Pressure, Temperature, and RMS Speed — Question 1

Section 19-3 · Physics pages 3072–3073

Question 1 Repeated elastic impacts produce an average wall force A molecule of mass m = 5.00 × 10−26 kg moves in a rectangular box with x-length .100 m. Its normal speed component has magnitude 400 m/s. Wall collisions are elastic, and no intermolecular collisions occur. The wall area is .0200 m2. vx −vx Elastic reflection reverses the normal velocity component. (a) Derive the mean force on one x wall from impulse and return time, then find its pressure contribution. (b) If the box length doubles while that speed component and wall area are fixed, find the new pressure contribution. Explain why the round-trip distance is 2L, not L.
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Question 1 - Solution Repeated elastic impacts produce an average wall force vx −vx (a) Method and calculation I = 2m|vx| = 4.00 × 10−23 N s, ∆t = 2L/|vx| = 5.00 × 10−4 s. F = I/∆t = mv2 x/L = 8.00 × 10−20 N, p1 = F/A = 4.00 × 10−18 Pa. (b) Interpretation and further calculation p1 = mv2 x AL = mv2 x V ⇒p1(2L) = 2.00 × 10−18 Pa. ∆tsame wall = L/|vx| + L/|vx|. The intervening impact is on the opposite wall and does not contribute force to the selected wall. Physical check The force averages discrete impulses over many wall returns; it is not a continuous microscopic force between collisions.

Question 1

Repeated elastic impacts produce an average wall force

A molecule of mass m=5.00×10−26m=5.00\times10^{-26} kg moves in a rectangular box with xx-length .100 m. Its normal speed component has magnitude 400 m/s. Wall collisions are elastic, and no intermolecular collisions occur. The wall area is .0200 m2^2.

Diagram shown in the original SVG worksheet.

  1. Derive the mean force on one xx wall from impulse and return time, then find its pressure contribution.

  2. If the box length doubles while that speed component and wall area are fixed, find the new pressure contribution. Explain why the round-trip distance is 2L2L, not LL.

Question 1 - Solution

Repeated elastic impacts produce an average wall force

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I=2m|vx|=4.00×10−23Ns,Δt=2L/|vx|=5.00×10−4s.I=2m|v_x|=4.00\times10^{-23}\,\mathrm{N\,s},\quad\Delta t=2L/|v_x|=5.00\times10^{-4}\,\mathrm s.F¯=I/Δt=mvx2/L=8.00×10−20N,p1=F¯/A=4.00×10−18Pa.\overline F=I/\Delta t=mv_x^2/L=8.00\times10^{-20}\,\mathrm N,\quad p_1=\overline F/A=4.00\times10^{-18}\,\mathrm{Pa}.

(b) Interpretation and further calculation

p1=mvx2AL=mvx2V⇒p1(2L)=2.00×10−18Pa.p_1=\frac{mv_x^2}{AL}=\frac{mv_x^2}{V}\ \Rightarrow\ p_1(2L)=2.00\times10^{-18}\,\mathrm{Pa}.Δtsamewall=L/|vx|+L/|vx|.\Delta t_{\mathrm{same\ wall}}=L/|v_x|+L/|v_x|.The intervening impact is on the opposite wall and does not contribute force to the selected wall.

Physical check

The force averages discrete impulses over many wall returns; it is not a continuous microscopic force between collisions.