The Adiabatic Expansion of an Ideal Gas — Question 3

Section 19-10 · Physics pages 3216–3217

Question 3 An adiabatic compression ratio sets a target temperature Use pV = nRT, R = 8.314 J/(mol K), and ∆U = Q −W with W positive for work done by the gas. A .200 mol ideal gas with γ = 1.40 and constant CV = 5R/2 starts at 300 K. It is compressed reversibly and adiabatically to one-fifth of its initial volume. V p Axes and labels specify the model; the sketch is schematic. (a) Find final temperature and work done on the gas. (b) Find the compression ratio Vi/Vf needed to reach 600 K from the same initial state. Explain the distinction between work on and work by the gas.
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Question 3 - Solution An adiabatic compression ratio sets a target temperature V p (a) Method and calculation Tf = 300(5)γ−1 = 300(5).400 ≈571.096 K. Won = ∆U = nCV (Tf −Ti) ≈(.200)(5 2)(8.314)(271.096) = 1126.947 J. (b) Interpretation and further calculation Tf Ti = ( Vi Vf ).400 ⇒Vi Vf = (600 300 )1/.400 = 25/2 ≈5.65685. Wby = −Won < 0. The temperature increase comes from mechanical work input; zero heat transfer does not imply zero energy transfer. Physical check The stronger compression needed for 600 K is consistent with the fivefold compression producing a slightly smaller temperature.

Question 3

An adiabatic compression ratio sets a target temperature

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 .200 mol ideal gas with γ=1.40\gamma=1.40 and constant CV=5R/2C_V=5R/2 starts at 300 K. It is compressed reversibly and adiabatically to one-fifth of its initial volume.

Diagram shown in the original SVG worksheet.

  1. Find final temperature and work done on the gas.

  2. Find the compression ratio Vi/VfV_i/V_f needed to reach 600 K from the same initial state. Explain the distinction between work on and work by the gas.

Question 3 - Solution

An adiabatic compression ratio sets a target temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Tf=300(5)γ−1=300(5).400≈571.096K.T_f=300(5)^{\gamma-1}=300(5)^{.400}\approx571.096\,\mathrm K.Won=ΔU=nCV(Tf−Ti)≈(.200)(52)(8.314)(271.096)=1126.947J.W_{\mathrm{on}}=\Delta U=nC_V(T_f-T_i)\approx(.200)(\tfrac52)(8.314)(271.096)=1126.947\,\mathrm J.

(b) Interpretation and further calculation

TfTi=(ViVf).400⇒ViVf=(600300)1/.400=25/2≈5.65685.\frac{T_f}{T_i}=\left(\frac{V_i}{V_f}\right)^{.400}\ \Rightarrow\frac{V_i}{V_f}=\left(\frac{600}{300}\right)^{1/.400}=2^{5/2}\approx5.65685.Wby=−Won<0.W_{\mathrm{by}}=-W_{\mathrm{on}}<0.The temperature increase comes from mechanical work input; zero heat transfer does not imply zero energy transfer.

Physical check

The stronger compression needed for 600 K is consistent with the fivefold compression producing a slightly smaller temperature.