The Angular Momentum of a Rigid Body Rotating About a Fixed Axis — Question 9

Section 11-9 · Physics pages 1728–1729

y Question 9 Independent coaxial rotors cannot be assigned one physical angular speed Two coaxial rotors have I1 = 0.20, I2 = 0.30 kg m2 and signed angular speeds +10 and −4 rad/s. They are not coupled. I1 = .20, ω1 = +10 I2 = .30, ω2 = −4 Coaxial rotors; the indicated senses use the same positive axis. (a) Find total axial angular momentum and total rotational energy. (b) Compare with a fictitious single rigid rotor of inertia I1 + I2 carrying the same total angular momentum.
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y Question 9 - Solution Independent coaxial rotors cannot be assigned one physical angular speed I1 = .20, ω1 = +10 I2 = .30, ω2 = −4 (a) Derivation and calculation Signed angular momenta add: Lz = I1ω1 + I2ω2 = .20(10) + .30(−4) = .800 kg m2/s . Energies add without sign cancellation: K = 1 2(.20)(10)2 + 1 2(.30)(−4)2 = 12.4 J . (b) Result and interpretation A fictitious rigid rotor with IΣ = .50 kg m2 and the same Lz would have ωcommon = Lz/IΣ = .80/.50 = 1.60 rad/s , Kcommon = L2 z/(2IΣ) = .640 J . The difference 12.4 −.64 = 11.76 J is associated with relative rotation. The actual uncoupled two-speed assembly is not a single rigid rotor. Physical check Opposite signed spin momenta partly cancel while both rotational energies remain positive.

Question 9

Independent coaxial rotors cannot be assigned one physical angular speed

Two coaxial rotors have I1=0.20I_1=0.20, I2=0.30kgm2I_2=0.30\,\mathrm{kg\,m^2} and signed angular speeds +10+10 and −4rad/s-4\,\mathrm{rad/s}. They are not coupled.

Diagram shown in the original SVG worksheet.

  1. Find total axial angular momentum and total rotational energy.

  2. Compare with a fictitious single rigid rotor of inertia I1+I2I_1+I_2 carrying the same total angular momentum.

Question 9 - Solution

Independent coaxial rotors cannot be assigned one physical angular speed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Signed angular momenta add: Lz=I1ω1+I2ω2=.20(10)+.30(−4)=.800kgm2/s.\boxed{L_z=I_1\omega_1+I_2\omega_2=.20(10)+.30(-4)=.800\ \mathrm{kg\,m^2/s}}. Energies add without sign cancellation: K=12(.20)(10)2+12(.30)(−4)2=12.4J.\boxed{K=\tfrac12(.20)(10)^2+\tfrac12(.30)(-4)^2=12.4\ \mathrm J}.

(b) Result and interpretation

A fictitious rigid rotor with IΣ=.50I_\Sigma=.50 kg m2^2 and the same LzL_z would have ωcommon=Lz/IΣ=.80/.50=1.60rad/s,\boxed{\omega_{\mathrm{common}}=L_z/I_\Sigma=.80/.50=1.60\ \mathrm{rad/s}}, Kcommon=Lz2/(2IΣ)=.640J.\boxed{K_{\mathrm{common}}=L_z^2/(2I_\Sigma)=.640\ \mathrm J}. The difference 12.4−.64=11.7612.4-.64=11.76 J is associated with relative rotation. The actual uncoupled two-speed assembly is not a single rigid rotor.

Physical check

Opposite signed spin momenta partly cancel while both rotational energies remain positive.