# Sg3 - PH1110 STUDY GUIDE 3 Work Energy and Momentum Objectives Term A10 15 Define work and calculate the work done by a constant force as the body

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PH1110 Term A10 STUDY GUIDE 3: Work, Energy, and Momentum Objectives 15. Define work and calculate the work done by a constant force as the body on which it acts is moved by a given amount. Be able to calculate the scalar product of two vectors. 16. Define kinetic energy. 17. State the work-energy theorem. Give examples of and solve problems for which the application of the work-energy theorem is appropriate. 18. Define power, and use the concept to solve problems involving the rate at which work is done. 19. Distinguish between conservative and non-conservative forces and give examples of each. 20. Calculate the work done on a particle by a uniform gravitational force and by a spring undergoing compression or extension. 21. Use the principle of mechanical energy conservation to solve appropriate problems. 22. Define the linear momentum of a particle and of a system of particles. 23. Define impulse of a force and relate it to the change in linear momentum that it causes. 24. Give examples of and solve problems for which conservation of linear momentum is appropriate. Distinguish between elastic and inelastic collisions. Suggested Study Procedure for Chapter 6. Study Secs. 6.1 through 6.4. Study Examples 2, 3, 4, 6, 7. Answer Questions 2, 5, 11, 12, 13. Do Exercises 3, 4, 17, 25, 29, 33, 37. Do Problems 57, 62, 69, 82, 91. A. As great as we have already found Newton's laws to be in helping us understand and predict the motion of objects, there are wondrous new and enormously powerful concepts lurking in those three disarmingly simple statements. Two such concepts that tumble mathematically right out of the Second Law are WORK and ENERGY, the subjects of Chapts. 6 and 7. 1. A FORCE carried through a DISPLACEMENT performs WORK. But be careful here! Work is NOT force times distance; rather, it involves only the component of force parallel to the displacement. In the special case of straight-line displacement with constant force (the case we will consider most of the time!), work is equal to the product of the force component parallel to the displacement with the distance traveled. 2. Work and energy are SCALAR quantities -- they are purely numbers WITHOUT spatial direction. DO NOT attach vector directions to work or energy; that's just plain WRONG! Now it may bother you that a scalar can result from the multiplication of two vector quantities (force and displacement), but that's the way it is. The mathematical operation that accomplishes this strange feat is called the "scalar product" and is discussed in detail in Sec. 6.1. Sections 6.1 through 6.3 provide discussion and worked examples on the subject.

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B. The WORK-ENERGY THEOREM (which comes mathematically straight out of the 2nd law!) states that the TOTAL WORK done on an object is equal to the CHANGE IN KINETIC ENERGY of the object (final minus initial). What's so great about that, you may ask? Well, for one thing, a scalar equation is invariably easier to work with than a vector equation. For another,
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## This note was uploaded on 10/25/2010 for the course PH 1110 taught by Professor Kiel during the Fall '08 term at WPI.

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Sg3 - PH1110 STUDY GUIDE 3 Work Energy and Momentum Objectives Term A10 15 Define work and calculate the work done by a constant force as the body

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