collisions © d hoult 2010. elastic collisions © d hoult 2010

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Page 1: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Collisions

© D Hoult 2010

Page 2: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Elastic Collisions

© D Hoult 2010

Page 3: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Elastic Collisions

1 dimensional collision

© D Hoult 2010

Page 4: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Elastic Collisions

1 dimensional collision: bodies of equal mass

© D Hoult 2010

Page 5: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Elastic Collisions

1 dimensional collision: bodies of equal mass

(one body initially stationary)

© D Hoult 2010

Page 6: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Elastic Collisions

1 dimensional collision: bodies of equal mass

(one body initially stationary)

© D Hoult 2010

Page 7: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

© D Hoult 2010

Page 8: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Before collision, the total momentum is equal to the momentum of body A

A B

uA

© D Hoult 2010

Page 9: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

After collision, the total momentum is equal to the momentum of body B

A B

vB

© D Hoult 2010

Page 10: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies)

© D Hoult 2010

Page 11: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies)

mAuA = mBvB

© D Hoult 2010

Page 12: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies)

mAuA = mBvB

so, if the masses are equal the velocity of B after

© D Hoult 2010

Page 13: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies)

mAuA = mBvB

so, if the masses are equal the velocity of B after is equal to the velocity of A before

© D Hoult 2010

Page 14: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Bodies of different mass

© D Hoult 2010

Page 15: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

© D Hoult 2010

Page 16: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

uA

© D Hoult 2010

Page 17: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

uA

Before the collision, the total momentum is equal to the momentum of body A

© D Hoult 2010

Page 18: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

vA vB

© D Hoult 2010

Page 19: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

vA vB

After the collision, the total momentum is the sum of the momenta of body A and body B

© D Hoult 2010

Page 20: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

vA vB

If we want to calculate the velocities, vA and vB we will use the

© D Hoult 2010

Page 21: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

vA vB

If we want to calculate the velocities, vA and vB we will use the principle of conservation of momentum

© D Hoult 2010

Page 22: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 23: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAuA = mAvA + mBvB

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 24: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAuA = mAvA + mBvB

If the collision is elastic then

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 25: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAuA = mAvA + mBvB

If the collision is elastic then kinetic energy is also conserved

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 26: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAuA = mAvA + mBvB

If the collision is elastic then kinetic energy is also conserved

½ mAuA2 = ½ mAvA

2 + ½ mBvB

2

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 27: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAuA = mAvA + mBvB

If the collision is elastic then kinetic energy is also conserved

mAuA2 = mAvA

2 + mBvB

2

½ mAuA2 = ½ mAvA

2 + ½ mBvB

2

The principle of conservation of momentum can be stated here as

© D Hoult 2010

Page 28: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

From these two equations, vA and vB can be found

mAuA = mAvA + mBvB

mAuA2 = mAvA

2 + mBvB

2

© D Hoult 2010

Page 29: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

From these two equations, vA and vB can be found

mAuA = mAvA + mBvB

mAuA2 = mAvA

2 + mBvB

2

BUT

© D Hoult 2010

Page 30: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

© D Hoult 2010

Page 31: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

* a very useful phrase !© D Hoult 2010

Page 32: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

In this case, the velocity of A relative to B, before the collision is equal to

uA

© D Hoult 2010

Page 33: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

In this case, the velocity of A relative to B, before the collision is equal to uA

uA

© D Hoult 2010

Page 34: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

and the velocity of B relative to A after the collision is equal to

vA vB

© D Hoult 2010

Page 35: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

and the velocity of B relative to A after the collision is equal to vB – vA

vA vB

© D Hoult 2010

Page 36: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision

for proof click here

and the velocity of B relative to A after the collision is equal to vB – vA

vA vB

© D Hoult 2010

Page 37: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision

equation 1

© D Hoult 2010

Page 38: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision

equation 1

equation 2

mAuA = mAvA + mBvB

© D Hoult 2010

Page 39: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision

equation 1

equation 2

mAuA = mAvA + mBvB

uA = vB – vA

© D Hoult 2010

Page 40: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

© D Hoult 2010

Page 41: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

© D Hoult 2010

Page 42: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

uA

© D Hoult 2010

Page 43: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Before the collision, the total momentum is equal to the momentum of body A

A B

uA

© D Hoult 2010

Page 44: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

After the collision, the total momentum is the sum of the momenta of body A and body B

A B

vA vB

© D Hoult 2010

Page 45: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Using the principle of conservation of momentum

© D Hoult 2010

Page 46: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Using the principle of conservation of momentum

mAuA = mAvA + mBvB

© D Hoult 2010

Page 47: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Using the principle of conservation of momentum

mAuA = mAvA + mBvB

A B

vA vB

© D Hoult 2010

Page 48: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Using the principle of conservation of momentum

mAuA = mAvA + mBvB

A B

vA vB

© D Hoult 2010

Page 49: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Using the principle of conservation of momentum

mAuA = mAvA + mBvB

A B

vA vB

One of the momenta after collision will be a negative quantity

© D Hoult 2010

Page 50: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision

© D Hoult 2010

Page 51: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision

© D Hoult 2010

Page 52: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

© D Hoult 2010

Page 53: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

© D Hoult 2010

Page 54: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

A B

Before the collision, the total momentum is equal to the momentum of body A

© D Hoult 2010

Page 55: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

© D Hoult 2010

Page 56: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

After the collision, the total momentum is equal to the sum of the momenta of both bodies© D Hoult 2010

Page 57: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

Now the sum must be a vector sum

© D Hoult 2010

Page 58: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mAvA

© D Hoult 2010

Page 59: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

© D Hoult 2010

Page 60: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

© D Hoult 2010

Page 61: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

© D Hoult 2010

Page 62: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

© D Hoult 2010

Page 63: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

p

mBvB

mAvA

© D Hoult 2010

Page 64: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

p

mAuA

© D Hoult 2010

Page 65: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

p

mAuA

© D Hoult 2010

Page 66: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

mBvB

mAvA

p

mAuA

© D Hoult 2010

Page 67: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

p = mAuA

mBvB

mAvA

p

mAuA

© D Hoult 2010

Page 68: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision: Example

Body A has initial speed uA = 50 ms-1

© D Hoult 2010

Page 69: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision: Example

Body A has initial speed uA = 50 ms-1

Body B is initially stationary

© D Hoult 2010

Page 70: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision: Example

Body A has initial speed uA = 50 ms-1

Body B is initially stationary

Mass of A = mass of B = 2 kg

© D Hoult 2010

Page 71: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision: Example

Body A has initial speed uA = 50 ms-1

Body B is initially stationary

Mass of A = mass of B = 2 kg

After the collision, body A is found to be moving at speed vA = 25 ms-1 in a direction at 60° to its original direction of motion

© D Hoult 2010

Page 72: Collisions © D Hoult 2010. Elastic Collisions © D Hoult 2010

2 dimensional collision: Example

Body A has initial speed uA = 50 ms-1

Body B is initially stationary

Mass of A = mass of B = 2 kg

After the collision, body A is found to be moving at speed vA = 25 ms-1 in a direction at 60° to its original direction of motion

Find the kinetic energy possessed by body B after the collision

© D Hoult 2010