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Chapter 6: Momentum and Collisions

Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

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Page 1: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Chapter 6:Momentum

and Collisions

Page 2: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Section 6 – 1Momentum and

Impulse

Page 3: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Momentum (p)A vector quantity defined as the product of an object’s mass and velocity.

Describes an object’s motion.

Page 4: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

• Why “p”?

–Pulse (Date: 14th century)

•from Latin pulsus, literally, beating, from pellere to drive, push, beat

http://www.madsci.org/posts/archives/dec99/945106537.Ph.r.html

Page 5: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Momentum = mass x velocity

p = mv

Units: kg-m/s

Page 6: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse
Page 7: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Conceptualizing momentum

Question –

Which has more momentum; a semi-truck or a Mini Cooper cruising the road at 10 mph?

Answer –

The semi-truck has more mass. Since the velocities are the same, the semi has more momentum.

Page 8: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Conceptualizing momentum

Question –

Which has more momentum; a parked semi-truck or a Mini Cooper moving at 10 mph?

Answer –

The velocity of the semi is 0 mph. That means its momentum is 0 and this time the Mini Cooper has more momentum.

Page 9: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Conceptualizing momentumQuestion –

Which has more momentum, a train moving at 1 mph or a bullet moving at 2000 mph?

Answer –

The mass of a train is very large, while the mass of a bullet is relatively small. Despite the large speed of the bullet, the train has more momentum.

Page 10: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 1: Gary is driving a 2500 kg

vehicle, what is his momentum if his

velocity is 24 m/s?

Page 11: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: m =2500 kg, v =24 m/s

U: p =?

E: p = mv

S: p = (2500 kg)(24m/s)

S: p = 60,000 kg-m/s

Page 12: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 2: Ryan throws a 1.5 kg football, giving it a momentum of 23.5 kg-

m/s. What is the velocity of the

football?

Page 13: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: m=1.5 kg, p =23.5 kg-m/s

U: v = ?

E: p = mv or v = p/m

S:v=(23.5 kg-m/s)/(1.5kg)

S: v = 15.7 m/s

Page 14: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

A change in momentum

p

(p = mv)

Takes force and time.

Page 15: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Momentums do not always stay the same. When a force is applied to a moving object, the momentum changes.

Page 16: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

ImpulseThe product of the force and

the time over which it acts on an object, for a constant

external force.

Impulse = Ft

Page 17: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

The change in the momentum is also

called the impulse.

Page 18: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Impulse – Momentum Theorem

Ft = por

Ft = mvf - mvi

Page 19: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 3: What is the impulse on a football

when Greg kicks it, if he imparts a force of 70 N

over 0.25 seconds? Also, what is the change

in momentum?

Page 20: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: F = 70 N, t = 0.25 s U: Impulse = ?E: Impulse = FtS: Impulse =(70 N)(0.25 s)S: Impulse = 17.5 kg-m/sFt = p =17.5 kg-m/s

Page 21: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 4: How long does it take a force of 100 N

acting on a 50-kg rocket to increase its speed from 100 m/s to 150

m/s?

Page 22: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: F = 100 N, vf = 150 m/s, vi = 100m/s, m = 50 kg

U: t = ?

E: t = m (vf - vi)/F

S:t=50kg(150–100m/s)/100s

S: t = 25 sec

Page 23: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Stopping times and distances depend

upon impulse-momentum

theorem.

Page 24: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 5: Crystal is driving a 2250 kg car west, she slows down from 20 m/s to 5 m/s. How long does it take the car to

stop if the force is 8450 N to the east? How far does the

car travel during this deceleration?

Page 25: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: m = 2250 kg F = 8450 N east = 8450 N

vi = 20 m/s west = - 20 m/s

vf = 5 m/s west = - 5 m/sU: t =?

E: F t = p = m (vf - vi)

t = m (vf - vi) / F

Page 26: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

S:t=[2250kg(-5– -20m/s)]

8450 N

Page 27: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

St=[2250kg(-5– -20m/s)]

8450 N

S: 4.0 s

Page 28: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

B)U: x = ?

E: x = ½(vi + vf )tS:x=½(-5+-20)m/s(4 s)

S: x = - 50 m x = 50 m west

Page 29: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Frictional forces will be disregarded

in most of the problems unless otherwise stated.

Page 30: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Section 6-2Conservation of

Momentum

Page 31: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Law of Conservation of Momentum

The total momentum of all objects interacting with one another remains constant regardless of the nature of the forces between them.

Page 32: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

What this means:Any momentum lost by

one object in the system is gained by one or more of the other objects in the

system.

Page 33: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

total initial momentum

total final momentum=

Page 34: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

ffii pppp ,2,1,2,1

total initial momentum

total final momentum=

Page 35: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

ffii vmvmvmvm ,22,11,22,11

ffii pppp ,2,1,2,1

total initial momentum

total final momentum=

Page 36: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

For objects that collide:

The momentum of the individual object(s) does not remain constant, but

the total momentum does.

Page 37: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Momentum is conserved when objects push away from each

other.Ex 1: Jumping, Initially there is

no momentum, but after you jump, the momentum of the you and the earth are equal and opposite.

Page 38: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 2: 2 skateboarders pushing away from each other. Initially neither has momentum. After pushing off one another they both have the same momentum, but in opposite direction.

Page 39: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Which skateboarder has the higher

velocity?The one with the

smaller mass.

Page 40: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse
Page 41: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 6: John, whose mass is 76 kg, is initially at rest in a stationary 45 kg boat, steps out of the boat and onto the dock with an a velocity of 2.5 m/s to the right. What is the final velocity of the boat?

Page 42: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: mjohn=76 kg, mboat= 45kg, vjohn, i = vboat,i = 0 m/s, vjohn,f = 2.5 m/s

U: vboat = ?E: Momentum is conserved.

PJ,i + pb,i = pJ,f + pb,f

0 + 0 = mjvJ,f + mbvb,f

Page 43: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vb,f = (mJvJ,f) /-mb

Page 44: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vb,f = (mJvJ,f) /-mb

S: vb,f = (76kg x 2.5m/s) - 45kg

Page 45: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vb,f = (mJvJ,f) /-mb

S: vb,f = (76kg x 2.5m/s) - 45kg

S: vb,f = - 4.2 m/s

Page 46: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vb,f = (mJvJ,f) /-mb

S: vb,f = (76kg x 2.5m/s) - 45kg

S: vb,f = - 4.2 m/s

or 4.2 m/s to the left

Page 47: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Newton’s 3rd Law leads to a

conservation of momentum.

Open books to page 219-220

Page 48: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Forces in real collisions are not

constant. They vary throughout the

collision, but are still opposite and equal.

Page 49: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Section 6 – 3 Elastic and

Inelastic Collisions

Page 50: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Perfectly Inelastic Collisions

A collision in which two objects stick together and move with a common velocity.

Page 51: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

fii vmmvmvm 21,22,11

Page 52: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 7: A toy engine having a mass of 5.0 kg and a speed of 3 m/s, east,

collides with a 4 kg train at rest. On colliding the two engines lock and remain

together.

Page 53: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

(a) What is the velocity of the

entangled engines after the collision?

Page 54: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G: m1 = 5.0 kg, m2 =4.0kg v1 = 3 m/s, & v2 = 0 m/s

U: v1+2 = ?

E: p1,i + p2,i = p1+2

m1v1 + m2v2 =m1+2 v1+2

Page 55: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

v1+2 =[m1v1 +m2v2]/m1+2

v1+2= [(5 x 3)+(4 x 0)]/9

v1+2= 1.66 m/s, east

Page 56: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

KE is not constant in inelastic collisions.

Some of the KE is converted into sound energy and internal energy as the objects are deformed.

Page 57: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

This KE can be calculated from the equation in Ch 5.

KE = KEf – KEi

KE =1/2mvf2 - 1/2mvi

2

Page 58: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 8: Two clay balls collide head on in a perfectly inelastic collision. The 1st ball with a mass of 0.5 kg and an initial velocity of 4 m/s to the right. The 2nd ball with a mass of 0.25 kg and an initial speed of 3 m/s to the left. a)What’s the final speed of the new ball after the collision? b)What’s the decrease in KE during the collision?

Page 59: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

a)G:m1,i=0.5 kg, v1,i =4 m/s, m2,i =0.25 kg, v2,i=-3 m/s

U: vf = ?E: m1v1 + m2v2=(m1+m2)vf vf, =[m1v1+m2v2]/m1+m2

Page 60: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vf=[(0.5x4)+(0.25x-3)] 0.75

Page 61: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

vf=[(0.5x4)+(0.25x-3)] 0.75

v1+2,f = 1.67 m/s,

to the right

Page 62: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

b)U: KE = ?

E: KE = KEf – KEi We need to find the combined final KE and both initial KE’s. Using the KE = ½ mv2.

Page 63: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

KEi = ½ mv1,i2 +½ mv2,i

2

KEi =½(0.5)(4)2+½(0.25)(-3)2

KEi = 5.12 J

KEf = ½(m1+m2)vf2

KEf = ½(0.5+0.25)(1.67)2

KEf = 1.05J

Page 64: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

S: KE=1.05 J – 5.12 J

S: KE = - 4.07 J

Page 65: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse
Page 66: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Elastic CollisionsA collision in which the total momentum and the total KE

remains constant. Also, the objects separate and

return to their original shapes.

Page 67: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

In the real world, most collisions are neither elastic nor perfectly inelastic.

Page 68: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Total momentum and total KE remain constant through

an elastic collision.

m1v1,I + m2v2,I

= m1v1,f + m2v2,f

Page 69: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

½m1v1,i2 + ½m2v2,i

2

=

½m1v1,f2 + ½m2v2,f

2

Page 70: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

Ex 9: An 0.015 kg marble moving to the right, at 0.225 m/s has an elastic collision with a 0.03 kg moving to

the left at 0.18 m/s. After the collision the smaller marble moves to the left at 0.315 m/s. Disregard friction. A) What is the velocity of

the 0.03 kg marble after the collision? B) Verify answer by confirming KE is conserved.

Page 71: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

G:m1=0.015 kg,m2=0.03 kg

v1,i= 0.225m/s

v2,i = - 0.18 m/s

v1,f= - 0.315m/s

U: v2,f = ?

Page 72: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

E:

m1v1,i + m2v2,i=m1v1,f +m2v2,f

m1v1,i =[m1v1,f+m2v2,f-m2v2,i]

Page 73: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

E:

m1v1,i + m2v2,i=m1v1,f +m2v2,f

m2v2,f =[m1v1,i+m2v2,i-m1v1,f]

v2,f = [m1v1,i + m2v2,i-m1v1,f]

m2

Page 74: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

S: v2,f = [(0.015 x 0.225) + (0.03 x – 0.18) –

(0.015 x – 0.315)] / 0.03

S: v2,f = 0.09 m/s (right)

Page 75: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

KEi = ½m1v1,i2 + ½m2v2,i

2

KEi = ½(0.015)(0.225)2

+ ½(0.03)(-0.18)2

KEi = 0.000866 J

KEf = ½m1v1,f2 + ½m2v2,f

2

Page 76: Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse

KEf = ½m1v1,f2 + ½m2v2,f

2

KEf = ½(0.015)(0.315)2

+ ½(0.03)(0.09)2

KEf = 0.000866 J

Since KEi = KEf,, KE is conserved.