HomeMaterials SciencePhonon Thermal Conductivity — the Umklapp Peak

Phonon Thermal Conductivity — the Umklapp Peak

Watch a phonon random-walk through a crystal lattice while a live κ(T) curve shows why thermal conductivity rises as T³ at low temperature, peaks, then falls as boundary scattering gives way to Umklapp phonon-phonon scattering.

Materials Science3DAdvanced60 FPS📱 Mobile-adapted
solid-state-physics ↗ Open standalone

Every crystalline solid's thermal conductivity κ(T) traces the same shape: it rises steeply at low temperature, peaks, then slowly falls as temperature keeps climbing. This simulator renders the two competing mechanisms behind that curve — a phonon gas whose heat capacity grows with temperature via the Debye model, and a mean free path that starts long (limited only by the crystal's grain boundaries) and collapses as Umklapp phonon-phonon scattering takes over. Pick a real material preset (diamond, silicon or rock salt), drag the temperature and grain-size sliders, and watch a single phonon's schematic random walk through a spring-coupled atomic chain while the live κ(T) chart traces out the conductivity peak in real time.

⚙ Under the hood

Watch a phonon random-walk through a crystal lattice while a live κ(T) curve shows why thermal conductivity rises as T³ at low temperature, peaks, then falls as boundary scattering gives way to Umklapp phonon-phonon scattering.

phononsthermal conductivitysolid state physicsumklapp scatteringdebye modelcrystal lattice

3D · Three.js / WebGL renderer · 60 FPS target · runs fully client-side, no install

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