KINETICS OF MECHANISM

  • Applied loads
  • Gravity forces
  • Spring forces

3.2 Internal Forces

3.3 Inertia Forces

  • Due to acceleration of mass
  • Opposes motion (Newtonโ€™s Second Law)

F=mโ‹…aF = m \cdot a

This is the foundation of kinetics analysis.

So,โˆ‘F+(โˆ’ma)=0\sum F + (-m a) = 0

This helps solve problems using static equilibrium equations.

(A) Static Force Analysis

  • No acceleration considered
  • Used in slow-speed machines

(B) Dynamic Force Analysis

  • Acceleration considered
  • Used in high-speed machines

Inertia Force:

Fi=mโ‹…aF_i = m \cdot a

Inertia Torque:

Ti=Iโ‹…ฮฑT_i = I \cdot \alpha

Where:

  • III = Mass moment of inertia
  • ฮฑ\alphaฮฑ = Angular acceleration

FBD is essential for kinetics analysis.

Steps:

  1. Isolate the link
  2. Show all forces acting
  3. Include inertia forces
  4. Apply equilibrium equations

Components:

  • Crank
  • Connecting rod
  • Piston

Forces:

  • Gas force on piston
  • Inertia force of piston
  • Connecting rod reactions

Important formula:Finertia=mโ‹…rโ‹…ฯ‰2(cosโกฮธ+cosโก2ฮธn)F_{inertia} = m \cdot r \cdot \omega^2 (\cos\theta + \frac{\cos2\theta}{n})

Where:

  • rrr = crank radius
  • ฯ‰\omegaฯ‰ = angular velocity
  • nnn = ratio of rod length to crank radius
  • Shows variation of torque over crank angle
  • Important for flywheel design

Key Terms:

  • Mean torque
  • Maximum torque
  • Fluctuation of energy

10. Flywheel

Purpose:

  • Stores excess energy
  • Maintains uniform speed

Energy stored:

E=12Iฯ‰2E = \frac{1}{2} I \omega^2

Occurs when a rotating body changes its axis.

Gyroscopic Couple:

C=Iโ‹…ฯ‰โ‹…ฯ‰pC = I \cdot \omega \cdot \omega_p

Where:

  • ฯ‰\omegaฯ‰ = spin velocity
  • ฯ‰p\omega_pฯ‰pโ€‹ = precession velocity

Types:

  • Static balancing
  • Dynamic balancing

Objective:

  • Reduce vibration
  • Improve machine life

Types:

  • Sliding friction
  • Rolling friction

Effects:

  • Energy loss
  • Wear and tear

Work=Change in Kinetic EnergyWork = Change\ in\ Kinetic\ EnergyWork=Changeย inย Kineticย Energy W=12mv2โˆ’12mu2W = \frac{1}{2}mv^2 – \frac{1}{2}mu^2

Power=Forceร—VelocityPower = Force \times VelocityP=Tโ‹…ฯ‰P = T \cdot \omega

  • IC Engines
  • Turbines
  • Pumps
  • Automobiles
  • Robotics
  • Dโ€™Alembertโ€™s principle
  • Inertia forces
  • Reciprocating engine analysis
  • Flywheel problems
  • Turning moment diagram

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