Chapter 02-theory of machines

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    Chapter 2: KinematicFundamentals

    Chapter Outcomes

    After covering this chapter, you should beable to: Identify mechanisms and predict their

    motion Calculate the degrees of freedom of

    mechanisms

    2.1: Degrees of Freedom (DoF)

    DoF: Number of independent parametersneeded to completely define a systemsposition in space

    Marker in 3-D space example (whiteboard) Marker in 2-D space example (whiteboard) Course coverage will be limited to

    2-D/planar systems

    2.2: Types of Motion

    Pure rotation: Object changes angularorientation about fixed axis (whiteboard)

    Pure translation: Object changes positionwithout changing angular orientation(whiteboard)

    Complex motion = rotation + translation(whiteboard)

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    2.3(A): Links Reminder: A mechanism is a collection of links

    connected by joints arranged to transmit a specific type

    of motion Link: Rigid body which possesses at least 2 nodes

    (nodes = points for attachment to other links) Links are classified according to # of nodes

    2.3(A): Links

    Simplified drawings of links (whiteboard)

    Students must be able to identify anddifferentiate types of links

    Links do not necessarily need to take theirobvious shapes (links are classifiedaccording to # of nodes, NOT theirshapes)

    Example (whiteboard)

    2.3(B): Joints

    Joint: Connection between 2 or more links(at their nodes) which allows somemotion

    Can be classified in several ways. We willfocus on 2: by the DoF allowed at the joint by the number of links joined (order of the

    joint)

    DoF Classification

    Pure roll: 1Pure slide: 1Roll & slide: 2

    Rollingcylinder

    2 (why?)Pin in slot

    2 (why?)Link againstplane

    1 (why?)Slider /Translational

    1 (why?)Pin /

    Rotational

    SimplifiedDiagram

    DoFDiagramName

    Link

    LinkJoint

    Joint (surface)

    Link

    Link

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    Order Classification

    Order = (# of links joined) - 1

    2 joints, each

    with 1 DoF(whiteboard)

    2Multiple

    joint

    11Single joint

    DoFOrder DiagramName

    2.3(C): Kinematic Chains

    Kinematic chain: An assembly of links and

    joints Mechanism: A kinematic chain with at

    least one link grounded Example (whiteboard)

    2.4: DoF of Planar Mechanisms

    Number of inputs needed to fully defineposition of mechanism

    Kutzbachs / Modified Grueblers equation:M = 3( L 1) 2 J 1 J 2where: M = DoF

    L = # of linksJ 1 = # of 1 DoF jointsJ 2 = # of 2 DoF joints

    Example (transparency) Reminder (whiteboard)

    2.5: Mechanisms and Structures

    If DoF > 0, its a mechanism If DoF = 0, its a structure If DoF < 0. its a preloaded structure (will have

    built in stresses with manufacturing error)

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    More on DoF Definitions

    For a body in free space , it is: The number of independent parameters

    needed to completely define a systemsposition in space

    For a mechanism , it is: The number of inputs needed to fully define

    position of mechanism Are they the same? So what is an input ?

    NO!!!

    Input Input = Source of Motion The device that introduces/produces motion for

    a mechanism Rotary Input Usually provided by a motor

    Linear Input Usually provided by a linear

    actuator

    Simply a piston in a cylindermoved by pneumatic orhydraulic pressure

    Computer simulation onnumber of Inputs

    Linear Actuator

    Piston

    Cylinder

    SlidingJoint

    2.11: Inversion

    Act of grounding a different link in akinematic chain

    Usually produces different motions fromthe mechanism

    Example (computer simulation)

    2.12: The Grashof Condition Fourbar link naming conventions:

    Ground: Link fixed to the ground Crank: Link which makes a complete revolution Rocker: Link which has oscillatory motion (rocks back

    and forth) Coupler: Link connecting input and output links

    Ground

    Crank

    Coupler

    Rocker

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    2.12: The Grashof Condition Grashof condition: Condition used to predict rotational

    behavior/motion of fourbar linkage based on link lengths

    Linkage is Grashof if S + L P + Q (whiteboard)where S : length of shortest link

    L: length of longest linkP : length of intermediate linkQ : length of another intermediate link

    Else linkage is non-Grashof Grashof linkage: At least one link will be able to make a

    full revolution Non-Grashof linkage: No link will be able to make a full

    revolution

    Grashof Classification(Transparency + Computer Simulation) Class 1: S + L < P + Q

    Either link attached to the shortest isgrounded Crank-Rocker Shortest link is grounded Double-Crank Link opposite the shortest is grounded

    Double Rocker Class 2: S + L > P + Q (non-Grashof)

    Tripler Rocker Class 3: S + L = P + Q (special case)

    Will have change points when all linksbecome collinear

    Output behavior at these points indeterminate

    Link Assembly

    In order for the four links to be assembledL < (S + P + Q )

    If L = S + P + Q , the links can beassembled but will not move (whiteboard)

    Course OutcomesIdentify mechanisms and predict their motionCalculate the degrees of freedom of mechanismsDesign mechanisms to fulfill motion generation and quick

    return requirementsDetermine the positions, velocities and accelerations of linksand points on mechanismsDerive SVAJ functions to fulfill cam design specificationsCalculate dynamic joint forces of mechanismsBalance simple rotating objects and pin-jointed fourbar linkagesWork in a team to analyze and modify existing mechanisms

    Present completed work in oral and written formUse related computer programs to design, model and analyzemechanisms

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    End of Chapter 2

    Please bring geometrical set +

    tracing paper during tutorialsession next week. Thank you.