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310                                CHAPTER 10  Systems of Particles


                                                      This is a direct consequence of the equality of the magnitudes of the action and reac-
                                                      tion forces that act on the shot and the gun during the firing. The force gives the
                                                      shot (of small mass) a large acceleration, and the reaction force gives the gun
                                                      (of large mass) a small acceleration.
                                                         In this calculation we neglected the mass and momentum of the gases released
                                                      in the explosion of the gunpowder.This extra momentum increases the recoil veloc-
                                                      ity somewhat.



                                                                     An automobile of mass 1500 kg traveling at 24 m/s crashes
                                                      EXAMPLE 3
                                                                     into a similar parked automobile.The two automobiles remain
                                                      joined together after the collision. What is the velocity of the wreck immediately
                                                      after the collision? Neglect friction against the road, since this force is insignifi-
                                                      cant compared with the large mutual forces that the automobiles exert on each
                                                      other.

                                                      SOLUTION: Under the assumptions of the problem, the only horizontal forces
                                                      are the mutual forces of one automobile on the other.Thus, momentum conservation
                                                      applies to the horizontal component of the momentum: the value of this compo-
                                                      nent must be the same before and after the collision. Before the collision, the
                                                      (horizontal) velocity of the moving automobile is v   24 m/s and that of the other
                                                                                             1
                                                      is v   0. With the x axis along the direction of motion (see Fig. 10.4), the total
                                                         2
                                                      momentum is therefore
                                                                          P   m v   m v   m v
                                                                           x    1 1   2 2    1 1
                                                      After the collision, both automobiles have the same velocity (see Fig. 10.4b). We
                                                      will designate the velocities of the automobiles after the collision by v  and v ,
                                                                                                                     2
                                                                                                               1
                                                      respectively. We can write v   v   v  (the automobiles have a common v , since
                                                                            1
                                                                                2
                                                      they remain joined), so the total momentum is
                                                                      P    m v    m v    (m   m )v
                                                                            1 1
                                                                                   2 2
                                                                                                2
                                                                                           1
                                                                       x
                  PROBLEM-SOLVING TECHNIQUES                     CONSERVATION OF MOMENTUM



                  Note that the solution of these examples involves three steps  momentum are conserved separately. Thus, before writing the
                  similar to those we used in examples of energy conservation:  expressions for the momentum, you need to select coordinate
                                                                    axes and decide which components of the momentum you
                  1 First write an expression for the total momentum P before
                                                                    want to examine. If the motion is one-dimensional, place one
                     the firing of the gun or the collision of the automobiles.
                                                                    axis along the direction of motion, such as the x axis in the
                  2 Then write an expression for the total momentum P
                                                                    above examples. It then suffices to examine the x component
                     after the firing or the collision.
                                                                    of the momentum.However,sometimes it is necessary to exam-
                  3 And then use momentum conservation to equate these  ine two components of the momentum (or, rarely, three); then
                     expressions.                                   two (or three) equations result.When writing the components
                                                                    of the momentum, pay attention to the signs; the component
                     However,in contrast to energy conservation,you must keep
                                                                    is positive if the motion is along the direction of the axis, neg-
                  in mind that momentum conservation applies to the compo-
                                                                    ative if the motion is opposite to the direction of the axis.
                  nents of the momentum—the x, y, and z components of the
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