4.5 Mechanisms

4.5 Mechanisms

1. Gyroscopic Effects

  1. Gyroscopic Couple:

    • When axis of spinning rotor is rotated, couple acts perpendicular to both.

    • T=IωωpT = I \omega \omega_p

    • II = moment of inertia, ω\omega = spin speed, ωp\omega_p = precession speed.

  2. Applications:

    • Stabilization: Ships, aircraft, satellites.

    • Steering Effects:

      • Motorcycle/bicycle turning.

      • Ship rolling causes turning (gyroscopic action).

  3. Reactive Forces:

    • Act on bearings supporting rotating shaft.

    • Direction depends on spin and precession directions.

2. Governors and Flywheels

  1. Governors:

    • Speed-regulating devices for engines.

    • Types:

      • Centrifugal: Watt, Porter, Proell, Hartnell.

      • Inertia: More sensitive but less stable.

    • Terminology:

      • Sensitiveness: N1N2N\frac{N_1 - N_2}{N}.

      • Isochronous: Constant speed at all radii.

      • Hunting: Continuous speed fluctuations.

  2. Flywheels:

    • Energy storage devices to minimize speed fluctuations.

    • Function: Store energy during excess, release during deficit.

    • Coefficient of Fluctuation of Speed:

      • Cs=ωmaxωminωavgC_s = \frac{\omega_{max} - \omega_{min}}{\omega_{avg}}

    • Energy Storage:

      • ΔE=12I(ωmax2ωmin2)=Iω2Cs\Delta E = \frac{1}{2} I (\omega_{max}^2 - \omega_{min}^2) = I \omega^2 C_s

    • Mass Calculation: I=mk2I = mk^2, kk = radius of gyration.

3. Balancing

  1. Static Balancing:

    • For objects in single plane of rotation.

    • Center of mass on axis of rotation.

    • mr=0\sum m r = 0.

  2. Dynamic Balancing:

    • For objects with width/length.

    • Requires multiple correction planes.

    • Conditions:

      • mr=0\sum m r = 0 (static balance).

      • mrl=0\sum m r l = 0 (couple balance).

  3. Balancing of Rotating Masses:

    • Single Plane: Vector polygon method.

    • Multiple Planes: Two-plane balancing required.

  4. Balancing of Reciprocating Masses:

    • Primary Force: Fp=mrω2cosθF_p = m r \omega^2 \cos \theta.

    • Secondary Force: Fs=mrω2cos2θnF_s = m r \omega^2 \frac{\cos 2\theta}{n}.

    • Complete Balance impossible with single cylinder.

    • Multi-cylinder arrangements (inline, V, radial) provide partial balance.

4. Cam and Follower

  1. Components:

    • Cam: Rotating/oscillating member with shaped profile.

    • Follower: Reciprocating/oscillating output member.

  2. Follower Types:

    • Knife-edge, Roller, Flat-face, Spherical.

    • Motion Path: Translating or oscillating.

  3. Cam Terminology:

    • Base Circle: Smallest circle to cam profile.

    • Trace Point: Reference point on follower.

    • Pressure Angle: Angle between follower motion and normal to cam profile.

  4. Follower Motions:

    • SHM: Smooth acceleration but infinite jerk at ends.

    • Uniform Velocity: Discontinuous acceleration.

    • Uniform Acceleration: Constant acceleration, finite jerk.

    • Cycloidal: No abrupt changes in acceleration (preferred for high speed).

  5. Design Considerations:

    • Pressure angle should be small (<30°) to prevent jamming.

    • Smaller base circle increases pressure angle.

5. SHM and Cycloidal Motion

  1. Simple Harmonic Motion (SHM):

    • Displacement: s=h2(1cosθ)s = \frac{h}{2}(1 - \cos \theta).

    • Velocity: v=hω2sinθv = \frac{h\omega}{2} \sin \theta.

    • Acceleration: a=hω22cosθa = \frac{h\omega^2}{2} \cos \theta.

    • Characteristics: Smooth acceleration, infinite jerk at ends.

  2. Cycloidal Motion:

    • Displacement: s=h(θβ12πsin2πθβ)s = h\left(\frac{\theta}{\beta} - \frac{1}{2\pi} \sin\frac{2\pi\theta}{\beta}\right).

    • Velocity: v=hωβ(1cos2πθβ)v = \frac{h\omega}{\beta}\left(1 - \cos\frac{2\pi\theta}{\beta}\right).

    • Acceleration: a=2πhω2β2sin2πθβa = \frac{2\pi h\omega^2}{\beta^2} \sin\frac{2\pi\theta}{\beta}.

    • Advantage: Zero acceleration and jerk at ends (smooth).

6. Belt, Rope, Chain Drives

  1. Belt Drives:

    • Types: Flat, V-belt, Timing (synchronous).

    • Velocity Ratio: N1N2=D2D1\frac{N_1}{N_2} = \frac{D_2}{D_1} (neglecting slip).

    • Slip: Difference between theoretical and actual speed.

    • Creep: Due to elasticity of belt.

    • Power Transmission: P=(T1T2)vP = (T_1 - T_2)v.

    • Centrifugal Tension: Tc=mv2T_c = m v^2.

  2. Rope Drives:

    • For larger power and center distances.

    • Grooved pulleys for better grip.

  3. Chain Drives:

    • Positive drive (no slip).

    • Velocity Ratio: N1N2=T2T1\frac{N_1}{N_2} = \frac{T_2}{T_1}.

    • Length Calculation: L=2C+T1+T22+(T1T2)24π2CL = 2C + \frac{T_1+T_2}{2} + \frac{(T_1-T_2)^2}{4\pi^2 C}.

    • Polygon Effect: Causes speed variations.

7. Gears and Gear Trains

  1. Gear Terminology:

    • Module (m): m=DTm = \frac{D}{T}.

    • Circular Pitch (p): p=πmp = \pi m.

    • Pressure Angle (ϕ\phi): Standard 14.5°, 20°, 25°.

    • Addendum: Radial height above pitch circle.

    • Dedendum: Radial depth below pitch circle.

  2. Gear Types:

    • Spur: Parallel axes, teeth parallel to axis.

    • Helical: Smoother, quieter, axial thrust.

    • Bevel: Intersecting axes (usually 90°).

    • Worm: High reduction ratio, self-locking.

    • Rack and Pinion: Rotary to linear motion.

  3. Law of Gearing:

    • Common normal at point of contact must pass through pitch point.

    • Ensures constant velocity ratio.

  4. Gear Trains:

    • Simple: NlastNfirst=±Product of driving teethProduct of driven teeth\frac{N_{last}}{N_{first}} = \pm \frac{\text{Product of driving teeth}}{\text{Product of driven teeth}}.

    • Compound: Multiple gears on same shaft.

    • Epicyclic (Planetary):

      • VR=1+TsunTringVR = 1 + \frac{T_{sun}}{T_{ring}} (for simple planetary).

      • Solved using tabular method or relative velocity.

    • Reverted: Input and output shafts co-axial.

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