Kinetics of Rigid Bodies: Force and Acceleration

Kinetics of Rigid Bodies: Force and Acceleration

This topic extends Newton's Second Law to rigid bodies, relating forces and torques to linear and angular acceleration.

Equations of Motion

For a rigid body in plane motion:

Fx=m(aG)x\sum F_x = m (a_G)_x Fy=m(aG)y\sum F_y = m (a_G)_y MG=IGα\sum M_G = I_G \alpha

Where:

  • GG is the center of mass.
  • IGI_G is the mass moment of inertia about GG.
  • α\alpha is the angular acceleration.

Mass Moment of Inertia ($I$)

A measure of a body's resistance to angular acceleration. I=r2dmI = \int r^2 \, dm Common shapes:

  • Slender Rod (end): I=13mL2I = \frac{1}{3} mL^2
  • Slender Rod (center): I=112mL2I = \frac{1}{12} mL^2
  • Disk (center): I=12mr2I = \frac{1}{2} mr^2
  • Sphere (center): I=25mr2I = \frac{2}{5} mr^2

Rotation about a Fixed Axis

For rotation about a fixed point OO: MO=IOα\sum M_O = I_O \alpha Where IO=IG+md2I_O = I_G + m d^2 (Parallel Axis Theorem).

Example: Unbalanced Wheel

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