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10/01/2013 PHY 113 C  Fall 2013 -- Lecture 10 10/01/2013 PHY 113 C  Fall 2013 -- Lecture 10

10/01/2013 PHY 113 C Fall 2013 -- Lecture 10 - PowerPoint Presentation

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10/01/2013 PHY 113 C Fall 2013 -- Lecture 10 - PPT Presentation

1 PHY 113 C General Physics I 11 AM 1215 P M MWF Olin 101 Plan for Lecture 10 Chapter 9 Linear momentum Impulse and momentum Conservation of linear momentum Examples collision ID: 639168

phy 2013 lecture 113 2013 phy 113 lecture fall collision elastic center momentum mass analysis physics iclicker balls proton frictionless surface moving

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Slide1

10/01/2013

PHY 113 C Fall 2013 -- Lecture 10

1

PHY 113 C General Physics I

11 AM – 12:15

P

M MWF Olin 101

Plan for Lecture 10

Chapter

9 -- Linear momentum

Impulse and momentum

Conservation of linear momentum

Examples – collision

analysis

Notion of center of massSlide2

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PHY 113 C Fall 2013 -- Lecture 10

2Slide3

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PHY 113 C Fall 2013 -- Lecture 10

3

Summary of physics “laws”Slide4

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PHY 113 C Fall 2013 -- Lecture 10

4

Another way to look at Newton’s second law:

iclicker

question:

Why would you want to define linear momentum?

To impress your friends.

To exercise your brain.

It might be helpful.

To distinguish it from angular momentum.Slide5

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PHY 113 C Fall 2013 -- Lecture 10

5

Relationship between Newton’s second law and linear momentum:

(if

m

is constant)Slide6

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6Slide7

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7

Suppose that a tennis ball with mass m=0.057 kg approaches a tennis racket at a speed of 45m/s. What is the impulse the racket must exert on the ball to return the ball in the opposite direction at the same speed. Assume that the motion is completely horizontal.Slide8

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8

Example: A 1500 kg car collides with a wall, with

v

i

= -15m/s and

v

f

=2.6m/s. What is the impulse exerted on the car?Slide9

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PHY 113 C Fall 2013 -- Lecture 10

9

Example of graphical representation of F(t)Slide10

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10

Physics of composite systemsSlide11

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11

Example – completely

inelastic

collision; balls moving on a frictionless surfaceSlide12

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12

Energy loss in this example:Slide13

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13

Example – completely

elastic

collision; balls moving on a frictionless surfaceSlide14

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14

Completely elastic collision; numerical example:Slide15

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PHY 113 C Fall 2013 -- Lecture 10

15

iclicker

exercise:

We have assumed that there is no net force acting on the system. What happens if there are interaction forces between the particles?

Analysis still applies

Analysis must be modifiedSlide16

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16

Example from homework:Slide17

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17

Example from homework

: -- continued

iclicker

question

Do you expect

K

f

-K

i

to be

>0

<0Slide18

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PHY 113 C Fall 2013 -- Lecture 10

18

Another example:

before

v

f

afterSlide19

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19

Examples of two-dimensional collision;

balls

moving on a frictionless surfaceSlide20

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20

Examples of two-dimensional collision;

balls

moving on a frictionless surfaceSlide21

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21

Example: two-dimensional totally inelastic collision

m

1

=1500kg

m

2

=2500kgSlide22

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22

iclicker

exercise:

Can this analysis be used to analyze a real collision?

Of course! The laws of physics must be obeyed.

Of course NOT! In physics class we only deal with idealized situations which never happen.Slide23

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23

Another example of 2-dimensional elastic collision:

m

v

i

v

f

mSlide24

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24

Energy analysis of a simple nuclear reaction :

Q=4.87 MeVSlide25

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25

Energy analysis of a simple reaction :

Q=4.87 MeVSlide26

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26

Elastic collision in two dimensionsSlide27

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27

Elastic collision in two dimensions --

example of elastic proton-proton scatteringSlide28

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28

Elastic collision in two dimensions --

example of elastic proton-proton scatteringSlide29

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29

The notion of the center of mass and the physics of composite systemsSlide30

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30Slide31

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31

Finding the center of massSlide32

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32

Example from

webassign

:

x

y

m

1

m

2

m

3

m

4Slide33

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33

Finding the center of mass

For a solid object composed of constant density material, the center of mass is located at the center of the object.