Take a pencil and a book to do an experiment as shown above. Make the book an inclined plane and use the pencil as a slider (use your hand as a guide). When you move the book smoothly upward, what happens to the pencil? It will be pushed up along the guide. By this method, you have transformed one motion into another motion by a very simple device. This is the basic idea of a cam. By rotating the cams in the figure below, the bars will have either translational or oscillatory motion.
The transformation of one of the simple motions, such as rotation, into any other motions is often conveniently accomplished by means of a cam mechanism A cam mechanism usually consists of two moving elements, the cam and the follower, mounted on a fixed frame. Cam devices are versatile, and almost any arbitrarily-specified motion can be obtained. In some instances, they offer the simplest and most compact way to transform motions.
A cam may be defined as a machine element having a curved
outline or a curved groove, which, by its oscillation or rotation
motion, gives a predetermined specified motion to another element
called the follower . The cam has a very important function
in
the operation of many classes of machines, especially those of the
automatic type, such as printing presses, shoe machinery, textile
machinery, gear-cutting machines, and screw machines. In any class of
machinery in which automatic control and accurate timing are
paramount, the cam is an indispensable part of mechanism. The possible
applications of cams are unlimited, and their shapes occur in great
variety. Some of the most common forms will be considered in this
chapter.
We can classify cam mechanisms by the modes of input/output motion, the configuration and arrangement of the follower, and the shape of the cam. We can also classify cams by the different types of motion events of the follower and by means of a great variety of the motion characteristics of the cam profile. (Chen 82)
Rotating Cam, Translating Follower
Load the SimDesign file simdesign/cam.translating.sim. If you
turn the cam, the follower will move. The weight of the follower
keeps them in contact. This is called a gravity constraint cam.
Rotating Cam/Rotating Follower
The SimDesign file is simdesign/cam.oscillating.sim. Notice
that a roller is used at the end of the follower. In addition, a
spring is used to maintain the contact of the cam and the roller.
If you try to calculate the degrees of
freedom (DOF) of the mechanism, you must imagine that the roller
is welded onto the follower because turning the roller does not
influence the motion of the follower.
Figure 6-10 illustrates some cam nomenclature:
When the cam turns through one motion cycle, the follower executes a
series of events consisting of rises, dwells and returns. Rise
is the motion of the follower away from the cam center, dwell
is the motion during which the follower is at rest; and return
is the motion of the follower toward the cam center.
There are many follower motions that can be used for the rises and the
returns. In this chapter, we describe a number of basic curves.
If the motion of the follower were a straight line, Figure 6-11a,b,c, it would have equal displacements
in equal units of time, i.e., uniform velocity from the
beginning to the end of the stroke, as shown in b. The acceleration,
except at the end of the stroke would be zero, as shown in c. The
diagrams show abrupt changes of velocity, which result in large forces
at the beginning and the end of the stroke. These forces are
undesirable, especially when the cam rotates at high velocity. The
constant velocity motion is therefore only of theoretical
interest.
(6-1)
Constant acceleration motion is shown in Figure 6-11d, e, f. As indicated in e, the velocity
increases at a uniform rate during the first half of the motion and
decreases at a uniform rate during the second half of the motion. The
acceleration is constant and positive throughout the first half of the
motion, as shown in f, and is constant and negative throughout the
second half. This type of motion gives the follower the smallest
value of maximum acceleration along the path of motion. In high-speed
machinery this is particularly important because of the forces that
are required to produce the accelerations.
When (6-2)
Figure 6-2 Classification of cam mechanisms
4.2.1 Modes of Input/Output Motion
The follower arm swings or oscillates in a circular arc with respect
to the follower pivot.
The follower system revolves with respect to the center line of the
vertical shaft.
Figure 6-3 Translating cam - translating follower
6.2.1 Follower Configuration
6.2.2 Follower Arrangement
The center line of the follower passes through the center line of the
camshaft.
The center line of the follower does not pass through the center line
of the cam shaft. The amount of offset is the distance between
these two center lines. The offset causes a reduction of the side
thrust present in the roller follower.
6.2.3 Cam Shape
The follower moves in a plane perpendicular to the axis of rotation of
the camshaft. A translating or a swing arm follower must be
constrained to maintain contact with the cam profile.
This is a plate cam with the follower riding in a groove in the face
of the cam.
Figure 6-4 Grooved cam
The roller follower operates in a groove cut on the periphery of a
cylinder. The follower may translate or oscillate. If the cylindrical
surface is replaced by a conical one, a conical cam results.
This cam has a rotating portion of a cylinder. The follower translates
or oscillates, whereas the cam usually rotates. The end cam is rarely
used because of the cost and the difficulty in cutting its contour.
Figure 6-5 Cylindrical cam and end cam
6.2.4 Constraints on the Follower
The weight of the follower system is sufficient to maintain contact.
The spring must be properly designed to maintain contact.
A groove maintains positive action.
(Figure 6-4 and Figure 6-5a)
For the cam in Figure 6-6, the follower has two rollers, separated by a fixed
distance, which act as the constraint; the mating cam in
such an arrangement is often called a constant-diameter cam.
Figure 6-6 Constant diameter cam
A mechanical constraint cam also be introduced by employing a dual or
conjugate cam in arrangement similar to what shown in Figure 6-7.
Each cam has its own roller, but the rollers are mounted on the same
reciprocating or oscillating follower.
Figure 6-7 Dual cam
6.2.5 Examples in SimDesign
Figure 6-8 SimDesign translating cam
6.3 Cam Nomenclature
Figure 6-10 Cam nomenclature
6.4 Motion events
Figure 6-11 Motion events
6.4.1 Constant Velocity Motion
6.4.2 Constant Acceleration Motion
,
(6-3)
A cam mechanism with the basic curve like g in Figure 6-7g will impart simple harmonic motion to the follower. The velocity diagram at h indicates smooth action. The acceleration, as shown at i, is maximum at the initial position, zero at the mid-position, and negative maximum at the final position.
(6-4)
The translational or rotational displacement of the follower is a function of the rotary angle of the cam. A designer can define the function according to the specific requirements in the design. The motion requirements, listed below, are commonly used in cam profile design.
Figure 6-12 is a skeleton diagram of a disk cam with a knife-edge translating follower. We assume that the cam mechanism will be used to realize the displacement relationship between the rotation of the cam and the translation of the follower.
Below is a list of the essential parameters for the evaluation of these types of cam mechanisms. However, these parameters are adequate only to define a knife-edge follower and a translating follower cam mechanism.
The method termed inversion is commonly used in cam profile design. For example, in a disk cam with translating follower mechanism, the follower translates when the cam turns. This means that the relative motion between them is a combination of a relative turning motion and a relative translating motion. Without changing this feature of their relative motion, imagine that the cam remains fixed. Now the follower performs both the relative turning and translating motions. We have inverted the mechanism.
Furthermore, imagine that the knife-edge of the follower moves along the fixed cam profile in the inverted mechanism. In other words, the knife edge of the follower draws the profile of the cam. Thus, the problem of designing the cam profile becomes a problem of calculating the trace of the knife edge of the follower whose motion is the combination of the relative turning and the relative translating.
In Figure 6-13, only part of the cam profile AK is displayed. Assume the cam turns clockwise. At the beginning of motion, the knife edge of the follower contacts the point of intersection A of the base circle and the cam profile. The coordinates of A are (So, e), and So can be calculated from equation
Suppose the displacement of the follower is S when the angular displacement of the cam is . At this moment, the coordinates of the knife edge of the follower should be (So + S, e).
To get the corresponding position of the knife edge of the follower in the inverted mechanism, turn the follower around the center of the cam in the reverse direction through an angle of . The knife edge will be inverted to point K, which corresponds to the point on the cam profile in the inverted mechanism. Therefore, the coordinates of point K can be calculated with the following equation:
(6-5)
Suppose the cam mechanism will be used to make the knife edge oscillate. We need to compute the coordinates of the cam profile that results in the required motion of the follower.
The essential parameters in this kind of cam mechanisms are given below.
The fundamental principle in designing the cam profiles is still inversion, similar to that that for designing other cam mechanisms, (e.g., the translating follower cam mechanism). Normally, the follower oscillates when the cam turns. This means that the relative motion between them is a combination of a relative turning motion and a relative oscillating motion. Without changing this feature of their relative motion, let the cam remain fixed and the follower performs both the relative turning motion and oscillating motion. By imagining in this way, we have actually inverted the mechanism.
In Figure 6-15, only part of the cam profile BK is shown. We assume that the cam turns clockwise.
At the beginning of motion, the knife edge of the follower contacts the point of intersection (B) of the base circle and the cam profile. The initial angle between the follower (AB) and the line of two pivots (AO) is 0. It can be calculated from the triangle OAB.
When the angular displacement of the cam is , the oscillating displacement of the follower is which measures from its own initial position. At this moment, the angle between the follower and the line passes through two pivots should be +0.
The coordinates of the knife edge at this moment will be
(6-6)
(6-7)
The basic principle of designing a cam profile with the inversion method is still used. However, the curve is not directly generated by inversion. This procedure has two steps:
The problem of calculating the coordinates of the cam profile is the problem of calculating the tangent points of a sequence of rollers in the inverted mechanism. At the moment shown Figure 6-17, the tangent point is P on the cam profile.
The calculation of the coordinates of the point P has two steps:
Since we have already have the coordinates of point K: (x, y), we can express the coordinates of point P as
(6-8)