kN
                which agrees with the applied shear load of 100 kN. The analysis of a fuselage which is
                tapered along its length is carried out using the method described in Section 10.1 and
                illustrated in Example 10.2.


                10.2.3  Torsion


                A  fuselage  section is  basically a  single cell closed section beam.  The  shear flow
                distribution produced by a pure torque is therefore given by Eq. (9.49) and is
                                                     T
                                                q=-                              (10.18)
                                                    2A
                It is immaterial whether or not the section has been idealized since, in both cases, the
                booms are assumed not to carry shear stresses.
                  Equation (10.18) provides an alternative approach to that illustrated in Example 10.5
                for the solution of  shear loaded sections in which the position of the shear centre is
                known. In Fig. 10.11 the shear centre coincides with the centre of  symmetry so that
                the loading system may be replaced by  the shear load of  100 kN acting through the
                shear centre together with a pure torque equal to 100 x lo3 x  150 = 15 x  lo6 Nmm
                as shown in Fig.  1C.14. The shear flow distribution due to the shear load may  be
                found using the method of Example 10.5 but with the left-hand side of the moment
                equation (iii) equal to zero for moments about the centre of symmetry. Alternatively,
                use may be made of  the symmetry of the section and the fact that the shear flow is


                                                 100 kN
                                                   I





















                Fig.  10.14  Alternative solution of Example 10.5.
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