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Figure 2.5

                 Let’s  define  the  virtual  work  of  external  and  internal
          forces on the movement of a single state, caused by the action of
          freight condition.
                 The work of external forces

                                 A     P .                        (2.10)
                                   зов
                 The work of internal forces (fig. 2.5)
                                                  M dx
                            вн 
                           A     M  zd , де d    z  ,
                                 l                 EJ  z
          that is
                                      M  zM dx
                                вн 
                               A          z   .                     (2.11)
                                    l   EJ  z
                 Equating  the  right  sides  of  (2.10)  and  (2.11)  we  obtain
          Mora’s formula (Mora’s integral)
                                    M  zM dx
                                       z  .                      (2.12)
                                   l   EJ z
                 Here  M  - expression of the bending moment that occurs
                         z
          in a single state  M  - an expression of the bending moment in the
                            z
          load condition.
                 If you need to determine the angular displacement at the
          point A, then in the formation of a single state instead of a single
          force  P  a single time  M  1must be applied.
                 In  the  case  of  a  spatial  problem,  following  the  formula
          (2.2), we obtain
                  N  xN dx   M  xM dx     M  zM dx    M  yM dx
                    x         x         z          y  .    (2.13)
                 l  EF      l   GJ k    l   EJ z     l   EJ y


          2.5  Calculation of Mora’s integral
           by Vereshchagin’s method

                 Each  of  the  integrals  which  is  included  in  the  formula
          (2.13) can be presented as


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