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CHAPTER 10: Collisions
Jieun Hwang, Lisa Boyette, Jason Steslace, Adam Gray, Matthew
Barnes
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PowerPoint Presentation (3.2MB)}
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*Denotes problem that may be on the Exam |
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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
- Use Conservation of Momentum
- Use Conservation of Kinetic Energy
- In Two Dimensions Treat Momentums as Vector Quantities (x, y) and solve
as usual.
- Use Conservation of Momentum
- NO CONSERVATION OF KINETIC ENERGY
- In Completely (Totally) Inelastic Collisions, Masses Stick Together
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