Cam Second Lecture.ppt

download Cam Second Lecture.ppt

of 8

Transcript of Cam Second Lecture.ppt

  • 7/30/2019 Cam Second Lecture.ppt

    1/8

    Axis of transmission is extended to intersect

    effective link 1, which is the ground link.

    This intersection is instant center I24 (labeled B)

    which by definition has the same velocity in link

    2(the cam) and in link 4(the follower) .

    Because link 4 is in pure translation, all points on it

    have identical velocities vfolower, which are equal to

    the velocity of I24 in link 2

    We can write the expression for the velocity of I24

    in terms of cam angular velocity and the radius b

    from cam center to I24

    Axis of the motion of the follower does not intersect the center of the cam

    Eccentricity: Perpendicular distance between the follower's axis of motion and the centerof the cam

    2

    3

    12

    23

    34

  • 7/30/2019 Cam Second Lecture.ppt

    2/8

    It can be expressed in terms of cam angular velocity and the radius b from cam

    center to I24

    Where s is the instantaneous displacement of the follower from the s diagram and

    s dot is its time derivative in units of length/s

    Distance b to the instant center I24 is equal to the velocity of the follower, v in

    units of length per radian

  • 7/30/2019 Cam Second Lecture.ppt

    3/8

    Distance b is expressed in termsof cam design parameters, primecircle radius Rp and the

    eccentricity

    arctanv

    s RP2 2

    From triangle CDO2

    22

    PRd

    Substitute this in equation for vand rearrange to get pressureangle in terms of camparameters and eccenticity

  • 7/30/2019 Cam Second Lecture.ppt

    4/8

    arctanv

    s RP2 2

    As Rp is increased, will be reduced, Practical limitation is the size and cost

    If small cam cannot be obtained with acceptable pressure angle, then eccentricity can beintroduced

    For positive , a positive value of eccentricity will decrease the pressure angle on the risebut will increase it on the fall. Negative eccentricity does the reverse

    This is of little value with a form closed(groove or track) cam, as it is driving the followerin both direction

    For a force closed cam with spring return, you can sometimes to afford to have a largerpressure angle on the fall than on the rise because the stored energy in the spring isattempting to speed up the camshaft on the fall

    When the cam function is asymmetrical and significant differences exist (with noeccentricity) between maximum pressure angles on rise and fall, introducing eccentricitycan balance the pressure angles and create a smoother running cam

  • 7/30/2019 Cam Second Lecture.ppt

    5/8

    Overturning Moment-Translating Flat Faced Follower

    Pressure angle can be seen to be zerofor all positions of cam and follower

    As the contact point moves left andright, the point of application for theforce between cam and followermoves with it

    There is an overturning moment onthe follower associated with this off-center force which tends to jam thefollower in its guide just as did toolarge a pressure angle in the roller

    follower case

    In this case keep the cam as small aspossible in order to minimize themoment arm of the force

  • 7/30/2019 Cam Second Lecture.ppt

    6/8

    Cam Synthesis

    Type Synthesis: Choose the type of cam and follower

    Type of follower (translation/oscillation; force/form closed; roller/flat faced)

    Type of cam( radial/axial)

    Distance between cam shaft and the center of the required oscillatory output

    Rotational speed of cam, loading on cam and follower, and masses to be moved

    Environmental and economical considerations

    Follower Motion

    Once a cam and follower pair has been chosen, the follower motion must be synthesized. In

    most cases a cam follower is required to be displaced through a specified rise or fall

    The shape of the displacement curve not important, but velocity , acceleration are of great

    importance

    Dimensional Synthesis of the Cam Profile

    Except in the case of radially translating point follower, interference of portions of a roller

    or flat face follower requires a more detailed cam profile synthesis procedure

  • 7/30/2019 Cam Second Lecture.ppt

    7/8

    Once the cam profile is synthesized, the design may not be acceptable for

    many reasons

    The pressure angle may be unacceptable The follower may not be able to follow the cam surface due to local

    curvature conditions

    Too large a return spring may be required to keep the follower in contact

    with the cam surface during the cycle

    Excessive dimensions may be required

    Usually following parameters can be varied to alleviate such problems

    Base circle diameter

    The offset of the follower travel (if a straight life translating follower is

    used) The relative locations of the fixed pivot of the follower arm to the center

    of the cam (if an oscillating follower is employed)

    Length of the follower arm

    Radius of the follower(if a roller or spherical follower is used)

    Cam Analysis

  • 7/30/2019 Cam Second Lecture.ppt

    8/8

    Choosing the Prime Circle

    Start with something about 3 times max lift h.

    Compute for all values ofq.

    Iterate to an acceptable condition.

    Maximum pressure angle for a translating roller

    follower should be < = 30 degrees.

    Eccentricity can be introduced to correctasymmetry in max and min if desired.