Some Special Cases of the First Law of Thermodynamics — Question 5

Section 18-10 · Physics pages 3000–3001

Question 5 Free expansion preserves internal energy but need not preserve temperature Use ∆U = Q −W, with work by the gas positive. A gas expands into vacuum inside a rigid insulated enclosure, from Vi = .0100 to Vf = .0200 m3. The initial temperature is 300 K. Neglect partition energy. Compare two supplied caloric models: ideal U = CT + U0 and nonideal U = CT −a/V + U0, with C = 15.0 J/K and a = 6.00 J m3. gas vacuum rigid, insulated enclosure Schematic; labels, not drawing lengths, specify the data. (a) Find Q, W, ∆U and the ideal-model final temperature. (b) Find the nonideal-model final temperature. Explain the physical role of the volume-dependent energy term in the result.
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Question 5 - Solution Free expansion preserves internal energy but need not preserve temperature gas vacuum rigid, insulated enclosure (a) Method and calculation Q = 0, W = 0, ∆U = 0. C(Tf −Ti) = 0 ⇒Tf,ideal = 300 K. (b) Interpretation and further calculation 0 = C(Tf −Ti) −a ( 1 Vf −1 Vi ) . Tf = 300 + 6 15(50 −100) = 280 K. The term −a/V increases by 300 J as volume grows; the CT term must fall by the same amount. Constant internal energy alone does not imply constant temperature for every substance. Physical check No quasistatic adiabatic pressure law should be imposed on free expansion.

Question 5

Free expansion preserves internal energy but need not preserve temperature

Use ΔU=Q−W\Delta U=Q-W, with work by the gas positive. A gas expands into vacuum inside a rigid insulated enclosure, from Vi=.0100V_i=.0100 to Vf=.0200m3V_f=.0200\,\mathrm{m^3}. The initial temperature is 300 K. Neglect partition energy. Compare two supplied caloric models: ideal U=CT+U0U=CT+U_0 and nonideal U=CT−a/V+U0U=CT-a/V+U_0, with C=15.0J/KC=15.0\,\mathrm{J/K} and a=6.00Jm3a=6.00\,\mathrm{J\,m^3}.

Diagram shown in the original SVG worksheet.

  1. Find QQ, WW, ΔU\Delta U and the ideal-model final temperature.

  2. Find the nonideal-model final temperature. Explain the physical role of the volume-dependent energy term in the result.

Question 5 - Solution

Free expansion preserves internal energy but need not preserve temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q=0,W=0,ΔU=0.Q=0,\quad W=0,\quad\Delta U=0.C(Tf−Ti)=0⇒Tf,ideal=300K.C(T_f-T_i)=0\ \Rightarrow\ T_{f,\mathrm{ideal}}=300\,\mathrm K.

(b) Interpretation and further calculation

0=C(Tf−Ti)−a(1Vf−1Vi).0=C(T_f-T_i)-a\left(\frac1{V_f}-\frac1{V_i}\right).Tf=300+615(50−100)=280K.T_f=300+\frac6{15}(50-100)=280\,\mathrm K.The term −a/V-a/V increases by 300 J as volume grows; the CTCT term must fall by the same amount. Constant internal energy alone does not imply constant temperature for every substance.

Physical check

No quasistatic adiabatic pressure law should be imposed on free expansion.