Rotational Kinetic Energy, Work & Power
A spinning wheel stores energy in the motion of all its parts.
Lesson at a glanceShow the key points
- A body rotating about a fixed axis has kinetic energy K = ½Iω²; it is just Σ½mᵢvᵢ² with vᵢ = rᵢω.
- Energy conservation must include the rotating parts: for a block falling a height h while unwinding a string from a wheel, mgh = ½mv² + ½I(v/r)².
- Power delivered by a torque: P = τω.
- Work done by a torque: dW = τ dθ, so W = ∫τ dθ (10.14).
A potter’s wheel keeps turning after the foot stops pushing; a flywheel smooths an engine’s jerks. Spinning things store energy, and we can count it.
Kinetic energy of a spinning body
A body turning about a fixed axis at angular speed ω has its i-th particle moving at . Add up the ordinary kinetic energies:
Energy bookkeeping with wheels
When a block on a string unwinds a wheel, the string doesn’t slip, so the rim moves as fast as the block: ω = v/r. As the block falls a height h, gravity’s lost potential energy goes into both bodies:
A 2.0 kg block hangs from a light string wrapped round a wheel of radius 20 cm and moment of inertia 0.20 kg·m², which turns freely. Released from rest, how fast is the block moving after falling 1.5 m?
Work and power from a torque
A torque that speeds a body up raises its kinetic energy at a rate
A motor delivers a steady torque of 20 N·m to a shaft turning at 3000 rpm. (a) What power does it supply? (b) How much work does it do in 10 revolutions?
- 1, the sum of ½mv² over the body.
- 2Include rotating parts in energy conservation; a non-slipping string links v = ωr.
- 3Power ; work .
Check yourself
Keep exploring
Hand-picked videos, simulations and readings that explain this idea from a different angle.