Page 23 - Aircraft Stuctures for Engineering Student
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8  Basic elasticity

               Taking moments about an axis through the centre of the element parallel to the z
             axis
                                                         SX


                                      - (ry,.~6y)6x6z-=0  6Y
                                                          2

             which simplifies to




             Dividing through by SxSySz and taking the limit as 6x and Sy approach zero

                                             rxy = Tyx  I
             Similarly                       7x2 = 7,x                           (1.4)
                                             Tyz  = 7.y
               Now considering the equilibrium of the element in the x direction





                                            - ryxSxSz+ (., +-SZ 2 ) SxSy
                                                        r
                                            - rzXSxSy + XSxSySz = 0
             which gives




             Or, writing T~~ = T~~ and T,,  = r,,  from Eqs (1.4)





             Similarly
                                        80,  a7,,
                                                   %y
                                       -+-+-+z=o               J
                                        dz    ax    ay
               The equations of equilibrium must be satisfied at all interior points in a deformable
             body under a three-dimensional force system.






             Most  aircraft  structural  components  are fabricated  from thin  metal  sheet  so that
             stresses across the thickness of the sheet are usually negligible. Assuming, say, that
             the  z  axis is  in  the  direction  of  the  thickness  then  the  three-dimensional  case  of
             Section 1.3 reduces to a two-dimensional  case in which c,, r,,  and ryz are all zero.
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