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Chapter 9. Impulse and Chapter 9. Impulse and Momentum Momentum Explosions and collisions obey some surprisingly simple laws that make problem solving easier when comparing the situation before and after an before and after an interaction. Chapter Goal: To introduce the ideas of impulse and momentum and to learn a new problem-solving strategy based on conservation laws.

Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

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Page 1: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Chapter 9. Impulse and Chapter 9. Impulse and MomentumMomentum

Explosions and collisions

obey some surprisingly

simple laws that make

problem solving easier when

comparing the situation

before and after an before and after an

interaction.

Chapter Goal: To introduce

the ideas of impulse and

momentum and to learn a

new problem-solving strategy

based on conservation laws.

Page 2: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Topics:

• Momentum and Impulse

• Solving Impulse and Momentum

Problems

• Conservation of Momentum

Chapter 9. Impulse and Chapter 9. Impulse and Momentum Momentum

• Conservation of Momentum

• Inelastic Collisions

• Explosions

• Momentum in Two Dimensions

Page 3: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Momentum

A B10 m/s

After the collision

A Bv u

3

What is the velocity of ball A after the collision? ball B?

What is conserved during the collision?

MOMENTUM

The total momentum is the sum of momentum of ball A and

momentum of ball B.

p mv====r rr rr rr r

Page 4: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Momentum

The total momentum of the system is conserved during the collision:

A B10 m/s

AB

v u

p mv====r rr rr rr r

,A A i A Bm v m v m u= += += += +

4

v u

• Momentum is a vector. It has the same direction as corresponding

velocity.

• General expression for the momentum conservation: the total

momentum before the collision is equal to the total momentum after

the collision

Page 5: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Momentum

A

B

A

p mv====r rr rr rr r

• General expression for the momentum conservation: the total

momentum before the collision is equal to the total momentum after

the collision

,A ivrrrr

,B ivrrrr

,A fvrrrr

vrrrr

5

B

, , , ,A A i B B i A A f B B fm v m v m v m v+ = ++ = ++ = ++ = +

r r r rr r r rr r r rr r r r

,B fvrrrr

Usually this equation is written in terms of components.

Page 6: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Example:

A B10 m/s

After the collision the balls are moving together (have the same velocity). What is their velocity?

A B

1A

m kg==== 4B

m kg====

6

A Bv

,10

i A A i

kg mp m v

s

⋅⋅⋅⋅= == == == =Momentum before the collision:

Momentum after the collision: ( ) 5f A B

p m m v v= + == + == + == + =

Conservation of momentum: i fp p====

10 5v==== 2 /v m s====

Page 7: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Newton’s second law:

momentum

netF ma====rrrr rrrr

Why do we have conservation of total momentum?

Acceleration:dv

adt

====

rrrrrrrr

Then( )

net

dv d mv dpF m

dt dt dt= = == = == = == = =

r r rr r rr r rr r rrrrr

7

The area under curve.

It is called IMPULSE, J.

netF m

dt dt dt= = == = == = == = =

2

1

t

net

t

p F dt∆ =∆ =∆ =∆ = ∫∫∫∫rrrrrrrr

After integration

( )net

F trrrr

2

1

t

net

t

J F dt==== ∫∫∫∫r rr rr rr r

The impulse of the force is equal to the change of the momentum of the object.

p J∆ =∆ =∆ =∆ =rrrrrrrr

Page 8: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

i ixp mv====

0f fx

p mv= <= <= <= <

8

0x f i

J p p= − <= − <= − <= − <

Page 9: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

2

1

1 ,1 1 ,1 ,2 1

t

fx ix x on

t

m v m v F dt− =− =− =− = ∫∫∫∫2

1

2 ,2 2 ,2 ,1 2

t

fx ix x on

t

m v m v F dt− =− =− =− = ∫∫∫∫

Newton’s third law:

,1 2 ,2 1x on x onF F= −= −= −= −

9

,1 2 ,2 1x on x onF F= −= −= −= −

Then

2 2

1 1

,1 2 ,2 1

t t

x on x on

t t

F dt F dt= −= −= −= −∫ ∫∫ ∫∫ ∫∫ ∫

(((( ))))2 ,2 2 ,2 1 ,1 1 ,1fx ix fx ixm v m v m v m v− = − −− = − −− = − −− = − −

Page 10: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

(((( ))))2 ,2 2 ,2 1 ,1 1 ,1fx ix fx ixm v m v m v m v− = − −− = − −− = − −− = − −

1 ,1 2 ,2 1 ,1 2 ,2ix ix fx fxm v m v m v m v+ = ++ = ++ = ++ = +

,1 ,2 ,1 ,2ix ix fx fxp p p p+ = ++ = ++ = ++ = +

10

,1 ,2 ,1 ,2ix ix fx fxp p p p+ = ++ = ++ = ++ = +

, ,ix total fx totalp p====

The law of conservation of momentum

Page 11: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Momentum

A A

p mv====r rr rr rr r

,A ivrrrr

vrrrr

The law of conservation of momentum:

The total momentum of an isolated system (no external forces) does not change.

Interactions within system do not change the system’s total momentum

isolated system

11

B

B

, , , ,A A i B B i A A f B B fm v m v m v m v+ = ++ = ++ = ++ = +

r r r rr r r rr r r rr r r r

,A iv

,B ivrrrr

,A fv

,B fvrrrr

Page 12: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Momentum p mv====r rr rr rr r

The ball is dropped onto a hard floor:

� The ball is not an isolated system (interaction with the floor)

� no conservation of momentum for the ball

� Initial momentum is

� Final momentum (after collision) is

i ip mv====r rr rr rr r

f fp mv====r rr rr rr r

12

ivrrrr

fvrrrr

� The ball+ the floor is an isolated system

� The total momentum (ball+floor) is conserved

Page 13: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Example: Find2 x

v

Isolated system

13

Motion with constant acceleration:

2

1 , 1( ) 2 16

x B xv a x= == == == =

1 ,4 /

x Bv m s====

Isolated system

Momentum before the “collision”:

, 1 , 1 , 1 ,75 4 300

i total B x B C x C B x B

kg mp m v m v m v

s

⋅⋅⋅⋅= + = = ⋅ == + = = ⋅ == + = = ⋅ == + = = ⋅ =

Momentum after the “collision”:

, 2 , 2 , 2 2( ) 100

f total B x B C x C B C x xp m v m v m m v v= + = + == + = + == + = + == + = + =

Conservation of momentum:

, ,f total i totalp p====

2100 300

xv ==== 2

3 /x

v m s====

Page 14: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Perfectly inelastic collision:

A collision in which the two objects stick together and move with a

common final velocity.

, 1 ,1 2 ,2i total ix ixp m v m v= += += += +

14

, 1 2( )

f total fxp m m v= += += += +

1 ,1 2 ,2 1 2( )

ix ix fxm v m v m m v+ = ++ = ++ = ++ = +

1 1

,2 ,1

2 2

3 31 0.5 2.25 /

2 2ix fx ix

m mv v v m s

m m

= + − = − ⋅ − = −= + − = − ⋅ − = −= + − = − ⋅ − = −= + − = − ⋅ − = −

Page 15: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Chapter 9. Summary SlidesChapter 9. Summary Slides

Page 16: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

General Principles

Page 17: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

General Principles

Page 18: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Important Concepts

Page 19: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Important Concepts

Page 20: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Applications

Page 21: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Applications

Page 22: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Chapter 9. QuestionsChapter 9. Questions

Page 23: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

The cart’s change of momentum is

A. 30 kg m/s.

B. 10 kg m/s.

C.–10 kg m/s.

D.–20 kg m/s.

E.–30 kg m/s.

Page 24: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

The cart’s change of momentum is

A. 30 kg m/s.

B. 10 kg m/s.

C.–10 kg m/s.

D.–20 kg m/s.

E.–30 kg m/s.

Page 25: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

A. They exert equal impulses because they

have equal momenta.

A 10 g rubber ball and a 10 g clay ball are

thrown at a wall with equal speeds. The

rubber ball bounces, the clay ball sticks.

Which ball exerts a larger impulse on the

wall?

have equal momenta.

B. The clay ball exerts a larger

impulse because it sticks.

C. Neither exerts an impulse on the

wall because the wall doesn’t move.

D. The rubber ball exerts a larger impulse

because it bounces.

Page 26: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

A. They exert equal impulses because they

have equal momenta.

A 10 g rubber ball and a 10 g clay ball are

thrown at a wall with equal speeds. The

rubber ball bounces, the clay ball sticks.

Which ball exerts a larger impulse on the

wall?

have equal momenta.

B. The clay ball exerts a larger

impulse because it sticks.

C. Neither exerts an impulse on the

wall because the wall doesn’t move.

D. The rubber ball exerts a larger impulse because it bounces.

Page 27: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Objects A and C are made of different materials, with different

“springiness,” but they have the same mass and are initially at rest.

When ball B collides with object A, the ball ends up at rest. When ball B

is thrown with the same speed and collides with object C, the ball

rebounds to the left. Compare the velocities of A and C after the

collisions. Is vA greater than, equal to, or less than vC?

A. vA > vC

B. vA < vC

C. vA = vC

Page 28: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

Objects A and C are made of different materials, with different

“springiness,” but they have the same mass and are initially at rest.

When ball B collides with object A, the ball ends up at rest. When ball B

is thrown with the same speed and collides with object C, the ball

rebounds to the left. Compare the velocities of A and C after the

collisions. Is vA greater than, equal to, or less than vC?

A. vA > vC

B. vA < vC

C. vA = vC

Page 29: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

The two particles are both moving to the right. Particle 1 catches up with particle 2 and collides with it. The particles stick together and continue on with velocity vf. Which of these statements is true?

A. vf = v2.

B. vf is less than v2.

C. vf is greater than v2, but less than v1.

D. vf = v1.

E. vf is greater than v1.

Page 30: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

The two particles are both moving to the right. Particle 1 catches up with particle 2 and collides with it. The particles stick together and continue on with velocity vf. Which of these statements is true?

A. vf = v2.

B. vf is less than v2.

C. vf is greater than v2, but less than v1.

D. vf = v1.

E. vf is greater than v1.

Page 31: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

An explosion in a rigid pipe shoots out three pieces. A 6 g piece comes out the right end. A 4 g piece comes out the left end with twice the speed of the 6 g piece. From which end does the third piece emerge?piece emerge?

A. Right end

B. Left end

Page 32: Chapter 9. Impulse and Momentum - Physics & Astronomy · 2011. 3. 10. · Chapter 9. Impulse and Momentum Explosions and collisions obey some surprisingly simple laws that make problem

An explosion in a rigid pipe shoots out three pieces. A 6 g piece comes out the right end. A 4 g piece comes out the left end with twice the speed of the 6 g piece. From which end does the third piece emerge?piece emerge?

A. Right end

B. Left end