AP Physics B Ch 7 Review PPT

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    Chapter 6 energy

    transformations involved

    only one object

    Chapter 7 momentum is

    transferred when 2 or more

    objects interact in a collision

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    Impulse changes momentum

    Bat applies an average

    force over a short time

    interval to accelerate the

    ball

    Must stop the ball, change

    its direction and send it in

    the opposite direction

    v F ma mt

    F t m v

    (! !

    (

    ( ! (g g

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    Impulse = Favgy(time

    Impulse from the bat changes the

    momentum of the ball

    Actual force builds to a very highmaximum value and then drops off

    We will most often study forces that

    have a constant average value

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    variable force

    constant force

    Impulse = area under force time graph

    Impulse = vector quantity in

    same direction as force vector

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    A ball hits a wall and bounces off

    at the same speed.

    What is the direction of the

    impulse acting on the ball?

    f iImpulse = p = p - p(

    pf

    pi

    6

    (p

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    Linear Momentum

    Product of an objects mass and velocity

    vector quantity with same direction as velocity

    vector

    Units:

    units for momentum are the same for impulse

    p mv!ur r

    2

    m mkg kg s N s

    s s

    y ! ! y

    g g

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    Impulse momentum theorem

    Impulse = change in momentum

    Equivalent or identical?

    equivalence means that if you calculate the

    impulse you know what the change in

    momentum is equal to equivalence means that if you know the mass

    and velocity change of the object then you know

    the value of the impulse that changed its velocity

    0 0f f F t m v mv mv p p py ( ! ( ! ! ! (r r r r r r r

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    Airbag-watermelon drop-balloon toss2 identical 1 kg watermelons are dropped from rest from a 3 meter diving board

    concrete vf= 0

    3 m

    conservation of

    energy to solve for

    velocity just before

    collision

    211 9.8 3 12

    7.7 /

    PE KE

    v

    v m s

    !

    !

    !

    g g g g

    3 m

    water vf= 0

    (p for both cases is the same = 0 7.7 kgm/s = - 7.7 kgm/s

    Impulses for both water and concrete are both 7.7 kgm/s

    Collision time for concrete (t = .001 s Force = - 7700 N (up)

    Collision time for water(t = 1 s Force = - 7.7 N

    TIME IS THE DETERMINING FACTOR, NOT THE FORCE

    +

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    Application ofImpulse Momentum Theorem

    Airbag principle water balloon toss

    2 extremes in changing momentum from large value to

    zero

    Very high force acting over a very short time

    Lower force acting over a longer time

    Time is what determines the force NOT force which

    determines the time

    1000 0.01 10

    10 1 10

    F t p

    N s N s

    N s N s

    7 y ( ! (

    !

    !

    r r

    g g

    g g

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    Force plate ball drop example

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    Conservation ofLinear Momentum

    During collision each ball exerts an equal force on the other in the

    opposite direction according to Newtons3rd L

    aw of MotionTherefore since the time interval is the same for both forces it can be

    said that the impulses of A on B and B on A are equal and opposite in

    direction

    Impulse from A changes Bs momentum; Impulse from B changes As

    momentum 12

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    Total Linear Momentum stays constant

    A B

    B A

    Bf Bi Af Ai Ai Af

    Bf Af Ai Bi

    B Bf A Af B Bi A Ai

    F t F t

    p p

    p p p p p p

    p p p p

    m v m v m v m v

    ( ! (

    ( ! (

    ! !

    !

    !

    r rgr r Impulses are equal and opposite

    change in momentums are equal and opposite

    Total momentum after the collision equals the total momentum beforethe collision.

    Assumes that system is closed and isolated

    Isolated = no external forces

    Closed = no mass or particles being added or removed from system 13

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    Conservation of Momentum Examples

    When two particles stick together after the collision thereis only one mass (total of m1 + m2) and only one final

    velocity vf

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    Momentum is a vector

    Total momentum before

    collision = 0

    Must have + and signs on the

    final velocities for total

    momentum after the collision =

    push to be equal to 0

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    7-4 Conservation of Energy and Momentum

    in Collisions

    Momentum is conserved

    in all collisions.

    Collisions in which

    kinetic energy is

    conserved as well are

    called elastic collisions,and those in which it is

    not are called inelastic.

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    Elastic, Inelastic Collisions

    Momentum is always conserved for alltypes of collisions, in a closed, isolated

    system

    However energy has the ability to do work

    in the form of deformation of one of the

    objects in the collision or to generate heat

    Collisions are classified by amount of

    kinetic energy that is used up doing workduring collision

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    Completely Elastic total KE before = total KE after

    Inelastic total KE before > total KE after

    some KE used up to compressand expand the ball during

    collision Completely Inelastic

    objects stick together aftercollision

    may or may not be moving

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    7-5 Elastic Collisions in One Dimension

    Here we have two objects

    colliding elastically. We

    know the masses and the

    initial speeds.

    Since both momentumand kinetic energy are

    conserved, we can write

    two equations. This

    allows us to solve for thetwo unknown final

    speeds.

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    Ballistic Pendulum

    They may be a bullet shot

    into a block which rises or a

    ball which swings down and

    strikes a block which then

    moves to the right.

    Use energy conservation to

    solve for speed height

    change relationship

    Use momentumconservation to solve for

    velocities before/after

    collision

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    Ballistic Pendulum

    Completely inelastic collision between

    bullet and block

    KE of bullet > KE of bullet+block some of bullets KE used to deform block

    cannot equate final PE of pendulum with

    initial KE of bullet

    cannot equate initial and final KEs

    momentum is conserved for the collision

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    2 dimensional collisions

    total initial momentum in x = total final momentum in x

    total initial momentum in y = total final momentum in y

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    A two dimensional collision

    U

    J

    i f!

    r r

    xi xf!

    1v

    1'v

    2'v

    1 1 1 1 2 2' cos ' cosm v m v m vU!

    yi yfP P!

    1 1 2 20 ' sin ' sinm v m vU J! 24