The Distribution of Molecular Speeds — Question 3

Section 19-6 · Physics pages 3136–3137

Question 3 A temperature change stretches the distribution while preserving area The normalized Maxwell speed distribution at temperature T is fT (v). The same species is heated to 4T, remaining in classical equilibrium. Its original most probable speed is 300 m/s. v f(v) solid T, dashed 4T Axes and labels specify the model; the sketch is schematic. (a) Express f4T (v) in terms of fT and find the new mode and peak height relative to the old peak. (b) If 40.0% of the original population lies between 200 and 500 m/s, identify an interval containing 40.0% after heating and verify the probability transformation.
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Question 3 - Solution A temperature change stretches the distribution while preserving area v f(v) solid T, dashed 4T (a) Method and calculation fT (v) ∝T −3/2v2e−mv2/(2kBT) ⇒f4T (v) = 1 2fT (v/2). vmp,4T = 600 m/s, max f4T = 1 2 max fT . (b) Interpretation and further calculation P4T (400 < v < 1000) = ∫1000 400 1 2fT (v/2)dv. u = v/2 ⇒P4T = ∫500 200 fT (u)du = .400. Every speed quantile doubles; probability density halves at corresponding rescaled speeds. Physical check Heating broadens the normalized curve; it does not increase the total probability.

Question 3

A temperature change stretches the distribution while preserving area

The normalized Maxwell speed distribution at temperature TT is fT(v)f_T(v). The same species is heated to 4T4T, remaining in classical equilibrium. Its original most probable speed is 300 m/s.

Diagram shown in the original SVG worksheet.

  1. Express f4T(v)f_{4T}(v) in terms of fTf_T and find the new mode and peak height relative to the old peak.

  2. If 40.0% of the original population lies between 200 and 500 m/s, identify an interval containing 40.0% after heating and verify the probability transformation.

Question 3 - Solution

A temperature change stretches the distribution while preserving area

Diagram shown in the original SVG worksheet.

(a) Method and calculation

fT(v)∝T−3/2v2e−mv2/(2kBT)⇒f4T(v)=12fT(v/2).f_T(v)\propto T^{-3/2}v^2e^{-mv^2/(2k_BT)}\ \Rightarrow\ f_{4T}(v)=\tfrac12f_T(v/2).vmp,4T=600m/s,max⁡f4T=12max⁡fT.v_{{\mathrm{mp}},4T}=600\,\mathrm{m/s},\quad\max f_{4T}=\tfrac12\max f_T.

(b) Interpretation and further calculation

P4T(400<v<1000)=∫400100012fT(v/2)dv.P_{4T}(400<v<1000)=\int_{400}^{1000}\tfrac12f_T(v/2)dv.u=v/2⇒P4T=∫200500fT(u)du=.400.u=v/2\ \Rightarrow\ P_{4T}=\int_{200}^{500}f_T(u)du=.400.Every speed quantile doubles; probability density halves at corresponding rescaled speeds.

Physical check

Heating broadens the normalized curve; it does not increase the total probability.