Page 204 - Dynamics of Mechanical Systems
P. 204

0593_C06_fm  Page 185  Monday, May 6, 2002  2:28 PM





                       Forces and Force Systems                                                    185


                       the particle. However, the inertia force is directed opposite to the acceleration. Thus, if P
                       is a particle with mass m and with acceleration a in an inertial reference frame R, then the
                                   *
                       inertia force F  exerted on P is:
                                                            *
                                                          F =−m  a                              (6.9.1)

                        An inertial reference frame is defined as a reference frame in which Newton’s laws of
                       motion are valid. From elementary physics, we recall that from Newton’s laws we have
                       the expression:

                                                           F = m a                              (6.9.2)

                       where F represents the resultant of all applied forces on a particle P having mass m and
                       acceleration a. By comparing Eqs. (6.9.1) and (6.9.2), we have:

                                                            +
                                                               *
                                                          FF = 0                                (6.9.3)
                        Equation (6.9.3) is often referred to as  d’Alembert’s principle. That is, the sum of the
                       applied and inertia forces on a particle is zero. Equation (6.9.3) thus also presents an
                       algorithm or procedure for the analysis of dynamic systems as though they were static
                       systems.
                        For rigid bodies, considered as sets of particles, the inertia force system is somewhat
                       more involved than for that of a single particle due to the large number of particles making
                       up a rigid body; however, we can accommodate the resulting large number of inertia
                       forces by using equivalent force systems, as discussed in Section 6.5. To do this, consider
                       the representation of a rigid body as a set of particles as depicted in Figure 6.9.1. As B
                       moves in an inertial frame R, the particles of B will be accelerated and thus experience
                       inertia forces; hence, the inertia force system exerted on B will be made up of the inertia
                       forces on the particles of B. The inertia force exerted on a typical particle P  of B is:
                                                                                          i

                                                          F =− m a                              (6.9.4)
                                                           *
                                                           i     i i
                       where m  is the mass of P  and A  is the acceleration of P  in R.
                                             i
                                                    i
                                                                         i
                              i
                        Using the procedures of Section 6.5, we can replace this system of many forces by a
                       single force F  passing through an arbitrary point, together with a couple having a torque
                                  *
                                                                                            B
                                                                          P  (m  )
                                                                           2   2
                                                                              r
                                                                 P  (m  )      i
                                                                  1  1
                                                                                     P  (m  )
                                                                                      i  i
                                                                           P  (m   )
                                                                            N   N
                       FIGURE 6.9.1
                       Representation of a rigid body as a  R
                       set of particles.
   199   200   201   202   203   204   205   206   207   208   209