INGENIA

MEC-29

Flywheel fluctuation energy

ΔE = I ω² Cs with Cs = (ωmax−ωmin)/ω. Stored kinetic buffer.

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EnergyShigley

Governing equation

ΔE=Iω2Cs\Delta E=I\omega^2 C_s

where

I
Inertia (kg·m²)
\omega
Mean speed (rad/s)
C_s
Fluctuation coeff. ()
\Delta E
Energy fluctuation (kJ)

Lecture brief

Historical brief

Machine design grew from Coulomb torsion and Hertz contact (1881) through Soderberg fatigue and the heat-engine cycle. The lab writes shaft, bearing, contact and thermodynamic limits in SI. This sheet (MEC-29 — Flywheel fluctuation energy) is the form associated with Shigley. Working symbols: II, ω\omega, CsC_s \rightarrow ΔE\Delta E. A flywheel stores ½ I ω². The energy exchanged while speed fluctuates by Cs is I ω² Cs.

Purpose

Purpose: compute ΔE\Delta E from II, ω\omega, CsC_s in Mechanical via ΔE=Iω2Cs\Delta E=I\omega^2 C_s ΔE = I ω² Cs with Cs = (ωmax−ωmin)/ω. Stored kinetic buffer. Use it when a real mechanical question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given I=4.000kgm2I = 4.000\,\mathrm{kg·m^{2}}, ω=150.000rad/s\omega = 150.000\,\mathrm{rad/s}, Cs=0.050C_s = 0.050\,\mathrm{—}, the governing relation ΔE=Iω2Cs\Delta E=I\omega^2 C_s yields ΔE=4.500kJ\Delta E = 4.500\,\mathrm{kJ}. A disk, an ω band, an energy pulse. Move a slider: the numbers are this situation, not a canned story.

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Outputs

  • Energy fluctuation \Delta E4.500 kJ
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MEC-29 · pendulum
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Narration of this film

A disk, an ω band, an energy pulse.

A flywheel stores ½ I ω². The energy exchanged while speed fluctuates by Cs is I ω² Cs.

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Watch on YouTube