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234                                CHAPTER 7  Work and Energy


                  4. In each case, the force is opposite to the displacement  3. The kinetic energy of the golf ball is largest at the beginning
                    (whether pushing against the front or pulling on the rear, the  (and end, if we neglect air resistance) of the trajectory; at
                    force is rearward), and so negative work is done on the cart in  higher points, the force of gravity has slowed the ball down.
                    both cases.                                          The kinetic energy is smallest at thetop of the trajectory,
                  5. No.The tension provides a centripetal acceleration, which is per-  where there is only a horizontal contribution to the speed
                                                                                 2
                                                                                     2
                    pendicular to the (tangential) motion, and thus does no work.  (v   2v   v  ).  The kinetic energy is not zero while the
                                                                                     y
                                                                                 x
                                                                         ball is in the air (unless the ball was accidentally launched ver-
                  6. The work is positive in (b) and (c), where the angle between
                                                                         tically; in that case, the kinetic energy would be zero at the top
                    the force and displacement is less than 90 ; the work is nega-
                                                                         of the trajectory).
                    tive in (a), where the angle is greater than 90 . The work is
                    zero in (d), where the force is perpendicular to the displace-  4. No. For the work–energy theorem to apply, one must con-
                    ment. The work is largest when the force is most nearly paral-  sider the net external force on the sled. If traveling at con-
                    lel to the displacement; for force vectors (and displacement  stant velocity (zero acceleration), the total force must be zero
                    vectors) of equal magnitude, this occurs in (c).     (the horse’s pull does positive work and is canceled by the
                                                                         friction force, which does negative work), and so the total
                  7. (E) 4 and 5. To calculate the work done by a constant force, W
                                                                         work done on the sled is zero. Thus there is no change in
                      Fs cos  , you do not need to know the mass, acceleration, or
                                                                         kinetic energy.
                    speed. You do need to know the force, the displacement, and                1   2
                    the angle between the two.                         5. (E) 9. The kinetic energy, K   mv , is proportional to the
                                                                                               2
                                                                         square of the speed; thus increasing the speed by a factor of 3
                Checkup 7.2                                              increases the kinetic energy by a factor of 9.
                  1. The work done by a variable force is equal to the area under the  Checkup 7.4
                    F(x) vs. x curve. Assuming the two plots are drawn to the same
                    vertical scale, for a displacement from a to b, the upper plot  1. As in Example 8, the velocity at the bottom depends only on
                    clearly has a greater area between the F(x) curve and the x axis.  the height of release (the cars do not even have to have the
                                                                         same mass!); thus, the upper roller coaster will provide the
                  2. If we consider a plot such as Fig. 7.13 and imagine extending
                                                                         larger speed at the bottom, since  y is greater.
                    the curve to the left to x   b [where F(x)   kb], then we
                    see that positive work is done on the particle as it moves from  2. The gravitational potential energy U decreases as the piano is
                    x   b to x   0 [where the area between the F(x) curve and  brought to street level from the first house; U remains con-
                    the x axis is above the x axis]. Negative work is done on the  stant during the trip to the nearby house (assuming travel
                    particle as it moves from x   0 to x   b [where the area  over flat ground); then, the gravitational potential energy
                    between the F(x) curve and the x axis is below the origin].  increases back to its original value as the piano is brought up
                    Thus the net work is zero.                           to the second floor of the second house (assuming similar
                                                                         houses).
                  3. The work you must do on the spring is the opposite of what
                    the spring does on you, since the forces involved are an  3. No. At constant speed, K is constant; since U decreases as the
                    action–reaction pair. Thus the work you do is the negative of  truck moves down, E   K   U decreases also, and so is not
                                             1
                                                   2
                                                2
                    the result of Example 4, or W    k(b   a ).          conserved.
                                             2
                                                        2
                                                      1
                  4. (D) 3W.The work to stretch from equilibrium is  kx , so the first  4. Since both the girl and the boy change height by the same
                                                      2
                                   1
                                     2
                    stretch requires W  kd .The second stretch requires work  amount, they both reach the pool with the same speed (at any
                                   2
                          1  2 2d  1   2  1  2                           vertical height, they have the same speed, but the boy’s velocity
                     W    kx    `    k (2d)    kd    4W   W   3W.
                          2   d   2       2
                                                                         has a horizontal component, so his vertical velocity is slower
                Checkup 7.3                                              than that of the girl). Since the girl’s velocity is all vertical, a
                                                                         larger vertical velocity implies that she reaches the pool first.
                                          1
                                             2
                  1. Yes—the kinetic energy, K   mv , depends only on the
                                          2
                    square of the speed, and not on the direction of the velocity.  5. (A)  22.   As in Example 8, the speed at the bottom (starting
                                                                         from rest) is proportional to the square root of the initial
                    Thus if the two equal masses have the same speed, they have
                                                                         height. Thus, for twice the height, the speed of the first bicy-
                    the same kinetic energy.
                                                                         clist will be 22  times as large at the bottom.
                  2. Yes, the kinetic energies can be equal. Since the kinetic energy is
                    proportional to mass and proportional to the square of the speed
                        1
                           2
                    (K  mv ), if the car has twice the speed of the truck (a factor
                        2
                    of 4 contribution to the kinetic energy), then the kinetic energies
                    can be equal if the truck has 4 times the mass of the car.
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