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0593_C04*_fm  Page 97  Monday, May 6, 2002  2:06 PM





                       Kinematics of a Rigid Body                                                   97





                       4.9  Relative Velocity and Relative Acceleration of Two Points
                            on a Rigid Body
                       Consider a body B moving in a reference frame R as in Figure 4.9.1. Let P and Q be points
                       fixed in B. Consider the velocity and acceleration of P and Q and their relative velocity
                       and acceleration in reference frame R. Let O be a fixed point (the origin) of R. Let vectors
                       p and q locate P and Q relative to O and let vector r locate P relative to Q. Then, from
                       Figure 4.9.1, these vectors are related by the expression:

                                                            =
                                                               +
                                                           pq r                                 (4.9.1)
                       By differentiating we have:


                                         V =  V +   ddt      or      V −  V =  d dt=  V         (4.9.2)
                                        R  P  R  Q  R         R  P  R  Q  R     R  P Q
                                                                           r
                                                     r
                       Because P and Q are fixed in B, r is fixed in B. Hence, from Eq. (4.5.2), we have:
                                                         ddt= ωω  ×  r                          (4.9.3)
                                                        R      R  B
                                                          r
                       Then, by substituting into Eq. (4.9.2), we have:

                                             R  P Q  R  B      R  P  R  Q  R  Q
                                               V   = ωω  ×  r   or     V =  V + ωω  ×  r        (4.9.4)
                       By differentiating in Eq. (4.9.4), we obtain the following relations for accelerations:


                                                       R
                                                 R  P Q = αα B  × r+ ωω B ×( ωω B  × r)
                                                                    R
                                                              R
                                                   a                                            (4.9.5)
                       and
                                                     a + αα
                                                                      R
                                                                R
                                                R a = R Q  R  B  × r+ ωω B ×( ωω B × r)         (4.9.6)
                                                  P
                                                                                           B


                                                                         Q             P
                                                                              r


                                                                  q
                                                                             p
                       FIGURE 4.9.1
                       A body  B moving in a reference       R
                       frame R with points P and Q fixed        O
                       in B.
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