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Universiti Tenaga Nasional, 2006 Mechanical Design and CAD Laboratory SLOTTED LINK MECHANISM EXPERIMENT OBJECTIVE The objective of this experiment is to investigate the motion of a slotted link and to see if the piston rod moves with Simple Harmonics Motion THEORY Simple Harmonic Motion is defined as when a mass or point moves in such a way that its accelerations is proportional to its displacement from a fixed point in its path and is directed to that point, the motion is said to be simple harmonic. The Simple Harmonic Circle enables us to establish a relationship between displacement and accelerations. Consider the diagram below: A B t ω O P ω x Q is a point which rotates at constant at constant velocity ω in a circle of a radius r. AB is a diameter and O the center of the circle of rotation. Point P is the projection of Q upon the diameter AB at any instant. The displacement of P from O is x. Clearly point P oscillates between A and B as q moves around the circle. So P can only have velocities along AB at any instant in time, similarly for accelerations. Now if we resolve the centripetal accelerations into two components parallel and perpendicular to AB, then the parallel components will represents the accelerations of P.

Slotted Link Mechanism

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  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    SLOTTED LINK MECHANISM EXPERIMENT

    OBJECTIVE

    The objective of this experiment is to investigate the motion of a slotted link and to see if

    the piston rod moves with Simple Harmonics Motion

    THEORY

    Simple Harmonic Motion is defined as when a mass or point moves in such a way that its

    accelerations is proportional to its displacement from a fixed point in its path and is

    directed to that point, the motion is said to be simple harmonic.

    The Simple Harmonic Circle enables us to establish a relationship between displacement

    and accelerations. Consider the diagram below:

    A B

    t

    O P

    x

    Q is a point which rotates at constant at constant velocity in a circle of a radius r. AB is

    a diameter and O the center of the circle of rotation. Point P is the projection of Q upon

    the diameter AB at any instant. The displacement of P from O is x. Clearly point P

    oscillates between A and B as q moves around the circle. So P can only have velocities

    along AB at any instant in time, similarly for accelerations. Now if we resolve the

    centripetal accelerations into two components parallel and perpendicular to AB, then the

    parallel components will represents the accelerations of P.

  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    BO

    Q

    Ptr cos.2

    t

    r

    a

    2

    =

    Acceleration parallel to AB given by this equation:

    trAB .cos.2 =

    Now displacement x is

    trx .cos. =

    So the accelerations of P is

    aP =

    xP 2=

    Thus the accelerations of P is proportional to its displacement, x, from O and is clearly

    towards O. Therefore the motion is Simple Harmonic Motions.

    Alternatively we may consider the following method:

    trx .cos. =

    trdt

    xd

    trdt

    dx

    .cos..

    .sin..

    2

    2

    2

    =

    =

    But: trx .cos. =

    trdt

    xd.cos..2

    2

    2

    =

    The minus sign indicates that the accelerations is to the left and thus the center of

    rotations O.

  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    What do you note about the displacement, velocity and accelerations? They vary

    sinusoidally

    Periodic Time

    This is the time taken for a complete oscillation from B to A and back again. The time

    taken is also that for a complete revolution of particle Q which is an angular distance is

    pi2 radians, so:

    pi

    2

    =

    However from previous analysis we know that:

    21

    =x

    a

    a

    xpi 2=

    Slotted Link Mechanism or Scotch Yoke

    The apparatus is diagrammatically below:

    It is clear that the driving pin which is fixed to the crank is similar to the point Q

    on the SHM circle. The piston rod with a slotted link is constrained to move is a straight

    line. The limits of the motions are either end of a diameter of the circle of the drive pin

    rotations. So the motions of the slotted link and piston rod are identical to point P in the

    foregone analysis. Thus the link and anything attached there to will move with SHM.

  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    APPARATUS

    Slotted link Mechanism

  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    PROCEDURES

    1. Set the crank at zero degrees. Record the piston displacement.

    2. Move the crank by 10 and record the displacement.

    3. Repeat steps 1 and 2 for one complete revolution of the crank.

    4. Tabulate your results in the table given.

    5. Calculate the theoretical piston rod displacement in the table.

    RESULTS

    1. Plot a graph of the experimental piston rod displacement versus crack angle.

    2. Plot on the same graph the theoretical piston rod displacement against crank angle

    3. From the experimental piston rod displacement data plot a graph of experimental

    velocity and accelerations versus crank angle.

    4. From the theoretical Simple Harmonic Motion equations, plot a graphs of

    theoretical velocity and accelerations versus crank angle.

    DISCUSSION

    1. Prove the theoretical displacement ( )cos1= rx

    2. Compare the experimental and theoretical piston rod displacement, velocity and

    accelerations. How well do your experimental results agree with theory?

    3. What is the motion produced by the Slotted Link mechanism? Explain your

    answer.

    4. Where do maximum displacement, velocity and acceleration on the slide occur?

    Explain your answer

    5. Where does the maximum force on the drive pin occur? Explain your answer

  • Universiti Tenaga Nasional, 2006

    Mechanical Design and CAD Laboratory

    RESULT SHEET

    Slotted Link Mechanism Experiment

    Crank Radius = 35 mm

    Crank Angles, (degrees)

    Experimental Piston Rod

    displacement, x, (mm)

    Theoretical,

    ( )cos1= rx (mm) 0

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