INGENIA

CND-06

Debye T³ heat capacity

C_V = (12 π⁴ / 5) N k_B (T/θ_D)³ at T ≪ θ_D. The phonon T³ law.

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PhononsDebye T³

Governing equation

CV=12π45NkB(T/θD)3C_V=\dfrac{12\pi^4}{5}Nk_B(T/\theta_D)^3

T∈[0.5,80]T \in \left[0.5, 80\right]

where

T
Temperature (K)
\theta_D
Debye temperature (K)
n
Amount (mol)
C_V
Heat capacity (J/K)

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CND-06 · phase
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①

Governing law — red

CV=12π45NkB(T/θD)3C_V=\dfrac{12\pi^4}{5}Nk_B(T/\theta_D)^3

T∈[0.5,80]T \in \left[0.5, 80\right]

T=0.5T = 0.5CV=9×10−6C_V = 9\times 10^{-6}

②

Domain of the variable — blue

Tmin⁡=0.5,Tmax⁡=80T_{\min} = 0.5,\quad T_{\max} = 80

T∈[0.5,80]T \in \left[0.5, 80\right]

T=0.5T = 0.5T=0.5T = 0.5

③

Response curve — green

CV=12π45NkB(T/θD)3C_V=\dfrac{12\pi^4}{5}Nk_B(T/\theta_D)^3

T∈[0.5,80]T \in \left[0.5, 80\right]

T=0.5T = 0.5CV=9×10−6C_V = 9\times 10^{-6}

④

Rate of change — amber

dCVdT\frac{\mathrm{d}C_V}{\mathrm{d}T}

T∈[0.5,80]T \in \left[0.5, 80\right]

T=1T = 1CV′=2.34×10−4C_V^{\prime} = 2.34\times 10^{-4}

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-06 — Debye T³ heat capacity) is the form associated with Debye T³. Working symbols: TT, θD\theta_D, nn →\rightarrow CVC_V. Three acoustic branches, linear ω = v k, density of states ∝ ω². Dulong–Petit recovered at high T.

Purpose

Purpose: compute CVC_V from TT, θD\theta_D, nn in Condensed matter via CV=12π45NkB(T/θD)3C_V=\dfrac{12\pi^4}{5}Nk_B(T/\theta_D)^3 C_V = (12 π⁴ / 5) N k_B (T/θ_D)³ at T ≪ θ_D. The phonon T³ law. 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 T=10.000 KT = 10.000\,\mathrm{K}, θD=300.000 K\theta_D = 300.000\,\mathrm{K}, n=1.000 moln = 1.000\,\mathrm{mol}, the governing relation CV=12π45NkB(T/θD)3C_V=\dfrac{12\pi^4}{5}Nk_B(T/\theta_D)^3 yields CV=0.0720 J/KC_V = 0.0720\,\mathrm{J/K}. A C(T) that starts as T³. Move a slider: the numbers are this situation, not a canned story.

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Outputs

  • Heat capacity C_V0.0720 J/K
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CND-06 · phase
00:0 / 00:08

Narration of this film

A C(T) that starts as T³.

Three acoustic branches, linear ω = v k, density of states ∝ ω². Dulong–Petit recovered at high T.

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