EFFECTS OF INITIAL SHEAR STRESS AND VIBRATION FREQUENCY ON THE DYNAMIC STRENGTH CHARACTERISTICS OF SATURATED CLAY
Abstract
Initial shear stress is inevitable in actual engineering slopes, subgrades and foundations. The soils exhibit different dynamic characteristics under an initial shear stress. The dynamic strength characteristics of saturated clay under cyclic loading were studied through a dynamic triaxial test of remoulded clay in the Wenchuan area. The effects of the failure criterion, initial shear stress and vibration frequency on the dynamic strength characteristics of saturated clay were also analysed. The results showed that the strain failure criterion with a strain value of 2.5 % or the transitional strain εtp can reflect the soil damage realistically and evaluate the dynamic strength of the soil objectively. εp = 2.5 % can be used to replace εp = εtp when the dynamic strength parameter of the saturated clay was calculated under seismic loading equivalent failure vibration times. The dynamic strength parameters of the saturated clay under different earthquake magnitudes were calculated by introducing the equivalent failure vibration times of the soil under seismic loading, thereby providing data support for the stability analysis of the clay foundation under seismic loading. The initial shear stress and vibration frequency have a considerable effect on the dynamic strength of saturated clay. Under the same vibration frequency, the larger the initial shear stress is, the smaller the required dynamic stress is for the soil to break, and the smaller the dynamic strength parameter is. The existence of the initial shear stress reduces the dynamic strength of the soil. Under the same vibration times, the higher the vibration frequency is, the greater the required dynamic stress is for the soil to break, the larger the dynamic strength parameter is, and the greater the dynamic strength of the soil is.
References
2Y. Feng,W. Zhang,Y.X. M,“Experimental study on stress-water content-strain relationship of remolded loess under directional shear stress path,”Journal of Qinghai University,vol.36,no.1,pp.47-53,2018.
3Z.L. Zhou,G.X. Chen,Q. Wu,“Effect of initial static shear stress on liquefaction and large deformation behaviors of saturated silt,”Yantu Lixue/rock & Soil Mechanics,vol.38,no.5,pp.1314-1320,2017.
4Z.X. Yang,K. Pan,“Flow deformation and cyclic resistance of saturated loose sand considering initial static shear effect,”Soil Dynamics & Earthquake Engineering,vol.92,pp.68-78,2017.
5Z.H. Zhang,X.C Huang,Q.T. Bi,“Effect of initial shear stress and phase difference on dynamic characteristics of saturated sand,”Yangtze River,vol.48,no.3,pp.70-74,2017.
6G. Suazo,A. Fourie,J.Doherty,“Effects of confining stress, density and initial static shear stress on the cyclic shear response of fine-grained unclassified tailings,”Geotechnique,vol.66,no.5,pp.1-12,2016.
7J. Wang,P. Luo,F.Y. Liu,“Effect of angle between directions of initial shear stress and cyclic
load on softening properties of soft clay,”Chinese Journal of Rock Mechanics and Engineering,vol.35,no.5,pp.1072-1080,2016.
8J.T. Cao,“Experimental study on dynamic behaviors of Wenchuan earthquake area saturated sand under cyclic loading,” Nanjing,Hohai University,2014.
9 T. Wichtmann , T. Triantafyllidis,“Influence of the Grain-Size Distribution Curve of Quartz Sand on the Small Strain Shear Modulus Gmax,”Journal of Geotechnical and Geoenvironmental Engineering,vol.35,no.10,pp.1404-1418,2009.
10Y. Yilmaz,M. Mollamahmutoglu,“Characterization of Liquefaction Susceptibility of Sands by Means of Extreme Void Ratios and/or Void Ratio Range,”Journal of Geotechnical and Geoenvironmental Engineering,vol.135,no.12,pp.1986-1990,2009.
11K.Yasuhara,“Post-cyclic undrained strength for cohesive soils,” Journal of Geotechnical Engineering,vol.120,no.11,pp.1961~1979,1994.
12I. Ishibashi,M. Kawamura,S.K. Bhatia,“Effect of initial shear on cyclic behavior of sand,” Journal of the Geotechnical Engineering,vol.119,no.12,pp.1395-1412,1985.
13H.B. Seed,C.K. Chan, “Clay strength under earth quake loading conditions,” Journal of Soil Mechanics and Foundations,vol.92,no.2,pp. 53-78,1966.
14T.F. Zimmie,C.Y. Lien,“Response of clay subjected to combined cyclic and initial static shear stress,”Proc 3rd Can. Con.fon Marine Geotech. Engrg,1986.
15A.M. Goulois,R.V. Whitman,K. Hoeg,“Effects of sustained shear stresses on the cyclic degradation of clay,” Strength testing of marine sediments. ASTM STP 883,R C Chaney and K R Demars,eds. ASTM. Philadelphia,1985.
16G.Lefebvre,P. Pfendler,“Strain rate and preshear effects in cyclic resistance of soft clay,” Journal of Geotechnical Engineering,vol.122,no.1,pp.21-26,1996.
17K.Tan,M. Vucetic,“Behavior of medium and low plasticity clays under cyclic simple shear conditions,”Proc 4 th Int. Con fon Soil Dyn and Earthquake Engrg. A. S. Cakmak and I. ,Herra. eds. Mexico City, Mexico,1989.
18T. Matsui,H. Ohara,T. Ito,“Cyclic stress strain history and shear characteristic of clays,” Journal of Geotechnical Engineering,vol.106,no.10,pp.1101- 1120,1980.
19J.H. Liao,M.H. Yu,T. Akira,“Dynamic shear strength of loessial soils and volcanic cohesive soils,”Journal of Xi’an Jiaotong University,vol.32,no.10,pp.70-74,1998.
20Y.M. Chen,X.M. Ji,B. Huang,“Effect of cyclic loading frequency on undrained behaviors of undisturbed marine clay,”China Ocean Engineering,vol.18,no.4,pp.634-651,2004.