54
IB Physics 11 Mr. Jean December 4 th , 2013

IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Embed Size (px)

Citation preview

Page 1: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

IB Physics 11

Mr. Jean

December 4th, 2013

Page 2: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

The plan:

Page 3: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

– If object 1 loses 75 units of momentum, then object 2 gains 75 units of momentum. Yet, the total momentum of the two objects (object 1 plus object 2) is the same before the collision as it is after the collision. The total momentum of the system (the collection of two objects) is conserved

Page 4: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Law of Conservation of Momentum:

Page 5: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

• Collisions commonly occur in contact sports (such as football) and racket and bat sports (such as baseball, golf, tennis, etc.). Consider a collision in football between a fullback and a linebacker during a goal-line stand. The fullback plunges across the goal line and collides in midair with the linebacker. The linebacker and fullback hold each other and travel together after the collision. The fullback possesses a momentum of 100 kg*m/s, East before the collision and the linebacker possesses a momentum of 120 kg*m/s, West before the collision. The total momentum of the system before the collision is 20 kg*m/s, West (review the section on adding vectors if necessary). Therefore, the total momentum of the system after the collision must also be 20 kg*m/s, West. The fullback and the linebacker move together as a single unit after the collision with a combined momentum of 20 kg*m/s. Momentum is conserved in the collision.

Page 6: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

• Now suppose that a medicine ball is thrown to a clown who is at rest upon the ice; the clown catches the medicine ball and glides together with the ball across the ice. The momentum of the medicine ball is 80 kg*m/s before the collision. The momentum of the clown is 0 m/s before the collision. The total momentum of the system before the collision is 80 kg*m/s. Therefore, the total momentum of the system after the collision must also be 80 kg*m/s. The clown and the medicine ball move together as a single unit after the collision with a combined momentum of 80 kg*m/s. Momentum is conserved in the collision.

Page 7: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

One Dimensional Collisions:

• In a one dimensional collision both the magnitude and the direction of the momentum must be conserved.

• For complex momentum situations break all momentums into components and then sum the components. This too will conserve momentum.

Page 8: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Collisions:

• Collisions can be classified according to the energy interaction that takes place:

• Elastic collision kinetic energy is conserved

• Inelastic collision kinetic energy is not conserved

• Perfectly inelastic collision objects stick together and have the same velocity.

Page 9: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Example:

• An old lady driving a 2.5x103 kg H2 Hummer drives into the back of your 1.0x103 kg Lotus Elan. The two cars stick together. What is their velocity after the collision if the old lady was originally travelling at 8.0m/s?

Page 10: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 11: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Example #2:

• The cue ball collides with the ‘8’ ball. The cue ball has twice as much mass as the ‘8’ ball. The objects do not stay attached. – What is the velocity of the ‘8’ ball?– Is this collision realistic? (Why or why not?)

Page 12: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 13: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Cannon Recoil: • A 2000kg cannon contains a 100kg

armour piercing shell. The cannon fires the projectile horizontally with a velocity of 1000m/s. – What is the velocity of the cannon after the

shot?

Page 14: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

• Before: After:

Page 15: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 16: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

“Loose Cannon”:

• An unpredictable person or thing, liable to cause damage if not kept in check by others.

• Also a place to eat in Halifax on Argyle Street.

Page 17: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Rifle Recoil:

• .50 Cal Rifle

• “Surprising Recoil”

Page 18: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

The momentum before firing is zero. After firing, the net momentum is still zero because the momentum of the cannon is equal and opposite to the momentum of the cannonball.

Conservation of Momentum

Page 19: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

The force on the cannonball inside the cannon barrel is equal and opposite to the force causing the cannon to recoil. The action and reaction forces are internal to the system so they don’t change the momentum of the cannon-cannonball system.

• Before the firing, the momentum is zero.• After the firing, the net momentum is still zero.• Net momentum is neither gained nor lost.

Conservation of Momentum

Page 20: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Momentum has both direction and magnitude. It is a vector quantity.

• The cannonball gains momentum and the recoiling cannon gains momentum in the opposite direction.

• The cannon-cannonball system gains none.• The momenta of the cannonball and the cannon are

equal in magnitude and opposite in direction.• No net force acts on the system so there is no net

impulse on the system and there is no net change in the momentum.

Conservation of Momentum

Page 21: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

In every case, the momentum of a system cannot change unless it is acted on by external forces.

When any quantity in physics does not change, we say it is conserved.

Conservation of Momentum

Page 22: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

The law of conservation of momentum describes the momentum of a system:

If a system undergoes changes wherein all forces are internal, the net momentum of the system before and after the event is the same. Examples are:

• atomic nuclei undergoing radioactive decay,• cars colliding, and• stars exploding.

Conservation of Momentum

Page 23: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

a. A moving ball strikes a ball at rest.

8.5 Collisions

Page 24: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

a. A moving ball strikes a ball at rest.

b. Two moving balls collide head-on.

8.5 Collisions

Page 25: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

a. A moving ball strikes a ball at rest.

b. Two moving balls collide head-on.

c. Two balls moving in the same direction collide.

8.5 Collisions

Page 26: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Inelastic Collisions

A collision in which the colliding objects become distorted and generate heat during the collision is an inelastic collision.

Momentum conservation holds true even in inelastic collisions.

Whenever colliding objects become tangled or couple together, a totally inelastic collision occurs.

8.5 Collisions

Page 27: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

In an inelastic collision between two freight cars, the momentum of the freight car on the left is shared with the freight car on the right.

8.5 Collisions

Page 28: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

The freight cars are of equal mass m, and one car moves at 4 m/s toward the other car that is at rest.

net momentum before collision = net momentum after collision

(net mv)before = (net mv)after

(m)(4 m/s) + (m)(0 m/s) = (2m)(vafter)

8.5 Collisions

Page 29: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Twice as much mass is moving after the collision, so the velocity, vafter, must be one half of 4 m/s.

vafter = 2 m/s in the same direction as the velocity before the

collision, vbefore.

8.5 Collisions

Page 30: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!Consider a 6-kg fish that swims toward and swallows a 2-kg fish that is at rest. If the larger fish swims at 1 m/s, what is its velocity immediately after lunch?

Momentum is conserved from the instant before lunch until the instant after (in so brief an interval, water resistance does not have time to change the momentum).

8.5 Collisions

Page 31: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 32: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!

8.5 Collisions

Page 33: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!Suppose the small fish is not at rest but is swimming toward the large fish at 2 m/s.

8.5 Collisions

Page 34: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!Suppose the small fish is not at rest but is swimming toward the large fish at 2 m/s.

If we consider the direction of the large fish as positive, then the velocity of the small fish is –2 m/s.

8.5 Collisions

Page 35: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!The negative momentum of the small fish slows the large fish.

8.5 Collisions

Page 36: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!If the small fish were swimming at –3 m/s, then both fish would have equal and opposite momenta.

Zero momentum before lunch would equal zero momentum after lunch, and both fish would come to a halt.

8.5 Collisions

Page 37: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

do the math!Suppose the small fish swims at –4 m/s.

The minus sign tells us that after lunch the two-fish system moves in a direction opposite to the large fish’s direction before lunch.

8.5 Collisions

Page 38: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Example of a perfectly Inelastic collision:

Page 39: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 40: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 41: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 42: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Questions to do:

Page 43: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 44: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 45: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 46: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 47: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 48: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 49: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 50: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 51: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 52: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:

Challenge Question:

Page 53: IB Physics 11 Mr. Jean December 4 th, 2013. The plan:
Page 54: IB Physics 11 Mr. Jean December 4 th, 2013. The plan: