Aristo Kinematics - Module 17 - Relative Vel - JEE 2003

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  • 8/12/2019 Aristo Kinematics - Module 17 - Relative Vel - JEE 2003

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    Kinematics

    Scene 1

    A pencil writes & draws the following (free hand):

    Physics

    Kinematics

    (Sketch of a car, then the car speeds away)

    Scene 2

    On screen:

    What you will see now is another IIT JEE problem on relative velocity.

    Voiceover:

    What you will see now is another IIT JEE problem on relative velocity.

    Scene 3

    On screen:

    Example 1 (IIT JEE 2003)

    A particle of mass m, moving in a circular path of radius R with a constant speed2

    v is located at

    point (2R, 0) at time t = 0, and a man starts moving with a velocity1v along the +ve y-axis from the

    origin at time t = 0. Calculate the velocity of the particle w.r.t the man as a function of time.

    Voiceover:

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    The problem is from IIT JEE 2003. It says - A particle of mass m, moving in a circular path of radius R

    with a constant speed2

    v is located at point (2R, 0) at time t = 0, and a man starts moving with a

    velocity1v along the +ve y-axis from the origin at time t = 0. Calculate the velocity of the particle

    w.r.t the man as a function of time.

    Scene 4

    On screen:

    So, if we write1

    v and2

    v in their vector form we will get 2 1v

    1 1v v j

    Voiceover:

    We have been asked to find out the velocity of the particle relative to the man, or 2 1v .

    Now, 2 1 2 1v v v

    So, if we write1

    v and2

    v in their vector form we will get 2 1v

    It is very easy to write1

    v in the vector form with respect to the coordinate axes shown.

    1 1v v j

    Scene 5

    On screen:

    1: Man

    2: Particle

    We have to determine 2 1v

    2 1 2 1v v v

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    ( cos ) ( sin )r R R i R j

    2v

    R

    2 ( sin ) ( cos ) ( sin ) ( cos )

    d r d d v R i R j R i R j

    dt dt dt

    Or 2 2 2 ( sin ) ( cos )v v i v j

    Voiceover:

    Writing2

    v is not that simple, though. That is because unlike1

    v ,2

    v is constantly changing in its

    direction.

    Suppose at time t, the particle is at point P. Then, itsposition vector can be written as

    ( cos ) ( sin )r R R i R j

    We must recognize here that r is a function of time because is continuously changing with time.

    Since the particle is moving in circle with constant speed 2v , its angular velocity is also constant.

    2v

    R

    Lets now differentiate the position vector with respect to time.

    2 ( sin ) ( cos ) ( sin ) ( cos )

    d r d d v R i R j R i R j

    dt dt dt

    Or 2 2 2 ( sin ) ( cos )v v i v j

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    Scene 6

    2 1 2 1v v v

    But 1 1v v j

    And 2 2 2 ( sin ) ( cos )v v i v j

    So, 2 1 2 2 1 ( sin ) ( cos )v v i v v j

    Voiceover:

    We said earlier that

    2 1 2 1v v v

    And have found1 1

    v v j

    And 2 2 2 ( sin ) ( cos )v v i v j

    So, 2 1 2 2 1 ( sin ) ( cos )v v i v v j