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8/9/2019 Md-16 Clutches and brakes .pdf
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August 15, 2007August 15, 2007 11
16. Clutches and Brakes16. Clutches and Brakes
ObjectivesObjectives•• Recognize the basic geometries of clutch and brakeRecognize the basic geometries of clutch and brake
systems.systems.
•• Calculate the frictional forces and torque capabilitiesCalculate the frictional forces and torque capabilities
in brake systems.in brake systems.
•• Understand the principles of heat generation andUnderstand the principles of heat generation and
heat removal from brake systems.heat removal from brake systems.
•• Calculate frictional brake horsepower and recognizeCalculate frictional brake horsepower and recognize
how to use it.how to use it.
August 15, 2007August 15, 2007 22
IntroductionIntroduction
Clutch is a device that connects and disconnectsClutch is a device that connects and disconnects
two collinear shafts.two collinear shafts. Similar to couplingsSimilar to couplings
Friction and hence heat dissipationFriction and hence heat dissipation
Purpose of a brake is to stop the rotation of aPurpose of a brake is to stop the rotation of ashaft.shaft.
Braking action is produced by friction as aBraking action is produced by friction as astationary part bears on a moving part.stationary part bears on a moving part.
Heat dissipation is a problemHeat dissipation is a problem
Brake fade during continuous application of brakingBrake fade during continuous application of brakingdue to heat generateddue to heat generated
August 15, 2007August 15, 2007 33
Plate clutchPlate clutch
Uses Spring loaded flat surfaces
Transmit power in either direction
August 15, 2007August 15, 2007 44
Cone clutchCone clutch
Uses tapered friction surfaces
Easy to engage
August 15, 2007August 15, 2007 55
Caliper disc brakeCaliper disc brake
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Drum brakeDrum brake
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August 15, 2007August 15, 2007 77
Drum brakeDrum brake
August 15, 2007August 15, 2007 88
Block brakeBlock brake –– Wagon brakeWagon brake
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Band brakeBand brake
Belt wrapped around the wheel
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Fig. 16Fig. 16--7 Disc brake7 Disc brake
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Friction MaterialsFriction Materials
Asbestos fibers embedded in an epoxyAsbestos fibers embedded in an epoxy--type materialtype material
Good thermal propertiesGood thermal properties
High friction coefficient (0.35 to 0.50)High friction coefficient (0.35 to 0.50)
Environmental concernsEnvironmental concerns
Polymer compounds with impregnated materialPolymer compounds with impregnated material
Metal shavingsMetal shavings
GraphiteGraphite
Sintered ironSintered iron
August 15, 2007August 15, 2007 1212
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Torque and ForcesTorque and Forces
Sliding frictionSliding friction
Friction force, FFriction force, Ff f = f N= f N
f = coefficient of frictionf = coefficient of friction
N = normal force N = normal force
August 15, 2007August 15, 2007 1414
Plate type clutchPlate type clutch
Rotating torque,Rotating torque, TTf f ==
R R oo = outside radius= outside radius
R R ii = inside radius= inside radius
⎟ ⎠
⎞⎜⎝
⎛ +
2
R Nf io R
August 15, 2007August 15, 2007 1515
Plate type clutchPlate type clutch
Friction power can be calculated as,Friction power can be calculated as,
PPf f ==63,000
nTf
August 15, 2007August 15, 2007 1616
• A plate-type clutch has the following properties:
– Ro
= 12 in
– Ri= 9 in
– engagement force of 120 lb (normal force)
– turns at 2000 rpm
• Friction disc has coefficient of friction of .3.
• Determine torque and power that can be transmitted by this system.
Example Problem 16-1: Torques and Forces onClutches and Brakes
August 15, 2007August 15, 2007 1717
• Torque capacity:(16-2)
T f = f N( r o + r i )
2
T f = .3 (120 lb)
⎝
⎜⎛
⎠
⎟ ⎞
12 in + 9 in
2
T f = 378 in-lb
• Power:(16-3)
P f =T f n
63,000
P f =378 (2000)
63,000
P f = 12 hp
Example Problem 16-1: Torques and Forces on
Clutches and Brakes (cont’d.)
August 15, 2007August 15, 2007 1818
Example Problem 16-2: Torques and Forces on
Clutches and Brakes
• For the short-shoe drum brake
shown, determine the braking
torque for the following dimensions:
– a = 4 in
– L = 20 in
– D = 12 in
– f = .4
– W = 100 lb:
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August 15, 2007August 15, 2007 1919
• Find moments to determine normal force:
Σ M p = WL – a N
Σ M p = 100 lb 20 in – 4 in N
N = 500 lb
• Torque friction:
T f = f N D
2
T f = .4 (500 lb)12 in
2
T f = 1200 in-lb
• This analysis assumes the lever arms stay approximately horizontal.
Example Problem 16-2: Torques and Forces on
Clutches and Brakes (cont’d.)
August 15, 2007August 15, 2007 2020
Cone clutchCone clutch
This becomes a bit complicated because ofThis becomes a bit complicated because of
the cone anglethe cone angle
In this case the frictional force is given byIn this case the frictional force is given by
TTf f = F= Ff f r r mm= f N= f N r r mm
Normal force, N = Normal force, N =
FFaa = axial force= axial force
ΑΑ = cone angle= cone angle
αcosf αsin
Fa
+
August 15, 2007August 15, 2007 2121
Fig. 16.8 Cone clutch geometryFig. 16.8 Cone clutch geometry
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Cone clutchCone clutch
Combining the above two equations we getCombining the above two equations we get
αcosf αsin
Fr f T am
f +
=
August 15, 2007August 15, 2007 2323
Example Problem 16-3: Torques and Forces on
Clutches and Brakes
• For the cone clutch shown,
determine the torque-
transmitting capacity based on
the following parameters:
– Dmean
= 12 inches
– Fa
= 75 lb
– f = .35
– α = 20°
• Also solve if α = 10° and
compare the results.
August 15, 2007August 15, 2007 2424
(16-5)
T f = f r m F a
sin α + f cos α
T f =
.35⎝ ⎜⎛
⎠⎟ ⎞
12 in
2 75 lb
sin 20° + .35 cos 20°
T f = 235 in-lb
For α = 10°:
T f =
.35⎝ ⎜⎛
⎠⎟ ⎞
12 in
2 75 lb
sin 10° + .35 cos 10°
T f = 304 in-lb
• The smaller angle creates a greater wedging force and, correspondingly,larger torque capacity.
Example Problem 16-3: Torques and Forces on
Clutches and Brakes (cont’d.)
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August 15, 2007August 15, 2007 2525
Example Problem 16-4: Torques and Forces on
Clutches and Brakes
• A truck has total weight of 40,000 lb and is
traveling 60 mph.
• The brake design calls for it to be able to stop in
400 feet.
• Determine stopping force required.
• Determine stopping torque required if wheels are
36 inches in diameter.
• Determine torque per brake, assuming there are
10 sets of brakes.
• Assuming each brake is a disc brake with mean
radius of 10 inches, determine normal brake force if
f = .4.August 15, 2007August 15, 2007 2626
60 mph 5280 ft mile
hr 3600 sec
= 88 ft/sec
Example Problem 16-4: Torques and Forces on
Clutches and Brakes
•First, find the rate of deceleration. Converting 60 mph to ft/sec:
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• Find the stopping rate:
D = V a t
t = D
V a
t =400 ft
88
2 ft/sec
t = 9 sec
V = a t
a =V
t
a =88 ft/sec
9 sec
a = 9.8 ft/sec2
• Find the stopping force:
F =W
g a
F = 40,000 lb32.2 ft/sec2 9.8 ft/sec2
F = 12,100 lb
Example Problem 16-4: Torques and Forces on
Clutches and Brakes (cont’d.)
August 15, 2007August 15, 2007 2828
• Find the torque, if the wheels are 36 inches in diameter :
T = F r
T = 12,100 lb36 in
2
T = 217,800 in-lb
− For each wheel:T = 21,780 in-lb
− Braking normal force:(16-2)
T f = f N r m
N =T f
f r m
N =21,780 in-lb
.4 10 in
N = 5,450 lb
• This is a significant normal force, especially for a disc brake system.
Example Problem 16-4: Torques and Forces on
Clutches and Brakes (cont’d.)
August 15, 2007August 15, 2007 2929
Rotational Inertia and Brake PowerRotational Inertia and Brake Power
Inertia and frictional horsepower Inertia and frictional horsepower
Energy from rotating torqueEnergy from rotating torque
UUf f = F= Fππ
DD N Ntt == TTf f 22ππ
N Ntt
UUf f = Frictional work = Frictional work
D = effective diameter D = effective diameter
N Ntt = number of turns= number of turns
August 15, 2007August 15, 2007 3030
Rotational Inertia and Brake PowerRotational Inertia and Brake Power
Power associated with stoppingPower associated with stopping
TTf f inin--lblb
n rpmn rpm
t secondst seconds
t550
U
63,000
nTP f f
f ==
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Energy absorbed can be the potential energy orEnergy absorbed can be the potential energy or
the kinetic energythe kinetic energy Potential energy,Potential energy, ∆∆PE = W (hPE = W (h11 – – hh22))
Potential energy,Potential energy, ∆∆K K E =E = )V(Vg2
W 2
2
2
1 −
August 15, 2007August 15, 2007 3232
Heat generatedHeat generated
Temperature rise isTemperature rise is
c = specific heatc = specific heat
= 101 ft= 101 ft--lb/lb/lb/lb/°°F for cast ironF for cast iron
= 93 ft= 93 ft--lb/lb/lb/lb/°°F for steelF for steel
= 15 ft= 15 ft--lb/lb/lb/lb/°°F for aluminumF for aluminum
WWmm = weight of brake system that can absorb= weight of brake system that can absorbthe heatthe heat
cW
U∆T
m
f =
August 15, 2007August 15, 2007 3333
• 3500-pound automobile is traveling 50 mph
and decelerates on flat ground at a rate of
20 ft/sec2.
• Each of the four steel brake drums weighs
10 pounds.
• Assuming all heat is absorbed by the
drums during this period, find energy
absorbed, average frictional power, and
temperature rise of drums.
Example Problem 16-5: Rotational Inertia
and Brake Power
August 15, 2007August 15, 2007 3434
− Converting 50 mph to ft/sec:
50 mphhr
3600 sec
5280 ft
mile = 73 ft/sec
− Kinetic energy to be absorbed:(16-9)
KE =W V
2
2g
KE =3500 lb (73 ft)
2
2(32.2 ft/sec2) sec2
KE = 289,620 ft-lb
(Energy gain U = KE lost.)
Example Problem 16-5: Rotational Inertia
and Brake Power
August 15, 2007August 15, 2007 3535
(16-12)
U f = W c ∆ T
∆T =U f
W c
∆T =289,620 ft-lb
40 lb 93
ft-lb
lb°F
∆T = 78°
− Finding the stopping time:
∆V = a t
t =∆V
a
t =73 ft/sec
20 ft/sec2
t = 3.7 sec
Example Problem 16-5: Rotational Inertia
and Brake Power (cont’d.)
August 15, 2007August 15, 2007 3636
− Frictional power could then be found:
(16-7)
f hp =U f
550 t =
KE
550 t
f hp =289,620
550 (3.7)
f hp = 142
Example Problem 16-5: Rotational Inertia
and Brake Power (cont’d.)
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Automotive brakeAutomotive brake