Kinetic Energy of Rotation — Question 8

Section 10-5 · Physics pages 1466–1467

Question 8 A variable rate stores more average energy than its mean suggests A flywheel of constant inertia I = 0.40 kg m2 has angular velocity ω(t) = 10 + 2 cos(Ωt) rad/s. Average over a whole modulation cycle; use ⟨cos⟩= 0 and ⟨cos2⟩= 1/2. Ωt ω 10 12 8 2π One complete modulation cycle about the nonzero mean rate; angular speeds are in rad/s. (a) Find the average kinetic energy. (b) Compare with computing energy from the average angular velocity, and give a general expression for the difference.
Show solutionHide solution
Question 8 - Solution A variable rate stores more average energy than its mean suggests Ωt ω 10 12 8 2π (a) Derivation and calculation Square before averaging: ω2 = 100 + 40 cos(Ωt) + 4 cos2(Ωt). ⟨ω2⟩= 100 + 40(0) + 4(1/2) = 102, ⟨K⟩= 1 2(0.40)(102) = 20.4 J . (b) Result and interpretation The energy evaluated at the mean rate is K(⟨ω⟩) = 1 2(0.40)(10)2 = 20 J. Generally, ⟨K⟩−K(⟨ω⟩) = 1 2I ( ⟨ω2⟩−⟨ω⟩2) = 1 2I Var(ω) ≥0 . ∆K = 1 2(0.40)(2) = 0.40 J . Physical check The difference vanishes only when the angular rate has zero variance.

Question 8

A variable rate stores more average energy than its mean suggests

A flywheel of constant inertia I=0.40kgm2I=0.40\,\mathrm{kg\,m^2} has angular velocity ω(t)=10+2cos⁡(Ωt)rad/s\omega(t)=10+2\cos(\Omega t)\,\mathrm{rad/s}. Average over a whole modulation cycle; use ⟨cos⁡⟩=0\langle\cos\rangle=0 and ⟨cos⁡2⟩=1/2\langle\cos^2\rangle=1/2.

Diagram shown in the original SVG worksheet.

  1. Find the average kinetic energy.

  2. Compare with computing energy from the average angular velocity, and give a general expression for the difference.

Question 8 - Solution

A variable rate stores more average energy than its mean suggests

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Square before averaging: ω2=100+40cos⁡(Ωt)+4cos⁡2(Ωt).\omega^2=100+40\cos(\Omega t)+4\cos^2(\Omega t). ⟨ω2⟩=100+40(0)+4(1/2)=102,⟨K⟩=12(0.40)(102)=20.4J.\langle\omega^2\rangle=100+40(0)+4(1/2)=102,\qquad \boxed{\langle K\rangle=\tfrac12(0.40)(102)=20.4\ \mathrm J}.

(b) Result and interpretation

The energy evaluated at the mean rate is K(⟨ω⟩)=12(0.40)(10)2=20K(\langle\omega\rangle)=\tfrac12(0.40)(10)^2=20 J. Generally, ⟨K⟩−K(⟨ω⟩)=12I(⟨ω2⟩−⟨ω⟩2)=12IVar⁡(ω)≥0.\boxed{\langle K\rangle-K(\langle\omega\rangle) =\tfrac12I\left(\langle\omega^2\rangle-\langle\omega\rangle^2\right) =\tfrac12I\operatorname{Var}(\omega)\ge0}. ΔK=12(0.40)(2)=0.40J.\boxed{\Delta K=\tfrac12(0.40)(2)=0.40\ \mathrm J}.

Physical check

The difference vanishes only when the angular rate has zero variance.