Translational Kinetic Energy — Question 9

Section 19-4 · Physics pages 3108–3109

Question 9 The same mean energy does not specify a speed distribution Two isotropic populations consist of particles of identical mass m. Population A has every speed equal to v0. In B, half the particles are at rest and half have speed √ 2v0. Both have zero mean velocity. No Maxwell-distribution assumption is made. A: one speed B: two speeds Separate samples or species for comparison. (a) Compare their mean kinetic energies, rms speeds and mean speeds. (b) Calculate the kinetic-energy variance in each population. Can assigning the same energy-equivalent temperature prove either distribution is thermal equilibrium?
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Question 9 - Solution The same mean energy does not specify a speed distribution A: one speed B: two speeds (a) Method and calculation ⟨v2⟩A = v2 0, ⟨v2⟩B = 1 2(0) + 1 2(2v2 0) = v2 0. ⟨K⟩A = ⟨K⟩B = K0 = 1 2mv2 0, vrms,A = vrms,B = v0. ⟨v⟩A = v0, ⟨v⟩B = v0/ √ 2. (b) Interpretation and further calculation VarA(K) = 0, VarB(K) = 1 2(0 −K0)2 + 1 2(2K0 −K0)2 = K2 0. Tenergy = 2K0/(3kB) is the same for both. Equal mean energy fixes only one moment. These artificial discrete distributions need not be equilibrium distributions. Physical check Pressure in the isotropic kinetic model also agrees at equal number density, despite the different higher moments.

Question 9

The same mean energy does not specify a speed distribution

Two isotropic populations consist of particles of identical mass mm. Population A has every speed equal to v0v_0. In B, half the particles are at rest and half have speed 2v0\sqrt2v_0. Both have zero mean velocity. No Maxwell-distribution assumption is made.

Diagram shown in the original SVG worksheet.

  1. Compare their mean kinetic energies, rms speeds and mean speeds.

  2. Calculate the kinetic-energy variance in each population. Can assigning the same energy-equivalent temperature prove either distribution is thermal equilibrium?

Question 9 - Solution

The same mean energy does not specify a speed distribution

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨v2⟩A=v02,⟨v2⟩B=12(0)+12(2v02)=v02.\langle v^2\rangle_A=v_0^2,\quad\langle v^2\rangle_B=\tfrac12(0)+\tfrac12(2v_0^2)=v_0^2.⟨K⟩A=⟨K⟩B=K0=12mv02,vrms,A=vrms,B=v0.\langle K\rangle_A=\langle K\rangle_B=K_0=\tfrac12mv_0^2,\quad v_{{\mathrm{rms}},A}=v_{{\mathrm{rms}},B}=v_0.⟨v⟩A=v0,⟨v⟩B=v0/2.\langle v\rangle_A=v_0,\quad\langle v\rangle_B=v_0/\sqrt2.

(b) Interpretation and further calculation

Var⁡A(K)=0,Var⁡B(K)=12(0−K0)2+12(2K0−K0)2=K02.\operatorname{Var}_A(K)=0,\quad\operatorname{Var}_B(K)=\tfrac12(0-K_0)^2+\tfrac12(2K_0-K_0)^2=K_0^2.Tenergy=2K0/(3kB)is the same for both.T_{\mathrm{energy}}=2K_0/(3k_B)\quad\text{is the same for both}.Equal mean energy fixes only one moment. These artificial discrete distributions need not be equilibrium distributions.

Physical check

Pressure in the isotropic kinetic model also agrees at equal number density, despite the different higher moments.