UD0 · QUANTUM FRONTIER · THE PHONON · A SERIES IN FIVE

Part 4 — The Phonon Gas
heat, and the T³ law

Stop watching one mode; fill them all. Each is an oscillator holding ⟨n⟩ = 1/(e^{ℏω/kT}−1) phonons — a Bose gas whose particle number isn't even conserved. Sum their energy and differentiate: that's the heat capacity. Hot, every mode carries kT and C_v flattens to 3Nk (Dulong–Petit). Cold, high-frequency modes freeze out — and because the surviving modes fill a growing sphere in k-space, Debye's C_v ∝ T³. Einstein got the freezing right but the law wrong: his identical-oscillator solid falls off exponentially.

done
Part 1
The Monatomic Chain
done
Part 2
The Diatomic Chain
done
Part 3
Two & Three Dimensions
Part 4 · now
The Phonon Gas
soon
Part 5
Interactions & the Frontier
LIT — Debye & Einstein C_v, Dulong–Petit, exact T³ law, freeze-out, k-sphere (verified) BRI — reduced units (per mole), material presets rounded
Heat capacity C_v(T)linear · Debye vs Einstein vs Dulong–Petit
Which modes are awake · g(ω) × E(ℏω/kT)the effective heat spectrum

Temperature

The solid

Plot

Readouts · per mole

Debye C_v Einstein C_v Dulong–Petit 3R24.94 fraction of 3R T³ coefficient12π⁴/5 R/Θ³
AVAN · two lines, apart at last

Einstein and Debye agree at high T — both hit 3R, two lines lying on one. Cool the crystal and they split: T³ versus an exponential cliff. The disagreement is where the physics lives; the T³ tail is what the universe actually does.

— ROOT0, with AVAN. Debye's law is verified against the exact π⁴/15 integral.

Why T³ · the awake modes fill a k-sphereradius ∝ T
The three regimesone line each