Energy, Impulse and Momentum

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    1

    Assoc. Prof. Raafat Ibrahim

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    2

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    ENERGY (joules)

    3

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    Conservation of ENERGY

    IF,

    In a mass system where internal friction forces are sufficiently

    small to be neglected

    AND

    No work is done on the system during an interval of motionby external force (other than gravitational force)

    4

    That is,

    THEN The net energy of the system remains constant

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    Conservation of ENERGY

    That is,

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    The net energy of the system remains constant

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    EXAMPLE 1

    The 3kg slider is released from rest at position 1 and slides withnegligible friction in a vertical plane along the circular rod. The

    attached spring has a stiffness of 350 N/m and has an unstretchedlength of 0.6m. Determine the velocity of the slider as it passesposition 2.

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    EXAMPLE 1

    The 3kg slider is released from rest at position 1 and slides withnegligible friction in a vertical plane along the circular rod. The

    attached spring has a stiffness of 350 N/m and has an unstretchedlength of 0.6m. Determine the velocity of the slider as it passesposition 2.

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    The 3kg slider is released from rest at position 1 and slides with

    negligible friction in a vertical plane along the circular rod. The

    attached spring has a stiffness of 350 N/m and has an unstretched

    length of 0.6m. Determine the velocity of the slider as it passes

    position 2.

    8

    EXAMPLE 1

    Substituting in conservation of energy equation

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    Linear momentum of the system

    is the vector sum of the linear

    momenta of all its particles

    Linear momentum of a system of particles

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    Linear momentum (G) = mv

    For a particle of mass of the

    system

    (1)

    m

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    Linear momentum of a system of particles

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    Substituting in Eq. (1)

    From the definition of center of mass

    Therefore,

    m

    Velocity of mass w.r.t O

    velocity of center of mass

    velocity of w.r.t translating

    reference frame moving with Cm

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    Linear Impulse-Momentum principle

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    Product of force and time Linear Impulse

    Total external linear impulse (impact force) on the particle equals the

    corresponding change in the linear momentum

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    EXAMPLE 2

    z

    y

    F

    mg

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    Angular momentum of a system of particles

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    m

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    Angular momentum of a system of particles

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    m

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    Angular momentum of a system of particles

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    m

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    Angular Impulse-Momentum

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    EXAMPLE 3

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    Conservation of Momentum

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    In the absence of an external impulse, the momentum of a system

    remains unchanged

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    EXAMPLE 4

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    The 25Mg flatcar supports a 7.5Mg vehicle on a 5o ramp built on

    the flatcar. If the vehicle is released from rest with the flat caralso at rest, determine the velocity v of the flatcar when the

    vehicle has rolled s =12m down the ramp just before hitting the

    stop at B. Neglect all friction and treat the flatcar as particles.

    s

    x

    y

    v

    o

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    EXAMPLE 4

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    s

    x

    y

    v

    o

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    EXAMPLE 4

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    s

    x

    y

    v

    o

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    EXAMPLE 4

    22

    s

    x

    y

    v

    o

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    What You Learned!

    Work and Energy

    Conservation of Energy

    Impulse and Momentum

    Linear Impulse and Momentum

    Angular Impulse and Momentum

    Conservation of Momentum