A Hint of Quantum Theory — Question 1

Section 19-9 · Physics pages 3192–3193

Question 1 An energy gap suppresses excited populations at low temperature An internal molecular mode has two nondegenerate levels, E0 = 0 and E1 = ∆. Thermal equilibrium gives P1/P0 = e−∆/(kBT) and P0 + P1 = 1. Let Θ = ∆/kB = 400 K. E0 = 0 ∆ one state Horizontal lines represent allowed internal energies, not spatial positions. (a) Find the excited fraction at 100 K and 400 K. (b) Find the largest temperature for which the excited fraction is at most 1.00%. Explain why comparing kBT with the gap is a crossover estimate rather than an abrupt activation threshold.
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Question 1 - Solution An energy gap suppresses excited populations at low temperature E0 = 0 ∆ one state (a) Method and calculation P1 = e−Θ/T 1 + e−Θ/T = 1 eΘ/T + 1. P1(100) = 1 e4 + 1 ≈.0179862, P1(400) = 1 e + 1 ≈.268941. (b) Interpretation and further calculation P1 ≤.0100 ⇒e400/T ≥99 ⇒T ≤400 ln 99 ≈87.0489 K. 0 < P1(T) < 1 2 for finite T > 0. Occupation changes smoothly; a specified small population defines a quantitative freeze-out criterion. Physical check An exponentially small excited population is not mathematically zero at finite positive temperature.

Question 1

An energy gap suppresses excited populations at low temperature

An internal molecular mode has two nondegenerate levels, E0=0E_0=0 and E1=ΔE_1=\Delta. Thermal equilibrium gives P1/P0=e−Δ/(kBT)P_1/P_0=e^{-\Delta/(k_BT)} and P0+P1=1P_0+P_1=1. Let Θ=Δ/kB=400\Theta=\Delta/k_B=400 K.

Diagram shown in the original SVG worksheet.

  1. Find the excited fraction at 100 K and 400 K.

  2. Find the largest temperature for which the excited fraction is at most 1.00%. Explain why comparing kBTk_BT with the gap is a crossover estimate rather than an abrupt activation threshold.

Question 1 - Solution

An energy gap suppresses excited populations at low temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P1=e−Θ/T1+e−Θ/T=1eΘ/T+1.P_1=\frac{e^{-\Theta/T}}{1+e^{-\Theta/T}}=\frac1{e^{\Theta/T}+1}.P1(100)=1e4+1≈.0179862,P1(400)=1e+1≈.268941.P_1(100)=\frac1{e^4+1}\approx.0179862,\quad P_1(400)=\frac1{e+1}\approx.268941.

(b) Interpretation and further calculation

P1≤.0100⇒e400/T≥99⇒T≤400ln⁡99≈87.0489K.P_1\le.0100\ \Rightarrow\ e^{400/T}\ge99\ \Rightarrow\ T\le\frac{400}{\ln99}\approx87.0489\,\mathrm K.0<P1(T)<12for finite T>0.0<P_1(T)<\tfrac12\quad\text{for finite }T>0.Occupation changes smoothly; a specified small population defines a quantitative freeze-out criterion.

Physical check

An exponentially small excited population is not mathematically zero at finite positive temperature.