Change a spinning body's moment of inertia and watch its spin rate answer instantly. Like a skater pulling their arms in, sliding the masses inward drops I and spikes ω — while L = Iω stays locked. Rotational KE, though, is not conserved: the skater does the work.
↻ Spin ω● Point masses▮ KE gaugeTop-down view · L conserved
Setup
Arm radius r0.70 m
Point mass m2.0 kg
Platform M4.0 kg
Platform radius R0.70 m
Initial spin ω₀6.0 rad/s
6.00
Angular velocity ω (rad/s)
2.9
I (kg·m²)
6.0
ω (rad/s)
17.3
L = Iω (const)
52.0
KE_rot (J)
L = Iω conservedpull in → I↓ → ω↑KE = ½Iω²
Playback
Try this: pull the arms all the way in (r → 0.15) and watch ω spike while L holds steady. Then hit Drop disc I₂: a still disc lands on top, they lock into a common ω — L survives but KE takes a hit.