Degrees of Freedom and Molar Specific Heats — Question 6

Section 19-8 · Physics pages 3182–3183

Question 6 Internal modes divide stored energy without changing translational pressure Use classical equipartition: each active independent quadratic energy term contributes 1 2kBT per molecule. Let f count these terms, so for constant f, CV = fR/2, Cp = CV + R and γ = Cp/CV . Take R = 8.314 J/(mol K). A diatomic gas has three active translations, two rotations and one fully active harmonic vibration. Choose the thermal energy reference so that U = fnRT/2. At an equilibrium state pV = 1200 J. A B Rigid-bond model; the indicated transverse axis supports rotation. (a) Find total thermal energy and its translational, rotational and vibrational portions. (b) For quasistatic fixed-pressure heating with all modes remaining active, find the fractions of supplied heat entering translation, rotation, vibration and expansion work.
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Question 6 - Solution Internal modes divide stored energy without changing translational pressure A B (a) Method and calculation f = 3 + 2 + 2 = 7, U = 7 2pV = 4200 J. Utr = 3 2pV = 1800 J, Urot = pV = 1200 J, Uvib = pV = 1200 J. (b) Interpretation and further calculation Q = nCp∆T = 9 2nR∆T. ∆Utr Q = 1 3, ∆Urot Q = 2 9, ∆Uvib Q = 2 9, W Q = 2 9. 1 3 + 2 9 + 2 9 + 2 9 = 1. Pressure is still determined by center-of-mass translation; internal modes change the energy required to reach a temperature. Physical check Total thermal energy exceeds 3pV/2 because not all energy is translational.

Question 6

Internal modes divide stored energy without changing translational pressure

Use classical equipartition: each active independent quadratic energy term contributes 12kBT\tfrac12k_BT per molecule. Let ff count these terms, so for constant ff, CV=fR/2C_V=fR/2, Cp=CV+RC_p=C_V+R and γ=Cp/CV\gamma=C_p/C_V. Take R=8.314R=8.314 J/(mol K). A diatomic gas has three active translations, two rotations and one fully active harmonic vibration. Choose the thermal energy reference so that U=fnRT/2U=f nRT/2. At an equilibrium state pV=1200pV=1200 J.

Diagram shown in the original SVG worksheet.

  1. Find total thermal energy and its translational, rotational and vibrational portions.

  2. For quasistatic fixed-pressure heating with all modes remaining active, find the fractions of supplied heat entering translation, rotation, vibration and expansion work.

Question 6 - Solution

Internal modes divide stored energy without changing translational pressure

Diagram shown in the original SVG worksheet.

(a) Method and calculation

f=3+2+2=7,U=72pV=4200J.f=3+2+2=7,\quad U=\tfrac72pV=4200\,\mathrm J.Utr=32pV=1800J,Urot=pV=1200J,Uvib=pV=1200J.U_{\mathrm{tr}}=\tfrac32pV=1800\,\mathrm J,\quad U_{\mathrm{rot}}=pV=1200\,\mathrm J,\quad U_{\mathrm{vib}}=pV=1200\,\mathrm J.

(b) Interpretation and further calculation

Q=nCpΔT=92nRΔT.Q=nC_p\Delta T=\tfrac92nR\Delta T.ΔUtrQ=13,ΔUrotQ=29,ΔUvibQ=29,WQ=29.\frac{\Delta U_{\mathrm{tr}}}Q=\frac13,\quad\frac{\Delta U_{\mathrm{rot}}}Q=\frac29,\quad\frac{\Delta U_{\mathrm{vib}}}Q=\frac29,\quad\frac WQ=\frac29.13+29+29+29=1.\frac13+\frac29+\frac29+\frac29=1.Pressure is still determined by center-of-mass translation; internal modes change the energy required to reach a temperature.

Physical check

Total thermal energy exceeds 3pV/23pV/2 because not all energy is translational.