Page 7 - Vibrations 5
P. 7

Multi-degree of freedom systems



        A system with several components each with their own


        resonance is more representative of a real machine.








































        Consider the free vibrations of the two masses which have


        F 1 acting on the first and F                  2 acting on the other.


        These can be two components within a mechanical


        structure which are attached to each other.



            ̈ + ( +  )̇ −  ̇ + ( + ) −   = 
                                                      2 2
                                             1
                              1
                                       2
                                                                                              2 2
                                                                                                            1
                                                                                    1
                                                                      1
                                                                              2
               1 1
            ̈ −  ̇ + ( +  )̇ −   + ( + ) = 
                                                           2
                                                                                            3
                                                                    2 1
                                                                                    2
                                                     3
                                                                                                            2
                            2 1
                                           2
                                                                                                  2
               2 2
            1    0      ̈ 1      +  2      − 2      ̇ 1      + 2      − 2       1       1
                                     1
                                                                          1
         (            ) ( ) + (                           ) ( ) + (                          ) ( ) = ( )
            0      2    ̈ 2       − 2       +  3    ̇ 2       − 2      + 3      2       2
                                                  2
                                                                                      2
        These are now coupled equations as you would expect, as
        one mass moves the other will as well.
                                                            6
   2   3   4   5   6   7   8   9   10   11   12