Mean Free Path — Question 7

Section 19-5 · Physics pages 3124–3125

Question 7 Mean free path can greatly exceed the typical molecular spacing For identical dilute hard-sphere molecules of diameter d and number density ν, use λ = 1/( √ 2πd2ν). Let ν = 1024 m−3 and d = .300 nm. Define a characteristic spacing s = ν−1/3; this is a volume-per-particle scale, not a fixed lattice spacing in the gas. s Spacing is a statistical scale; the arrow need not meet a molecular center. (a) Calculate s, λ and their ratio. (b) Derive λ/s in terms of s/d. If density rises by a factor of eight at fixed diameter, find the changes in spacing, mean free path and their ratio.
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Question 7 - Solution Mean free path can greatly exceed the typical molecular spacing s (a) Method and calculation s = 10−8 m = 10.0 nm, λ = 1 √ 2π(.300 × 10−9)2(1024) ≈2.50088 µm. λ/s ≈250.088. (b) Interpretation and further calculation ν = s−3 ⇒λ s = 1 √ 2π (s d )2 . ν →8ν : s →s/2, λ →λ/8, λ/s →(λ/s)/4. A moving molecule usually passes between many neighbors because its collision cross section is small. Physical check Mean free path is not simply the distance to the nearest particle.

Question 7

Mean free path can greatly exceed the typical molecular spacing

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). Let ν=1024m−3\nu=10^{24}\,\mathrm{m^{-3}} and d=.300d=.300 nm. Define a characteristic spacing s=ν−1/3s=\nu^{-1/3}; this is a volume-per-particle scale, not a fixed lattice spacing in the gas.

Diagram shown in the original SVG worksheet.

  1. Calculate ss, λ\lambda and their ratio.

  2. Derive λ/s\lambda/s in terms of s/ds/d. If density rises by a factor of eight at fixed diameter, find the changes in spacing, mean free path and their ratio.

Question 7 - Solution

Mean free path can greatly exceed the typical molecular spacing

Diagram shown in the original SVG worksheet.

(a) Method and calculation

s=10−8m=10.0nm,λ=12π(.300×10−9)2(1024)≈2.50088μm.s=10^{-8}\,\mathrm m=10.0\,\mathrm{nm},\quad\lambda=\frac1{\sqrt2\pi(.300\times10^{-9})^2(10^{24})}\approx2.50088\,\mu\mathrm m.λ/s≈250.088.\lambda/s\approx250.088.

(b) Interpretation and further calculation

ν=s−3⇒λs=12π(sd)2.\nu=s^{-3}\ \Rightarrow\ \frac\lambda s=\frac1{\sqrt2\pi}\left(\frac sd\right)^2.ν→8ν:s→s/2,λ→λ/8,λ/s→(λ/s)/4.\nu\to8\nu:\quad s\to s/2,\quad\lambda\to\lambda/8,\quad\lambda/s\to(\lambda/s)/4.A moving molecule usually passes between many neighbors because its collision cross section is small.

Physical check

Mean free path is not simply the distance to the nearest particle.