8. cons of p (1-d)

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    UNIT 1: CONSERVATION LAWS

    Lesson 8:

    Conservation of Momentum (1-D)

    CENTRE HIGH: PHYSICS 30

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    Recommended Reading:

    Heath pp. 244 - 248

    Ladner pp. 43 - 44

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    Momentum is conserved for collisions and explosions

    Collisions:

    STICK!

    Explosions:

    BOOM!

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    F. Law of Conservation of Momentum

    1 2

    When two objects collide:

    3rd Law: They exert equal and opposite forces

    for the same period of time

    So,

    Fon 1 = - Fon 2

    Fon 1 t = - Fon 2 t

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    Fon 1 = - Fon 2

    Fon 1 t = - Fon 2 t

    Based on the equation F t = m v, it follows

    m v1 = - m v2

    p1

    = - p2

    or

    p1 + p2 = 0

    No overall change in momentum

    (conserved)

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    F1. Conservation of Momentum (1-D)

    For collisions and explosions, there are two equations:

    1. Total Momentum is conserved (constant)

    pT = pT '

    - the total momentum before the collision

    is the same as the total momentum after the collision

    - this is also true for explosions

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    F1. Conservation of Momentum (1-D)

    For collisions and explosions, there are two equations:

    1. Total Momentum is conserved (constant)

    pT = pT '

    These are vector sums

    Need a reference direction

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    2. No overall change in momentum

    p1 + p2 = 0

    or

    p1 = - p2

    Equal but opposite impulses

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    Conditions for momentum to be conserved :

    1. A closed system

    - no objects lost / gained

    2. Fnet = 0 on the whole system

    - the objects must move at a constant velocity

    before and after the collision

    e.g.

    No friction

    Level surface

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    Consider a collision:

    10 kgm/s 6 kgm/s 3 kgm/s p?

    Boom!

    What is the total momentum before the collision?

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    Ref: Right is positive

    10 kgm/s -6 kgm/s -3 kgm/s p?

    Boom!

    Remember, for 1-D vectors,

    you must determine a positive direction (i.e. a ref system)

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    10 kgm/s -6 kgm/s -3 kgm/s p?

    Boom!

    pT = 10 - 6 = 4 kgm/s

    What is the total momentum after the collision?

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    10 kgm/s -6 kgm/s -3 kgm/s p?

    Boom!

    pT = 10 - 6 = 4 kgm/s pT ' = 4 kgm/s

    pT = pT ' = 4 kg m/s

    Total momentum remains constant throughout the collision!

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    10 kgm/s -6 kgm/s -3 kgm/s

    Boom!

    pT = 10 - 6 = 4 kgm/s pT ' = 4 kgm/s

    So, what is the momentum of the blue object after the collision?

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    10 kgm/s -6 kgm/s -3 kgm/s 7 kgm/s

    Boom!

    pT = 10 - 6 = 4 kgm/s pT ' = 4 kgm/s

    So, p = +7 kgm/s

    The momentum of the two objects must add up to 4 kgm/s

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    10 kgm/s -6 kgm/s -3 kgm/s 7 kgm/s

    Boom!

    Calculate the change in momentum for object 1 and 2

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    10 kgm/s -6 kgm/s -3 kgm/s 7 kgm/s

    Boom!

    Also,

    p1 = p1 ' - p1 = (-3 kgm/s) - (10 kgm/s)

    = -13 kgm/s

    p2 = p2 ' - p2 = (7 kgm/s) - (-6 kgm/s)

    = +13 kgm/s

    Equal but opposite impulses (no overall change)

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    Animation:

    Air Track collisionshttp://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassM

    echanics/AirTrack/AirTrack.html

    Attempt to predict the answers before you run the animation- use the equations to calculate

    Be aware that an inelastic collision is when they stick

    together

    http://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.htmlhttp://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.htmlhttp://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.htmlhttp://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.html
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    Ex. 1 A 12.5 kg object, moving East at 4.0 m/s, collides with

    a 13.0 kg object moving West at 7.0 m/s. If they stick

    together (an inelastic collision), then the magnitude oftheir velocity is _________ m/s.

    Your 2-digit answer is

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    Solution:

    4.0 m/s 7.0 m/s v ?

    Stick!12.5 kg 13.0 kg 25.5 kg

    Draw a picture first.

    Show clearly before and after the collision.

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    Solution:

    +4.0 m/s -7.0 m/s v ?

    Stick!12.5 kg 13.0 kg 25.5 kg

    Ref: East is +

    pT = pT'

    p1 + p2 = pT'

    m1 v1 + m2 v2 = mT v

    The two masses combine

    Treat as one (total) mass

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    m1 v1 + m2 v2 = mT v

    (12.5 (4.0) + (13.0) (-7.0) = 25.5 v

    -41 = 25.5 v

    v = -1.6 m/s

    So, v = 1.6 m/s West

    Numerical Response:

    1 . 6

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    Ex. 2 A 750 kg car is moving East and collides with a 580 kg car

    moving West at 20.00 m/s. After the collision, the 580 kg car is

    moving East at 5.00 m/s.

    The magnitude of the impulse on Car 1 is b x 10w N s.

    Your 3-digit value for b is

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    Solution:

    Recall, for momentum to be conserved,the impulses have to be equal and opposite

    i.e.

    Both cars experience the same magnitude of impulse,but in opposite directions

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    Ref: East is positive

    750 kg 580 kg 1 2

    -20.00 m/s Boom! +5.00 m/s

    Find impulse on Car 2:

    m2 v2 = m2 (v2' - v2)

    = 580 kg [ (+5.00 m/s) - (-20.00 m/s) ]

    = +1.45 x 104 kg m/s (East)

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    The cars will experience equal but opposite impulses

    (Cons of momentum)

    Thus, Impulse on Car 1 = -1.45 x 104 kg m/s

    = 1.45 x 104 Ns West

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    Numerical Response format (b 10w)

    1.45 x 10

    4

    w

    b

    So, the 3-digit value for b is

    1 . 4 5

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    Practice Problems:

    TryLadner p. 46 #1 - 12

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    SUMMARY

    1. Conservation of momentum is based on which law?

    2. What are the two equations for Cons of p?

    3. What conditions are required for Cons of p?

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    SUMMARY

    1. Conservation of momentum is based on which law?

    Newton's 3rd Law- equal and opposite forces

    - so, equal and opposite impulses

    2. What are the two equations for Cons of p?Total p is constant

    pT = pT'

    No overall change in momentum

    p1 + p2 = 0

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    3. What conditions are required for Cons of p?

    Closed system - no objects lost or gained

    Fnet = 0 on system- objects have constant velocity before and after

    the collision / explosion

    - no friction / level surface

    4. Review Animations:

    Air Track collisions

    2 Block collisions

    http://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.htmlhttp://www.geocities.com/thesciencefiles/collisions/collisions.htmlhttp://www.geocities.com/thesciencefiles/collisions/collisions.htmlhttp://faraday.physics.utoronto.ca/PVB/Harrison/Flash/ClassMechanics/AirTrack/AirTrack.html