Dynamics of a System of Particles

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    Momentum, Impulse & Collisions

    Linear Momentum

    Conservation of Linear Momentum

    Impulse

    Collisions : Elastic & Inelastic Collisions

    Collisions in 2-Dimensions

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    Linear Momentum

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    Conservation of Linear Momentum

    The principle of conservation of momentum states thatwhen no external forces act on a system consisting of

    two objects that collide with each other, the total

    momentum of the system before the collision is equal to

    the total momentum of the system afterthe collision.

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    Law of Conservation of Linear Momentum

    The general statement of the law of conservation of

    linear momentum states that

    The total momentum of an isolated system of bodies

    remains constant

    and is given by

    pinitial = pfinal

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    Newtons Second Law of Motion

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    A 10,000 kg railroad car traveling at a speed of 24

    m s-1 strikes an identical car at rest. If the cars lock

    together as a result of the collision, what is their

    common speed afterward ?

    EXAMPLE

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    SOLUTION

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    Impulse

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    Impulse

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    A 0.375 kg rubber ball traveling horizontally to the right at10 m s-1 hits a wall and bounces back at 6 m s-1 to the left.

    What is the total impulse exerted by the wall?

    EXAMPLE

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    Impulse, I = p = Ft

    = mv - mu

    = m (v u )

    = (0.375 kg)(-6 -10 m s-1)

    = (0.375 kg)(-16 m s-1)

    I = -6.0 N s

    SOLUTION

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    A baseball, of mass 0.2 kg, is pitched at 40 m s-1 and is hit

    straight back at the pitcher at 90 m s-1. Assume the positive x-

    axis points toward the pitcher

    (a) Find the impulse exerted by the bat on the ball

    (b) If the ball is in contact with the bat for 3.5 ms, find

    the average force exerted on the ball(c) How would the result of part (b) change if the

    contact time were one-third as long

    EXAMPLE

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    SOLUTION

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    Collisions

    Inelastic Collisions

    Elastic Collisions

    Stationary Target

    Moving Target

    Collisions in 2-Dimensions

    (Glancing Collisions)

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    Inelastic Collisions

    Collisions in which kinetic energy is not conserved.

    Initial kinetic energy is transformed into other types of

    energy (thermal, potential etc.)Total final kinetic energy is less than the total initial

    kinetic energy.

    If two objects stick togetheras a result of the collision,

    the collisions is inelastic. Even though the kinetic energy is not conserved, the

    total energy is conserved.

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    1-Dimensional Inelastic Collisions

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    Before Collision

    m1 m2 at rest

    +x

    V

    v

    After Collision

    m1 + m2

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    1-Dimensional Inelastic Collisions

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    A ballistic pendulum is a device that was used to measure thespeeds of bullets before electronic timing devices weredeveloped.

    The device consists of a large block of wood of mass M= 5.4kg, hanging from two long cords. A bullet of mass m = 9.5 g isfired into the block, coming quickly to rest. The block + bulletswing upward, their center of mass rising a vertical distance h =6.3 cm before the pendulum comes momentarily to rest.

    (a) What was the speed v of the bullet just prior to thecollisions.

    (b) What is the initial kinetic energy? How much

    energy remains as mechanical energy?

    EXAMPLE

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    Elastic Collisions

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    Elastic Collisions

    then[1]&[2]becomes

    m1(v1iv1f)=m2v2f[3]

    m1(v1iv1f)(v1i+v1f)=m2v2f2

    [4][4][3]

    if v

    mm

    mmv

    1

    21

    21

    1

    ifv

    mm

    mv

    1

    21

    1

    2

    2

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    BeforeCollision

    m1 m2atrest

    v1i

    v2i=0

    AfterCollision

    m1m2

    v1f v2f

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    Elastic CollisionsMovingTarget

    Conservationoflinearmomentumstatesthat

    m1v1i+m

    2v2i=m

    1v1f+m

    2v2f[1]

    Conservationofkineticenergystatesthat

    m1v1i2+m2v2i

    2=m1v1f2+m2v2f

    2[2]

    Combiningtheequations[1]&[2]willgiveus

    and

    iif vmm

    mv

    mm

    mmv

    2

    21

    2

    1

    21

    21

    1

    2

    iifv

    mm

    mmv

    mm

    mv

    2

    21

    12

    1

    21

    1

    2

    2

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    Collisions in 2-Dimensions

    Thevectornatureofmomentumespeciallyin2-

    dimensionsisveryimportant.

    Commontypeofnonhead-oncollisionisthatamovingobjectstrikesasecondobjectinitiallyatrest

    Lawofconservationofmomentumstatesthat

    x: p1x+p2x=p1x+p2x m1v1=m1v1cos1+m2v2cos2[1]

    y:p1y+p2y=p1y+p2y

    0=m1v1sin1+m2v2sin2[2]

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    Collisions in 2-Dimensions

    Ifthecollisionsiselastic,thenthelawofconservation

    ofenergystatesthat

    m1v12=m1v1

    2+m2v22[3]

    Fromequations[1],[2]&[3],wecansolveforv1,v2,

    1and2ifm1,m2,v1andv2isgiven.

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    Example

    Abilliardballmovingwithspeedv1=3.0ms-1inthe+x

    directionstrikesanequalmassballinitiallyatrest.Thetwoballsareobservedtomoveoffat45,ball1

    abovethex-axisandball2belowthex-axis.Thatis

    1=45and2=-45.

    Whatarethespeedsofthetwoball?

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    SolutionAssumethatthetwoballshavethesamespeed(from

    symmetry).Conservationofmomentumgives

    x: mv1=mv1cos(45)+mv2cos(-45)

    v1=v1cos(45)+v2cos(45)=2v1cos(45)

    y: 0=mv1sin(45)+mv2sin(-45)

    then

    v2=-v1[sin(45)/sin(-45)]=v1

    so v1=v2=v1/2cos(45)

    =(3.0ms-1)/[2(0.7071)]

    = 2 1 m s-1