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104  Energy methods of structural analysis

                  at the points of application of the complete system of loads are then




                                                                                     (4.28)




                  or, in matrix form










                  which may be written in shorthand matrix notation as
                                                -PI = [AI-w

                    Suppose now that an elastic body is subjected to a gradually applied force P1 at a
                  point  1 and then, while P1 remains in position, a force P2 is gradually applied at
                  another point 2. The total strain energy U of the body is given by




                  The third term on the right-hand side of Eq. (4.29) results from the additional work
                  done by P1 as it is displaced through a further distance a12P2 by the action of P2. If we
                  now remove the loads and apply P2 followed by P1  we have




                  By the principle of superposition the strain energy stored is independent of the order
                  in which the loads are applied. Hence
                                                  u, = u2
                  and it follows that

                                                  a12  = a21                         (4.31)
                  Thus in its simplest form the reciprocal theorem states that:
                    The deflection at a point 1 in a given direction due to a unit load at apoint 2 in a second
                    direction is equal to the deflection at the point 2 in the second direction due to a unit
                    load at the point 1 in the first direction.
                    In a similar manner, we  derive the relationship between moments and rotations,
                  thus:

                    The rotation at a point 1 due to a unit moment at a point 2 is equal to the rotation at
                    the point 2 produced by a unit moment at the point 1.
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