2016
DOI: 10.1088/0965-0393/24/4/045003
|View full text |Cite
|
Sign up to set email alerts
|

Application of the pair torque interaction potential to simulate the elastic behavior of SLMoS2

Abstract: This paper is devoted to the application of the pair torque interaction potential for the simulation of the elastic behavior of a promising two-dimensional material: single layer molybdenium disulphide (SLMoS2). It is demonstrated that both Mo–Mo and S–S interactions can be regarded as pair force interactions with sufficient accuracy. Using both experimental and calculated numerically elastic moduli, and also the phonon spectrum available in the literature, the parameters of the Morse potential are determined … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
8
0

Year Published

2017
2017
2020
2020

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 9 publications
(8 citation statements)
references
References 24 publications
(35 reference statements)
0
8
0
Order By: Relevance
“…The inequality ( 67) is satisfied identically for β > 1 − x2 ; β also satisfies the second inequality from (63). Then evaluation of the integral with respect to β, yields:…”
Section: Thermal Contact Of Hot and Cold Half-planesmentioning
confidence: 96%
See 1 more Smart Citation
“…The inequality ( 67) is satisfied identically for β > 1 − x2 ; β also satisfies the second inequality from (63). Then evaluation of the integral with respect to β, yields:…”
Section: Thermal Contact Of Hot and Cold Half-planesmentioning
confidence: 96%
“…This lattice is considered in detail in section 9. Two-dimensional scalar lattices can be considered as simplest models for out-of-plane (transverse) vibrations of 2D materials such as graphene [59,60,61,62], molybdenum disulphide [63,64], boron nitride [62], etc. Remark.…”
Section: Equations Of Motion and Initial Conditionsmentioning
confidence: 99%
“…As discussed below, the model is now fully cast into a vector-based format. 36,37 Figure 1(a) illustrates the mDEM representation of a CNT (left), where each mesoscopic distinct element (center) lumps a finite number of atoms of the atomistic model. The distinct elements in direct contact interact via the enhanced vector model (EVM) potential, 37 which describes the resistance to stretching, shear, bending, and torsional deformation displacements of the CNT portion of length T and radius r CNT as a Euler-Bernoulli beam.…”
Section: B Mdem For Cntsmentioning
confidence: 99%
“…The mDEM model for CNTs 20,24 was introduced in our previous works in conjunction with its implementation in the popular distinct element code PFC3D. 31 More recently, the model was adapted to a vector-based format 32 and implemented 30,33 in the code WaLBerla. 34 Relying on a scalable message passing interface framework, WaLBerla enables deterministic evolution of millions of distinct elements of given mass and moment of inertia.…”
Section: Mdem For Cntsmentioning
confidence: 99%
“…At nano scale level, covalent bonds (e.g. in graphene [4][5][6]22] and molybdenum disulfide [23]) can be simulated. At micro scale level, the EVM can be incorporated into coarse-grained models of macromolecules [13,14], nanotubes [15,16], aerogels, ceramics [11] etc.…”
Section: Discussionmentioning
confidence: 99%