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9.1 Bending of open and closed section beams  277

               and displacements, investigate the effect of choice of section on the positive directions
               of these parameters and discuss the determination of the components of a bending
               moment applied in any longitudinal plane.



               9.1 .I Sign conventions and notation
               "-                 e---                        I-IY.II*IIII-"-PICI.-
               Forces, moments and displacements are referred to an arbitrary system of axes Oxy~,
               of which Oz is parallel to the longitudinal axis of the beam and Oxy are axes in the
               plane  of  the cross-section. We  assign the symbols M, S, P, T and  w  to bending
               moment, shear force, axial or direct load, torque and distributed load intensity respec-
               tively, with suffixes where appropriate to indicate sense or direction. Thus, M, is a
               bending moment about the x  axis, S, is a shear force in the x direction and so on.
               Figure 9.1 shows positive directions and senses for the above loads and moments
               applied externally to a beam and also the positive directions of the components of
               displacement u, w and w  of any point in the beam cross-section parallel to the x, y
               and z axes respectively. A further condition defining the signs of the bending moments
               M, and My is that they are positive when they induce tension in the positive xy quad-
               rant of the beam cross-section.
























               Fig. 9.1  Notation and sign convention for forces, moments and displacements.

                If  we  refer internal forces and moments to that face of  a section which is seen
              when viewed in the direction z0 then, as shown in Fig. 9.2, positive internal forces
              and moments are in the same direction and  sense as the externally applied loads
              whereas on the opposite face they form an opposing system. The former system,
              which we shall use, has the advantage that direct and shear loads are always positive
              in the positive directions of the appropriate axes whether they are internal loads or
              not.  It  must  be  realized,  though,  that  internal  stress  resultants  then  become
              equivalent to  externally applied forces and  moments and  are  not  in  equilibrium
              with them.
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