1 / 20

Puzzler:

Puzzler: A monkey hangs on a rope. The rope goes up over a pulley, and on the other end is a weight, which exactly balances the monkey. Everything is balanced, and is initially stationary. (As usual, friction is negligible, and so are mass of rope and pulley.)

alexis-woodard
Download Presentation

Puzzler:

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Puzzler: • A monkey hangs on a rope. The rope goes up over a pulley, and on the other end is a weight, which exactly balances the monkey. Everything is balanced, and is initially stationary. • (As usual, friction is negligible, and so are mass of rope and pulley.) • The monkey tries to climb the rope. What happens? • Only monkey rises • Monkey & weight both rise, but monkey faster • Monkey & weight both rise together • Monkey & weight both rise, but weight faster • Only weight rises http://activityworkshop.net/puzzlesgames/monkey/

  2. ANNOUNCEMENTS

  3. Carts A and B move on frictionless tracks. Cart A has a thruster directed along the track applying a force F. Cart B has its thruster applying force F directed at 60 deg with respect to the track. Both are released and allowed to travel 2 m. During their flights, the work done on B by the thruster was Zero. Less than half the work done on A. Half the work done on A. Equal to the work done on A. 1 of 3 F A B F 3

  4. 2 of 3 • Body A is dropped from rest into vertical free fall. Body B is released from rest down a frictionless incline. The kinetic energy gained by body B is • Greater than that gained by A. • Equal to that gained by A. • Less than that gained by A. • Zero. A B 4

  5. 3 of 3 • Body A is released from rest down a frictionless incline. Body B is released from rest to travel down a frictionless curvy track. It is assumed that B stays on the track and reaches the bottom. The kinetic energy gained by body B is • Greater than that gained by A. • Equal to that gained by A. • Less than that gained by A. • Zero. A B 5

  6. ANNOUNCEMENTS

  7. x Deriving the Work-Energy Theorem from Newton’s Second Law of Motion Newton’s 2nd Law of Motion “path integrating” Newton’s 2nd Law y A little displacement along the path of motion dr The “dot” product: Multiply the magnitude of one vector times the component of the other that lies along the first: q path of motion 7

  8. Deriving the Work-Energy Theorem from Newton’s Second Law of Motion Newton’s 2nd Law of Motion “path integrating” Newton’s 2nd Law Take a little displacement, multiply by the component of the net force acting along the path, and add all those up along the path of motion. This is called the “net work:” = This is called the “Work – Energy Theorem” 8

  9. The Work of a Force Because of … It is meaningful to speak of the “work of a force:” 9

  10. Compare and Contrast Two Methods of Dynamical Analysis 10

  11. Must be careful when applying work-energy principles to non-particulate or non-rigid bodies: • Both particles and rigid bodies are structureless, ideal entities, not thought of as being composed of any smaller interacting structures. • A particle or rigid body has no “internal degrees of freedom” in which to store internal energy (thermal energy). • Real bodies such as blocks, crates, automobiles, and people, are obviously not particles or rigid bodies. • The application of particle and rigid body mechanics to non-particulate and non-rigid bodies will result in energetic inaccuracies. • Augmenting the principles of work and energy to include systems with internal structure is called Thermodynamics. 11

  12. The work of friction is not computable by particulate means (FDx), because its displacement is not known. The friction force arises from interactions between bits and pieces of the body and its environment that are in motion relative to the body. 12

  13. III1 Exit Homework Problem #1

  14. III1 Exit Homework Problem #1

  15. III1 Exit Homework Problem #2

  16. III1 Exit Homework Problem #2

  17. Carts A and B move on frictionless tracks. Cart A has a thruster directed along the track applying a force F. Cart B has its thruster applying force F directed at 60 deg with respect to the track. Both are released and allowed to travel 2 m. During their flights, the work done on B by the thruster was Zero. Less than half the work done on A. Half the work done on A. Equal to the work done on A. 1 of 3 F A B F 17

  18. 2 of 3 • Body A is dropped from rest into vertical free fall. Body B is released from rest down a frictionless incline. The kinetic energy gained by body B is • Greater than that gained by A. • Equal to that gained by A. • Less than that gained by A. • Zero. A B 18

  19. 3 of 3 • Body A is released from rest down a frictionless incline. Body B is released from rest to travel down a frictionless curvy track. It is assumed that B stays on the track and reaches the bottom. The kinetic energy gained by body B is • Greater than that gained by A. • Equal to that gained by A. • Less than that gained by A. • Zero. A B 19

  20. PROJECTION SCREEN 1 4 1 4 1 4 1 4 2 5 2 5 2 5 2 5 3 6 3 6 3 6 3 6 III1: HAND IN TODAY’S ACTIVITIES SHEETS 21

More Related