KHAEMENES ACADEMY · PHYSICS 12 · WEEK 22 · DAY 01

Rotational Kinetic Energy

How is energy partitioned in rolling systems?

Explicit physics instruction

A rolling object can have translational kinetic energy ½Mv² and rotational kinetic energy ½Iω² at the same time.

For rolling without slipping, v=rω links translation and rotation. The moment of inertia determines how much energy is stored in rotation for a given mass and speed.

Energy conservation can compare gravitational potential energy with translational and rotational kinetic energy when losses are negligible.

Core relations: K_total=½Mv²+½Iω² and v=rω.

Worked example

For a rolling body with M=2 kg, v=3 m/s, I=0.50 kg·m², and ω=6 rad/s, K_trans=9 J and K_rot=9 J, so total KE=18 J.

Guided question

Calculate rotational KE for I=0.8 kg·m² and ω=5 rad/s.

Independent work

  1. Solve three rotational-energy or rolling calculations.
  2. Draw an energy bar chart.
  3. State one condition where v=rω fails.

Misconception check

Rolling does not mean all kinetic energy is translational; rotation stores part of the total.

Formative check

What extra energy term must be included for a rolling object?

Reveal response

Rotational kinetic energy ½Iω².

Mentor evidence conference

Ask Archaemenes to audit rolling constraints, moment-of-inertia reasoning, and energy accounting.

Teacher guidance

Foundation: Calculate K_rot and v=rω.

Core: Combine translational and rotational energy.

Extended: Compare shapes using I and conservation residuals.