2003
DOI: 10.1016/s0020-7683(02)00584-x
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Non-linear micropolar and classical continua for anisotropic discontinuous materials

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Cited by 113 publications
(102 citation statements)
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“…However, for this class of composites the classical (Cauchy) homogenization may have disadvantages and non-local constitutive models may be necessary to include geometric and 3 material length scales to appreciate the influence of block size and of high stress and strain gradients (see for instance Bacigalupo and Gambarotta, 2011, 2012, 2014. The rotational degrees of freedom of the blocks suggests to consider the Cosserat model as equivalent continuum and accordingly homogenization techniques in the static field have been proposed for blocky rocks (Mühlhaus, 1993), granular regularly packed materials (see Kruyt, 2003, Li et al, 2010, among the others) and periodic masonry (Masiani et al, 1995, Trovalusci and Masiani, 2003, Pau and Trovalusci, 2012, Baraldi et al, 2015, among the others).…”
Section: Introductionmentioning
confidence: 99%
“…However, for this class of composites the classical (Cauchy) homogenization may have disadvantages and non-local constitutive models may be necessary to include geometric and 3 material length scales to appreciate the influence of block size and of high stress and strain gradients (see for instance Bacigalupo and Gambarotta, 2011, 2012, 2014. The rotational degrees of freedom of the blocks suggests to consider the Cosserat model as equivalent continuum and accordingly homogenization techniques in the static field have been proposed for blocky rocks (Mühlhaus, 1993), granular regularly packed materials (see Kruyt, 2003, Li et al, 2010, among the others) and periodic masonry (Masiani et al, 1995, Trovalusci and Masiani, 2003, Pau and Trovalusci, 2012, Baraldi et al, 2015, among the others).…”
Section: Introductionmentioning
confidence: 99%
“…Normal force and bending moments must satisfy the following conditions: First and second conditions in Equation (8) have been already adopted by authors for the in plane case [11] and they turn out to be coincident to those adopted by Trovalusci and Masiani [16]. In particular, the first condition may be defined as 'detachment' condition, whereas the second and third ones may be defined as 'rotation' conditions with respect to y 1 and y 2 axis.…”
Section: Normal and Flexural Interface Strengthmentioning
confidence: 88%
“…In the last years, several modifications to the classical CHM have been proposed, and a review on recent developments can be found in [35] and in the references therein. Some approaches regularize the response of the RVE by using a higher order theory at the macro-scale, such that the information about a material characteristic length is naturally taken into account [3,16,17,18,22,23,52]. Others, known as continuousdiscontinuous approaches, up-scale the RVE response to a traction-separation law (upon strain localization) used by a discontinuity inserted into the macro-scale model [6,8,30,31,32,33,37,39].…”
Section: Introductionmentioning
confidence: 99%