INGENIA

CND-18

Curie–Weiss susceptibility

χ = C / (T − θ). Mean-field magnet above a Curie (or Néel) temperature.

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Electrons in solidsCurie–Weiss

Governing equation

χ=C/(T−θ)\chi=C/(T-\theta)

T∈[5,800]T \in \left[5, 800\right]

where

C
Curie constant (K)
\theta
Weiss temperature (K)
T
Temperature (K)
\chi
Susceptibility (—)

The figure, part by part

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CND-18 · phase
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①

Governing law — red

χ=C/(T−θ)\chi=C/(T-\theta)

T∈[5,800]T \in \left[5, 800\right]

T=5T = 5χ=6\chi = 6

②

Domain of the variable — blue

Tmin⁡=5,Tmax⁡=800T_{\min} = 5,\quad T_{\max} = 800

T∈[5,800]T \in \left[5, 800\right]

T=5T = 5T=5T = 5

③

Response curve — green

χ=C/(T−θ)\chi=C/(T-\theta)

T∈[5,800]T \in \left[5, 800\right]

T=5T = 5χ=6\chi = 6

④

Rate of change — amber

dχdT\frac{\mathrm{d}\chi}{\mathrm{d}T}

T∈[5,800]T \in \left[5, 800\right]

T=10T = 10χ′=0\chi^{\prime} = 0

Lecture brief

Historical brief

Drude electrons, Bloch waves, BCS pairing (1957) and Wiedemann–Franz heat are the first solids-and-metals laws. The lab is conductivity, gap and phonon heat in closed form. This sheet (CND-18 — Curie–Weiss susceptibility) is the form associated with Curie–Weiss. Working symbols: CC, θ\theta, TT →\rightarrow χ\chi. θ > 0 ferromagnetic, θ < 0 antiferromagnetic. Divergence is cut off by order.

Purpose

Purpose: compute χ\chi from CC, θ\theta, TT in Condensed matter via χ=C/(T−θ)\chi=C/(T-\theta) χ = C / (T − θ). Mean-field magnet above a Curie (or Néel) temperature. Use it when a real condensed matter question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given C=1.200 KC = 1.200\,\mathrm{K}, θ=100.000 K\theta = 100.000\,\mathrm{K}, T=300.000 KT = 300.000\,\mathrm{K}, the governing relation χ=C/(T−θ)\chi=C/(T-\theta) yields χ=0.006 —\chi = 0.006\,\mathrm{—}. A 1/(T−θ) curve, a pole at θ. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Susceptibility \chi0.006 —
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CND-18 · phase
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Narration of this film

A 1/(T−θ) curve, a pole at θ.

θ > 0 ferromagnetic, θ < 0 antiferromagnetic. Divergence is cut off by order.

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