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Linear momentum and its conservation Impulse and momentum Collisions Two-dimensional collisions Center of mass Systems of particles. Momentum and collisions (chapter eight)

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Page 1: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Linear momentum and its conservation

Impulse and momentum Collisions Two-dimensional collisions Center of mass Systems of particles.

Momentum and collisions (chapter eight)

Page 2: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Linear Momentum

Linear momentum is defined as the mass times the velocity of an object:

This is a vector equation - in terms of the Cartesian coordinates:

vmp

zz

yy

xx

mvp

mvp

mvp

Page 3: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Linear momentumThe time rate of change of momentum of a

particle equals the net force acting on it

amdt

vdm

dt

pdF

Page 4: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Momentum conservationConsider an isolated system of two-particles,

interacting with each other.The force on object 1 exerted by object 2 is

The reaction force to this is the force on 2 by 1

Since these make up an action-reaction pair

ConcepTest

dt

pdF 1

21

dt

pdF 2

12

02121

1221 ppdt

d

dt

pd

dt

pdFF

Page 5: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Momentum conservation

The result is a basic statement of the law of conservation of the total momentum for an isolated system.

We can use this result to solve many types of collision and interaction problems in which we can choose the system to include two (or more) interacting objects.

Momentum is a vector, so its conservation holds separately for each component

Page 6: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum
Page 7: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum
Page 8: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum
Page 9: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum
Page 10: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Examples

Two carts (masses m1 and m2) are held together at rest on a frictionless cart with a spring between them. When released, what are their velocities?

Before m1 m2

After

1v

2v

02211 iii vmvmp

ff

fff

vm

mv

vmvmp

12

12

2211 0

Page 11: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Conservation of momentum

Examples Demo ConcepTest

Page 12: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Impulse and momentum

The change in momentum of an object during a collision is caused by a net force. Integrating the differential for the momentum:

This quantity (the net force integrated over time) is called impulse, and results in another statement of Newton:s 2nd law: The total impulse of the net force equals the change in momentum of the particle.

IdtFpdpf

i

f

i

t

t

t

t

Page 13: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Impulse approximation

The time average of the force is defined as

f

i

t

t

dtFt

F 1

So the impulse momentum theorem can be written

tFpI

In the impulse approximation, we assume one of the forces acting on the object is much larger than the others, but acts only for a small interval.

Page 14: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Collisions

Use the impulse approximation - forces of collisions much larger, shorter duration than other forces on objects.

Two extremes of collisions:

Elastic - kinetic energy conserved (e.g. billiard balls)

Perfectly inelastic - object stick together (maximum KE loss)

Momentum is conserved in both

Page 15: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Collisions, cont.

One dimensional elastic

222

211

222

211

22112211

2

1

2

1

2

1

2

1ffii

ffii

vmvmvmvm

vmvmvmvm

Momentum conservation

Energy conservation

After lots of algebra

iif

iif

vmm

mmv

mm

mv

vmm

mv

mm

mmv

221

121

21

12

221

21

21

211

2

2

Page 16: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

2-d Collisions

Momentum conservation – vector equation – holds for each component

For elastic collisions – conservation of kinetic energy (magnitude of the velocity)

Example

Page 17: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Center of mass

= the average position of a system’s mass

in the case of discrete point objects

for an extended object

ii

iii

CM m

rmr

dmr

Mdm

dmrrCM

1

Page 18: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

The white part if your fingernail is called the lunia. No U.S. President has had brown eyes. In the year 2160, there will be two lunar eclipses and

five solar eclipses. Benjamin Franklin invented the rocking chair. 3 out of 4 people make up 75% of the population.

Page 19: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Motion of a system of particles

CMi

itot

iii

i

ii

CMCM

vMpp

vmMdt

rdm

Mdt

rdv

11

= the velocity of the center of mass of a system of particles is just

in other words, the total momentum is just the total mass times the velocity of the center of mass. The acceleration of the COM is

CMi

i

iii

i

ii

CMCM

aMF

amMdt

vdm

Mdt

vda

11

Page 20: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

Motion of a system of particlesThe forces Fi has terms that are internal and external, but the internal forces sum to zero by Newton’s 3rd law

dt

pdaMFF totCM

iiext

So the system moves like a particle of mass M located at the COM.

If the net external force is zero, the total momentum of the system is conserved

Page 21: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

The hardness of butter is directly proportional to the softness of the bread.

To steal ideas from one person is plagiarism; to steal from many is research.

For every action there is an equal and opposite criticism.

If the speed of light is 186,000 miles/sec., what's the speed of darkness?

The sooner you fall behind the more time you'll have to catch up.

Page 22: _ Linear momentum and its conservation _ Impulse and momentum _ Collisions _ Two-dimensional collisions _ Center of mass _ Systems of particles. Momentum

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