Mean Free Path — Question 4

Section 19-5 · Physics pages 3118–3119

Question 4 Transmission through a gas column can infer its pressure For identical dilute hard-sphere molecules of diameter d and number density ν, use λ = 1/( √ 2πd2ν). An ideal gas at 300 K has molecular diameter .300 nm. A supplied attenuation model gives collision-free transmission S = e−L/λ over L = 1.00 µm. Measured S = e−2. Use kB = 1.381 × 10−23 J/K and ν = p/(kBT). L gas Schematic; labels, not drawing lengths, specify the data. (a) Infer mean free path and pressure. (b) At the same temperature, what pressure would double transmission? Explain why this does not halve pressure.
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Question 4 - Solution Transmission through a gas column can infer its pressure L gas (a) Method and calculation −ln S = L/λ = 2 ⇒λ = .500 µm. p = kBT √ 2πd2λ = 1.381 × 10−23(300) √ 2π(.300 × 10−9)2(.500 × 10−6) ≈2.072 × 104 Pa. (b) Interpretation and further calculation Snew = 2e−2, pnew p = −ln Snew −ln S = 2 −ln 2 2 ≈.653426. pnew ≈.653426p. Transmission is exponential in pressure at fixed geometry, so a factor of two in transmission corresponds to an additive change in optical depth. Physical check The inferred pressure uses the supplied effective exponential model, not an assumption that every molecular trajectory has the same speed.

Question 4

Transmission through a gas column can infer its pressure

For identical dilute hard-sphere molecules of diameter dd and number density ν\nu, use λ=1/(2πd2ν)\lambda=1/(\sqrt2\pi d^2\nu). An ideal gas at 300 K has molecular diameter .300 nm. A supplied attenuation model gives collision-free transmission S=e−L/λS=e^{-L/\lambda} over L=1.00μL=1.00\,\mum. Measured S=e−2S=e^{-2}. Use kB=1.381×10−23k_B=1.381\times10^{-23} J/K and ν=p/(kBT)\nu=p/(k_BT).

Diagram shown in the original SVG worksheet.

  1. Infer mean free path and pressure.

  2. At the same temperature, what pressure would double transmission? Explain why this does not halve pressure.

Question 4 - Solution

Transmission through a gas column can infer its pressure

Diagram shown in the original SVG worksheet.

(a) Method and calculation

−ln⁡S=L/λ=2⇒λ=.500μm.-\ln S=L/\lambda=2\ \Rightarrow\lambda=.500\,\mu\mathrm m.p=kBT2πd2λ=1.381×10−23(300)2π(.300×10−9)2(.500×10−6)≈2.072×104Pa.p=\frac{k_BT}{\sqrt2\pi d^2\lambda}=\frac{1.381\times10^{-23}(300)}{\sqrt2\pi(.300\times10^{-9})^2(.500\times10^{-6})}\approx2.072\times10^4\,\mathrm{Pa}.

(b) Interpretation and further calculation

Snew=2e−2,pnewp=−ln⁡Snew−ln⁡S=2−ln⁡22≈.653426.S_{\mathrm{new}}=2e^{-2},\quad\frac{p_{\mathrm{new}}}p=\frac{-\ln S_{\mathrm{new}}}{-\ln S}=\frac{2-\ln2}{2}\approx.653426.pnew≈.653426p.p_{\mathrm{new}}\approx.653426p.Transmission is exponential in pressure at fixed geometry, so a factor of two in transmission corresponds to an additive change in optical depth.

Physical check

The inferred pressure uses the supplied effective exponential model, not an assumption that every molecular trajectory has the same speed.