Mean Free Path — Question 5

Section 19-5 · Physics pages 3120–3121

Question 5 Counting binary collisions requires a factor of one-half A uniform gas contains N = 2.00 × 1020 molecules. Its mean speed is 400 m/s and mean free path 100 nm. Use per-molecule collision rate z = v/λ as the model rate. A B one encounter, two participants Schematic; labels, not drawing lengths, specify the data. (a) Find the mean free time and total number of distinct binary collisions per second. (b) If the gas amount doubles at fixed volume and temperature, find how λ, z and the distinct total collision rate change.
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Question 5 - Solution Counting binary collisions requires a factor of one-half A B one encounter, two participants (a) Method and calculation τ = λ/v = 10−7/400 = 2.50 × 10−10 s, z = 4.00 × 109 s−1. ˙Ncollisions = 1 2Nz = 4.00 × 1029 s−1. (b) Interpretation and further calculation ν →2ν : λ →λ/2, z →2z, N →2N. ˙Ncollisions →4 ˙Ncollisions = 1.60 × 1030 s−1. Each binary encounter is counted for both partners in Nz, so division by two avoids duplication. Physical check The total collision rate scales as density squared at fixed volume and thermal speed.

Question 5

Counting binary collisions requires a factor of one-half

A uniform gas contains N=2.00×1020N=2.00\times10^{20} molecules. Its mean speed is 400 m/s and mean free path 100 nm. Use per-molecule collision rate z=v¯/λz=\overline v/\lambda as the model rate.

Diagram shown in the original SVG worksheet.

  1. Find the mean free time and total number of distinct binary collisions per second.

  2. If the gas amount doubles at fixed volume and temperature, find how λ\lambda, zz and the distinct total collision rate change.

Question 5 - Solution

Counting binary collisions requires a factor of one-half

Diagram shown in the original SVG worksheet.

(a) Method and calculation

τ=λ/v¯=10−7/400=2.50×10−10s,z=4.00×109s−1.\tau=\lambda/\overline v=10^{-7}/400=2.50\times10^{-10}\,\mathrm s,\quad z=4.00\times10^9\,\mathrm{s^{-1}}.Ṅcollisions=12Nz=4.00×1029s−1.\dot N_{\mathrm{collisions}}=\tfrac12Nz=4.00\times10^{29}\,\mathrm{s^{-1}}.

(b) Interpretation and further calculation

ν→2ν:λ→λ/2,z→2z,N→2N.\nu\to2\nu:\quad\lambda\to\lambda/2,\quad z\to2z,\quad N\to2N.Ṅcollisions→4Ṅcollisions=1.60×1030s−1.\dot N_{\mathrm{collisions}}\to4\dot N_{\mathrm{collisions}}=1.60\times10^{30}\,\mathrm{s^{-1}}.Each binary encounter is counted for both partners in NzNz, so division by two avoids duplication.

Physical check

The total collision rate scales as density squared at fixed volume and thermal speed.