Technical Explanation: Flywheel Mechanics and Energy Sizing
A flywheel is an energy reservoir that stores mechanical energy in the form of rotational inertia. It absorbs excess energy when torque supplied by a prime mover exceeds load requirements and delivers energy when peak demand exceeds continuous motor capacity.
Kinetic Energy & Usable Power Delivery
The total kinetic energy stored in a rotor spinning at angular velocity ω (rad/s) is:
E = 0.5 · I · ω²
When supplying a peak transient load (such as a metal punch stroke or rock crusher impact), the rotor decelerates from ω₁ to ω₂. The usable energy released during this slowdown is:
ΔE = 0.5 · I · (ω₁² - ω₂²) = I · ω_mean² · Cs
Coefficient of Speed Fluctuation (Cs)
The allowable cyclic speed drop is governed by the application:
- Crushers and Forging Presses: Cs = 0.10 – 0.20 (larger speed drop allowed to minimize motor size).
- Machine Tools and Pumps: Cs = 0.03 – 0.05 (tight speed stability required).
- AC Generator Synchronous Drives: Cs = 0.005 – 0.02 (strict grid frequency regulation).
Centrifugal Rim Stress Limits
As a flywheel spins, centrifugal forces create circumferential tensile hoop stress:
σ_hoop ≈ ρ · v_tip² = ρ · (ω · R_o)²
Gray cast iron (Class 30) flywheels must strictly remain below tip speeds of 30–40 m/s to prevent catastrophic burst fragmentation, whereas high-grade forged alloy steels can safely handle tip speeds above 100 m/s.