Page 357 - Dynamics of Mechanical Systems
P. 357

0593_C10_fm  Page 338  Monday, May 6, 2002  2:57 PM





                       338                                                 Dynamics of Mechanical Systems







                                                                     k




                                                             B
                                                                 m
                       FIGURE 10.9.2
                                                                         Y
                       A vertical mass–spring system.
                       and the block, with the sum of the potential energy of the spring and the kinetic energy
                       of the block being constant. (We will discuss potential energy in the next chapter.)
                        As another example of work–energy transfer, consider the mass–spring system arranged
                       vertically as in Figure 10.9.2. Suppose B  is held in a position where the spring is
                       unstretched. If B is then released from rest from this position, it will fall and stretch the
                       spring and eventually come to rest at an extreme downward position. Questions arising
                       then include how far does B fall and what is the spring force when B reaches this maximum
                       downward displacement? To answer these questions, consider that as B falls, the weight
                       (or gravity) force on B is in the direction of the movement of B, whereas the spring force
                       on B is opposite to the movement of B. Because B is at rest at both the beginning and the
                       end of the movement, there is no change in the kinetic energy of B. The net work on B is
                       then zero. That is,

                                                     W ==   mgd −( ) 2  kd 2                   (10.9.8)
                                                         0
                                                                  1
                       where d is the distance B moves downward. By solving for d we obtain:

                                                          d = 2 mg k                           (10.9.9)


                       The spring force in this extended position is, then,

                                                         F =  kd = 2 mg                       (10.9.10)

                        The result of Eq. (10.9.10) shows that a suddenly applied weight load on a spring creates
                       a force twice that of the weight. This means that if a weight is suddenly placed on a
                       machine or structure the force generated is twice that required to support the weight in
                       a static equilibrium configuration.






                       10.10 Skidding Vehicle Speeds: Accident Reconstruction Analysis

                       The work–energy principle is especially useful in determining speeds of accident vehi-
                       cles by using measurements of skid-mark data. Indeed, the work–energy principle
                       together with the conservation of momentum principles are the primary methods used
                       by accident reconstructionists when attempting to determine vehicle speeds at various
                       stages of an accident.
   352   353   354   355   356   357   358   359   360   361   362