Pressure, Temperature, and RMS Speed — Question 7

Section 19-3 · Physics pages 3084–3085

Question 7 An oblique molecular beam transfers only normal momentum to a smooth wall A dilute collimated beam has number density ν = 1020 m−3, molecular mass m = 4.00 × 10−26 kg and speed 500 m/s. It strikes a flat wall at angle 60◦to the normal and reflects specularly. Use incident number flux J = νv cos θ. normal 60◦ Schematic; labels, not drawing lengths, specify the data. (a) Derive the normal force per wall area and evaluate it. (b) Find the ratio to normal incidence and explain why two cosine factors appear. Is there a tangential force for ideal specular reflection?
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Question 7 - Solution An oblique molecular beam transfers only normal momentum to a smooth wall normal 60◦ (a) Method and calculation ∆pn,wall = 2mv cos θ, F A = J∆pn = 2νmv2 cos2 θ. F/A = 2(1020)(4 × 10−26)(500)2(1/2)2 = .500 Pa. (b) Interpretation and further calculation p(60◦) p(0) = cos2 60◦= 1 4, p(0) = 2.00 Pa. ∆pt = 0 ⇒Ft/A = 0. One cosine reduces the incidence rate per wall area; the other reduces normal momentum transfer per collision. Physical check This directed-beam force is not the isotropic-equilibrium formula with a 1/3 factor.

Question 7

An oblique molecular beam transfers only normal momentum to a smooth wall

A dilute collimated beam has number density ν=1020m−3\nu=10^{20}\,\mathrm{m^{-3}}, molecular mass m=4.00×10−26m=4.00\times10^{-26} kg and speed 500 m/s. It strikes a flat wall at angle 60∘60^\circ to the normal and reflects specularly. Use incident number flux J=νvcos⁡θJ=\nu v\cos\theta.

Diagram shown in the original SVG worksheet.

  1. Derive the normal force per wall area and evaluate it.

  2. Find the ratio to normal incidence and explain why two cosine factors appear. Is there a tangential force for ideal specular reflection?

Question 7 - Solution

An oblique molecular beam transfers only normal momentum to a smooth wall

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δpn,wall=2mvcos⁡θ,FA=JΔpn=2νmv2cos⁡2θ.\Delta p_{n,\mathrm{wall}}=2mv\cos\theta,\quad\frac FA=J\Delta p_n=2\nu mv^2\cos^2\theta.F/A=2(1020)(4×10−26)(500)2(1/2)2=.500Pa.F/A=2(10^{20})(4\times10^{-26})(500)^2(1/2)^2=.500\,\mathrm{Pa}.

(b) Interpretation and further calculation

p(60∘)p(0)=cos⁡260∘=14,p(0)=2.00Pa.\frac{p(60^\circ)}{p(0)}=\cos^2 60^\circ=\frac14,\quad p(0)=2.00\,\mathrm{Pa}.Δpt=0⇒Ft/A=0.\Delta p_t=0\ \Rightarrow\ F_t/A=0.One cosine reduces the incidence rate per wall area; the other reduces normal momentum transfer per collision.

Physical check

This directed-beam force is not the isotropic-equilibrium formula with a 1/31/3 factor.