1998
DOI: 10.1139/t98-028
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A numerical solution of cavity expansion problem in sand based directly on experimental stress-strain curves

Abstract: A numerical solution of a spherical and cylindrical cavity expansion problem in sand is presented herein. The underlying theory is unbiased in that it is based directly on experimentally determined stress-strain curves. The solution makes it possible to follow the continuous variation of strains, stresses, and volume changes produced by cavity expansion. It essentially uses the "strain path" approach to determine the state of stress around the cavity, taking into account large strains and the effect of spheric… Show more

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Cited by 24 publications
(5 citation statements)
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“…We select a value of M c at the lower end of this range because we expect that the effective pressure in the sediment is low as a result of generally high water pressures (locally exceeding ice-overburden pressure) in the hydraulically unconnected region of the glacier bed [e.g., Hubbard et al, 1995]. The value of L is taken between 0.3 and 0.6 m (10 -20 rod diameters) as determined by the cavity expansion theory [e.g., Ladanyi and Foriero, 1998]. Together with typical peak-to-peak velocity variations of $0.02 -0.03 m day À1 (Figure 3a) and hydraulic diffusivities for subglacial sediment ranging from 10 À7 to 10 À4 m 2 s À1 [Freeze and Cherry, 1979] in equations (3) and (2), we obtain amplitudes of excess pore-pressure variations immediately in front of the rod tip between 0.4 and 1.6 m.…”
Section: Calculation Of Pore Water Pressurementioning
confidence: 99%
“…We select a value of M c at the lower end of this range because we expect that the effective pressure in the sediment is low as a result of generally high water pressures (locally exceeding ice-overburden pressure) in the hydraulically unconnected region of the glacier bed [e.g., Hubbard et al, 1995]. The value of L is taken between 0.3 and 0.6 m (10 -20 rod diameters) as determined by the cavity expansion theory [e.g., Ladanyi and Foriero, 1998]. Together with typical peak-to-peak velocity variations of $0.02 -0.03 m day À1 (Figure 3a) and hydraulic diffusivities for subglacial sediment ranging from 10 À7 to 10 À4 m 2 s À1 [Freeze and Cherry, 1979] in equations (3) and (2), we obtain amplitudes of excess pore-pressure variations immediately in front of the rod tip between 0.4 and 1.6 m.…”
Section: Calculation Of Pore Water Pressurementioning
confidence: 99%
“…TICT/WICT excited-state formation is strongly favoured in polar solvents, 39 however, the nature of emitting species and their temperature dependencies are more complex in polar solvents. The specific solvent-solute interactions play a significant role in the nature of excited-state charge distribution, 40 in particular, the solvent molecules reorient themselves in the vicinity of solute molecules with decreasing temperatures, 41 and excited-state energy is transferred from the solute to solvent, so that the fluorescence peak exhibits a thermally-activated and solvent polarity assisted behaviour. 42 However, for potential use in optical devices, ICT emission has to be stabilised in the solid state.…”
Section: Introductionmentioning
confidence: 99%
“…This theory leads to a conclusion that at the cavity wall the shear strain is in®nite, when the cavity is expanded from zero radius (Collins & Yu, 1996). Ladanyi & Foriero (1998) have shown that, when the large strain assumption is followed throughout the development, it leads to the conclusion that the shear strain at the expanding cavity wall cannot exceed a value of ða2, or about 157%. This alternative result casts some doubt on the authors' conclusion that`the s u value interpreted directly from the corrected cone resistance will be 59% higher than the reference s u .…”
Section: B Ladanyi E â Cole Polytechnique Montre âAl Canadamentioning
confidence: 99%
“…This de®nition results in in®nite shear strain when the radial strain is in®nite or when the cavity is expanded from zero radius. Ladanyi & Foriero (1998) reported that that the shear strain at the expanding cavity cannot exceed a value of ða2. This conclusion is believed to be applicable only to compression or extension of a long cylinder and thus is not applicable to the cavity expansion problem.…”
Section: Authors' Replymentioning
confidence: 99%