kinematics of planar rigid body motion - may 11 lecture

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  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Kinematics of planar rigid bodymotion analysis using

    rans a ng axesHibbeler chapter 16

    May 11, 2011 lecture

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Objective of kinematic analysis

    using translating axes

    Establish:

    a) relationships between the

    motion (velocity &

    acceleration) ofpoints on

    the same rigid body;

    b) relationships between the

    motion (velocity &acceleration) ofpoints on

    rigid bodies connected with

    non-slipping joints.

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Last lecture Established relationships

    between the motion (velocity &

    acceleration) of points on the

    same rigid body:

    ABA rrv /rrr

    +=

    Black vectors absolute

    motion of A & B (seen from

    the fixed frame).

    Green vectors relative

    motion of B w.r.t. the axes

    translating with A (motion of

    B seen from the frame thattranslates with A).

    ABAABnABtA

    ABABA

    ABAB

    AB

    ABAABA

    aaaaa

    rra

    rrva

    vvrv

    //,/,

    //

    //

    //

    )(rrrrr

    rrr

    rr

    r

    rr

    rrr

    r

    rrrrr

    +=++=

    ++=

    ++=

    +=+=

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Today Use velocity & acceleration

    equations from last lecture to:

    a) Illustrate problem solving

    procedure.

    c) Establish relationships betweenthe motion (velocity &acceleration) ofpoints on rigid

    bodies connected with non-slipping joints.

    na yze part cu ar r g o ymotions:

    Translation.

    Rotation about a fixed axis.

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Problem solving procedure1. Identify body connections:

    they provide kinematicconstraints (relationships thatvelocities & accelerations mustobey).

    2. Write velocity &acceleration equations:

    connect point with known

    direction of velocity (locallyknown path) to point withknown velocity & acceleration.

    3. Solve for the unknowns.

    Example

    1. Joints: sliders at A & B. Write

    corresponding kinematic constraints.

    2. Point with known motion: A.3. Point with known direction of

    velocity: B.

    4. Write velocity & acceleration of B

    w.r.t. A.5. Solve.

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Slider (joint) B imposes that:

    A.

    B.

    OBa

    OBv

    Bn

    B

    ,

    r

    Oxa

    Oxv

    A

    A

    r

    r

    C.

    D.

    ABa

    ABv

    Bn

    B

    ,

    r

    r

    Oxa

    Oxv

    OBa

    OBv

    A

    A

    Bn

    B

    r

    r

    r

    r

    ,

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Translation Definition: any line of the body remains parallel to

    itself throughout the motion.

    r

    0

    =

    AB

    AB

    def

    aa

    vvrr

    rr

    rr

    0

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Translation

    important notes.

    Rectilinear translation

    All points on a translating

    rigid body move on parallel

    paths, with the same velocityand the same acceleration.

    The paths of points on a

    Curvilinear translation( )trr AArr

    =

    trans at ng r g o y are

    determined by the bodys

    connections (kinematic

    constraints).

    A rigid body in planartranslation has 2DOF

    (translation is fully described

    by the displacement of one

    point ).

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Translation

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    Rotation about a fixed axis Definition: a line/axis of the

    body is at rest throughout themotion.

    ==

    kk r

    Choose O on axis of rotation:

    0

    0

    O

    O

    a

    vr

    r

    ====

    kkk rr

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Rotation about a fixed axis

    velocity equation

    rr

    In the plane of motion (perpendicular on the fixed axis of

    rotation).

    Perpendicular on the distance from P to the axis of rotation.

    =

    OP

    OPrif

    P

    OP

    OPOPP

    rvvrv

    /

    /

    /

    //

    ,

    rr

    rrrr

  • 8/3/2019 Kinematics of Planar Rigid Body Motion - May 11 Lecture

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    Rotation about a fixed axis

    acceleration equation

    ( )

    PnPtOP

    OPOPP

    aaa

    rra

    ,,/

    //rrr

    rrr

    rr

    r

    +

    +

    ( )OP

    OPrif

    OPPn

    OP

    OPrif

    Pt

    OP

    OPPt

    rra

    ra

    r

    ra

    /

    2/

    /,

    /

    /

    ,

    /

    /,

    ,

    rrrr

    r

    rr

    rr

    rr

    ==

    =

    =

    In the plane of motion.

    Perpendicular on the

    distance from P to the axisof rotation.

    In the plane of motion.

    From P to the axis ofrotation.

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    Rotation about a fixed axis

    important notes All points on a rigid body rotating

    about a fixed axis move on

    circular paths centered on the

    axis of rotation.

    fixed axis of rotation move fasterthan points closer to it.

    A rigid body in rotation about a

    fixed axis has 1DOF (rotationabout a fixed axis is fully

    described by the angular

    displacement about the axis of

    rotation ).( )t=

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    Examples: bodies pinned to the ground.Rotation about a fixed axis

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    Examples (2): bodies pinned to the ground.Rotation about a fixed axis

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    Examples (3): bodies pinned to the ground.Rotation about a fixed axis

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    A. B rotates about A.

    B. A translates with B and

    rotates about B.

    C. A does not move.

    D. All of the above.

    .

    A does not move.

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    Rotation abouta fixed axis

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    Rotation abouta fixed axis