Mean Free Path — Question 8

Section 19-5 · Physics pages 3126–3127

Question 8 Random flights accumulate path length faster than net displacement In a deliberately simplified three-dimensional random walk, each flight has fixed length ℓ= 100 nm, speed v = 500 m/s and an independent isotropic direction. Use ⟨ri · rj⟩= 0 for distinct flights. This fixed-length model differs from exponential free paths. Successive flights form a path longer than the net displacement. (a) Derive rms displacement after N flights and find the number needed for an rms displacement of 1.00 mm. (b) Find the elapsed time and total path length. Compare with a straight 1.00 mm flight at the same speed.
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Question 8 - Solution Random flights accumulate path length faster than net displacement (a) Method and calculation ⟨R2⟩= ⟨∑ i,j ri · rj ⟩ = Nℓ2 ⇒Rrms = ℓ √ N. N = (10−3/10−7)2 = 108. (b) Interpretation and further calculation t = Nℓ/v = 108(10−7)/500 = .0200 s, Lpath = Nℓ= 10.0 m. tstraight = 10−3/500 = 2.00 × 10−6 s, t/tstraight = 104. An rms displacement target is not a first-passage-time condition. Physical check The cancellation of differently directed steps separates diffusion from ballistic travel.

Question 8

Random flights accumulate path length faster than net displacement

In a deliberately simplified three-dimensional random walk, each flight has fixed length ℓ=100\ell=100 nm, speed v=500v=500 m/s and an independent isotropic direction. Use ⟨𝒓i⋅𝒓j⟩=0\langle\mathbf r_i\cdot\mathbf r_j\rangle=0 for distinct flights. This fixed-length model differs from exponential free paths.

Diagram shown in the original SVG worksheet.

  1. Derive rms displacement after NN flights and find the number needed for an rms displacement of 1.00 mm.

  2. Find the elapsed time and total path length. Compare with a straight 1.00 mm flight at the same speed.

Question 8 - Solution

Random flights accumulate path length faster than net displacement

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨R2⟩=⟨∑i,j𝒓i⋅𝒓j⟩=Nℓ2⇒Rrms=ℓN.\langle R^2\rangle=\left\langle\sum_{i,j}\mathbf r_i\cdot\mathbf r_j\right\rangle=N\ell^2\ \Rightarrow\ R_{\mathrm{rms}}=\ell\sqrt N.N=(10−3/10−7)2=108.N=(10^{-3}/10^{-7})^2=10^8.

(b) Interpretation and further calculation

t=Nℓ/v=108(10−7)/500=.0200s,Lpath=Nℓ=10.0m.t=N\ell/v=10^8(10^{-7})/500=.0200\,\mathrm s,\quad L_{\mathrm{path}}=N\ell=10.0\,\mathrm m.tstraight=10−3/500=2.00×10−6s,t/tstraight=104.t_{\mathrm{straight}}=10^{-3}/500=2.00\times10^{-6}\,\mathrm s,\quad t/t_{\mathrm{straight}}=10^4.An rms displacement target is not a first-passage-time condition.

Physical check

The cancellation of differently directed steps separates diffusion from ballistic travel.