Abstract
The coefficient of earth pressure at rest K 0 of fine-grained soils is often being estimated empirically from the overconsolidation ratio (OCR). The relationships adopted in this estimation, however, assume that K 0 is caused by pure mechanical unloading and do not consider that a significant proportion of the apparent preconsolidation pressure may be caused by the effects of ageing, in particular by secondary compression. In this work, K 0 of Brno Tegel, which is a clay of stiff to hard consistency (apparent vertical preconsolidation pressure of 1800 kPa, apparent OCR of 7), was estimated based on back-analysis of convergence measurements from unsupported cylindrical cavity. The values were subsequently verified by analysing a supported exploratory adit and a two-lane road tunnel. As the simulation results are primarily influenced by soil anisotropy, it was quantified in an experimental programme. The ratio of shear moduli \(\alpha _G\) was 1.45, the ratio of horizontal and vertical Young's moduli \(\alpha _E\) was 1.67, and the value of Poisson ratio \(\nu _{tp}\) was close to 0. The soil was described using a hypoplastic model considering very small strain stiffness anisotropy. For the given soil, the OCR-based estimation yielded \(K_0=1.3\), while Jáky formula estimated \(K_0=0.63\) for the state of normal consolidation. The back-analysed value of K 0 was 0.75. The predicted tunnel displacements agreed well with the monitoring data, giving additional confidence into the selected modelling approach. It was concluded that OCR-based equations should not be used automatically for K 0 estimation. K 0 of many clays may actually be lower than often assumed.
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Notes
Their distance in the portal area is 10 m, and their axes are diverging, but most of their lengths run parallel at an average distance of 70 m.
\(\alpha _G=1.35\) was a preliminary experimental estimate of \(\alpha _G\), more detailed experimental study has later indicated \(\alpha _G=1.45\).
References
Bača J, Dohnálek V (2009) Královo Pole tunnels—experience obtained during the construction to date. Tunel 18(3):27–32
Bjerrum L, Andersen K (1972) In-situ measurement of lateral pressures in clay. In: Proceedings of the 5th European conference on soil mechanics and geotechnical engineering, Madrid, vol 1, pp 12–20
Boháč J, Mašín D, Malát R, Novák V, Rott J (2013) Methods of determination of \(K_0\) in overconsolidated clay. In: Delage P, Desrues J, Frank R, Puech A, Schlosser F (eds) Proceedings of the 18th international conference on soil mechanics and geotechnical engineering, vol 1, pp 203–206
Borja RI (1990) Analysis of incremental excavation based on critical state theory. J Geotech Eng ASCE 116(6):964–985
Burland JB, Maswoswe J (1982) Discussion on In situ measurements of horizontal stress in overconsolidated clay using push-in spade-shaped pressure cells. Géotechnique 32(2):285–286
Doležalová M (2002) Approaches to numerical modelling of ground movements due to shallow tunnelling. In: Proceedings of the 2nd international conference on soil structure interaction in urban civil engineering, ETH Zürich, pp 365–376
Doran I, Sivakumar V, Graham J, Johnson A (2000) Estimation of in situ stresses using anisotropic elasticity and suction measurements. Géotechnique 50(2):189–196
Franzius JN, Potts DM, Addenbrooke TI, Burland JB (2005) The influence of building weight on tunnelling-induced ground and building deformation. Soils Found 44(1):25–38
Gudehus G (1996) A comprehensive constitutive equation for granular materials. Soils Found 36(1):1–12
Gudehus G, Mašín D (2009) Graphical representation of constitutive equations. Géotechnique 59(2):147–151
Hamouche K, Leroueil S, Roy M, Lutenegger AJ (1995) In situ evaluation of k0 in eastern canada clays. Can Geotech J 32(4):677–688
Horák V (2009) Královo Pole tunnel in Brno from designer point of view. Tunel 18(1):67–72
Jáky J (1944) The coefficient of earth pressure at rest (in Hungarian). J Soc Hung Archit Eng 78:355–357
Kavazanjian E, Mitchell JK (1984) Time dependence of lateral earth pressure. J Geotech Eng ASCE 110(4):530–533
Lefebvre G, Bozozuk M, Philibert A, Hornych P (1991) Evaluating k0 in champlain clays with hydraulic fracture tests. Can Geotech J 28(3):365–377
Marchetti S (1980) In situ tests by flat dilatometer. J Geotech Eng Div ASCE 106(NoGT3):299–321
Mašín D (2005) A hypoplastic constitutive model for clays. Int J Numer Anal Methods Geomech 29(4):311–336
Mašín D (2012) Asymptotic behaviour of granular materials. Granul Matter 14(6):759–774
Mašín D (2012) Hypoplastic Cam-clay model. Géotechnique 62(6):549–553
Mašín D (2013) Clay hypoplasticity with explicitly defined asymptotic states. Acta Geotech 8(5):481–496
Mašín D (2014) Clay hypoplasticity model including stiffness anisotropy. Géotechnique 64(3):232–238
Mašín D, Rott J (2014) Small strain stiffness anisotropy of natural sedimentary clays: review and a model. Acta Geotech 9(2):299–312
Mayne PW, Kulhawy FH (1982) \({K}_0\)-OCR relationships in soil. Proc ASCE J Geotech Eng Div 108:851–872
Mesri G, Castro A (1987) \(C_\alpha \)/\(C_c\) concept and \(K_0\) during secondary compression. J Geotech Eng ASCE 113(3):230–247
Mesri G, Hayatt TM (1993) The coefficient of earth pressure at rest. Can Geotech J 30:647–666
Niemunis A, Herle I (1997) Hypoplastic model for cohesionless soils with elastic strain range. Mech Cohes Frict Mater 2(4):279–299
Pavlík J, Klímek L, Rupp D (2004) Geotechnical exploration for the Dobrovského tunnel, the most significant structure on the large city ring road in Brno. Tunel 13(2):2–12
Potts DM, Zdravkovic L (1999) Finite element analysis in geotechnical engineering. Volume I: Theory. Thomas Telford, London
Rott J (2014) Homogenisation and modification of composite steel-concrete lining, with the modulus of elasticity of sprayed concrete growing with time. Tunel (www.ita-aites.cz/en/casopis) 23(3):53–60
Schmertmann JH (1983) A simple question about consolidation. J Geotech Eng ASCE 109(1):119–122
Skempton AW (1961) Horizontal stresses in an over-consolidated eocene clay. In: Proceedings of the 5th international conference on soil mechanics and foundation engineering, vol 1, pp 351–357
Svoboda T, Mašín D, Boháč J (2009) Hypoplastic and mohr-coulomb models in simulations of a tunnel in clay. Tunel 18(4):59–68
Svoboda T, Mašín D, Boháč J (2010) Class a predictions of a NATM tunnel in stiff clay. Comput Geotech 37(6):817–825
Svoboda T, Mašín D (2011) Comparison of displacement fields predicted by 2D and 3D finite element modelling of shallow NATM tunnels in clays. Geotechnik 34(2):115–126
Tedd P, Charles JA (1981) In situ measurements of horizontal stress in overconsolidated clay using push-in spade-shaped pressure cells. Géotechnique 31(4):554–558
Wroth C, Hughes J (1973) An instrument for the in-situ measurements of the properties of soft clays. In: Proceedings of the 8th international conference on soil mechanics and foundation engineering, Moscow, vol 1, pp 487–494
Zemánek I, Lossmann J, Socha K (2003) Impact of exploration galleries for the Dobrovského tunnel on surface development in Brno; application of the observation method. Tunel 12(3):33–37
Acknowledgments
Financial support by the research grants 15-05935S, 14-32105S and P105/12/1705 of the Czech Science Foundation and by the research grant No. GAUK 243-253370 of the Charles University Grant Agency is greatly appreciated.
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Rott, J., Mašín, D., Boháč, J. et al. Evaluation of K 0 in stiff clay by back-analysis of convergence measurements from unsupported cylindrical cavity. Acta Geotech. 10, 719–733 (2015). https://doi.org/10.1007/s11440-015-0395-7
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DOI: https://doi.org/10.1007/s11440-015-0395-7