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9.5 Torsion of closed section beams  31 5

              whence
                                              TL



              The total angle of twist from end to end of the beam is 28, therefore
                                        28     T   /2a  2b\


              or





              as in Eq. (9.52).
                Substituting for 8 in either of  the expressions for the  axial displacement of  the
              corner 1 gives the warping wl  at 1. Thus

                                      ab  TL  fa  b\          T   a


              i.e.
                                         wl=-(----) T   b  a
                                              8abG  tb
              as before. It can be seen that the warping of the cross-section is produced by a com-
              bination of the displacements caused by twisting and the displacements due to the
              shear strains; these shear strains correspond to the shear stresses whose values are
              fixed by statics. The angle of twist must therefore be such as to ensure compatibility
              of displacement between the webs and covers.



              9.5.2  Condition for zero warping at a section


              The geometry of the cross-section of a closed section beam subjected to torsion may
              be such that no warping of the cross-section occurs. From Eq. (9.53) we see that this
              condition arises when



              or

                                                                                 (9.54)

              Differentiating Eq. (9.54) with respect to s gives
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