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5.4 Combined bending and in-plane loading  137

           Substitution for MI from Eq. (i) into the expressions for bending moment, Eqs (5.7)
         and (5.8), yields

                                         [(m2/a2) + v(n2/h2)] .  m7rx   n7ry
                                                                   sin
                                        mn[(m2/a2) + (n2/b2)12   sin -        (iii)
                                                                a
                                         [v(m2/a2) + (n2/h2)] .  m7rx  .  n7ry
                                                                   sin
                  M,. = -                                   sin - -           (iv)
                                        mn[(m2/a2) + (n2/h2)12   a    h
         Maximum values occur at the centre of the plate. For a square plate a = h and the first
         five terms give
                                M,,,,,   = M,,,,,  = 0.0479qoa2

           Comparing Eqs (5.3) with Eqs (5.5) and (5.6) we  observe that
                                      12M,z        12M"Z
                                            ,  ay=-
                                 a,y = -
                                        t3           t3
         Again  the  maximum  values  of  these  stresses  occur  at  the  centre  of  the  plate  at
         z = ft/2 so that
                                        6MX           6M,
                                ax,rnax = - ay,rnax  = -
                                         t2
                                            >
                                                       t2
         For the square plate
                                                       a2
                                 ax,rnax = gypax = 0.287q0 -
                                                       t2
           The twisting moment and shear stress distributions follow in a similar manner.







         So far our discussion has been limited to small deflections of thin plates produced by
         different forms of transverse loading. In these cases we assumed that the middle or
         neutral plane of the plate remained unstressed. Additional in-plane tensile, compres-
         sive or shear loads will produce stresses in the middle plane, and these, if of sufficient
         magnitude, will affect the bending of the plate. Where the in-plane stresses are small
         compared with the critical buckling stresses it is sufficient to consider the two systems
         separately; the total stresses are then obtained by superposition. On the other hand, if
         the in-plane stresses are not small then their effect on the bending of the plate must be
         considered.
           The elevation  and plan  of  a  small element  SxSy of  the  middle  plane  of  a  thin
         deflected plate are shown in Fig. 5.12. Direct and shear forces per unit length pro-
         duced by the in-plane loads are given the notation Nx, Ny and Nxy and are assumed
         to be acting in positive senses in the directions shown. Since there are no resultant
         forces in the x or y  directions from the transverse loads (see Fig. 5.9) we need only
         include the in-plane loads shown in Fig.  5.12 when considering the equilibrium  of
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