A platform for research: civil engineering, architecture and urbanism
Cyclic secant shear modulus versus pore water pressure in sands at small cyclic strains
Abstract Cyclic strain-controlled behavior of fully saturated sands in undrained condition is analyzed at small cyclic shear strain amplitudes, γ c, around the threshold shear strain for cyclic pore water pressure buildup, γ tp≈0.01%. The cyclic triaxial and simple shear test results obtained in the past by different researchers and the results of new cyclic simple shear tests reveal that: (i) at very small γ c below γ tp where there is no buildup of cyclic pore water pressure, Δu N, with the number of cycles, N, the cyclic secant shear modulus, G SN, initially increases with N for 10–20% of its initial value G S1 and then levels off or just slightly decreases, (ii) at small γ c between γ tp≈0.01% and 0.10–0.15%, Δu N continuously increases with N while the modulus G SN first increases for up to 10% of G S1 and then gradually decreases, and (iii) at γ c larger than approximately 0.15%, relatively large Δu N develops with N while the modulus G SN constantly and significantly decreases. This means that at γ c between γ tp and 0.10–0.15% the sand stiffness initially increases with N in spite of the reduction of effective stresses caused by the cyclic pore water pressures buildup. In this range of γ c, the pore water pressure Δu N can reach up to 40% of the initial effective confining stress before G SN drops below G S1. The microstructural mechanisms believed to be responsible for such a complex behavior are discussed. It is suggested that during cyclic loading the changes at mineral-to-mineral junctions of grain contacts can cause soil stiffening while, at the same time, the buildup of cyclic pore water pressure causes the softening.
Highlights Behavior of fully saturated sand at small cyclic strains, γ c, is analyzed. Focus is on γ c around threshold for cyclic pore water pressure γ tp≈0.01%. Change of secant shear modulus, G SN, and cyclic pore pressure, Δu N, are correlated. At γ tp<γ c<0.10% G SN increases and then decreases, while Δu N always increases. Consequently, at γ tp<γ c<0.10% stiffness goes up while effective stress goes down.
Cyclic secant shear modulus versus pore water pressure in sands at small cyclic strains
Abstract Cyclic strain-controlled behavior of fully saturated sands in undrained condition is analyzed at small cyclic shear strain amplitudes, γ c, around the threshold shear strain for cyclic pore water pressure buildup, γ tp≈0.01%. The cyclic triaxial and simple shear test results obtained in the past by different researchers and the results of new cyclic simple shear tests reveal that: (i) at very small γ c below γ tp where there is no buildup of cyclic pore water pressure, Δu N, with the number of cycles, N, the cyclic secant shear modulus, G SN, initially increases with N for 10–20% of its initial value G S1 and then levels off or just slightly decreases, (ii) at small γ c between γ tp≈0.01% and 0.10–0.15%, Δu N continuously increases with N while the modulus G SN first increases for up to 10% of G S1 and then gradually decreases, and (iii) at γ c larger than approximately 0.15%, relatively large Δu N develops with N while the modulus G SN constantly and significantly decreases. This means that at γ c between γ tp and 0.10–0.15% the sand stiffness initially increases with N in spite of the reduction of effective stresses caused by the cyclic pore water pressures buildup. In this range of γ c, the pore water pressure Δu N can reach up to 40% of the initial effective confining stress before G SN drops below G S1. The microstructural mechanisms believed to be responsible for such a complex behavior are discussed. It is suggested that during cyclic loading the changes at mineral-to-mineral junctions of grain contacts can cause soil stiffening while, at the same time, the buildup of cyclic pore water pressure causes the softening.
Highlights Behavior of fully saturated sand at small cyclic strains, γ c, is analyzed. Focus is on γ c around threshold for cyclic pore water pressure γ tp≈0.01%. Change of secant shear modulus, G SN, and cyclic pore pressure, Δu N, are correlated. At γ tp<γ c<0.10% G SN increases and then decreases, while Δu N always increases. Consequently, at γ tp<γ c<0.10% stiffness goes up while effective stress goes down.
Cyclic secant shear modulus versus pore water pressure in sands at small cyclic strains
Vucetic, Mladen (author) / Mortezaie, Ahmadreza (author)
Soil Dynamics and Earthquake Engineering ; 70 ; 60-72
2014-12-05
13 pages
Article (Journal)
Electronic Resource
English
Cyclic secant shear modulus versus pore water pressure in sands at small cyclic strains
Online Contents | 2015
|Strain-Rate Effect on Soil Secant Shear Modulus at Small Cyclic Strains
British Library Online Contents | 2003
|Strain-Rate Effect on Soil Secant Shear Modulus at Small Cyclic Strains
Online Contents | 2003
|Pore Pressure Generation of Silty Sands due to Induced Cyclic Shear Strains
Online Contents | 2009
|