A thermoelectric leg converts a temperature gradient directly into electricity via the Seebeck effect. Its efficiency is set by the dimensionless figure of merit:
ZT = S²σT / κ
κ = κ_e + κ_lat (electronic + lattice/phonon)
κ_e = L·σ·T (Wiedemann-Franz law, L = Lorenz number)
1/κ_lat(d) grows as grain size d shrinks below the
phonon mean free path Λ → boundary scattering
Doping sets the carrier concentration n, which trades off two quantities in opposite directions — this is the classic thermoelectric bottleneck:
S(n) ∝ n^(-2/3) (Mott/degenerate-semiconductor formula: more carriers → less entropy per carrier → lower Seebeck voltage)
σ(n) ∝ n (more carriers → higher electrical conductivity)
The nanostructuring trick: grain boundaries scatter heat-carrying phonons (mean free path ~100–300 nm in most semiconductors) far more strongly than they scatter the much shorter-wavelength electrons. Shrinking the grain size d below the phonon mean free path collapses κlat while leaving S and σ almost untouched — a "phonon-glass, electron-crystal." That is exactly what the animation shows: electrons (blue) drift smoothly hot→cold, while phonons (orange) zig-zag and lose forward progress as the grains get smaller.
- Grain size — sets how often phonons scatter at a boundary; smaller grains ⇒ lower κlat ⇒ higher ZT, down to the amorphous limit.
- Carrier concentration — the Seebeck/conductivity trade-off; there is an optimum n that maximizes the power factor S²σ.
- Th / Tc — the driving temperature difference ΔT; output power scales with ΔT².
Real-world relevance: this phonon-glass/electron-crystal strategy (nanograined Bi₂Te₃, SiGe superlattices, skutterudites) is how modern thermoelectric generators recover waste heat from engines, spacecraft radioisotope generators, and industrial exhaust.