Ideal Gases — Question 7

Section 19-2 · Physics pages 3064–3065

Question 7 An isothermal atmosphere has an exponential pressure profile Treat the gas as ideal, pV = nRT, and use R = 8.314 J/(mol K). For an ideal gas atmosphere with constant temperature 300 K, molar mass .0290 kg/mol and g = 9.80 m/s2, use hydrostatic balance dp/dz = −ρg. At z = 0, pressure is 100 kPa. Assume the idealized atmosphere remains isothermal over the height of interest. z p Axes and labels specify the model; the sketch is schematic. (a) Derive the pressure scale height and pressure profile. (b) Find the altitude where pressure falls to one-half its base value. Compare with a constant-density linear extrapolation using the base density.
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Question 7 - Solution An isothermal atmosphere has an exponential pressure profile z p (a) Method and calculation ρ = Mp RT , dp p = −Mg RT dz ⇒p(z) = p0e−z/H. H = RT Mg = 8.314(300) .0290(9.80) ≈8776.21 m. (b) Interpretation and further calculation z1/2 = H ln 2 ≈6083.21 m. plinear = p0(1 −z/H) ⇒z1/2,linear = H/2 ≈4388.11 m. Constant-density extrapolation falls too quickly because it does not account for the diminishing weight per unit height. Physical check The linear form is only a small-height approximation to the exponential.

Question 7

An isothermal atmosphere has an exponential pressure profile

Treat the gas as ideal, pV=nRTpV=nRT, and use R=8.314J/(molK)R=8.314\,\mathrm{J/(mol\,K)}. For an ideal gas atmosphere with constant temperature 300 K, molar mass .0290 kg/mol and g=9.80m/s2g=9.80\,\mathrm{m/s^2}, use hydrostatic balance dp/dz=−ρgdp/dz=-\rho g. At z=0z=0, pressure is 100 kPa. Assume the idealized atmosphere remains isothermal over the height of interest.

Diagram shown in the original SVG worksheet.

  1. Derive the pressure scale height and pressure profile.

  2. Find the altitude where pressure falls to one-half its base value. Compare with a constant-density linear extrapolation using the base density.

Question 7 - Solution

An isothermal atmosphere has an exponential pressure profile

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ρ=MpRT,dpp=−MgRTdz⇒p(z)=p0e−z/H.\rho=\frac{Mp}{RT},\quad\frac{dp}{p}=-\frac{Mg}{RT}dz\ \Rightarrow\ p(z)=p_0e^{-z/H}.H=RTMg=8.314(300).0290(9.80)≈8776.21m.H=\frac{RT}{Mg}=\frac{8.314(300)}{.0290(9.80)}\approx8776.21\,\mathrm m.

(b) Interpretation and further calculation

z1/2=Hln⁡2≈6083.21m.z_{1/2}=H\ln2\approx6083.21\,\mathrm m.plinear=p0(1−z/H)⇒z1/2,linear=H/2≈4388.11m.p_{\mathrm{linear}}=p_0(1-z/H)\ \Rightarrow\ z_{1/2,\mathrm{linear}}=H/2\approx4388.11\,\mathrm m.Constant-density extrapolation falls too quickly because it does not account for the diminishing weight per unit height.

Physical check

The linear form is only a small-height approximation to the exponential.