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Physics 101 General Physics Who am I? Dr. Bruton I may be teaching the remainder of this course for Mr. Carlton. We have similar teaching styles. There.

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Presentation on theme: "Physics 101 General Physics Who am I? Dr. Bruton I may be teaching the remainder of this course for Mr. Carlton. We have similar teaching styles. There."— Presentation transcript:

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2 Physics 101 General Physics

3 Who am I? Dr. Bruton I may be teaching the remainder of this course for Mr. Carlton. We have similar teaching styles. There will be extra credit. I will “teach to” Mr. Carlton’s test. I will hit the highlights of the chapters with PowerPoint presentations.

4 Let’s take notes…

5 Chapter 6 Momentum

6 Momentum and Collisions This chapter is concerned with inertia and motion. Momentum helps us understand collisions.

7 Momentum and Collisions Elastic Collisions –objects rebound –e.g. superball Inelastic Collisions –object stick together an usually become distorted and generate heat –e.g. clay ball

8 Momentum Momentum = mass  velocity p = mv Momentum is a vector quantity.

9 A large truck has more momentum than a car moving at the same speed because it has a greater mass. Which is more difficult to slow down? The car or the large truck?

10 Large Momentum Examples: –Huge ship moving at a small velocity –High velocity bullet P = m v

11 Impulse In order to change the momentum of an object you must apply a force over some time interval. Impulse = Force  time interval = F t

12 Impulse and Momentum Impulse = Change in Momentum = Final (mv) - Initial (mv) F t =  (mv)

13 Case 1: Increasing Momentum –Apply a force for a long time. –Examples: Follow through on a golf swing. Pushing a car. FtFt

14 Case 2: Decreasing Momentum –Apply a force for a long time. –Examples: Air bags in cars. Catching an egg. Boxing, Figure 6.6 Soft collisions, Figure 6.3. FtFt

15 Case 3: Decreasing Momentum –Apply a force for a short time. –Examples: Boxing Karate FtFt

16 Conservation of Momentum This means that the momentum doesn’t change. Recall that F t =  mv) In this equation, F is the "external force". Internal forces cannot cause a change in momentum.

17 Examples Conservation of Momentum: If there are no external forces, the total momentum for a system remains unchanged. Example 1: a person sitting inside a car pushing against the dashboard Example 2: a bullet fired from a rifle Example 3: a rocket is space

18 Example Problems...


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