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An in-depth analysis of various types of power transmission systems, focusing on belts, ropes, and chains. It covers the design and functionality of flat belts, v-belts, stepped pulleys, cone pulleys, ropes, and chains. The document also includes formulas for calculating belt length and chain length, as well as discussions on speed ratios and directional relations of shafts connected by belts.
Typology: Summaries
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Elements Of Mechanism Sixth Edition
When the distance between the
driving shaft and the driven shaft
is too great (usually less than 6 ft)
to be connected by gears, a
flexible connector is used. If the
wheel A, Fig. 12-1 , is turning at a
certain angular speed about the
axis S, its outer surface will have a
linear speed dependent upon the
angular speed and the diameter
of A.
For convenience the word band may be used as a general term to denote all kinds of
flexible connectors.
Bands for communicating continuous motion are endless.
Bands for communicating reciprocating motion are usually made fast at their ends to
the pulleys or drums which they connect.
1. Belts made of leather, rubber, or woven fabrics are flat and thin,
and require pulleys nearly cylindrical with smooth surfaces. Flat
belts are used to connect shafts as much as 30 ft apart.
Belts may be run economically at speeds
as high as 4500 fpm. Belts are also made
with V-shaped cross section to be used on
grooved pulleys. V-belts are usually used
for connecting shafts which are less than
15 ft apart. Speed ratios up to 7 to 1 and
belt speeds up to 5000 fpm may be used.
surface i is drawn firmly against the surface of the pulley while the
The outer part of the belt must therefore
stretch somewhat and the inner part
compress. There will be some section
between i and o which is neither
stretched nor compressed, and the
name neutral section may be given to
this part of the belt.
surface o bends over a circle whose
radius is greater than that of the surface
of the pulley by an amount equal to the
belt thickness 2p.
In a flat belt the neutral section may be assumed to be halfway
between the outer and inner surfaces. An imaginary cylindrical surface
around the pulley, to which the neutral section of the belt is tangent, is
the pitch surface of the pulley, the radius of this being the effective
radius of the pulley. A line in the neutral section of the belt at the
center of its width is the line of connection between two pulleys and is
tangent to the pitch surfaces, and coincides with a line in each pitch
surface known as the pitch line.
That is, the angular speeds of the shafts are in the inverse ratio of the
effective diameters of the pulleys, and this ratio is constant for circular
pulleys. As the thickness of belts generally is small as compared with
the diameters of the pulleys, it may be neglected. The speed ratio will
then become
which is the equation almost always used in practical calculations.
The relative directions in which the pulleys tum depend upon the manner in which
the belt is put on the pulleys. The belt shown in Fig. 12-1 is known as an open belt
and the pulleys turn in the same direction as suggested by the arrows.
The belt shown in Fig. 12-4 is known as a crossed belt and the pulleys turn in
opposite directions as indicated.
Leather belts are made by gluing or riveting together strips of leather
cut lengthwise of the hide, near the animal's back. If single thicknesses
of the leather are fastened end to end, the belt is known as a
single belt and is usually about 3/16 in. thick.
If two thicknesses of leather are glued together, flesh side to flesh side,
the belt is known as a double belt and is from 5/16 in. to 3/8 in. thick.
The manner of uniting the ends of the strips to form a belt, and of
fastening together the ends of the belt to make a continuous band for
running over pulleys, is very important.
The amount of power which a given belt can transmit depends upon its
speed, its strength, and its ability to adhere to the surf ace of the
pulleys. The speed is usually assumed to be the same as the surface
speed of the pulleys. The strength, of course, depends upon the width
and thickness and upon the nature of the material of which the belt is
made. The ability to cling to the pulley in order to run with little or no
slipping depends upon the condition of the pulley surfaces and of the
surface of the belt which is in contact with the pulleys, and upon the
tightness with which the belt is stretched over the pulleys.
Suppose now that some external force is applied to the shaft S causing
it to tend to turn in the direction indicated by the arrow. This tendency
to turn will increase the tension in the lower part of the belt (say
between m and n) and decrease the tension in the upper part. Let the
new tension in the lower or tight side of the belt be represented by T 1
(which is greater than T 0
) and the tension in the upper or slack side by
2
(which is less than T 0
If the belt sticks to the pulley B so that there is no slipping, the force T 1
tends to cause the pulley B to turn as shown by the full arrow, and the
force T 2
tends to cause B to turn as shown by the dotted arrow. As soon
as T 1
becomes enough greater than T 2
to overcome whatever resistance
the shaft S offers to turning, the pulleys will begin to turn in the
direction of the full arrow. The unbalanced force, then, which makes
the driven pulley B turn is the difference between the tension T 1
on the
tight side of the belt and the tension T 2
on the slack side of the
belt. This difference in tensions is
called the effective pull of the belt
and is here represented by the
letter E.