Ideal Gases — Question 10

Section 19-2 · Physics pages 3070–3071

Question 10 Differentiating the gas law separates filling from heating Treat the gas as ideal, pV = nRT, and use R = 8.314 J/(mol K). A rigid .0100 m3 tank is instantaneously at p = 200 kPa and T = 300 K. Gas enters while the tank temperature rises at 2.00 K/s. Pressure rises at 3.00 kPa/s. Treat these as instantaneous uniform-state rates. rigid tank inflow Representative particles; dots do not depict the actual count or scale. (a) Derive ˙n from the gas law and calculate the molar inflow rate. (b) Find the apparent inflow rate if temperature change were ignored, and the threshold ˙p corresponding to zero inflow at the stated ˙T.
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Question 10 - Solution Differentiating the gas law separates filling from heating rigid tank inflow (a) Method and calculation n = pV RT ⇒˙n = V RT ( ˙p −p T ˙T ) . ˙n = .0100 8.314(300) ( 3000 −200000 300 (2) ) ≈.00668217 mol/s. (b) Interpretation and further calculation ˙nisothermal = .0100(3000) 8.314(300) ≈.0120279 mol/s. ˙n = 0 ⇐⇒ ˙p = p T ˙T = 1333.33 Pa/s. Only the pressure-rise portion above this thermal contribution indicates inflow; the isothermal estimate is 1.8 times the correct rate. Physical check An increasing pressure does not alone prove that molecules are entering.

Question 10

Differentiating the gas law separates filling from heating

Treat the gas as ideal, pV=nRTpV=nRT, and use R=8.314J/(molK)R=8.314\,\mathrm{J/(mol\,K)}. A rigid .0100 m3^3 tank is instantaneously at p=200p=200 kPa and T=300T=300 K. Gas enters while the tank temperature rises at 2.00 K/s. Pressure rises at 3.00 kPa/s. Treat these as instantaneous uniform-state rates.

Diagram shown in the original SVG worksheet.

  1. Derive ṅ\dot n from the gas law and calculate the molar inflow rate.

  2. Find the apparent inflow rate if temperature change were ignored, and the threshold ṗ\dot p corresponding to zero inflow at the stated Ṫ\dot T.

Question 10 - Solution

Differentiating the gas law separates filling from heating

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n=pVRT⇒ṅ=VRT(ṗ−pTṪ).n=\frac{pV}{RT}\ \Rightarrow\ \dot n=\frac V{RT}\left(\dot p-\frac pT\dot T\right).ṅ=.01008.314(300)(3000−200000300(2))≈.00668217mol/s.\dot n=\frac{.0100}{8.314(300)}\left(3000-\frac{200000}{300}(2)\right)\approx.00668217\,\mathrm{mol/s}.

(b) Interpretation and further calculation

ṅisothermal=.0100(3000)8.314(300)≈.0120279mol/s.\dot n_{\mathrm{isothermal}}=\frac{.0100(3000)}{8.314(300)}\approx.0120279\,\mathrm{mol/s}.ṅ=0⇔ṗ=pTṪ=1333.33Pa/s.\dot n=0\ \Longleftrightarrow\ \dot p=\frac pT\dot T=1333.33\,\mathrm{Pa/s}.Only the pressure-rise portion above this thermal contribution indicates inflow; the isothermal estimate is 1.8 times the correct rate.

Physical check

An increasing pressure does not alone prove that molecules are entering.