Mechanics of Unsaturated Geomaterials 2013
DOI: 10.1002/9781118616871.ch4
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Experimental Techniques for Unsaturated Geomaterials

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Cited by 5 publications
(6 citation statements)
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“…Finally shearing of the samples was achieved in drained conditions, with a vertical strain rate of 0.0025 mm/min. This strain rate corresponds to the recommendations available in literature for similar soil texture (Delage, 2002;Gulhati & Satija, 1981) and enables to guarantee that the difference between pore water pressure and air pressure (uw-ua) remains constant during shearing. The crosssection of samples under loading was calculated according to Head & Epps (1980).…”
Section: Suction-controlled Triaxial Testssupporting
confidence: 66%
“…Finally shearing of the samples was achieved in drained conditions, with a vertical strain rate of 0.0025 mm/min. This strain rate corresponds to the recommendations available in literature for similar soil texture (Delage, 2002;Gulhati & Satija, 1981) and enables to guarantee that the difference between pore water pressure and air pressure (uw-ua) remains constant during shearing. The crosssection of samples under loading was calculated according to Head & Epps (1980).…”
Section: Suction-controlled Triaxial Testssupporting
confidence: 66%
“…In macro-scale experiments, to relate cohesion, or strength in general, to suction, it is customary to first bring an originally unloaded sample to a desired level of saturation, and then at a constant saturation, load the material until yielding (see e.g. Delage, 2013). At micro-scale, however, the attractive adhesion force has its maximum at a close contact of the grains (almost, but not necessarily, at zero separation) and decreases during an increasing separation, lowering the strength of adhesion, as seen in experiments with evaporation and extension of two-grain systems (Mielniczuk et al, 2014a).…”
Section: Micro-scale Experimentsmentioning
confidence: 99%
“…Because of the multiscale structure of clay minerals, a continuum of water populations, usually divided into interparticle and interlayer water, is observed when smectites are exposed to water vapor, Figure . The interlayer water can be further separated into water that directly hydrates the interlayer cation (termed cation-coordinated water herein), H-bonded water that surrounds the cation-coordinated water, and water that is loosely H-bonded to the clay mineral surface. Some of the interlayer water can be strongly bound, having suction potentials well in excess of several tens to hundreds of MPa . The intraparticle water includes water found at the edges and external surfaces of the layer structure and some of this may indeed act as weakly H-bonded interlayer water.…”
Section: Introductionmentioning
confidence: 99%
“…Simplistic model of the water population continuum in Ca-Mt usually divided into interparticle (water residing within pores) and interlayer (cation-coordinated water that is retained to very high suction potentials, tightly H-bonded water that hydrates the cation-coordinated water and water that is weakly H-bonded to the clay mineral surface) water . The energy of H-bonded water decreases from cation-coordinated to tightly H-bonded to weakly H-bonded interlayer water to bulklike intra- and interparticle water.…”
Section: Introductionmentioning
confidence: 99%