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distorted during the action on the impulsive forces, but they return to their
               original shapes and the ball springs away from the plate. In this case the
               bodies are only temporary deformed and they regain their original shapes
               immediately  after  the  collision.  Bodies  which  return  to  their  original

               shapes after the collision are said to be elastic.
                            The perfectly elastic collision is an impact after which the shapes
                  of  the  bodies  are  completely  restored,  the  movements  of  bodies  are

                  independent and mechanical energy does not transform into other forms
                  of energy.




                                                                                      before

                                                                                    collision



                                                                                       after

                                                                                    collision






                                                   Figure 5.9

                     Let us consider the following closed and conservative system.

                     In  a  perfectly  elastic  collision  both  the  energy  and  the  impulse  are
                  conserved. If two bodies collide along the line connecting their centers
                  of mass (Fig. 5.9) we can write:


                                                 2           2         2          2
                                          m 1 v 10   m  2 v 20    m 1 v 1   m 2 v 2
                                                                                  ,                      (5.36)
                                             2          2          2         2

                                                   m 1 v   m 2 v 20    m 1 v   m 2 v  .                          (5.37)
                                                                       1
                                                                                2
                                                  10
                     From system of these equations  follows that
                                                                           
                                                        
                                                  2m   v     m    m   v
                                                  v   2  20      1     2   10   ,                            (5.38)
                                              1
                                                            m    m 2
                                                              1

                                                                       
                                               2m   v     m     m  v
                                               v   1  10      2      1   20   .                               (5.39)
                                           2
                                                         m    m  2
                                                           1
                            Consider particular case, when  m             m  and second body before
                                                                             2
                                                                      1
                  collision is in  the state of rest as shown in fig 5.10. Then, as follows
                                                                                       
                  from (5.38)    v    1    0 (first body stopped), but    v           v . It means that
                                                                                          01
                                                                                   2
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