9 - kinetics of rigid body - impulse & momentum

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    Principle of L inear Impulse and Momentum

    Ken Youssefi 1Mechanical Engineering Dept.

    dt

    vdmF

    122

    1

    vmvmdtFt

    t

    The Principle of Linear Impulse and Momentum states that the (linear)

    impulse from external forces acting on a rigid body over a given time interval

    equals the change in linear momentum with respect to the center of mass.

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    Principle of Angular impulse and Momentum

    Ken Youssefi Mechanical Engineering Dept. 2

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    Principle of Angular impulse and Momentum Rigid Body

    Ken Youssefi Mechanical Engineering Dept. 3

    The Principle of Angular Impulse and Momentum states that the

    (angular) impulse from external moments acting on a rigid body

    over a given time interval equals the change in angular momentum.

    =+

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    Principle of I mpulse and Momentum

    Ken Youssefi Mechanical Engineering Dept. 4

    Impulse and momentum equations for the Planar motion

    with rotation about the center of gravity

    2D scalar equations

    Linear

    Angular

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    Non-centroidal Rotation

    Ken Youssefi Mechanical Engineering Dept. 5

    Principle of angular impulse and momentum

    Rotation about point O

    Use the parallel axis theorem to find

    the angular momentum Ho

    of the body

    about point O.

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    Principle of I mpulse and Momentum

    Ken Youssefi Mechanical Engineering Dept. 6

    The principle can be applied to an entire system of connected

    bodies. No need to account for the interaction impulses which

    occurs at the connections.

    Same reference point, O, should be used to determine the systems

    angular impulse and angular momentum

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    Conservation of Angular Momentum

    Ken Youssefi Mechanical Engineering Dept. 7

    The impulses of the external forces are zero when there are

    no external forces applied to a rigid body.

    Conservation of Linear Momentum of a system

    Conservation of Angular Momentum of a system

    Diver executing a somersault

    (IG)1 = (IG)2 = constant

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    Example 1

    Ken Youssefi Mechanical Engineering Dept. 8

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    Example 1

    Ken Youssefi Mechanical Engineering Dept. 9

    Principle of impulse and momentum for Gear A

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    Example 1

    Ken Youssefi Mechanical Engineering Dept. 10

    Principle of impulse and momentum for Gear B

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    Example 2

    Ken Youssefi Mechanical Engineering Dept. 11

    Apply the principle of impulse to the sphere at time zero when it comes in contact

    with the surface until the time when it starts rolling on the surface.

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    Example 2

    Ken Youssefi Mechanical Engineering Dept. 12

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    Example 2

    Ken Youssefi Mechanical Engineering Dept. 13

    Substitute tin 2 equation

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    Example 3

    Ken Youssefi Mechanical Engineering Dept. 14

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    Example 3

    Ken Youssefi Mechanical Engineering Dept. 15

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    Example 3

    Ken Youssefi Mechanical Engineering Dept. 16

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    Example 4

    Ken Youssefi Mechanical Engineering Dept. 17

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    Example 4

    Ken Youssefi Mechanical Engineering Dept. 18

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    Example 4

    Ken Youssefi Mechanical Engineering Dept. 19

    Mass moment of inertia of the plate about the center of the gravity

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    Example 4

    Ken Youssefi Mechanical Engineering Dept. 20