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330    Chapter 7  Conservation of Energy and an Introduction to Energy and Work


                     to your face and releasing it from rest, as shown in     25.   As you pedal a bike up a hill, predict
                     part (a) of the figure.                                 (a)   the sign of the work done by the gravitational

                                                                             force on you,
                        (a)                      (b)                        (b)  the sign of the work done by your foot on the bike

                                                                             pedal as it pushes the pedal down, and
                                                                            (c)   the sign of the work done by the pedal on your
                                                                             foot as the pedal moves downward.
                                                       L      L
                                                        0
                                                                          Hint : Remember that predictions are always supported
                                     ∆h                                   by reasoning and that coordinate systems are chosen
                                                     ∆L                   for convenience.

                                                                         26.   A 1.0-kg object is at rest when a force is exerted on
                                                                          the object. The positions at several times are shown in
                                                                          the figure.
                                                                                  t = 0.5 s
                                                                             t = 0 s   t = 1 s  t = 1.5 s  t = 2 s
                                                                                0.0   0.2   0.4   0.6    0.8
                  Note: Figure not drawn to scale.                                                           x (m)

                                                                             (a)   Use mathematical reasoning to express displace-


                        (a)   Predict what will happen to the relative height,   ∆h ,   ment as a function of time for the object by evalu-
                        to which the ball rises if the ball is pushed rather   ating the acceleration.
                        than released from rest in terms of the work done,     (b)  Calculate the numerical value of the force exerted

                        W on ball     , by the push.                         on the object.
                       A teacher tires of this demonstration and attaches     (c)   Express work done by the force on the object and
                     the bowling ball to an ideal spring with constant  k .   kinetic energy of the object as functions of time.
                     As shown in part (b) of the figure, the equilibrium
                     length of the spring hanging vertically when the       The external force is switched off and the object is
                                      L

                     ball is attached is   . 0   Lying on the floor with the   returned to the original initial position. At the instant
                     bowling ball suspended at rest above his chest       the force is switched on again a second object with


                     he pulls down slightly on the ball a distance   ∆L ,   a mass of 2.0 kg enters along a parallel path with an



                                                                                                              v
                     and releases it.                                     initial position   =x  0  and an initial speed of   = 1m/s.

                       (b)  Take the ball to be initially at rest above the teacher’s   Interactions between the two objects are negligible.
                                                   .

                                              L  +∆L  What are the         At    = 1t       s the external force is switched off.
                        chest with a spring length   0

                        forces exerted on the ball at this time?            (d)   Express the displacements of both objects as a

                       (c)   Using the conservation of energy, describe the   function of time.
                        motion of the ball after the teacher releases it.       (e)   Express the kinetic energy of the two-object system


                       (d)   Which demonstration is safer, do you think? Justify   as a function of time.

                        your answer in terms of the subsequent motion of     (f)   Explain why the kinetic energy of the two-object
                        the ball in each case, (a) and (c).                  system is constant for   > 1s.t
                                                                                                  Prep for the   AP ®  Exam
                        AP   Group Work
                     ®
                     Directions: The following problem is designed to be done as     and she draws the graph of force versus spring compres-
                 group work in class.                                 sion as shown in the following graph. Gwen argues that
                   As part of a lab experiment that uses a horizontal air track,   the energy added to the spring is the area under the force-

                 Allison pushes an air-track cart of mass  m up against a spring   displacement graph, and points out that the two shaded
                 to compress the spring with spring constant  k  by an amount   triangles have the same area. So a second compression by a

                    ∆x  from its equilibrium length. The air track has negligible   distance  d beyond a first compression by a distance  d  doubles

                 friction. When Allison lets go, the spring launches the cart.   the area and therefore doubles the energy. The energy is pro-
                       Allison’s lab partner Gwen predicts that because the   portional to the velocity squared. So, Gwen argues, the square
                 force increases linearly as the spring is compressed, the   of the velocity should be proportional to the compression.
                 square of the velocity when the spring is released should
                 increase in proportion to the compressed length. So the           F
                 velocity should increase in proportion to the square root
                 of the displacement. To support her claim she refers to the
                 kinematic equation                                                         kd          kd
                                                                                         d          d      x
                                       v 2  = v 2  + 2a ∆x
                                    f    i
                            Uncorrected proofs have been used in this sample. Copyright © Bedford, Freeman & Worth Publishers.
                            Distributed by Bedford, Freeman & Worth Publishers. For review purposes only. Not for redistribution.
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