Paramagnetism — Question 1

Section 32-9 · Physics pages 5332–5333

Question 1 Two thermal populations produce a bounded paramagnetic magnetization Independent moments have field-axis projections +µ and −µ, energies −µB and +µB, and number density n. Let x = µB/(kBT) and assign Boltzmann weights to the two states. −µB, +µ +µB, −µ 2µB Schematic; labels, not drawing lengths, specify the data. (a) Normalize the populations and derive M as a function of x. (b) Find x and the population ratio when M is one-half of the saturation magnetization.
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Question 1 - Solution Two thermal populations produce a bounded paramagnetic magnetization −µB, +µ +µB, −µ 2µB (a) Method and calculation P+ = ex ex + e−x , P−= e−x ex + e−x . M = nµ(P+ −P−) = nµ tanh x . (b) Interpretation and further calculation M/(nµ) = 1/2 ⇒e2x −1 e2x + 1 = 1 2 ⇒e2x = 3. x = 1 2 ln 3, N+/N−= 3 . Physical check Saturation is nmu, because it counts the largest allowed field-axis projection of every moment.

Question 1

Two thermal populations produce a bounded paramagnetic magnetization

Independent moments have field-axis projections +μ+\mu and −μ-\mu, energies −μB-\mu B and +μB+\mu B, and number density n. Let x=μB/(kBT)x=\mu B/(k_BT) and assign Boltzmann weights to the two states.

Diagram shown in the original SVG worksheet.

  1. Normalize the populations and derive M as a function of x.

  2. Find x and the population ratio when M is one-half of the saturation magnetization.

Question 1 - Solution

Two thermal populations produce a bounded paramagnetic magnetization

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P+=exex+e−x,P−=e−xex+e−x.P_+=\frac{e^x}{e^x+e^{-x}},\quad P_-=\frac{e^{-x}}{e^x+e^{-x}}.M=nμ(P+−P−)=nμtanh⁡x.\boxed{M=n\mu(P_+-P_-)=n\mu\tanh x}.

(b) Interpretation and further calculation

M/(nμ)=1/2⇒e2x−1e2x+1=12⇒e2x=3.M/(n\mu)=1/2\Rightarrow\frac{e^{2x}-1}{e^{2x}+1}=\frac12\Rightarrow e^{2x}=3.x=12ln⁡3,N+/N−=3.\boxed{x=\tfrac12\ln3,\quad N_+/N_-=3}.

Physical check

Saturation is nmu, because it counts the largest allowed field-axis projection of every moment.