Degrees of Freedom and Molar Specific Heats — Question 7

Section 19-8 · Physics pages 3184–3185

Question 7 Equipartition gives unequal angular speeds for unequal moments of inertia A classical rigid nonlinear molecule has rotational energy Erot = 1 2I1ω2 1 + 1 2I2ω2 2 + 1 2I3ω2 3. Its principal moments satisfy I2 = 2I1 and I3 = 3I1. At the specified temperature, √ kBT/I1 = 2.00 × 1012 rad/s. All three rotations are active. axis 1 axis 2 Principal-axis sketch; the third axis is perpendicular to the page. (a) Find each rms angular-velocity component and its mean energy contribution. (b) Compare the rms angular-momentum components Li = Iiωi. Does equal energy imply equal angular momentum or equal angular speed?
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Question 7 - Solution Equipartition gives unequal angular speeds for unequal moments of inertia axis 1 axis 2 (a) Method and calculation 1 2Ii⟨ω2 i ⟩= 1 2kBT ⇒ωi,rms = √ kBT/Ii. (ω1,rms, ω2,rms, ω3,rms) = 2.00 × 1012(1, 1/ √ 2, 1/ √ 3) rad/s. (b) Interpretation and further calculation Li,rms = Iiωi,rms = √ IikBT. L1,rms : L2,rms : L3,rms = 1 : √ 2 : √ 3, ⟨Ei⟩= 1 2kBT. A larger moment of inertia reduces angular-speed fluctuations while increasing angular-momentum fluctuations. Physical check Equipartition applies to the quadratic energies, not to the coordinates or momenta by themselves.

Question 7

Equipartition gives unequal angular speeds for unequal moments of inertia

A classical rigid nonlinear molecule has rotational energy Erot=12I1ω12+12I2ω22+12I3ω32E_{\mathrm{rot}}=\tfrac12I_1\omega_1^2+\tfrac12I_2\omega_2^2+\tfrac12I_3\omega_3^2. Its principal moments satisfy I2=2I1I_2=2I_1 and I3=3I1I_3=3I_1. At the specified temperature, kBT/I1=2.00×1012\sqrt{k_BT/I_1}=2.00\times10^{12} rad/s. All three rotations are active.

Diagram shown in the original SVG worksheet.

  1. Find each rms angular-velocity component and its mean energy contribution.

  2. Compare the rms angular-momentum components Li=IiωiL_i=I_i\omega_i. Does equal energy imply equal angular momentum or equal angular speed?

Question 7 - Solution

Equipartition gives unequal angular speeds for unequal moments of inertia

Diagram shown in the original SVG worksheet.

(a) Method and calculation

12Ii⟨ωi2⟩=12kBT⇒ωi,rms=kBT/Ii.\tfrac12I_i\langle\omega_i^2\rangle=\tfrac12k_BT\ \Rightarrow\omega_{i,\mathrm{rms}}=\sqrt{k_BT/I_i}.(ω1,rms,ω2,rms,ω3,rms)=2.00×1012(1,1/2,1/3)rad/s.(\omega_{1,\mathrm{rms}},\omega_{2,\mathrm{rms}},\omega_{3,\mathrm{rms}})=2.00\times10^{12}(1,1/\sqrt2,1/\sqrt3)\,\mathrm{rad/s}.

(b) Interpretation and further calculation

Li,rms=Iiωi,rms=IikBT.L_{i,\mathrm{rms}}=I_i\omega_{i,\mathrm{rms}}=\sqrt{I_ik_BT}.L1,rms:L2,rms:L3,rms=1:2:3,⟨Ei⟩=12kBT.L_{1,\mathrm{rms}}:L_{2,\mathrm{rms}}:L_{3,\mathrm{rms}}=1:\sqrt2:\sqrt3,\quad\langle E_i\rangle=\tfrac12k_BT.A larger moment of inertia reduces angular-speed fluctuations while increasing angular-momentum fluctuations.

Physical check

Equipartition applies to the quadratic energies, not to the coordinates or momenta by themselves.