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Physics 207 WebPages - Fall 1999
Chapter 10


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Chapter 4
Chapter 5
Chapter 6
Chapter 7
Chapter 8
Chapter 9
Chapter 10
Chapter 11
Chapter 12
Chapter 13
Chapter 14
Chapter 16

CHAPTER 10: Collisions

Jieun Hwang, Lisa Boyette, Jason Steslace, Adam Gray, Matthew Barnes

{Download PowerPoint Presentation (3.2MB)}

*Denotes problem that may be on the Exam

 


The Take-Home Message on Chapter 10

  • If two bodies are exerting STRONG forces on each other over a short period of time, then you have a collision problem.
  • Linear Momentum is ALWAYS conserved.
  • Kinetic Energy is NOT always conserved.
    • Kinetic Energy is conserved during an elastic collision.
    • Kinetic Energy is not necessarily conserved during an inelastic collision.
  • Impulse-Linear Momentum Theorem
    • Relates strength and duration of collision force to change in momentum
    • Similar to Work-Kinetic Energy Theorem

Equations

  • D p = pf - pi = J (10-4)
  • J = F D t (10-8)
  • (10-10)
  • (10-18)
  • (10-19)
  • (10-28)
  • (10-29)
  • (10-34)
  • (10-36)
  • (10-30)

 

Problem Types

  • Impulse and Linear Momentum
    • Series of Collisions
  • Elastic Collision
    • 1-D
    • 2-D
  • Moving Target vs. Stationary Target
  • Inelastic Collision
    • 1-D
    • 2-D

 

How to Solve Them

  • Impulse and Linear Momentum
  • Use Conservation of Momentum
  • Impulse-Linear Momentum Theorem
  • Series of Collisions
  • Use Equation (10-10)
  • Elastic Collisions
  • Use Conservation of Momentum
  • Use Conservation of Kinetic Energy
  • In Two Dimensions Treat Momentums as Vector Quantities (x, y) and solve as usual.
  • Inelastic Collisions
  • Use Conservation of Momentum
  • NO CONSERVATION OF KINETIC ENERGY
  • In Completely (Totally) Inelastic Collisions, Masses Stick Together
 

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