Thermodynamics of Crystals and Melting

Max Born Max Born
1939 The Journal of Chemical Physics 730 citations

Abstract

The Helmholtz free energy, A, of a rigid body is a function of temperature, and of the six homogeneous strain components. If the crystal is to be rigid, three inequalities must be satisfied for the derivatives of A with respect to the six strain components, for a regular (cubic) lattice. This enables one to limit the pressure-temperature range for which the crystal is stable. The violation of the condition c44>0, that the crystal resist shearing, is interpreted as leading to melting. From a knowledge of the forces between the molecules the phase integral, and therefore the free energy, may be calculated as a function of T, V, and the six strain components. The numerical calculations are carried out for a body-centered cubic lattice. The product of all the frequencies is calculated directly, so that the assumption that the Debye equation for the frequency distribution holds, is not necessary. The melting curve, pressure against temperature, is then determined.

Keywords

Helmholtz free energyShearing (physics)ThermodynamicsCrystal (programming language)Debye modelLattice (music)Phase transitionMelting pointCubic crystal systemCrystal structureMaterials scienceCondensed matter physicsPhysicsChemistryCrystallographyQuantum mechanics

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Publication Info

Year
1939
Type
article
Volume
7
Issue
8
Pages
591-603
Citations
730
Access
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Max Born (1939). Thermodynamics of Crystals and Melting. The Journal of Chemical Physics , 7 (8) , 591-603. https://doi.org/10.1063/1.1750497

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DOI
10.1063/1.1750497