Dielectrics: An Atomic View — Question 3

Section 25-6 · Physics pages 4116–4117

Question 3 A two-orientation model saturates through unequal thermal populations Independent permanent dipoles of magnitude p can point only parallel or antiparallel to E. Their energies are -pE and +pE. At temperature T their probabilities are proportional to e−U/(kBT). Define x = pE/(kBT). −pE +pE E Schematic; labels, not drawing lengths, specify the data. (a) Find the population ratio and average moment along E. (b) Find weak-field susceptibility for number density n and the strong-field saturation polarization.
Show solutionHide solution
Question 3 - Solution A two-orientation model saturates through unequal thermal populations −pE +pE E (a) Method and calculation N+ N− = e2x, ⟨pz⟩= pex −e−x ex + e−x = p tanh x. P = np tanh x. (b) Interpretation and further calculation x ≪1 : P ≃np2 kBT E ⇒χ = np2 ϵ0kBT . x →+∞: P →np. Physical check This restricted two-state model is not the same as freely rotating three-dimensional dipoles.

Question 3

A two-orientation model saturates through unequal thermal populations

Independent permanent dipoles of magnitude p can point only parallel or antiparallel to E. Their energies are -pE and +pE. At temperature T their probabilities are proportional to e−U/(kBT)e^{-U/(k_BT)}. Define x=pE/(kBT)x=pE/(k_BT).

Diagram shown in the original SVG worksheet.

  1. Find the population ratio and average moment along E.

  2. Find weak-field susceptibility for number density n and the strong-field saturation polarization.

Question 3 - Solution

A two-orientation model saturates through unequal thermal populations

Diagram shown in the original SVG worksheet.

(a) Method and calculation

N+N−=e2x,⟨pz⟩=pex−e−xex+e−x=ptanh⁡x.\frac{N_+}{N_-}=e^{2x},\quad\langle p_z\rangle=p\frac{e^x-e^{-x}}{e^x+e^{-x}}=p\tanh x.P=nptanh⁡x.P=np\tanh x.

(b) Interpretation and further calculation

x≪1:P≃np2kBTE⇒χ=np2ϵ0kBT.x\ll1:\quad P\simeq\frac{np^2}{k_BT}E\Rightarrow\chi=\frac{np^2}{\epsilon_0k_BT}.x→+∞:P→np.x\to+\infty:\quad P\to np.

Physical check

This restricted two-state model is not the same as freely rotating three-dimensional dipoles.