chapter_6

# chapter_6 - A small buck from the massive bull transfers a...

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160 6 CHAPTER OUTLINE 6.1 Momentum and Impulse 6.2 Conservation of Momentum 6.3 Collisions 6.4 Glancing Collisions 6.5 Rocket Propulsion © Reuters/Corbis A small buck from the massive bull transfers a large amount of momentum to the cowboy, resulting in an involuntary dismount. Momentum and Collisions What happens when two automobiles collide? How does the impact affect the motion of each vehicle, and what basic physical principles determine the likelihood of serious injury? How do rockets work, and what mechanisms can be used to overcome the limitations im- posed by exhaust speed? Why do we have to brace ourselves when Fring small projectiles at high velocity? ±inally, how can we use physics to improve our golf game? To begin answering such questions, we introduce momentum . Intuitively, anyone or any- thing that has a lot of momentum is going to be hard to stop. In politics, the term is metaphorical. Physically, the more momentum an object has, the more force has to be applied to stop it in a given time. This concept leads to one of the most powerful principles in physics: conservation of momentum . Using this law, complex collision problems can be solved without knowing much about the forces involved during contact. We’ll also be able to derive informa- tion about the average force delivered in an impact. With conservation of momentum, we’ll have a better understanding of what choices to make when designing an automobile or a moon rocket, or when addressing a golf ball on a tee. 6.1 MOMENTUM AND IMPULSE In physics, momentum has a precise defnition. A slowly moving brontosaurus has a lot oF momentum, but so does a little hot lead shot From the muzzle oF a gun. We thereFore expect that momentum will depend on an object’s mass and velocity. The linear momentum oF an object oF mass m moving with velocity is the product oF its mass and velocity : [6.1] SI unit: kilogram-meter per second (kg ? m/s) p : ; v : v : p : Doubling either the mass or the velocity oF an object doubles its momentum; dou- bling both quantities quadruples its momentum. Momentum is a vector quantity Linear momentum ©

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6.1 Momentum and Impulse 161 with the same direction as the object’s velocity. Its components are given in two di- mensions by p x ± mv x p y ± mv y where p x is the momentum of the object in the x -direction and p y its momentum in the y -direction. Changing the momentum of an object requires the application of a force. This is, in fact, how Newton originally stated his second law of motion. Starting from the more common version of the second law, we have [6.2] where the mass m and the forces are assumed constant. The quantity in parenthe- ses is just the momentum, so we have the following result: The change in an object’s momentum divided by the elapsed time D t equals the constant net force acting on the object: [6.3] This equation is also valid when the forces are not constant, provided the limit is taken as D t becomes inFnitesimally small. Equation 6.3 says that if the net force on an object is zero, the object’s momentum doesn’t change. In other words, the linear
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## This note was uploaded on 09/14/2009 for the course PHY 303K taught by Professor Turner during the Spring '08 term at University of Texas.

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chapter_6 - A small buck from the massive bull transfers a...

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