2006
DOI: 10.1103/physreve.73.051304
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Shear strength properties of wet granular materials

Abstract: We investigate shear strength properties of wet granular materials in the pendular state (i.e. the state where the liquid phase is discontinuous) as a function of water content. Sand and glass beads were wetted and tested in a direct shear cell and under various confining pressures. In parallel, we carried out three-dimensional molecular dynamics simulations by using an explicit equation expressing capillary force as a function of interparticle distance, water bridge volume and surface tension. We show that, d… Show more

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Cited by 224 publications
(230 citation statements)
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“…7). This domain corresponds to low water contents when the capillary cohesion increases with the water content as shown by Soulié et al [11] and Richefeu et al [10]. During wetting, the capillary bridges merge and the liquid phase becomes continuous in the sample.…”
Section: Discussionmentioning
confidence: 97%
“…7). This domain corresponds to low water contents when the capillary cohesion increases with the water content as shown by Soulié et al [11] and Richefeu et al [10]. During wetting, the capillary bridges merge and the liquid phase becomes continuous in the sample.…”
Section: Discussionmentioning
confidence: 97%
“…In other words, considering only the lengths of the contacts, the weakest "link" in our system is the path of intercell contacts having the shortest length. In this sense, the variability of compressive strength reflects the statistics of all paths (with their different lengths and directions), on one hand, and the heterogeneous distribution of forces, as generally observed in granular materials, on the other hand [56,69,85,86].…”
Section: Scale Dependencementioning
confidence: 99%
“…The rupture can thus be regarded as brittle -although for low P * c samples may still withstand smaller tensions, as they get progressively torn apart in a strain-controlled test. Classically, the strength of a cohesive material is assessed with the so-called Rumpf formula [9], which amounts in the present case to replacing the average normal force F N by −F 0 in relation F N = 7πaP/(zΦ) (which is nearly exact [10] and directly stems from the classical expression of stresses as sums over contacts involving forces and branch vectors). The Rumpf formula was proposed decades ago [14], based on the assumption that a large population of contacts simultaneously break in tension.…”
Section: Tensile Strengthmentioning
confidence: 99%
“…The present communication investigates those phenomena by discrete element simulations in quasistatic conditions. Such a situation, with loose systems, has hardly been addressed by numerical means, as the recent literature rather explored dynamic compaction [4,5], gravity deposition [6], steady flows [7], or denser materials [8,9]. We introduce a simple model material and report on its consolidation properties, in relation to its microstructure, thus presenting a brief account of studies published in two recent papers [10,11], to which a section with new results on the resistance to tension is added.…”
Section: Introductionmentioning
confidence: 99%