The Adiabatic Expansion of an Ideal Gas — Question 2

Section 19-10 · Physics pages 3214–3215

Question 2 A large reversible expansion can be checked by two work formulas Use pV = nRT, R = 8.314 J/(mol K), and ∆U = Q −W with W positive for work done by the gas. A .500 mol monatomic ideal gas initially at 600 K expands reversibly and adiabatically from Vi to 8Vi. Take CV = 3R/2 and γ = 5/3. V p Vi →8Vi Axes and labels specify the model; the sketch is schematic. (a) Find final temperature, pressure ratio and work done by the gas. (b) Evaluate work again from W = (piVi −pfVf)/(γ −1) and show why pressure falls by a greater factor than the inverse volume ratio.
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Question 2 - Solution A large reversible expansion can be checked by two work formulas V p Vi →8Vi (a) Method and calculation Tf = Ti(Vi/Vf)γ−1 = 600(1/8)2/3 = 150 K. pf/pi = (1/8)5/3 = 1/32, W = nCV (Ti −Tf) = 2805.975 J. (b) Interpretation and further calculation W = ∫Vf Vi piV γ i V −γdV = piVi −pfVf γ −1 . W = nR(600 −150) 2/3 = 2805.975 J, pf pi = Tf/Ti Vf/Vi = 1/4 8 = 1 32. Expansion reduces both number density and thermal energy per molecule. Physical check The final energy remains positive; the extracted work is less than the initial thermal energy.

Question 2

A large reversible expansion can be checked by two work formulas

Use pV=nRTpV=nRT, R=8.314R=8.314 J/(mol K), and ΔU=Q−W\Delta U=Q-W with WW positive for work done by the gas. A .500 mol monatomic ideal gas initially at 600 K expands reversibly and adiabatically from ViV_i to 8Vi8V_i. Take CV=3R/2C_V=3R/2 and γ=5/3\gamma=5/3.

Diagram shown in the original SVG worksheet.

  1. Find final temperature, pressure ratio and work done by the gas.

  2. Evaluate work again from W=(piVi−pfVf)/(γ−1)W=(p_iV_i-p_fV_f)/(\gamma-1) and show why pressure falls by a greater factor than the inverse volume ratio.

Question 2 - Solution

A large reversible expansion can be checked by two work formulas

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Tf=Ti(Vi/Vf)γ−1=600(1/8)2/3=150K.T_f=T_i(V_i/V_f)^{\gamma-1}=600(1/8)^{2/3}=150\,\mathrm K.pf/pi=(1/8)5/3=1/32,W=nCV(Ti−Tf)=2805.975J.p_f/p_i=(1/8)^{5/3}=1/32,\quad W=nC_V(T_i-T_f)=2805.975\,\mathrm J.

(b) Interpretation and further calculation

W=∫ViVfpiViγV−γdV=piVi−pfVfγ−1.W=\int_{V_i}^{V_f}p_iV_i^\gamma V^{-\gamma}dV=\frac{p_iV_i-p_fV_f}{\gamma-1}.W=nR(600−150)2/3=2805.975J,pfpi=Tf/TiVf/Vi=1/48=132.W=\frac{nR(600-150)}{2/3}=2805.975\,\mathrm J,\quad\frac{p_f}{p_i}=\frac{T_f/T_i}{V_f/V_i}=\frac{1/4}{8}=\frac1{32}.Expansion reduces both number density and thermal energy per molecule.

Physical check

The final energy remains positive; the extracted work is less than the initial thermal energy.