Thermoelectric

last updated 2026-05-04 · +11 sources in last 30d

Physics / mechanism

Thermoelectrics convert a temperature gradient directly into electrical voltage (Seebeck effect) or drive heat flow using electrical current (Peltier effect). The figure of merit ZT = S²σT/κ governs efficiency, where S is the Seebeck coefficient, σ electrical conductivity, and κ thermal conductivity. Commercial bismuth telluride (Bi₂Te₃) modules sit at ZT ≈ 0.8–1.0, yielding ~5–8% conversion efficiency at ΔT ~200 K. Research materials—half-Heuslers, skutterudites, PbTe alloys, GeTe—push ZT to 1.5–2.5 in lab conditions. Nanostructuring and phonon engineering (grain boundary scattering, rattler atoms) are the dominant levers to suppress κ without degrading σ. Solid-state, no moving parts, long MTBF.

Competitive landscape

Competing cooling approaches: vapour-compression refrigeration (COP 2–4×, but mechanically complex), heat pipes (passive, no conversion), and phase-change materials (latent heat storage, not active). On the power-generation side, organic Rankine cycles and piezoelectrics compete for waste-heat harvesting at different temperature regimes.

ApproachEfficiencyScalabilityMoving parts
Thermoelectric5–8%Chip-to-kWNone
Vapour-compression30–50% (cooling COP)kW–MWYes
ORC (waste heat)10–20%kW–MWYes

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