KHAEMENES ACADEMY · PHYSICS 12 · WEEK 21 · DAY 02

Conservation Calculations

Why can rotational speed change when mass distribution changes?

Explicit physics instruction

Use L=Iω and ΔL=τ_extΔt. Conservation problems compare I₁ω₁ with I₂ω₂ when external torque is negligible.

A rotating system has I=4 kg·m² and ω=2 rad/s, so L=8 kg·m²/s. If I decreases to 2 kg·m² with negligible external torque, ω rises to 4 rad/s.

Check whether the assumed system actually excludes significant external torque.

Core relation: L=Iω and ΔL=τ_extΔt.

Worked example

A rotating system has I=4 kg·m² and ω=2 rad/s, so L=8 kg·m²/s. If I decreases to 2 kg·m² with negligible external torque, ω rises to 4 rad/s.

Guided question

If I changes from 6 to 3 kg·m² while ω starts at 2 rad/s, what final ω preserves L?

Independent work

  1. Solve three angular-momentum or torque-time problems.
  2. Declare the system and external-torque assumption.
  3. Record one unit/assumption check.

Misconception check

Conserved angular momentum does not mean angular speed is constant; I can change.

Formative check

If I is halved with L conserved, what happens to ω?

Reveal response

It doubles.

Mentor evidence conference

Ask Archaemenes to audit the system boundary, moment-of-inertia reasoning, and external-torque claim.

Teacher guidance

Foundation: Compute L=Iω.

Core: Solve conservation and torque-time changes.

Extended: Evaluate conservation residuals with uncertainty.