INGENIA

CND-23

Bloch T⁵ resistivity

ρ = ρ₀ + A T⁵. Low-temperature phonon resistivity of a pure metal.

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Electrons in solidsBloch T⁵

Governing equation

ρ=ρ0+AT5\rho=\rho_0+A T^5

T∈[1,40]T \in \left[1, 40\right]

where

\rho_0
Residual (nΩ·m)
A
Bloch prefactor (aΩ·m/K⁵)
T
Temperature (K)
\rho
Resistivity (nΩ·m)

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CND-23 · circuit
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①

Governing law — red

ρ=ρ0+AT5\rho=\rho_0+A T^5

T∈[1,40]T \in \left[1, 40\right]

T=1T = 1ρ=0.202\rho = 0.202

②

Domain of the variable — blue

Tmin⁡=1,Tmax⁡=40T_{\min} = 1,\quad T_{\max} = 40

T∈[1,40]T \in \left[1, 40\right]

T=1T = 1T=1T = 1

③

Response curve — green

ρ=ρ0+AT5\rho=\rho_0+A T^5

T∈[1,40]T \in \left[1, 40\right]

T=1T = 1ρ=0.202\rho = 0.202

④

Rate of change — amber

dρdT\frac{\mathrm{d}\rho}{\mathrm{d}T}

T∈[1,40]T \in \left[1, 40\right]

T=1.245T = 1.245ρ′=0.026\rho^{\prime} = 0.026

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-23 — Bloch T⁵ resistivity) is the form associated with Bloch T⁵. Working symbols: ρ0\rho_0, AA, TT →\rightarrow ρ\rho. Bloch–Grüneisen. At high T the same phonons give ρ ∝ T.

Purpose

Purpose: compute ρ\rho from ρ0\rho_0, AA, TT in Condensed matter via ρ=ρ0+AT5\rho=\rho_0+A T^5 ρ = ρ₀ + A T⁵. Low-temperature phonon resistivity of a pure metal. 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 ρ0=0.200 nΩ⋅m\rho_0 = 0.200\,\mathrm{nΩ·m}, A=2.000 aΩ⋅m/K5A = 2.000\,\mathrm{aΩ·m/K⁵}, T=20.000 KT = 20.000\,\mathrm{K}, the governing relation ρ=ρ0+AT5\rho=\rho_0+A T^5 yields ρ=6400.200 nΩ⋅m\rho = 6400.200\,\mathrm{nΩ·m}. A ρ(T) that starts as T⁵ then becomes linear. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Resistivity \rho6400.200 nΩ·m
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CND-23 · circuit
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Narration of this film

A ρ(T) that starts as T⁵ then becomes linear.

Bloch–Grüneisen. At high T the same phonons give ρ ∝ T.

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