TY - JOUR
T1 - Chirality in isotropic linear gradient elasticity
AU - Papanicolopulos, S.-A.
N1 - Copyright 2011 Elsevier B.V., All rights reserved.
PY - 2011/3/1
Y1 - 2011/3/1
N2 - Chirality is, generally speaking, the property of an object that can be classified as left- or right-handed. Though it plays an important role in many branches of science, chirality is encountered less often in continuum mechanics, so most classical material models do not account for it. In the context of elasticity, for example, classical elasticity is not chiral, leading different authors to use Cosserat elasticity to allow modelling of chiral behaviour. Gradient elasticity can also model chiral behaviour, however this has received much less attention than its Cosserat counterpart. This paper shows how in the case of isotropic linear gradient elasticity a single additional parameter can be introduced that describes chiral behaviour. This additional parameter, directly linked to three-dimensional deformation, can be either negative or positive, with its sign indicating a discrimination between the two opposite directions of torsion. Two simple examples are presented to show the practical effects of the chiral behaviour.
AB - Chirality is, generally speaking, the property of an object that can be classified as left- or right-handed. Though it plays an important role in many branches of science, chirality is encountered less often in continuum mechanics, so most classical material models do not account for it. In the context of elasticity, for example, classical elasticity is not chiral, leading different authors to use Cosserat elasticity to allow modelling of chiral behaviour. Gradient elasticity can also model chiral behaviour, however this has received much less attention than its Cosserat counterpart. This paper shows how in the case of isotropic linear gradient elasticity a single additional parameter can be introduced that describes chiral behaviour. This additional parameter, directly linked to three-dimensional deformation, can be either negative or positive, with its sign indicating a discrimination between the two opposite directions of torsion. Two simple examples are presented to show the practical effects of the chiral behaviour.
KW - Chirality
KW - Microstructure
KW - Gradient elasticity
KW - Isotropy
KW - Torsion
UR - http://www.scopus.com/inward/record.url?partnerID=yv4JPVwI&eid=2-s2.0-78651407515&md5=c49f6e5ee18bfd7ad1b0e7b18ed3dcf4
U2 - 10.1016/j.ijsolstr.2010.11.007
DO - 10.1016/j.ijsolstr.2010.11.007
M3 - Article
AN - SCOPUS:78651407515
SN - 0020-7683
VL - 48
SP - 745
EP - 752
JO - International Journal of Solids and Structures
JF - International Journal of Solids and Structures
IS - 5
ER -