An atomistic-based finite deformation continuum membrane model for monolayer Transition Metal Dichalcogenides. (November 2022)

• Record Type: Journal Article
• Authors: Yadav, Upendra; Ghosh, Susanta
• Is Part Of: Journal of the mechanics and physics of solids. Volume 168(2022)
• Publication Date: 2022-11
• Subjects: Crystal-elasticity -- Molybdenum Disulfide -- Transition Metal Dichalcogenide (TMD) -- Cauchy–Born rule -- 2D materials; Mechanics, Applied -- Periodicals; Solids -- Periodicals; Mechanics -- Periodicals; Mécanique appliquée -- Périodiques; Solides -- Périodiques; Mechanics, Applied; Solids; Periodicals; 531.05
• DOI: 10.1016/j.jmps.2022.105033
• Languages: English
• ISSNs: 0022-5096

Abstract

Abstract: A finite-deformation crystal-elasticity membrane model for Transition Metal Dichalcogenide (TMD) monolayers is presented. Monolayer TMDs are multi-atom-thick two-dimensional (2D) crystalline membranes having atoms arranged on three parallel surfaces. In the present formulation, the deformed configuration of a TMD-membrane is represented through the deformation map of its middle surface and two stretches normal to the middle surface. Crystal-elasticity -based kinematic rules are employed to express the deformed bond lengths and bond angles of TMDs in terms of the continuum strains. The continuum hyper-elastic strain energy of the TMD membrane is formulated from its inter-atomic potential. The relative shifts between two simple lattices of TMDs are also considered in the constitutive relation. A smooth finite element framework using B-splines is developed to numerically implement the present continuum membrane model. The proposed model generalizes the crystal-elasticity -based membrane theory of purely 2D membranes, such as graphene, to the multi-atom-thick TMD crystalline membranes. The significance of relative shifts and two normal stretches are demonstrated through numerical results. The proposed atomistic-based continuum model accurately matches the material moduli, complex post-buckling deformations, and the equilibrium energies predicted by the purely atomistic simulations. It also accurately reproduces the experimental results for large-area TMD samples containing tens of millions of atoms. Highlights: A finite-deformation crystal-elastic membrane model for TMD monolayers is presented. Strains of the middle surface and two normal-stretches describe the deformation. The continuum hyperelastic strain energy is obtained from an interatomic potential. The present model matches well with the purely atomistic simulations.