12. Design of Brakes and Clutches free study material

FeatureBrakeClutch
FunctionStops motionTransmits power
EnergyDissipates energy as heatTransfers energy
ApplicationVehicles, machinesGearboxes, engines

(a) Block or Shoe Brake

brakes and clutches

2. Working Principle

The brake works on the principle of friction. When a force is applied to the brake lever:

  1. The brake shoe moves toward the rotating wheel or drum.
  2. The friction lining on the shoe comes into contact with the wheel/drum surface.
  3. A frictional force develops between the shoe and the rotating member.
  4. This friction opposes the motion of the wheel/drum.
  5. The kinetic energy of the rotating system is converted into heat energy.
  6. As a result, the wheel/drum slows down and eventually stops.

The braking torque produced by a shoe brake is:TB=ฮผร—RNร—rT_B = \mu \times R_N \times rWhere:

  • TBT_BTBโ€‹ = Braking torque (Nยทm)
  • ฮผ\muฮผ = Coefficient of friction
  • RNR_NRNโ€‹ = Normal force between shoe and drum (N)
  • rrr = Radius of brake drum (m)

(b) Band Brake

  • Flexible band wraps around a drum
  • Types:
  • Simple band brake
  • Differential band brake

(c) Disc Brake

Widely used in automobiles

Friction pads act on a rotating disc

(d) Internal Expanding Brake

Shoes expand inside a drum

(a) Single Plate Clutch

  • One friction plate
  • Common in cars

(b) Multi Plate Clutch

  • Multiple plates โ†’ higher torque capacity

(c) Cone Clutch

  • Conical friction surfaces

(d) Centrifugal Clutch

  • Engages automatically with speed
  • High coefficient of friction
  • Good wear resistance
  • Heat resistance

Common materials:

  • Asbestos (older, now replaced)
  • Sintered metals
  • Ceramics
  • Organic friction materials

For Both Brakes and Clutches

  • Torque to be transmitted
  • Coefficient of friction
  • Heat generation and dissipation
  • Wear resistance
  • Operating conditions (dry/wet)
  • Safety and reliability

(a) Braking Torque

T=ฮผWRT = \mu W RT=ฮผWR

Where:

  • ฮผ\muฮผ = coefficient of friction
  • WWW = normal force
  • RRR = effective radius

(b) Energy Absorbed

E=12Iฯ‰2E = \frac{1}{2} I \omega^2E=21โ€‹Iฯ‰2

  • Must be dissipated as heat

(c) Heat Dissipation

  • Heat generated = heat dissipated
  • Prevents brake fading

(a) Torque Capacity (Uniform Pressure Theory)

T=ฮผW2(Ro+Ri)T = \frac{\mu W}{2} (R_o + R_i)

(b) Torque Capacity (Uniform Wear Theory)

T=ฮผWRmT = \mu W R_m

Where:

  • RmR_m = mean radius

(c) Power Transmitted

P=2ฯ€NT60P = \frac{2\pi N T}{60}

9. Uniform Pressure vs Uniform Wear

AspectUniform PressureUniform Wear
AssumptionPressure constantWear uniform
ApplicationNew clutchWorn clutch
AccuracyLess realisticMore realistic

10. Failure of Brakes and Clutches

  • Overheating
  • Excessive wear
  • Slippage
  • Material failure
  • Poor lubrication (for wet clutches)

11. External Sources


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