Quick Recap — Advanced Rotation (Multi-step)

  • Landing/embedding (angular-momentum conservation about the axis): I1ω1=(I1+Iadded)ω2I_1\omega_1=(I_1+I_{added})\omega_2; a bullet/putty adds mr2mr^2. Linear momentum is not conserved when there is a pivot.
  • Rod released from horizontal (pivot at end): initial α=3g2L\alpha=\dfrac{3g}{2L}, so the tip's initial acceleration is 3g2>g\dfrac{3g}{2}>g — objects resting on the far end lift off.
  • Spin-up to rolling on the ground: angular momentum about the contact point is conserved; a disc set spinning at ω0\omega_0 ends at ω=ω03\omega=\dfrac{\omega_0}{3}.
  • Rolling identity: measure aa on an incline, then ImR2=gsinθa1\dfrac{I}{mR^2}=\dfrac{g\sin\theta}{a}-1.
  • Rigid-body scaling: for fixed mass, L=IωL=I\omega constant means shrinking the radius by nn raises ω\omega by n2n^2.

Worked mini-example. A disc (M=4M=4 kg) spins at ω\omega; a 22 kg putty lands on its rim. Here Idisc=12MR2=2R2I_{disc}=\tfrac12MR^2=2R^2 and the putty adds mR2=2R2mR^2=2R^2, so ω=2R22R2+2R2ω=ω2\omega'=\dfrac{2R^2}{2R^2+2R^2}\omega=\dfrac{\omega}{2}.