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326  Open and closed, thin-wailed beams
























                                          172.5
                  Fig. 9.43  Shear flow distribution in beam of Example 9.9 (all shear flows in Wmm).


                                 1.5mrn    1        2 rnm







                                                                 I
                                           2                     4
                                            I       600 mm      -1

                  Fig. 9.44  Wing section of Example 9.10.

                    It may be assumed, in a simplified approach, that the torsional rigidity GJ of the
                  complete section is the sum of the torsional rigidities of the open and closed portions.
                  For the closed portion the torsional rigidity is, from Eq. (9.52)
                                             4A2G  4 x 200002 x 25000
                                     (GJ)cl  =     =  (900 + 300)/1.5
                  which gives
                                          (GJ),, = 5000 x lo7 Nmm2
                  The torsional rigidity of the open portion is found using Eq. (9.59), thus

                                                   st3  25000 x 900 x Z3
                                     (GJ),,  = G   - =
                                                   3           3
                  i.e.

                                           (GJ),, = 6 x  107Nmm2
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