The atomistic representation of first strain-gradient elastic tensors
Nikhil Chandra Admal, Jaime Marian, Giacomo Po

TL;DR
This paper derives atomistic formulas for strain-gradient elastic tensors in multi-lattices, linking atomic interactions to continuum elasticity, and analyzes their properties and stability implications.
Contribution
It provides closed-form, local atomistic expressions for all first strain-gradient elastic tensors, extending classical elasticity theory to include higher-order effects.
Findings
Odd-order tensors vanish in centrally symmetric lattices.
Strain-gradient tensors are indefinite for many potentials.
Cauchy relations hold for central potentials in simple lattices.
Abstract
We derive the atomistic representations of the elastic tensors appearing in the linearized theory of first strain-gradient elasticity for an arbitrary multi-lattice. In addition to the classical (2nd-Piola) stress and elastic moduli tensors, these include the rank-three double-stress tensor, the rank-five tensor of mixed elastic moduli, and the rank-six tensor of strain-gradient elastic moduli. The atomistic representations are closed-form analytical expressions in terms of the first and second derivatives of the interatomic potential with respect to interatomic distances, and dyadic products of relative atomic positions. Moreover, all expressions are local, in the sense that they depend only on the atomic neighborhood of a lattice site. Our results emanate from the condition of energetic equivalence between continuum and atomistic representations of a crystal, when the kinematics of…
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