Projectile Motion Amazing Shit will get you a 7 in IB

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    Fields and Forces

    Topic 9.1 Projectile Motion

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    Components of Motion

    When a body is in free motion, (movingthrough the air without any forces apart from

    gravity and air resistance), it is called aprojectile

    Normally air resistance is ignored so the onlyforce acting on the object is the force due to

    gravityThis is a uniform force acting downwards

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    Therefore if the motion of the projectile isresolved into the verticaland horizontal

    componentsThe horizontal componentwill be unaffectedas there are no forces acting on it

    The vertical componentwill be accelerated

    downwards by the force due to gravity

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    These two components can beconsidered as independent factors in

    the motion of a projectile in a uniformfield

    In the absence of air resistance the

    path taken by anyprojectile is parabolic

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    Solving Problems

    In solving problems it is necessary toconsider the 2 components

    independently

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    Therefore the horizontal motion it isnecessary to use the equation

    speed = distancetime

    Where speed is the horizontal

    component of the velocity

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    Therefore the vertical motion it isnecessary to use the kinematic

    equations for uniform accelerationi.e. Using the s.u.v.a.tequations

    Where uand vare the initialand final

    verticalcomponents of the velocity

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    To be able to calculate the horizontal

    distance we need to know thehorizontal speed, and the time.

    The horizontal distance is easy tocalculate by resolving the velocity

    40.0o

    10.0ms-110.0 sin 40.0o

    10.0 cos 40.0o

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    However, to calculate the time we willneed to use the vertical component and

    the s.u.v.a.t. Equations

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    s= ?

    u= 10.0 sin 40.0o ms-1

    v= ?a= -10.0 ms-2 (Up is positive, thereforeacceleration here is negative)

    t= ?We only have 2 of the values when weneed three to find any other

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    However, if we ignore air resistance,then the final vertical component of the

    velocity will be equal and opposite ofthe initial component

    i.e. v= -10.0 sin 40.0o ms-1

    Looking at the equations for uniformacceleration, we need an equation thatlinks u, v, aand t.

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    v = u + at

    Rearranging to make tthe subject

    t = v

    ua

    Substitute in

    t =-10.0 sin 40.0o

    10.0 sin 40.0o

    -10

    t= 1.286 seconds

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    Now returning to the horizontalcomponents

    Using speed = distancetime

    Rearranging distance = speed x time

    Distance = 10.0 cos 40.0o x 1.286

    Distance = 9.851 = 9.9 metres

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    Using the Conservation ofEnergy

    In some situations the use of theconservation of energy can be a muchsimpler method than using the kinematicequations

    Solving projectile motion problems makes useof the fact that Ek+ Ep=constant at every

    point in the objects flight (assuming no lossof energy due to friction)

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    Example

    A ball is projected at 25.0 ms-1 at anangle of 40.00 to the horizontal. The ball

    is released 2.00m above the ground.Taking g = 10.0 ms-2. Find themaximum height it reaches.

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    Solution

    2.0m

    25.0 ms-1

    A

    Bv = v

    horizontal

    H

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    Total energy at A is given by

    Ek+ Ep= m (25.0)2+ mg x 2.0

    =312.5m + 20m

    = 332.5m

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    Next, to find the total energy at B weneed to know the velocity at B, which is

    given by the horizontal component ofthe velocity at A

    Total energy at B is given by

    Ek

    + Ep

    = m (25.0 cos 40o)2+ mg x H

    =183.38m+ 10mH

    Then using the conservation of energy

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    Equating the 2 equations

    332.5m = 183.38m + 10mH

    332.5 = 183.38 + 10H

    332.5183.38 = 10H

    10H = 149.12

    H = 14.912 = 14.9m