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not  depend  on  action  of  other  forces.  It  is  principle  of    forces
                  superposition(principle of independent action of forces).Then the total
                  acceleration is given by:

                                                                         n  
                                                                               a                             (3.8)
                                                     aa  1   a 2   ...  a n     i
                                                                            i 1
                          The law     F      m   a   i   , is fulfilled for each force and we can sub-
                                          i
                  stitute    
                           F
                      a      i  m
                       i
                                        1   n                              n            
                                       a     F                                    F   m  a 
                                                                                  i
                                                 i
                                         m   i 1                           i1                             (3.9)
                         The resultant force is the force that causes the same action as
                  all forces applied to an object together:
                                                         n 
                                                          F      F i
                                                           i 1                                                   (3.10)

                          So, instantaneous acceleration  is  the second derivative of  vector
                                                                                 2 
                  displacement    with    respect  to  time      a             d   r    2  .The  differential
                                                                                      dt
                  equation of motion is given by
                                                              d  2 
                                                                   r
                                                                 F   m
                                                                dt  2                                               (3.11)
                  and is called the  main equation of motion. In terms of components:

                                                                     d  2 x
                                                        F   m   a   m
                                                            x
                                                 x
                                                                     dt  2
                                                                    d  2 y
                                                       F   m   a   m
                                                 y          y           2
                                                                     dt
                                                                      2
                                                                    d   z
                                                        F   m  a   m
                                                 z
                                                            z
                                                                    dt  2                                          (3.12)
                               The  basic  equation is  called  so because  if  forces  that act  on  an
                  object and its mass are given it is possible to determine all characteristics

                  (parameters) of motion.
                                                                                                 
                             Note, that Newton's second law in the form  F                   m   a   is valid
                  only  for  objects  with  constant  mass.  In  general  case  the  concept  of

                  impulse is introduced:



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