The term coupling is a device used to connect two shafts together at their ends for transmitting the power. There are a number of coupling devices used to couple two shafts but in this chapter, only a few important couplings have been introduced for an understanding of the students. There are two general types of couplings: (i) rigid, and (ii) flexible.
Rigid couplings are designed to draw two shafts together tightly so that no relative motion can occur between them. This design is used for some special kinds of equipment in which precise alignment of two shafts is required. In such cases, the coupling must be capable of transmitting the torque in the shafts. Rigid couplings should be used only when the alignment of the two shafts can be maintained very accurately, not only at the time of installation but also during operation. If significant angular, radial or axial misalignment occurs, stresses that are difficult to predict and that may lead to early failure due to fatigue will be induced in the shafts. The load path is from the driving shaft to its flange, through the bolts, into the mating flange, and out to the driven shaft. The torque places the bolts in shear.
It consists of two cast iron flanges which are keyed to the shafts to be joined as shown in Figure 16.1. The flanges are brought together and are bolted in the annular space between the hub and the projecting flange. The protective flange is provided to guard the projecting bolt heads and nuts. The bolts are placed equispaced on a bolt circle diameter and the number of bolts depends on the shaft diameter d.
FIGURE 16.1
Rigid Flange Coupling
Advantages of Rigid Flange Coupling
Disadvantages of Rigid Flange Coupling
In a rigid coupling, the torque is transmitted from one-half of the coupling to the other through the bolts and in this arrangement, shafts need be aligned very well. However, in the bushed coupling, the rubber bushings over the pins (bolts) (as shown in Figure 16.2) provide flexibility and these coupling can accommodate some misalignment. Because of the rubber bushing, the design for pins should be considered carefully.
FIGURE 16.2
Flexible Bushed Coupling
Advantages of Flexible Bushed Coupling
Disadvantages of Flexible Bushed Coupling
To accommodate misalignment between mating shafts for more than the 3°, a universal joint is used. Angular misalignments of up to 45° are possible at low rotational speeds with single universal joints. It consists of two yokes, a center bearing block, and two pins that pass through the block at right angles. Approximately 20 to 30° is more reasonable for speeds about 10 rpm. Since universal joints have the disadvantage that the rotational speed of the output shaft is non-uniform in relation to the input shaft. A double universal joint allows the connected shafts to be parallel and offset by large amounts as shown in Figure 16.3. Furthermore, the second joint cancels the non-uniform oscillation of the first joint so the input and the output rotate at the same speed.
FIGURE 16.3
Universal Joint
Clutch is a device which is used to engage and disengage the driven shaft from driving shaft during the motion to change the gears meshing without stopping the driving shaft. Its operation is based on the friction between two surfaces; friction torque is applied by the driving shaft on the driven shaft.
Clutch may be classified as:
In a single plate clutch, a flywheel ‘A’ is bolted to a flange on the driving shaft B. The friction plate C is fixed to a hub which can slide on the spline i.e., driven shaft ‘D’. Two rings of friction material are riveted to flange ‘A’ and the plate ‘C’. The pressure plate ‘E’ is bushed internally, so as to revolve freely on shaft D and is integrated with withdrawal force F. A number of spiral springs are arranged around the clutch at ‘S’ as shown in Figure 16.4 (a), which provides axial thrust between friction surfaces.
FIGURE 16.4
(a) Single Plate Clutch (b) Friction Plate
When the withdrawal force is removed, the spring forces the pressure plate ‘E’ against the ring G. The friction between the contact surfaces of rings ‘G’ and plate ‘C’ transmits a torque on ‘D’ and driven shaft starts to rotate.
Let W = axial load on the plate
T = torque transmitted by clutch
P = axial pressure intensity
r1 and r2 = external and internal radii of friction plate
μ = coefficient of friction
Axial force on a small elemental ring of radius r and width dr, δW = P × 2πrdr
Frictional force, Fr = μδW = μ × P × 2πrdr
Torque, δT = Fr × r = μ × P × 2πrdr × r = μP2πr2dr
Now, there are two conditions: (i) Uniform pressure for new clutch plate, and (ii) uniform wear for old or weared clutch plate.
Putting the value of P, we get
where R is mean radius and equals to
Case II: Uniform Wear
or P × r = constant, C
Normal force on the ring
Total force on the friction plate,
or
Putting the value of C, we get
where R is mean radius and equals to
A single plate disc clutch, both sides effective, has outer and inner radii as 250 mm and 150 mm. The maximum intensity of pressure at any point in the contact surface is not to exceed 0.1 N/mm2. If the coefficient of friction is 0.25, find the power transmitted by the clutch at a speed of 3,000 rpm: (i) assuming uniform wear, and (ii) assuming uniform pressure.
W = P × 2πr2 (r1 − r2) = 0.1N / mm2 × 2π × 150 mm (250 mm − 150 mm)
= 9424.77 N
Mean radius,
Torque, T = n × µ × W × R = 2 × 0.25 × 9424.77 N × 0.2 m = 942.47 Nm.
Power,
W = P × π (r12 − r22 ) = 0.1N / mm2 × π((250 mm)2 − (150mm)2 ) = 12566.371N
Mean radius,
Torque, T = n × µ × W × R = 2 × 0.25 × 12566.371N × 0.204 m = 1282.871Nm.
Power,
A single plate disc clutch has both of its sides effective, transmits power at 250 rpm. The coefficient of friction is 0.25. The outer and inner radii of the friction plate are 100 mm and 40 mm, respectively. Assuming uniform wear of the clutch, the maximum pressure intensity is 0.1 N/mm2. If the moment of inertia of the rotating part of the clutch is 8 kgm2, calculate the time to attain the full speed by the machine and the energy lost during slipping of the clutch.
Assuming uniform pressure, find the intensity of pressure and compare the power transmitted with uniform wear to that with uniform pressure.
SOLUTION
W = P × 2πr2 (r1 − r2 ) = 0.1N / mm2 × 2π × 40 mm (100 mm − 40 mm) = 1507.96 N
Mean radius,
Torque, T = n × µ × W × R = 2 × 0.25 × 1507.96N × 0.07m = 52.774Nm.
Power,
Also,
Energy loss during slipping period
Mean radius,
Torque, T = n × µ × W × R = 2 × 0.25 × 1507.96 N × 0.074 m = 56 Nm.
Power,
The function of multi-disc clutch is similar to the single plate clutch but the number of discs in the multi-disc clutch is more than one, i.e., ‘n’ as shown in Figure 16.5.
FIGURE 16.5
Multi-disc Clutch
Torque for Uniform Pressure
Torque for Uniform Wear
A multi-disc clutch has 4-discs on the driving shaft and 3-discs on the driven shaft. The outside diameter of the contact surface is 240 mm and inside diameter 160 mm. Assuming uniform wear and coefficient of friction as 0.25, find the maximum axial intensity of pressure between the discs for transmission of 20 kW at 1,200 rpm.
Number of pair of contact surfaces = n1 + n2 − 1 = 4 + 3 − 1 = 6
Power
Considering uniform wear
Mean radius,
Torque,
FIGURE 16.6
Cone Clutch
In cone clutch, the friction surfaces make a cone of an angle 2β (Figure 16.6). The normal force on the cone is where β is the semi-cone angle. The main advantage of cone clutch is that the normal force is increased, since sin β ≤ 1.
Torque for Uniform Pressure
Torque for Uniform Wear
A cone clutch having a mean diameter of 200 mm and semi-cone angle of 12.5° transmits a torque of 200 Nm. The maximum normal pressure at the mean radius is 0.1 N/mm2. The coefficient of friction is 0.25. Calculate the width of the contact surface. Also, find the axial force to engage the clutch.
SOLUTION
T = µ × Fa × Rm × cosecβ
Also,
or,
A cone clutch has a cone angle of 30°. The maximum pressure between contact surfaces is limited to 0.25 N/mm2 and width of the contact surface is half of the mean radius. Find the radii of the conical surface to transmit 20 kW at 1500 rpm assuming uniform wear condition. Coefficient of friction is 0.25.
Solving Equations (16.1) and (16.2), we get
Centrifugal clutch works on the principle of centrifugal force. When the driving shaft rotates at high speed, the shoes move radially outward. The outer surfaces of the shoes are covered with friction material which engages the pulley. Thus, pulley rotates with the driving shaft. The engagement of shoes with the pulley is shown in Figure 16.7. This type of clutch is generally used in motor pulley. The spring force resists the centrifugal force, thus prevents the engagement at a lower speed.
where ω is the angular speed of the shaft.
Torque, T = F × R = μ.n.( Fc − Fs ).R
where n is a number of shoes.
FIGURE 16.7
Centrifugal Clutch
There are four shoes in a centrifugal clutch. The mass of each shoe is 10 kg and when the clutch is at rest, the force exerted by spring on the shoe is 400 N. The clearance between shoe and drum surface is 4 mm. Spring constant is 40 N/mm. The distance of the center of mass of shoe from the axis is 150 mm. The internal diameter of the drum is 320 mm. The coefficient of friction is 0.025; find the power transmitted by the clutch at 400 rpm.
SOLUTION
Operating radius, r1 = 150 + 4 = 154 mm.
Centrifugal force,
Spring force, Fs = 400 N + Kx = 400 N + 40N / mm × 4mm = 560 N
Tangential frictional force, Ft = µ(Fc − Fs ) = 0.25 × (2702.07 N − 560 N) = 535.51N
Power transmission
Brake is a device which is used to bring the body into rest while it is in motion or to hold a body in a state of rest by applying resisting force. There are four types of brakes as given below:
In this brake, a shoe or block is pressed against the drum. The force can be increased by using a lever as shown in Figure 16.8. The brake lining for friction is made of softer materials so that it can be replaced easily after wearing.
Let r = radius of drum
µ = Coefficient of friction
RN = Normal reaction on the shoes
P = Force applied on lever
F = Frictional force
In Figure 16.8 (a), taking moment about the pivot for clockwise rotation of drum
or
or
or
For anticlockwise rotation of drum,
In Figure16.8 (b), taking moment about pivot for clockwise rotation of drum
For anticlockwise rotation,
Due to pressure applied by single shoe, there is a side thrust on the shaft of the drum. To counter balance the side thrust, two shoes may be used opposite to each other. In this case, braking torque becomes double which is shown in Figure 16.8 (c).
A single block brake as shown in Figure 16.8 (b) has a diameter of brake drum 1.2 m. It can withstand 250 Nm torque at 500 rpm and coefficient of friction between block and drum is 0.3. Determine the force required to apply when the drum rotates in (a) clockwise direction and (b) anticlockwise direction. The angle of contact is 2θ = 30° and x = 140 mm, a = 30 mm, l = 1000 mm.
SOLUTION
For clockwise rotation
For anticlockwise rotation
= 182 N
In a double block spring loaded brake as shown in Figure 16.8 (c) following dimensions have been given: drum diameter = 600 mm, angle of contact (2θ) = 100°, coefficient of friction (μ) = 0.3, force applied on the spring = 6 kN, x = 0.5 m, l = 1m, c = 0.1 m. Find the braking torque applied.
For left side block
Taking moment about o.
or, 6000 N × 1m + 0.336 × RN1 (0.3m − 0.05m) − RN1 × 0.5m = 0
or,
For right side block
or, 6000 N × 1m − 0.336 × RN1 (0.3m − 0.05m) + RN1 × 0.5m = 0
or, RN2 = 10273.973N
Maximum braking torque, TB = µ'(RN1 + RN2 ) × r
= 0.336 × (14423.07 N + 10273.973 N ) × 0.3m = 2489.461 Nm
Band brake consists of a band in the form of belt, rope or steel band (Figure 16.9). When force is applied at the free end of the lever, the brand is pressed against the external surface of the drum.
Braking torque, T = (T1 – T2) × r
But where T1 is tension on tight side and T2 is tension in the slack side.
The effectiveness of braking force varies according to the direction of rotation of the drum, the ratio of length a and b, and the direction of force applied at the end of the lever.
Case I: when a > b and F acts in downward direction and drum rotates in counter clockwise direction.
Case II: when a < b and F acts in downward direction and drum rotates in clockwise direction. In this case, the tensions on the tight side and slack side are reversed, i.e., T2 > T1 and a > b. Brake will be effective only when T1a > T2b.
When becomes zero or negative, i.e., the brake becomes self-locking.
Case III: When a < b and F acts in upward direction and drum rotates in counter clockwise direction.
or
As T2 < T1 and b > a, brake will be effective only when T2 × b > T1 × a or
If brake becomes self-locking since force required is zero or negative.
Case IV: When a < b and F acts in upward direction and drum rotates in clockwise direction. T2 > T1 and b > a. when a = b, the band cannot be tightened and thus, the brake cannot be applied.
In a differential band brake as shown in Figure 16.9 (a), following data are given:
Drum diameter = 1000 mm, a = 50 mm, b = 250 mm, θ = 270°, μ = 0.3, r = d/2 = 5000 mm, F = 500 N, l = 1200 mm. Calculate braking torque.
SOLUTION
F × l − T1 × a − T2 × b = 0
T1 = 4.111T2
Now, F × l + 4.111T2 × a − T2 × b = 0 or 500 × 1200 + 4.111T2 × 5 − T2 × 250 = 0
⇒ T2 = 13498.313N
T1 = 55491.564N
Braking torque, TB = (T1 − T2) × r = (55491.564 − 13498.313) × 500 = 20.99 kNm
F × l − T1 × a − T2 × b = 0 and
or 500 × 1200 + T1 × 50 − 4.111 T1 × 250 = 0
60,000 + T1 (50 − 1027.75) = 0
T1 = 613.65N; T2 = 2522.73N
Braking torque, TB = (T2 − T1 ) × 500 = (2522.73 − 613.65) × 500
= 954.54 Nm
This is a combination of band and block brake. A number of blocks are mounted on the drum and inside the band and brake is applied by pressing the blocks against the drum with the help of the band. To increase the effectiveness of brake blocks are used under the band since blocks have a higher coefficient of friction.
Let T0 = Tension in band on slack side
T1 = Tension in band after one block
-----------------------------------------------
-----------------------------------------------
T = Tension in band after nth block
μ = coefficient of friction
Forces on the block are shown in Figure 16.10 (b).
(T1 − T0 )cosθ = µRN and (T1 + T0 )sinθ = RN
or
or
Similarly,
There are 15 blocks in a band and block brake. Each block subtends 30° angle at center. The data given for the brake are: radius of drum = 250 mm, block thickness = 50 mm, coefficient of friction = 0.3, a = 500 mm, b = 40 mm, F = 300 N, l = 1000 mm. Calculate the braking torque.
SOLUTION
Here, a > b, therefore, F should be downward and drum rotates in clockwise direction.
Taking moment about fulcrum, we get
Braking torque, TB = (Tn − T0 ) × (r + t) = (64615.3 N − 5769.2 N)(0.125m + 0.025m)
Internal expanding shoe brake has two semicircular shoes which are lined with friction materials. The outer diameter of the shoe is less than the inner diameter of the drum so that the drum can rotate freely. When the brake is applied, the shoes expand and press the inner surface of the drum and resist the motion. Working of internal expanding shoe brake is shown in Figure 16.11.
It is used in an automobile. It is self-energizing and good heat dissipative. A hydraulic pressure is generated in piston-cylinder arrangement. This hydraulic force is applied equally to both the shoes in the direction shown in Figure 16.11 (a). For counterclockwise rotation of the drum, the left shoe is primary leading shoe while the right shoe is secondary or trailing shoe. The pressure at any point A on the surface will be proportional to its distance l from the pivots.
Normal pressure, PN = K1 × l × cos(90°− β ) = K1 × l × sin β
The normal pressure will be maximum when θ is equal to 90°. Thus PNmax = K2 = PlN
PlN = Maximum pressure interfaced by leading shoe.
PN = K2 sinθ = PlN sinθ
Let b = width of brake lining
µ = coefficient of friction
consider a small element of brake lininon the leading shoe that makes an angle δθ at the center.
Taking moment about fulcrum O1, we get
or
Similarly, taking moment about fulcrum O2, we get
Here, t superscript is used for trailing shoe.
Thus, the maximum pressure intensities on leading and trailing shoes can be determined.
where R is mean radius and equals to
where R is mean radius and equals to
Torque, T = F × R = μ.n.(Fc – Fs).R where n is a number of shoes.
Braking torque;
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