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Momentum Momentum – Key Ideas – Key Ideas

Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement x, the product F x x = (Fcos ) x = Work

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Page 1: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

MomentumMomentum – Key Ideas– Key Ideas

Page 2: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Review – If a force Fx is applied to abody over a displacement x, theproduct Fx x = (Fcos)x = Work

Page 3: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Review – If a force Fx is applied to abody over a displacement x, theproduct Fx x = (Fcos)x = Work

If the friction force is less than Fx, the work increases the object’s Kinetic Energy

2 2o

1 12 2netW KE m m

Page 4: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

NOW ask: What is the effect of applyinga force over a time interval?

Vocabulary: events in which objects apply forces to each other are called

INTERACTIONS

Page 5: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

NOW ask: What is the effect of applyinga force over a time interval?

Vocabulary: events in which objects apply forces to each other are called

INTERACTIONS

You predicted the outcomes of someinteractions..

How did you do?

Page 6: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

You predicted the outcomes of someinteractions..

How did you do?

A general rule about interaction forces:

Page 7: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

A general rule about interaction forces:

Forces come in

12 21F F

Page 8: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

A general rule about interaction forces:

Forces come in

12 21F F

This is Newton’s 3rd Law.

Page 9: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

The product of mass and velocity

(a quantity) is called

(symbol: )

ve

Definition

t

c or

:

moment p

m

um

p

Page 10: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Newton's second law (one force):

Rearrange:

F ma mt

F t m

Impulse = Change of momentum

Page 11: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Newton's second law (one force):

Rearrange:

F ma mt

F t m

Impulse = Change of momentum

Newton meter (N mUni ) = kg m st:

Page 12: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

The impulse is the area under the force vs. time curve. The average force gives the same impulse to the object in the time interval Δt as the real time-varying force.

Page 13: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Conservation of Momentum

The principle of conservation of momentum states when no external forces act on a system consisting of two objects that collide with each other, the total momentum of the system remains constant in time.

Specifically, the total momentum before the collision will equal the total momentum after the collision.

Page 14: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Conservation of Momentum

Mathematically: 1 2 2 1 2 2f fm m m m

Momentum is conserved for the system of objects.The system includes all the objects interacting with each other.Assumes only internal forces are acting during the collision.Can be generalized to any number of objects.

Page 15: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Force as a function of time for the two colliding particles.

Page 16: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

In all collisions, total momentum is conserved.

We consider two types of collisions in one dimension:

1. Totally elastic

2. Totally inelastic

Page 17: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Perfectly Inelastic Collisions

When two objects stick together after the collision, they have undergone a perfectly inelastic collision.

Conservation of momentum becomes

1 2 22

1 2 1 2

1 2 12

1 2 2 1 2 2

1 2

1

2 1 2 2

2 1 2

Final vel

1 1 1 1

2 2 2 2

2

2

ocities:

f f

f f

f i

f i

m m m m

m m m

m m m m

m m m

m m

m m m m

m m

1 2 2 1 2i i fm m m m

Page 18: Momentum – Key Ideas. Review – If a force F x is applied to a body over a displacement  x, the product F x  x = (Fcos  )  x = Work

Elastic Collisions

Both momentum and kinetic energy are conserved.

1 2 22

1 2 1 2

1 2 12

1 2 2 1 2 2

1 2

1

2 1 2 2

2 1 2

Final vel

1 1 1 1

2 2 2 2

2

2

ocities:

f f

f f

f i

f i

m m m m

m m m

m m m m

m m m

m m

m m m m

m m