The Distribution of Molecular Speeds — Question 10

Section 19-6 · Physics pages 3150–3151

Question 10 A signed velocity component has a different distribution from speed An isotropic equilibrium gas has Cartesian component density h(vx) = e−v2 x/(2σ2)/( √ 2πσ) with σ = 250 m/s. Use erf(1/ √ 2) = .682689 and independent equal-variance components. vx h Schematic; labels, not drawing lengths, specify the data. (a) Find P(|vx| < 250 m/s), P(vx > 250 m/s) and the three-dimensional rms speed. (b) Find ⟨|vx|⟩by integration and compare it with the mean speed v = √ 8/πσ. Why can h peak at zero while the speed density does not?
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Question 10 - Solution A signed velocity component has a different distribution from speed vx h (a) Method and calculation P(|vx| < σ) = .682689, P(vx > σ) = 1 2(1 −.682689) = .1586555. vrms = √ ⟨v2x + v2y + v2z⟩= √ 3σ ≈433.013 m/s. (b) Interpretation and further calculation ⟨|vx|⟩= 2 √ 2πσ ∫∞ 0 vxe−v2 x/(2σ2)dvx = √ 2/πσ ≈199.471 m/s. v = 2⟨|vx|⟩≈398.942 m/s. A speed shell in three-dimensional velocity space contributes a 4πv2 factor; a one-component interval does not. Physical check Isotropy gives zero mean signed velocity, not zero mean speed or zero mean absolute component.

Question 10

A signed velocity component has a different distribution from speed

An isotropic equilibrium gas has Cartesian component density h(vx)=e−vx2/(2σ2)/(2πσ)h(v_x)=e^{-v_x^2/(2\sigma^2)}/(\sqrt{2\pi}\sigma) with σ=250\sigma=250 m/s. Use erf⁡(1/2)=.682689\operatorname{erf}(1/\sqrt2)=.682689 and independent equal-variance components.

Diagram shown in the original SVG worksheet.

  1. Find P(|vx|<250m/s)P(|v_x|<250\,\mathrm{m/s}), P(vx>250m/s)P(v_x>250\,\mathrm{m/s}) and the three-dimensional rms speed.

  2. Find ⟨|vx|⟩\langle|v_x|\rangle by integration and compare it with the mean speed v¯=8/πσ\overline v=\sqrt{8/\pi}\sigma. Why can hh peak at zero while the speed density does not?

Question 10 - Solution

A signed velocity component has a different distribution from speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P(|vx|<σ)=.682689,P(vx>σ)=12(1−.682689)=.1586555.P(|v_x|<\sigma)=.682689,\quad P(v_x>\sigma)=\tfrac12(1-.682689)=.1586555.vrms=⟨vx2+vy2+vz2⟩=3σ≈433.013m/s.v_{\mathrm{rms}}=\sqrt{\langle v_x^2+v_y^2+v_z^2\rangle}=\sqrt3\sigma\approx433.013\,\mathrm{m/s}.

(b) Interpretation and further calculation

⟨|vx|⟩=22πσ∫0∞vxe−vx2/(2σ2)dvx=2/πσ≈199.471m/s.\langle|v_x|\rangle=\frac2{\sqrt{2\pi}\sigma}\int_0^\infty v_xe^{-v_x^2/(2\sigma^2)}dv_x=\sqrt{2/\pi}\sigma\approx199.471\,\mathrm{m/s}.v¯=2⟨|vx|⟩≈398.942m/s.\overline v=2\langle|v_x|\rangle\approx398.942\,\mathrm{m/s}.A speed shell in three-dimensional velocity space contributes a 4πv24\pi v^2 factor; a one-component interval does not.

Physical check

Isotropy gives zero mean signed velocity, not zero mean speed or zero mean absolute component.