Chapter 9: Q1CP (page 356)
A barbell spins around a pivot at its center (Figure 9.16). The barbell consists of two small balls, each with massat the ends of a very low mass rod whose length is. The barbell spins with angular speed.Calculate.
Chapter 9: Q1CP (page 356)
A barbell spins around a pivot at its center (Figure 9.16). The barbell consists of two small balls, each with massat the ends of a very low mass rod whose length is. The barbell spins with angular speed.Calculate.
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Get started for freeIt is sometimes claimed that friction forces always slow an object down, but this is not true. If you place a box of mass Mon a moving horizontal conveyor belt, the friction force of the belt acting on the bottom of the box speeds up the box. At first there is some slipping, until the speed of the box catches up to the speed vof the belt. The coefficient of friction between box and belt is. (a) What is the distance d(relative to the floor) that the box moves before reaching the final speed v? Use energy arguments, and explain your reasoning carefully. (b) How much time does it take for the box to reach its final speed? (c) The belt and box of course get hot. Is the effective distance through which the friction force acts on the box greater than or less than d? Give as quantitative an argument as possible. You can assume that the process is quick enough that you can neglect transfer of energyQ due to a temperature difference between the belt and the box. Do not attempt to use the results of the friction analysis in this chapter; rather, apply the methods of that analysis to this different situation. (d) Explain the result of part (c) qualitatively from a microscopic point of view, including physics diagrams.E
Three uniform-density spheres are positioned as follows:
What is the location of the center of mass of this three-sphere system?
A runner whose mass is accelerates from a stop to a speed of in . (A good sprinter can run in about , with an average speed of .) (a) What is the average horizontal component of the force that the ground exerts on the runner’s shoes? (b) How much displacement is there of the force that acts on the sole of the runner’s shoes, assuming that there is no slipping? Therefore, how much work is done on the extended system (the runner) by the force you calculated in the previous exercise? How much work is done on the point particle system by this force? (c) The kinetic energy of the runner increases—what kind of energy decreases? By how much?
Consider the acceleration of a car on dry pavement, if there is no slipping. The axle moves at speed v, and the outside of the tire moves at a speed relative to the axle. The instantaneous velocity of the bottom of the tire is zero. How much work is done by the force exerted on the tire by the road? What is the source of the energy that increases the car’s translational kinetic energy?
Consider the acceleration of a car on dry pavement, if there is no slipping. The axle moves at speed v, and the outside of the tire moves at a speed relative to the axle. The instantaneous velocity of the bottom of the tire is zero. How much work is done by the force exerted on the tire by the road? What is the source of the energy that increases the car’s translational kinetic energy?
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