Degrees of Freedom and Molar Specific Heats — Question 9

Section 19-8 · Physics pages 3188–3189

Question 9 A classical solid stores potential energy that a monatomic ideal gas does not Model a classical solid as atoms independently oscillating harmonically in three directions. A monatomic ideal gas has only three free translational kinetic terms. One mole of each is brought into thermal contact in a rigid insulated apparatus. Initially the gas is at 600 K and the solid at 200 K. Assume both models remain classical and their capacities constant; neglect expansion and apparatus heat. atom harmonic restoring forces Lines indicate the independent restoring directions, with a third direction out of the page. (a) Derive the molar CV of each model and the final common temperature. (b) At that temperature, compare the gas mean kinetic energy per atom with the solid mean kinetic and potential energies per atom. Explain the factor of two in their heat capacities.
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Question 9 - Solution A classical solid stores potential energy that a monatomic ideal gas does not atom harmonic restoring forces (a) Method and calculation fgas = 3 : CV,g = 3 2R, fsolid = 3 + 3 = 6 : CV,s = 3R. 3 2R(600 −Tf) = 3R(Tf −200) ⇒Tf = 1000 3 K. (b) Interpretation and further calculation ⟨K⟩g = ⟨K⟩s = 3 2kBTf, ⟨V ⟩s = 3 2kBTf. ⟨E⟩s = 3kBTf = 2⟨E⟩g. Confining harmonic forces add three potential-energy terms. They do not double the kinetic energy at a common temperature. Physical check The classical solid result is a model limit; it is not asserted to hold at arbitrarily low temperature.

Question 9

A classical solid stores potential energy that a monatomic ideal gas does not

Model a classical solid as atoms independently oscillating harmonically in three directions. A monatomic ideal gas has only three free translational kinetic terms. One mole of each is brought into thermal contact in a rigid insulated apparatus. Initially the gas is at 600 K and the solid at 200 K. Assume both models remain classical and their capacities constant; neglect expansion and apparatus heat.

Diagram shown in the original SVG worksheet.

  1. Derive the molar CVC_V of each model and the final common temperature.

  2. At that temperature, compare the gas mean kinetic energy per atom with the solid mean kinetic and potential energies per atom. Explain the factor of two in their heat capacities.

Question 9 - Solution

A classical solid stores potential energy that a monatomic ideal gas does not

Diagram shown in the original SVG worksheet.

(a) Method and calculation

fgas=3:CV,g=32R,fsolid=3+3=6:CV,s=3R.f_{\mathrm{gas}}=3:\ C_{V,g}=\tfrac32R,\quad f_{\mathrm{solid}}=3+3=6:\ C_{V,s}=3R.32R(600−Tf)=3R(Tf−200)⇒Tf=10003K.\tfrac32R(600-T_f)=3R(T_f-200)\ \Rightarrow\ T_f=\frac{1000}{3}\,\mathrm K.

(b) Interpretation and further calculation

⟨K⟩g=⟨K⟩s=32kBTf,⟨V⟩s=32kBTf.\langle K\rangle_g=\langle K\rangle_s=\tfrac32k_BT_f,\quad\langle V\rangle_s=\tfrac32k_BT_f.⟨E⟩s=3kBTf=2⟨E⟩g.\langle E\rangle_s=3k_BT_f=2\langle E\rangle_g.Confining harmonic forces add three potential-energy terms. They do not double the kinetic energy at a common temperature.

Physical check

The classical solid result is a model limit; it is not asserted to hold at arbitrarily low temperature.