76
Linear Momentum Vectors again

Linear Momentum

  • Upload
    jerom

  • View
    27

  • Download
    0

Embed Size (px)

DESCRIPTION

Linear Momentum. Vectors again. Review. Equations for Motion Along One Dimension. Review. Motion Equations for Constant Acceleration. 1. 2. 3. 4. Review. 3 Laws of Motion If in Equilibrium If not in equilibrium Change in Motion is Due to Force Force causes a change in acceleration. - PowerPoint PPT Presentation

Citation preview

Page 1: Linear Momentum

Linear MomentumVectors again

Page 2: Linear Momentum

Review Equations for Motion Along One Dimension

dtdx

txv

txv

t

ave

0lim

dtdv

tva

tva

t

ave

0lim

Page 3: Linear Momentum

Review Motion Equations for Constant Acceleration

•1.

•2.

•3.

•4.

atvv 0

221

00 attvxx

20vvvave

xavv 220

2

Page 4: Linear Momentum

Review 3 Laws of Motion If in Equilibrium

If not in equilibrium Change in Motion is Due to Force

Force causes a change in acceleration

0F

maF

Page 5: Linear Momentum

Work

Energy

Review

UWFddFW

KWW

grav

Total

cos

2

2

21

21

kxU

mgyU

mvK

spring

grav

Page 6: Linear Momentum

Law of conservation of energy

Power

efficiency

Review

NCspringgravspringgrav WUUKUUK 000

aveave FvtWP

in

out

PPe

Page 7: Linear Momentum

If an 18 wheeler hits a car, what direction will the wreckage move?

What is the force between the 18 wheeler and the car?

Collisions

Page 8: Linear Momentum

Forces

dtvdmF

dtvdmF

amF

Page 9: Linear Momentum

Newtons 2nd law

Linear momentum

SI

Newton defined it as quantity of motion

Momentum

vmp

sNsmkg

dtpdF

Page 10: Linear Momentum

When an object collides with another, the forces on the object will momentarily spike before returning back to zero.

Impulse

Page 11: Linear Momentum

Impulse

pJ

ptFtpF

dtpdF

Page 12: Linear Momentum

We now define impulse, J, as the change in momentum of a particle during a time interval

SI unit

ImpulsepJ

tFpJ

tFpJ

aveyyy

avexxx

sNsmkg

Page 13: Linear Momentum

A ball with a mass of 0.40 kg is thrown against a brick wall. It hits the wall moving horizontally to the left at 30 m/s and rebounds horizontally to the right at 20 m/s. (a) find the impulse of the net force on the ball during the collision with the wall. (b) If the ball is in contact with the wall for 0.010s, find the average horizontal force that the wall exerts on the ball during impact.

Example

Page 14: Linear Momentum

Example

NtJF

tFJ

sNJ

vvmJ

vmvmJ

pJ

ave

ave

2000010.020

20

))30(20(4.0)( 0

0

Page 15: Linear Momentum

If a particle A hits particle B

Conservation of Momentum

dtpdF

dtpdF

dtpdF

ABonA

BAonB

Page 16: Linear Momentum

If there are no external forces acting on the system

Conservation of Momentum

0

0

dtpd

dtpdFF

F

ABBonAAonB

Page 17: Linear Momentum

Change in momentum over time is zero

The sum of momentums is constant

Conservation of Momentum

0)(

dtppd

dtpd

dtpd BAAB

constpp BA

Page 18: Linear Momentum

If there are no external forces acting on a system, Total Momentum of a system conserved

Conservation of Momentum

constpp BA

BABA pppp 00

pp 0

Page 19: Linear Momentum

Vector Addition

yx AAA cosAAx sinAAy

Page 20: Linear Momentum

A marksman holds a rifle of mass 3.00 kg loosely such that it’ll recoil freely. He fires a bullet of mass 5.00g horizontally with velocity relative to the ground of 300 m/s. What is the recoil velocity of the rifle?

Example - Recoil

Page 21: Linear Momentum

Example - Recoil

sm

R

sm

RRRR

sm

BBB

RBx

vvvmp

vmpppp

5.05.1)3(15)300)(05.0(

0

Page 22: Linear Momentum

Two battling robots are on a frictionless surface. Robot A with mass 20 kg moves at 2.0 m/s parallel to the x axis. It collides with robot B, which has a mass of 12 kg. After the collision, robot A is moving at 1.0 m/s in a direction that makes an angle α=30o. What is the final velocity of robot B?

Example – 2D example

Page 23: Linear Momentum

Example

sm

Bx

Bx

B

AxAAxABx

BxBAxAAxA

BxBAxAAxA

BxAxBxAx

xx

v

v

mvmvmv

vmvmvmvmvmvmpppp

pp

89.112

30cos)1)(20()2(20

0

0

0

00

0

Page 24: Linear Momentum

Example

sm

By

By

B

AyABy

ByBAyA

ByBAyA

ByAyByAy

yy

v

v

mvm

v

vmvm

vmvm

pppp

pp

83.012

30sin)1)(20(

000

0

Page 25: Linear Momentum

Example

2489.183.0arctan

1.2

83.089.1

22

sm

B

ByBxB

sm

By

sm

Bx

v

vvv

vv

Page 26: Linear Momentum

Elastic Collisions – Collisions where the kinetic energies are conserved. When the particles are in contact, the energy is momentarily converted to elastic potential energy.

Conservation of Momentum and Energy

Page 27: Linear Momentum

Inelastic Collisions – collisions where total kinetic energy after the collision is less than before the collision.

Completely Inelastic Collisions- When the two particles stick together after a collision.

Collisions can be partly inellastic

Conservation of Momentum and Energy

Page 28: Linear Momentum

Collisions where two objects will impact each other, but the objects stick together and move as one after the collision.

Completely Inelastic Collisions

Page 29: Linear Momentum

Momentum is still conserved Find v in terms of v0

Completely Inelastic Collisions

vmvmvmvmvvv

vmvmvmvmpppp

pp

BABBAA

BA

BBAABBAA

BABA

00

00

00

0

Page 30: Linear Momentum

Assume Particle B is initially at rest

Completely Inelastic Collisions

BA

AA

BAAA

BABBAA

mmvmv

vmvmvmvmvmvmvm

0

0

00

Page 31: Linear Momentum

Kinetic Energy

Completely Inelastic Collisions

BA

A

BA

AA

BA

AABABA

AA

mmm

KK

mmvmK

mmvmmmvmmK

vmK

0

20

2

02

200

)(21

)(21)(

21

21

If B is at rest

Page 32: Linear Momentum

At the intersection, a yellow subcompact car with mass travelling 950 kg east collides with a red pick up truck with mass 1900 kg travelling north. The two vehicles stick together and the wreckage travels 16.0 m/s 24o E of N. Calculate the speed of each of the vehicles. Assume frictionless.

Examples – Young and Freedman 8.37

Page 33: Linear Momentum

Young and Freedman 8.37

B

yBAyB

A

xBAxA

y

x

yByAyBB

xBxAxAA

BABBAA

mvmm

v

mvmmv

vvvv

vmvmvmvmvmvm

vmvmvmvm

)(

)(

24cos24sin

0

0

0

0

00

Page 34: Linear Momentum

Young and Freedman 8.37

sm

B

yBAyB

sm

A

xBAxA

y

x

mvmm

v

mvmmv

vvvv

9.21)(

5.19)(

6.1424cos1624cos51.624sin1624sin

0

0

Page 35: Linear Momentum

The ballistic pendulum is an apparatus to measure the speed of a fast moving projectile, such as a bullet. A bullet of mass 12g with velocity 380 m/s is fired into a large wooden block of mass 6.0 kg suspended by a chord of 70cm. (a) Find the height the block rises (b) the initial kinetic energy of the bullet (c) The kinetic energy of the bullet and block.

Problem – Ballistic Pendulum

Page 36: Linear Momentum

Velocity after impact

Kinetic energy after impact

Problem – Ballistic Pendulum

BA

AA

BAAA

BABBAA

mmvmv

vmvmvmvmvmvmvm

0

0

00

Jmm

vmKBA

AA 73.1)(2

1 20

Page 37: Linear Momentum

Kinetic energy after impact

Converted to potential at highest point

Problem – Ballistic Pendulum

)(2

1 20

BA

AA

mmvmK

gymmmm

vm

gymmUmm

vmK

BABA

AA

BA

BA

AA

)()(2

1

)()(2

1

20

20

Page 38: Linear Momentum

Problem – Ballistic Pendulum

my

y

mmvm

gy

gymmmm

vm

BA

AA

BABA

AA

0293.0)012.6)(8.9(2))380(012.0(

)(21

)()(2

1

2

2

2

20

20

JK

K

mvK

Bullet

Bullet

BBullet

866

)380(012.02121

2

2

Page 39: Linear Momentum

Momentum and Energy are conserved Find v in terms of v0

Elastic Collisions

BBAABBAA

BABA

vmvmvmvmpppp

pp

00

00

0

2220

20

00

0

21

21

21

21

BBAABBAA

BABA

vmvmvmvm

KKKKKK

Page 40: Linear Momentum

If particle B is at rest

Elastic Collisions – One Dimension

BBAAAA

BABA

vmvmvmpppp

pp

0

00

0

2220

00

0

21

21

21

BBAAAA

BABA

vmvmvm

KKKKKK

Page 41: Linear Momentum

If particle B is at rest

Elastic Collisions – One Dimension

BBAAA

BBAAAA

BBAAAA

vmvvmvmvmvmvmvmvm

)( 0

0

0

2220

2220

2220

)(21

21

21

21

21

21

BBAAA

BBAAAA

BBAAAA

vmvvm

vmvmvm

vmvmvm

Page 42: Linear Momentum

If particle B is at rest

Substitute back

Elastic Collisions – One Dimension

BAA

BBAAA

BBAAA

vvvvmvvm

vmvvm

0

2220

0

)(

)(

)()(

)()(

)()(

0

0

00

00

00

BA

ABAA

ABAABA

ABAAABAA

ABABAAAA

AABAAA

mmvmmv

vmmvmmvmvmvmvmvmvmvmvm

vvmvvm

Page 43: Linear Momentum

If particle B is at rest

Elastic Collisions – One Dimension

)(2

)()(

)()(

0

00

0

0

BA

AAB

BBA

ABAA

BAA

BA

ABAA

mmvmv

vmmvmmv

vvvmmvmmv

Page 44: Linear Momentum

If ma <<< mb

really small

Elastic Collisions – One Dimension

)(2

)()(

0

0

BA

AAB

BA

ABAA

mmvmv

mmvmmv

B

AA

BA

AAB

AB

ABA

mvm

mmvmv

vmvmv

00

00

2)(

2

Page 45: Linear Momentum

If ma>>>mb

If ma=mb

Elastic Collisions – One Dimension

00

00

22A

A

AAB

AA

AAA

vmvmv

vmvmv

00

0

22

0)(

)0(

AA

AAB

BA

AA

vmvmv

mmvv

Page 46: Linear Momentum

In a game of billiards a player wishes to sink a target ball in the cornet pocket. If the angle to the corner pocket is 35o, at what angle is the cue ball deflected? (Assume frictionless)

Example

Page 47: Linear Momentum

Mass is the same

Example

2220

20

00

BBAABBAA

BBAABBAA

vmvmvmvm

vmvmvmvm

2220

0

BAA

BAA

vvv

vvv

Page 48: Linear Momentum

Example

553590

0coscos20

202

)()(222

0

20

0020

2220

0

BA

BA

BBAAA

BABAA

AAA

BAA

BAA

vvvv

vvvvv

vvvvv

vvv

vvv

vvv

Page 49: Linear Momentum

Two particles with masses m and 3m are moving towards each other along the x axis with the same initial speeds. Particle m is travelling towards the left and particle 3m is travelling towards the right. They undergo an elastic glancing collision such that particle m is moving downward after the collision at right angles from initial direction. (a) Find the final speeds of the two particles. (b) What is the angle θ at which particle 3m is scattered.

Problem – Serway 9-36

Page 50: Linear Momentum

Elastic Collisions and relative velocity – One Dimensional

ABBA

BBAA

BBBAAA

BBBBAAAA

BBBAAA

BBBBAAAA

BBAABBAA

BBAABBAA

vvvvvvvv

vvmvvm

vmvmvmvm

vvmvvmvmvmvmvmvmvmvmvm

vmvmvmvm

00

00

20

2220

20

2220

00

00

2220

20

00

)()(

)()(

Page 51: Linear Momentum

In an elastic Collision, the relative velocities of the two objects have the same magnitude

Elastic Collisions and relative velocity

ABAB

ABEAEB

EAEBEAEB

EAEBEBEA

ABBA

vv

vvv

vvvv

vvvvvvvv

|0|0

|||

|||0|0

|||0|0

00

)(

Page 52: Linear Momentum

A 0.150 kg glider (puck on an air hockey table) is moving to the right with a speed of 0.80 m/s. It has a head-on collision with a 0.300 kg glider that is moving to the left with velocity 2.20 m/s. Find the final velocities of the two gliders. Assume elastic collision.

Young and Freedman 8.42

Page 53: Linear Momentum

A bat strikes a 0.145kg baseball. Just before impact the ball is travelling horizontally to the right at 50.0 m/s and it leaves the bat travelling to the left at an angle of 30o above the horizontal with a speed of 65.0 m/s. Find the horizontal and vertical components of the average force on the ball if the ball and bat were in contact for 1.75 ms.

Problems- Young and Freedman 8.12

Page 54: Linear Momentum

A 23 g bullet travelling at 230 m/s penetrates a 2.0kg block of wood and emerges cleanly at 170 m/s. If the wood is initially stationary on a frictionless surface, how fast does it move after the bullet emerges?

Giancoli 7-12

Page 55: Linear Momentum

A 90.0 kg full back running east with a speed 5.0 m/s is tackled by a 95.0kg opponent running north at 3.00 m/s. If the collision is completely inelastic, (a) find the velocity of the players just after the tackle. (b) find the mechanical energy lost during the collision.

Serway 9.28

Page 56: Linear Momentum

Giancoli 7-78 A 0.25kg skeet (clay target) is fired at an

angle of 30o to the horizon with a speed of 25 m/s. When it reaches its maximum height, it is hit from below by a 15g pellet traveling vertically upwards at 200 m/s. The pellet is embedded into the skeet. (a) how much higher does the skeet go up? (b) how much further does the skeet travel?

Prepare for pain

Page 57: Linear Momentum

Objects approximated to be point particles Objects only undergo translational motion

Assumptions so far

Page 58: Linear Momentum

Real objects also undergo rotational motion while undergoing translational motion.

But there is one point which will move as if subjected to the same net force.

We can treat the object as if all its mass was concentrated on a single point

Center of Mass

Page 59: Linear Momentum

Set an arbitrary origin point

Center of mass is the mass weighted average of the particles

Center of Mass

i

iicm m

mrmmmmrmrmrr......

321

332211

Page 60: Linear Momentum

A simplified water molecule is shown. The separation between the H and O atoms is d=9.57 x10-11m. Each hydrogen atom has a mass of 1.0 u and the oxygen atom has a mass of 16.0 u. Find the position of the center of mass.

Example

Page 61: Linear Momentum

For ease set origin to one of the particles

Example

ohh

ohh

i

iicm

ohh

ohh

i

iicm

i

iicm

mmmmdmdm

mmy

y

mmmmdmdm

mmx

x

mmr

mmmmrmrmrr

)0()5.52sin()5.52sin(

)0()5.52cos()5.52cos(

......

321

332211

Page 62: Linear Momentum

Example

0)0()5.52sin()5.52sin(

105.6)5.52cos(2 12

ohh

ohh

i

iicm

ohh

h

i

iicm

mmmmdmdm

mmy

y

mxmmm

dmmmx

x

Page 63: Linear Momentum

1) if there is an axis of symmetry, the center of mass will lie along the axis.

2) the center of mass can be outside of the body

Center of Mass

Page 64: Linear Momentum

The point of an object which gravity can be thought to act.

This is conceptually different from center of mass

For now the center of gravity of an object is also it’s center of mass.

Center of Gravity

Page 65: Linear Momentum

Motion of Center of Mass

Page 66: Linear Momentum

Motion of Center of Mass

pmvmv

mmv

mmmmvmvmvv

dtmrmrmrd

mmmdtrd

mmmmrmrmr

dtd

dtrd

mmr

mmmmrmrmrr

iiicm

i

iicm

cm

cm

i

iicm

......

...)(...

1

......

......

321

332211

332211

321

321

332211

321

332211

Page 67: Linear Momentum

External Forces and Center of Mass

cmiext

ernalexternal

iicmi

i

iicm

cm

cm

amF

FFF

Fmaam

mma

mmmmamamaa

mmmmvmvmv

dtd

dtvd

mmmmvmvmvv

)(

)(

......

......

......

int

321

332211

321

332211

321

332211

Page 68: Linear Momentum
Page 69: Linear Momentum
Page 70: Linear Momentum
Page 71: Linear Momentum

Center of mass computations useful for when mass of a system changes with time

Rockets

Page 72: Linear Momentum

Orbits

Page 73: Linear Momentum

James and Ramon are standing 20.0 m apart on a frozen pond. Ramon has a mass of 60.0 kg and James has mass of 90.0 kg. Midway between the two is a mug of their favourite beverage. They pull on the ends of a light rope. When James has moved 6.0 m how far has Ramon moved?

Example

Page 74: Linear Momentum

No external forces! Center of Mass will not move!

mr

mmr

r

cm

i

iicm

2150300

6090)60(10)90(10

Page 75: Linear Momentum

Center of Mass will not move! James moved 6m to the right

mrx

mxmmr

r

cm

i

iicm

160

)90(4)6090(

26090

)60()90(4

Page 76: Linear Momentum

A 1200 kg station wagon is moving along a straight highway at 12.0 m/s. Another car with mass 1800kg and speed 20.0 m/s has its center of mass 40.0 m away. (a) Find the position of the center of mass of the two cars. (b) Find magnitude of total momentum of the system. (c) Find the speed of the center of mass of the system. (d) Find total momentum using center of mass.

Problem – Young and Freedman 8.50