Degrees of Freedom and Molar Specific Heats — Question 3

Section 19-8 · Physics pages 3176–3177

Question 3 A vibrational mode stores equal kinetic and potential energies A classical harmonic bond coordinate q has energy E = p2 q/(2µ) + κq2/2, reduced mass µ = 1.00 × 10−26 kg and stiffness κ = 100 N/m. Take T = 500 K and kB = 1.381 × 10−23 J/K. The mode is stipulated to be in its classical regime. A B q relative to equilibrium Schematic; labels, not drawing lengths, specify the data. (a) Find rms bond-coordinate displacement and rms rate ˙q. (b) Find the mean total mode energy and its heat-capacity contribution for .200 mol of such modes. How do the rms amplitudes change if temperature quadruples?
Show solutionHide solution
Question 3 - Solution A vibrational mode stores equal kinetic and potential energies A B q relative to equilibrium (a) Method and calculation 1 2κ⟨q2⟩= 1 2kBT ⇒qrms = √ kBT/κ ≈8.30963 × 10−12 m. 1 2µ⟨˙q2⟩= 1 2kBT ⇒˙qrms = √ kBT/µ ≈830.963 m/s. (b) Interpretation and further calculation ⟨E⟩= kBT = 6.905 × 10−21 J, Csample = nR = .200(8.314) = 1.6628 J/K. T →4T : qrms →2qrms, ˙qrms →2 ˙qrms. The relative bond coordinate is not the center-of-mass displacement of the molecule. Physical check Equal energy in kinetic and potential terms does not imply equal numerical amplitudes; their coefficients have different units.

Question 3

A vibrational mode stores equal kinetic and potential energies

A classical harmonic bond coordinate qq has energy E=pq2/(2μ)+κq2/2E=p_q^2/(2\mu)+\kappa q^2/2, reduced mass μ=1.00×10−26\mu=1.00\times10^{-26} kg and stiffness κ=100\kappa=100 N/m. Take T=500T=500 K and kB=1.381×10−23k_B=1.381\times10^{-23} J/K. The mode is stipulated to be in its classical regime.

Diagram shown in the original SVG worksheet.

  1. Find rms bond-coordinate displacement and rms rate q̇\dot q.

  2. Find the mean total mode energy and its heat-capacity contribution for .200 mol of such modes. How do the rms amplitudes change if temperature quadruples?

Question 3 - Solution

A vibrational mode stores equal kinetic and potential energies

Diagram shown in the original SVG worksheet.

(a) Method and calculation

12κ⟨q2⟩=12kBT⇒qrms=kBT/κ≈8.30963×10−12m.\tfrac12\kappa\langle q^2\rangle=\tfrac12k_BT\ \Rightarrow\ q_{\mathrm{rms}}=\sqrt{k_BT/\kappa}\approx8.30963\times10^{-12}\,\mathrm m.12μ⟨q̇2⟩=12kBT⇒q̇rms=kBT/μ≈830.963m/s.\tfrac12\mu\langle\dot q^2\rangle=\tfrac12k_BT\ \Rightarrow\ \dot q_{\mathrm{rms}}=\sqrt{k_BT/\mu}\approx830.963\,\mathrm{m/s}.

(b) Interpretation and further calculation

⟨E⟩=kBT=6.905×10−21J,Csample=nR=.200(8.314)=1.6628J/K.\langle E\rangle=k_BT=6.905\times10^{-21}\,\mathrm J,\quad C_{\mathrm{sample}}=nR=.200(8.314)=1.6628\,\mathrm{J/K}.T→4T:qrms→2qrms,q̇rms→2q̇rms.T\to4T:\quad q_{\mathrm{rms}}\to2q_{\mathrm{rms}},\quad\dot q_{\mathrm{rms}}\to2\dot q_{\mathrm{rms}}.The relative bond coordinate is not the center-of-mass displacement of the molecule.

Physical check

Equal energy in kinetic and potential terms does not imply equal numerical amplitudes; their coefficients have different units.