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Chapter 7: Chapter 7: Linear Momentum (p) Linear Momentum (p)

Chapter 7: Linear Momentum (p)

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Chapter 7: Linear Momentum (p). (Linear) Momentum (p). Linear Momentum (p) is defined as the product of mass (m) and velocity (v): p = m v SI Units of linear momentum = kg.m/s p is a vector quantity: specified by magnitude and direction. - PowerPoint PPT Presentation

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Page 1: Chapter 7: Linear Momentum (p)

Chapter 7:Chapter 7:Linear Momentum (p)Linear Momentum (p)

Page 2: Chapter 7: Linear Momentum (p)

(Linear) Momentum (p)(Linear) Momentum (p) Linear Momentum (p) is defined as the

product of mass (m) and velocity (v):

p = m v

SI Units of linear momentum = kg.m/s

p is a vector quantity: specified by magnitude and direction.

The direction of p is the same as the direction of velocity v.

Page 3: Chapter 7: Linear Momentum (p)

Example: A car of mass 1,500 kg is traveling at a constant speed of 12 m/s due north. What is its linear momentum?

p = mv= (1,500 kg) x (12 m/s) = 18,000kg.m/s due north Constant momentum: Means both the mass

(m) and velocity (v) is not changing.Usually, mass stays constant during motion. Some exceptions:1. A rocket traveling: total mass changes as it

burns fuel.2. An open freight car being loaded while in

motion. Its mass will change as it moves

Page 4: Chapter 7: Linear Momentum (p)

Example:1. A car of mass 1,500 kg is traveling at a

constant speed of 12 m/s in a circular path. Is its linear momentum constant?

No: Because direction of velocity in a circular motion changes.

2. A ball of mass 0.2 kg is thrown horizontally at a wall. If it hits the wall at 25 m/s and bounces back with the same speed, what is the change in its momentum?

(A) 0 kg-m/s (B) 5 kg.m/s (C) -5 kg.m/s

(D) 10 kg.m/s (E) –10 kg.m/s

Page 5: Chapter 7: Linear Momentum (p)

Example:

3. A ball of mass 0.2 kg is thrown at an angle of 30o above the horizontal with a speed of 5 m/s and travels as a projectile.

(a)What is the y-component of its momentum at the instant it is thrown?

(b)At its maximum height, what is its momentum?

4. True/False? An object traveling with larger velocity must have larger momentum than another one traveling with smaller velocity.

Page 6: Chapter 7: Linear Momentum (p)

TOTAL MOMENTUM

Page 7: Chapter 7: Linear Momentum (p)

Example 1:

Car (1) is moving due east (+) at 30 m/s. Another car (2) is moving due east (+) at 30 m/s. For these two cars each of mass 1,500 kg, find their

(a) total kinetic energy.

(b) total momentum.

Page 8: Chapter 7: Linear Momentum (p)

Example 2:

Car (1) is moving due east (+) at 30 m/s. Another car (2) is moving due west (-) at 30 m/s. For these two cars each of mass 1,500 kg, find their

(a) total kinetic energy.

(b) total momentum.

Page 9: Chapter 7: Linear Momentum (p)

Example 3:

Yes/No?

Is it possible to have a system of objects where the total momentum is zero but the total kinetic energy is not zero?

Page 10: Chapter 7: Linear Momentum (p)

mAmB

V1(A) V1(B)

Total initial momentum:

pi = mA V1(A) + mB V1(B)

Conservation of Linear Momentum

Consider two objects with mass mA and mB moving towards each other with initial velocities v1(A) and v1(B)

Page 11: Chapter 7: Linear Momentum (p)

If these two objects collide and later their velocities after

impact are V2(A) and V2(B):

mAmB

V2(A) V2(B)

Total final momentum:

pf = mA V2(A) + mB V2(B)

Page 12: Chapter 7: Linear Momentum (p)

It has been established that on condition that no net external forces act on any system of colliding objects, the total momentum of the system will always remain conserved.

ie, pi = pf

OR:

mAV1(A) + mBV1(B) mA = mAV2(A) +mBV2(B)

Page 13: Chapter 7: Linear Momentum (p)

Law of Conservation of Linear Momentum:

Momentum is “Conserved” means it can not be created nor destroyed Can be transferred from one object to

another

Total Momentum does not change with time. Total momentum “before” = total momentum

“after.”This is a BIG deal! In science, any law of conservation is a

very powerful tool in understanding the physical universe.

Page 14: Chapter 7: Linear Momentum (p)

Law of Conservation of EnergyLaw of Conservation of Energy

In any natural process, total energy is always “conserved”, i.e. energy can not be created nor destroyed.

Can be transformed from one form to another.

Can be transferred from one system to

another.

In science, any law of conservation is a very powerful tool in understanding the physical universe.

Page 15: Chapter 7: Linear Momentum (p)

Example:

Jane and Fred are on skates facing each other. Jane then pushes Fred so he is going 2.0 m/s. If Fred is twice as heavy as Jane, how fast does Jane end up moving?

pinitial = pfinal

0 = mFred VFred + mJane VJane

VJane = mFred VFred / mJane = 4 m/s

Page 16: Chapter 7: Linear Momentum (p)

Example:

Car (1) is moving due east at 30 m/s. Another car (2) is moving due west at 30 m/s. For these two cars each of mass 1,500 kg, find

(a) Total kinetic energy.

(b) Total momentum.

(c) Yes/No? Is it possible to have a system of objects where the total momentum is zero but the total kinetic energy is not zero?

Page 17: Chapter 7: Linear Momentum (p)

A 15,000 kg open box-car is moving at 7 m/s on a level road. 3,000 kg of water then falls straight down into the box-car. The speed of the box-car now with the water in it is

A bullet of mass 20 grams initially traveling at a speed of 200 m/s lodges in a block of wood of mass 2 kg at rest on a frictionless floor. What is the velocity with which the bullet and block of wood travel after impact?

Page 18: Chapter 7: Linear Momentum (p)

Example 7.1: A car w/ mass 1200 kg is driving north at 30 m/s, and turns east driving 13.6 m/s. What is the magnitude of the car’s change in momentum?

pinitial = m vinitial = (1200 Kg) x 30 m/s = 36000 kg m/s North

pfinal = m vfinal = (1200 Kg) x 13.6 m/s = 16320 kg m/s East

North-South:pfinal – pinitial = (0 – 36000) = -36000 kg m/s

East-West:pfinal – pinitial = (16320 - 0) = +16320 kg m/s

Magnitude :Sqrt(p2

North – p2East ) = 39526 kg m/s

v1 = 30 m/s

v2 = 13.6 m/s

Page 19: Chapter 7: Linear Momentum (p)

A ball is projected straight up. Which graph shows the linear momentum of the ball as a function of time?

t t t

tt

t

(A) (B) (C) (D)

(E)(F)

Page 20: Chapter 7: Linear Momentum (p)

IMPULSE

Objects A and B colliding: The force of impact A exerts on B = FBA. This causes velocity of B to change from v1(B) to v2(B)

FBA = maB = m[v2(B) – v1(B)]/t

OR FBA t = m(v2(B) – v1(B)) = p

• The quantity FBA t is called impulse (of a force).

Impulse = F t = p Unit = N.s

• Change in momentum requires force acting over a time duration.

Page 21: Chapter 7: Linear Momentum (p)

IMPULSE

Time t (s)

Forc

e F

(N

)

Impulse = area under the graph

Page 22: Chapter 7: Linear Momentum (p)

Time t (s)

(a) Calculate the impulse

(b) If this impulse was applied on a 3 kg mass at rest, what would its final velocity be?

Force F (N)

0.2 0.4 0.60

200

Page 23: Chapter 7: Linear Momentum (p)

Example:

A force of 30 N is applied for 5 s to each of two objects of mass m and M (m < M). Which of the masses experience the greater

(a) Momentum change?

(b) Velocity change?

(c) Acceleration?

Ft = p

p = (mv) = m(v) and v = p/m

F = ma and a = F/m

Page 24: Chapter 7: Linear Momentum (p)

Why do we flex our knees when when jumping?

•Increases the time of contact for the ground to bring you to rest.

•In turn reduces force exerted on your body.

Page 25: Chapter 7: Linear Momentum (p)

A 160-gram baseball with a velocity of 20 m/s is hit by a bat and leaves at 25 m/s in the opposite direction. If the contact lasted for only 0.012 s, what was the magnitude of the average force on the ball? [1,000 grams = 1 kg]

Page 26: Chapter 7: Linear Momentum (p)

Example on conservation of momentum:

A bullet of mass 200 g traveling at a speed of 150 m/s hits a 3 kg block of wood at rest on a frictionless table. If the bullet lodges inside the block, with what speed will the bullet-block composite travel after impact?

Page 27: Chapter 7: Linear Momentum (p)

Elastic and Inelastic Collisions

1. Elastic Collisions:

Collisions in which the total kinetic energy is conserved.

Kinitial = Kfinal

2. Inelastic Collisions:

Collisions in which the total kinetic energy is NOT conserved.

Kinitial Kfinal

Page 28: Chapter 7: Linear Momentum (p)

mAmB

V1(A) V1(B)

Ki = ½ mAv21(A) + ½ mBv2

1(B)

Before:

mAmB

V2(A) V2(B)

Kf = ½ mAv22(A) + ½ mBv2

2(B)

After:

For Elastic Collision: Ki = Kf

OR ½ mAv21(A) + ½ mBv2

1(B) = ½ mAv22

(A) + ½ mBv22(B)

Page 29: Chapter 7: Linear Momentum (p)

•In most cases, collisions occur inelastically.

• Part of the total initial kinetic energy is converted to other forms of energy such as light, heat, sound, etc.

Ki = Kf + heat + sound + light, etc

•However, total energy and total linear momentum are still conserved even in inelastic collisions.

•Elastic collision is an ideal case. Collision of billiard balls when no heat is produced is the closest approximation to elastic collision.

Page 30: Chapter 7: Linear Momentum (p)

Center of MassCenter of Mass

Center of Mass = Balance point of a large object

= Balance point of a number of discrete objects

For an object with a regular shape (sphere, cylinder, cube etc, CM is located at its geometric center.

...

....

21

2211

mm

xmxmxcm

...

....

21

2211

mm

ymymycm

Page 31: Chapter 7: Linear Momentum (p)

Example

m5m

xCM = (0 + mL)/2m = L/2

xCM = (0 + 5mL)/6m = 5L/6X = 0 X = L

mmx

x

Page 32: Chapter 7: Linear Momentum (p)

Example

A 55-kg man walks his 5-kg dog using a 3 meter long lease. Where is the center of mass of the man-dog system?

Page 33: Chapter 7: Linear Momentum (p)

Example: Find the center of mass.

x

y

1 kg

3 kg

7 kg

0 2 4 6 8

2

4

6

8

Page 34: Chapter 7: Linear Momentum (p)

Collisions in Two Dimensions

When dealing with collisions in 2-D, momentum conservation is applied separately to the x and y components of the total momentum:

px (Before) = px (After) -----[x-components]

And

py (Before) = py (After) -----[y-components]

Page 35: Chapter 7: Linear Momentum (p)

y

x60o

30o

m1

m2

m2

0.4 kg

m1

0.1 kg

Before After

8 m/s At rest

(a) Find the speeds v1 and v2 after the collision.

(b) Is the collision elastic or inelastic?

v1

v2

Page 36: Chapter 7: Linear Momentum (p)

A large seed initially at rest explodes into two pieces which move off. Which of these could be possible paths the two pieces would take?

(I)

(II)

(III)

Page 37: Chapter 7: Linear Momentum (p)

Two objects with different masses (m and M with m < M) have the same kinetic energy. Which has the larger magnitude of momentum?

[Hint: K = ½ p2/m]

Page 38: Chapter 7: Linear Momentum (p)

A ball is projected straight up. Which graph shows the total energy of the ball as a function of time?

t t t

tt

t

(A) (B) (C) (D)

(E)(F)

Page 39: Chapter 7: Linear Momentum (p)

P7.35

A BMW of mass 2.0 x 103 kg is traveling at 42 m/s. It approaches a 1.0 x 103 kg VW going 25 m/s in the same direction and strikes it in the rear. Neither driver applies the brakes. Neglect frictional forces due to the road and air resistance. If the collision slows the BMW down to 33 m/s, what is the speed of the VW after collision?

Page 40: Chapter 7: Linear Momentum (p)

A 75-kg person jumps off a table and lands on the ground with a speed of 3.5 m/s. By flexing his knees, he comes to rest in 0.40 seconds. Determine the average force exerted on his body in this process.