Pressure, Temperature, and RMS Speed — Question 9

Section 19-3 · Physics pages 3088–3089

Question 9 One measured velocity component can determine an isotropic temperature A zero-drift equilibrium gas has one-component rms speed √ ⟨v2x⟩= 250 m/s. Its molecular mass is 6.40 × 10−26 kg. Use isotropy and m⟨v2 x⟩= kBT, with kB = 1.381 × 10−23 J/K. vx vy vz one-component measurement Schematic; labels, not drawing lengths, specify the data. (a) Find the three-dimensional rms speed and temperature. (b) An analyst interprets 250 m/s as the full rms speed. Find the inferred temperature and its ratio to the correct temperature. Explain why zero drift alone is not enough for the isotropy step.
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Question 9 - Solution One measured velocity component can determine an isotropic temperature vx vy vz one-component measurement (a) Method and calculation ⟨v2⟩= 3⟨v2 x⟩⇒vrms = 250 √ 3 = 433.013 m/s. T = 6.40 × 10−26(250)2 1.381 × 10−23 ≈289.645 K. (b) Interpretation and further calculation Twrong = m(250)2 3kB = T/3 ≈96.5484 K. ⟨v⟩= 0̸ ⇒⟨v2 x⟩= ⟨v2 y⟩= ⟨v2 z⟩. A distribution may be symmetric about zero yet broader along one axis; equilibrium isotropy supplies the extra information. Physical check The rms component is smaller than the full rms speed by √ 3, not by three.

Question 9

One measured velocity component can determine an isotropic temperature

A zero-drift equilibrium gas has one-component rms speed ⟨vx2⟩=250\sqrt{\langle v_x^2\rangle}=250 m/s. Its molecular mass is 6.40×10−266.40\times10^{-26} kg. Use isotropy and m⟨vx2⟩=kBTm\langle v_x^2\rangle=k_BT, with kB=1.381×10−23k_B=1.381\times10^{-23} J/K.

Diagram shown in the original SVG worksheet.

  1. Find the three-dimensional rms speed and temperature.

  2. An analyst interprets 250 m/s as the full rms speed. Find the inferred temperature and its ratio to the correct temperature. Explain why zero drift alone is not enough for the isotropy step.

Question 9 - Solution

One measured velocity component can determine an isotropic temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨v2⟩=3⟨vx2⟩⇒vrms=2503=433.013m/s.\langle v^2\rangle=3\langle v_x^2\rangle\ \Rightarrow\ v_{\mathrm{rms}}=250\sqrt3=433.013\,\mathrm{m/s}.T=6.40×10−26(250)21.381×10−23≈289.645K.T=\frac{6.40\times10^{-26}(250)^2}{1.381\times10^{-23}}\approx289.645\,\mathrm K.

(b) Interpretation and further calculation

Twrong=m(250)23kB=T/3≈96.5484K.T_{\mathrm{wrong}}=\frac{m(250)^2}{3k_B}=T/3\approx96.5484\,\mathrm K.⟨𝒗⟩=0⇏⟨vx2⟩=⟨vy2⟩=⟨vz2⟩.\langle\mathbf v\rangle=0\not\Rightarrow\langle v_x^2\rangle=\langle v_y^2\rangle=\langle v_z^2\rangle.A distribution may be symmetric about zero yet broader along one axis; equilibrium isotropy supplies the extra information.

Physical check

The rms component is smaller than the full rms speed by 3\sqrt3, not by three.