Ideal Gases — Question 2

Section 19-2 · Physics pages 3054–3055

Question 2 A falling pressure can mask simultaneous heating and gas loss Treat the gas as ideal, pV = nRT, and use R = 8.314 J/(mol K). A rigid tank of volume .0200 m3 initially contains gas at 300 kPa and 300 K. After a leak, its pressure is 240 kPa and temperature is 320 K. Pressures are absolute. tank leak Representative particles; dots do not depict the actual count or scale. (a) Find the fraction of gas lost and the amounts before and after. (b) What final pressure would have occurred without leakage at 320 K? Explain why the pressure-drop fraction alone underestimates the lost fraction.
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Question 2 - Solution A falling pressure can mask simultaneous heating and gas loss tank leak (a) Method and calculation nf ni = pf/Tf pi/Ti = 240(300) 300(320) = .750. ni = 300000(.0200) 8.314(300) ≈2.40558 mol, nf ≈1.80419 mol. (b) Interpretation and further calculation flost = 1 −.750 = .250, pf,sealed = 300(320/300) = 320 kPa. 1 −pf/pi = .200̸ = .250. Heating tends to increase pressure, partly concealing the effect of losing molecules. Physical check The inferred remaining amount is smaller despite the higher final temperature.

Question 2

A falling pressure can mask simultaneous heating and gas loss

Treat the gas as ideal, pV=nRTpV=nRT, and use R=8.314J/(molK)R=8.314\,\mathrm{J/(mol\,K)}. A rigid tank of volume .0200 m3^3 initially contains gas at 300 kPa and 300 K. After a leak, its pressure is 240 kPa and temperature is 320 K. Pressures are absolute.

Diagram shown in the original SVG worksheet.

  1. Find the fraction of gas lost and the amounts before and after.

  2. What final pressure would have occurred without leakage at 320 K? Explain why the pressure-drop fraction alone underestimates the lost fraction.

Question 2 - Solution

A falling pressure can mask simultaneous heating and gas loss

Diagram shown in the original SVG worksheet.

(a) Method and calculation

nfni=pf/Tfpi/Ti=240(300)300(320)=.750.\frac{n_f}{n_i}=\frac{p_f/T_f}{p_i/T_i}=\frac{240(300)}{300(320)}=.750.ni=300000(.0200)8.314(300)≈2.40558mol,nf≈1.80419mol.n_i=\frac{300000(.0200)}{8.314(300)}\approx2.40558\,\mathrm{mol},\quad n_f\approx1.80419\,\mathrm{mol}.

(b) Interpretation and further calculation

flost=1−.750=.250,pf,sealed=300(320/300)=320kPa.f_{\mathrm{lost}}=1-.750=.250,\quad p_{f,\mathrm{sealed}}=300(320/300)=320\,\mathrm{kPa}.1−pf/pi=.200≠.250.1-p_f/p_i=.200\ne.250.Heating tends to increase pressure, partly concealing the effect of losing molecules.

Physical check

The inferred remaining amount is smaller despite the higher final temperature.