1994
DOI: 10.1088/0965-0393/2/1/004
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Elastic and fracture properties of the two-dimensional triangular and square lattices

Abstract: Lattice models are finding increasing use in modeling the elastic and fracture behaviour of inhomogeneous or multi-phase systems. The elastic and failure properties of a rotationally invariant formulation of the bond-bending model on the two-dimensional triangular (with first-neighbour couplings) and on a novel version of the square lattice (involving first- and second-neighbour couplings) are examined. Expressions for the elastic constants of the bond-bending model on the above mentioned lattices are given in… Show more

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Cited by 144 publications
(97 citation statements)
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“…As a result, the external tension needed to break the first bond in any lattice of identical bonds depends on the direction of the tension. This anisotropy was quantified by Monette and Anderson [1994] for triangular and square lattices with and without bond bending resistance. They showed that for lattices without any disorder in the breaking thresholds, there is always anisotropy, mostly so for the triangular, central force network that we apply.…”
Section: Solid Elastic Componentmentioning
confidence: 99%
See 1 more Smart Citation
“…As a result, the external tension needed to break the first bond in any lattice of identical bonds depends on the direction of the tension. This anisotropy was quantified by Monette and Anderson [1994] for triangular and square lattices with and without bond bending resistance. They showed that for lattices without any disorder in the breaking thresholds, there is always anisotropy, mostly so for the triangular, central force network that we apply.…”
Section: Solid Elastic Componentmentioning
confidence: 99%
“…where E is Young's modulus and n the Poisson ratio [Landau and Lifshitz, 1959;Monette and Anderson, 1994] to identify the values…”
Section: Continuum Limitmentioning
confidence: 99%
“…We obtain the following equations We obtain two values of t from the quadratic (16). If either of the values are between 0 and 1 then we can substitute this value into (15) to obtain a value of s. If this yields Fig. 8 Intersection of a line (LB link) with a 'tile' (area between neighbouring nodes of a LSM lattice) a value of s between 0 and 1, we can substitute this value, and the t value, into (14) to obtain a value for u.…”
Section: Discussionmentioning
confidence: 99%
“…We consider simple Hookean springs where k ij is the spring constant. This form of the free energy can be linearised and mapped onto continuum elasticity theory to give the following inplane Young's modulus [14,15] …”
Section: Solid Mechanicsmentioning
confidence: 99%
“…If the spring constants of horizontal/vertical, diagonal and torsional springs are 2k, k and c, respectively, then the system is isotropic with elastic modulus, E, and the Poisson ratio, v, given by [54] …”
Section: Random Spring Network Modelmentioning
confidence: 99%