2008
DOI: 10.3208/sandf.48.727
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Behavior of Liquefied Sands Under Extremely Large Strain Levels in Cyclic Torsional Shear Tests

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Cited by 53 publications
(23 citation statements)
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“…It can be seen from Eq. (15) that the model gives pure elastic sand response at the onset of loading direction reversal as K p1 is infinite ðρ=ρ ¼ ∞Þ, which is supported by experimental observations (Kiyota et al 2008;Chiaro et al 2009). Whenρ ¼ ρ (corresponding to the virgin loading case),…”
Section: Plastic Modulus and Dilatancy Relation For Constant Mean Strsupporting
confidence: 56%
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“…It can be seen from Eq. (15) that the model gives pure elastic sand response at the onset of loading direction reversal as K p1 is infinite ðρ=ρ ¼ ∞Þ, which is supported by experimental observations (Kiyota et al 2008;Chiaro et al 2009). Whenρ ¼ ρ (corresponding to the virgin loading case),…”
Section: Plastic Modulus and Dilatancy Relation For Constant Mean Strsupporting
confidence: 56%
“…Experimental observations show that there is appreciable plastic strain accumulation in sand during cyclic shear (Oda et al 2001;Kiyota et al 2008;Chiaro et al 2009); hence, the authors employ a cone-shaped bounding surfacef 1 to describe sand behavior under such loading conditions (Fig. 1).…”
Section: Bounding Surfacef 1 and Yield Cap Fmentioning
confidence: 99%
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“…In addition, Kokusho (2000) reported that signiˆcant deformation could be associated not only with the driving force due to the gravity but also a formation of a water lm in the liqueˆed layer. In order to investigate the above large strain liquefaction properties, we modiˆed a torsional shear apparatus and performed a series of undrained cyclic torsional shear tests up to a double amplitude shear strain of about 100z (Kiyota et al, 2008). We found that there is a limiting value of double amplitude shear strain, g L(DA) , to initiate strain localization.…”
Section: Introductionmentioning
confidence: 99%