The simple harmonic motion is recommended for follower motion when cam rotates at low or moderate speeds.
FOLLOWER MOTION WITH SIMPLE HARMONIC MOTION
• The simple harmonic motion is
recommended for follower motion when cam rotates at low or moderate speeds.
• When a body rotates on a circular
path with uniform angular velocity, its projection on the diameter will have
simple harmonic motion (SHM).
• The velocity of the projection will
be maximum at the centre and ze at the ends of the diameter.
• In case of acceleration and
retardation, the values will be zero at the centre and maximum at the ends of
diameter.
• Accordingly, when a follower moves
with SHM during its outward stroke and return stroke, its motion will have the
same characteristics.
The
displacement diagram when the follower moves with SHM is shown in Fig.3.16.
The
displacement diagram can be constructed as follows:
Step 1:
Draw a semi-circle with lift (L) of the follower as diameter. This circle is
also known as harmonic circle.
Step 2:
Divide the semi-circle into any number of even equal parts (say 6 or 8).
Step 3:
Divide the outstroke angle (0 ̧) and return stroke angle (8,) into the same
number of equal parts.
Step 4:
Project intercepts on the semi-circle to corresponding divisions on the cam
displacement interval. Mark the points of intersection (A, B, C, .....) so
obtained.
Step 5:
Join the intersection points by free hand with a curve. The diagram so obtained
is the displacement curve for SHM.
(i) Displacement of the Follower
At
any instant, the displacement equation for the follower having SHM is given by
(ii) Velocity of the Follower
We
know that,
Velocity,
v = Rate of change of displacement with respect to time
v
= dy / dt
Velocity
of follower during outstroke is given by
Similarly,
the velocity of follower during return stroke is given by
Maximum velocity of follower during outward and return strokes:
Since
the variation in velocity is a sine curve, therefore the maximum velocity of
follower during outward stroke occurs at
Similarly,
the maximum velocity of follower during return stroke occurs at and is given
by
(iii) Acceleration of the Follower
We
know that, Acceleration = Rate of change of velocity with respect to time
a
= dv / dt
Acceleration
of follower during outward stroke is given by
Similarly,
acceleration of follower during return stroke is given by
Maximum
acceleration of follower during outward and return strokes
Since
the variation in acceleration is a cosine curve, therefore the maximum acceleration
of follower during outward stroke occurs at θ = 0 and θ = θ。.
Therefore,
substituting θ
= 0 and θ
= θ。in
equation (3.21), we get
(iv) Jerk of the Follower
We
know that,
Jerk
= Rate of change of acceleration with respect to time
Jerk,
j = da/dt
Jerk
of follower during outward stroke is given by
Similarly,
jerk of follower during return stroke is given by
Maximum
jerk of follower during outward and return strokes
Since
the variation in jerk is a sine curve, therefore the maximum jerk of follower
during outward 'stroke occurs at
• Fig.3.17
illustrates the displacement, velocity, acceleration and jerk diagrams when the
follower moves with SHM.
• From
Fig.3.17, the following points may be observed:
■
The velocity of the follower is zero at the beginning and at the end of its
strokes and increases gradually to a maximum at mid-stroke.
■
On the other hand, the acceleration of the follower is a maximum at the ends of
the stroke and decreases to zero at mid-stroke.
■
The jerk of the follower is zero at the beginning and at the end of its stroke
and increases gradually to a maximum at mid-stroke. However, there are two
infinite jerks at the beginning and end of stroke because a finite value of
acceleration is to be generated in no time.
• Because
of the presence of infinite jerks, the cam is subjected to large dynamic loads
which is not desirable. Hence the cams with SHM for followers are recommended
only. for low or moderate speeds.
Theory of Machines: Unit I: Kinematics of Mechanisms : Tag: : Kinematics of Mechanisms - Theory of Machines - follower motion with simple harmonic motion
Theory of Machines
ME3491 4th semester Mechanical Dept | 2021 Regulation | 4th Semester Mechanical Dept 2021 Regulation