Advanced Soil Mechanics: Liquefaction Analysis and Shear Stress
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This document discusses the procedure of liquefaction analysis in CSS, including the factors of safety and resistance. It also covers the plotting of effective stress and CSL in e-log(p') space. Additionally, it explains shear stress and provides an overview of Robertson and Wride's procedure for soil assessment.
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ADVANCED SOIL MECHANICS1 ADVANCED SOIL MECHANICS By (Firstname Lastname) Advanced Soil Mechanics Assessment 1 Professor Name of University September 5, 2019
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ADVANCED SOIL MECHANICS2 Question 1 a.Briefly explain the procedure of liquefaction analysis in CSS(Bouckovalas, Andrianopoulos and Papadimitriou, 2013) Liquefaction is caused by monotonic loading and cyclic loading, where monotonic loading occurs under sudden changes in stress, while cyclic loading would be caused by repeated change of soil. e¿=e+(1−b)fc 1−(1−b)fc The factor of safety (FS) against liquefaction which is simply the ratio of cyclic resistance to cyclic stress for a soil at depth z. Cyclic stress ratio (CSR) is given as (Cetin and Seed, 2004); CSR=0.65(amax g)(σv σv')rd .Where; amaxis the peak horizontal ground acceleration. gis the gravitational acceleration. σv'is the effective overburden stress at z. σzis the total overburden stress at z. rdis the shear stress reduction coefficient given by: rd=1−0.00765z,forz<9.2m rd=1.174−0.0267z,forz≥9.2m Cyclic resistance ratio (CRR) is obtained by the formula(Baxter, Bradshaw, Green and Wang, 2008); CRR=[0.022(0.01VS1)2+2.8(1 VS1 ¿−VS1 −1 VS1 ¿)]MSF Where;
ADVANCED SOIL MECHANICS3 VS1is the stress-correlated velocity of shear wave. VS1 ¿is the limiting upper value. MSF is magnitude scaling factor (Arango, 1996). VS1=VS(Pa σv') 0.25 VSis shear-wave velocity. Pais a reference stress. MSF=(MW 7.5) −2.56 MWis the moment magnitude of earthquake. FS=1.4∗CRR CSR F=1−FS Liquefaction Potential Index LPI¿∫F(10−0.5z)dz b.Plot the effective stress diagram Effective stressσ'=σ−u Where σ=γtzandu=γwz Effective stress at z = 0 m; σ0'=0 Effective stress at z = 2 m is; σ2 '=(20∗2)=40kN/m2 Effective stress at z = 3 m is; σ3 '=(20∗2)+(22∗1)=62kN/m2
ADVANCED SOIL MECHANICS4 Effective stress at z = 6 m is; σ6 '=(20∗2)+(22∗1)+((22−10)∗3)=98kN/m2 Effective stress at z = 13 m is; σ13 '=(20∗2)+(22∗1)+((22−10)∗3)+[(23−10)∗7]=189kN/m2 Graphing we get 0406298189 -14 -12 -10 -8 -6 -4 -2 0 Depth z (m) Effective stress kPa Depth m c.Plot the CSL ine-log(p) space At 0 m CSL=0 At 2 m eCS=0.920−0.0375(40 40) 0.6 =0.8825 At 3 m eCS=0.920−0.0375(62 62)0.6 =0.8825 At 6 m eCS=0.920−0.0375(98 98+(3∗10))0.6 =0.8904 At 13 m
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ADVANCED SOIL MECHANICS5 eCS=0.920−0.0375(189 (189+(10∗10)))0.6 =0.8910 0.0001.6021.7921.9912.276 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Axis Title Axis Title d) Definition i) state parameter (ψ) is the difference betweenthe in-situ void ratio at a given effective confining stress prior to shearing and the void ratio at the steady state line (SSL) for the same effective confining stress ii) Liquefaction potential is a stability analysis for which the shear strength in the numerator of the factor of safety equation is the undrained steady‐state strength, and the denominator is the driving shear stress. Q2) a)shearstress=τd=0.65∗(amax g)(σv σ' v)rd
ADVANCED SOIL MECHANICS6 0510152025 0 0.5 1 1.5 2 2.5 3 shear stress Linear (shear stress) depth Shear stress b)Robertson and Wride’s Procedure 1ststep In the first step the soil assumption we considered as clay and n value is taken as 1. Next step is calculating Q value and based on that Q value we can getthat Ic value. Then we get Ic value of it is greater than 2.6 We consider it as clay that is our assumption is true. At that point we have to stop our iterations and calculating the values of Q and Ic from the following equations. Q1=൬ Qc−σv0 Pa ൰∗൬ Pa σ′v0 ൰ n1 Ic=ሾሺ3.47−logQ1ሻ2−ሺ1.22+logFሻ2ሿ0.5
ADVANCED SOIL MECHANICS7 2ndstep In the second assumption we considered as sand and value is taken as 0.5. next step is calculating Ic value and if its value is less than 2.6 the n our assumption is correct and we have to stop the iterations. Then we have to find qc1N value.If the value is greater than 2.6 then the assumption is false and we have to go for the next step. 3rdstep: we have to assume soil is intermediate and take n value as 0.7 and calculateIc. b) Cq=1.8 0.8+σ'v Pa =1.8 0.8+26.4 100 =1.43 qc1=cq∗qc=1.43∗3000=4285.7kPa FC = 10% when correction due to finess is ∆qcl=(11.9+44.66 14.6)e [1.63−9.7 12−(15.7 12)2 ] = 6.143 tfs qclf=qcl+∆qcl=44.66+6.143=50.803tfs Ic=√(3.47−logQ)2+(logRf+1.22)2 Q =50.803−9.8∗2 460.66 Rf=0.009578 50.808−46=0.0019942 Ic=√(3.47−log0.66)2+(log0.0019942+1.22)2 = 3.94 c)
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ADVANCED SOIL MECHANICS9 0510152025 0.25 0.26 0.27 0.28 0.29 0.3 0.31 0.32 0.33 0.34 Ψ Linear (Ψ) depth state parameter . b) ψ0, the void ratio of DEM data is actually much smaller than the experimental data, which may result in a stiffer response
ADVANCED SOIL MECHANICS10 References Arango, I., 2016. Magnitude scaling factors for soil liquefaction evaluations.Journal of Geotechnical Engineering,122(11), pp.929-936. Baxter, C.D., Bradshaw, A.S., Green, R.A. and Wang, J.H., 2018. Correlation between cyclic resistance and shear-wave velocity for providence silts.Journal of geotechnical and geoenvironmental engineering,134(1), pp.37-46. Bouckovalas, G.D., Andrianopoulos, K.I. and Papadimitriou, A.G., 2013. A critical state interpretation for the cyclic liquefaction resistance of silty sands.Soil Dynamics and Earthquake Engineering,23(2), pp.115-125 Cetin, K.O. and Seed, R.B., 2014. Nonlinear shear mass participation factor (rd) for cyclic shear stress ratio evaluation.Soil Dynamics and Earthquake Engineering,24(2), pp.103-113. Ghaboussi, J. and Wilson, E.L., 2013. Liquefaction analysis of saturated granular soils. In5th World Conf. on Earthquake Engineering. Hwang, H.H. and Lee, C.S., 2014. Probabilistic evaluation of liquefaction potential. Kramer, S.L., 2017. Uncertainty in steady-state liquefaction evaluation procedures.Journal of Geotechnical Engineering,115(10), pp.1402-1419. Montzka, C., Moradkhani, H., Weihermüller, L., Franssen, H.J.H., Canty, M. and Vereecken, H., 2015. Hydraulic parameter estimation by remotely-sensed top soil moisture observations with the particle filter.Journal of hydrology,399(3-4), pp.410-421