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simple expression of the dynamic stiffness of grouped piles

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30SIMPLE EXPRESSIONS OF THE DYNAMIC STIFFNESS OF GROUPED PILES2.4. SUMMARYPiles <strong>grouped</strong> beneath a superstructure can be viewed as a single equivalent uprightbeam when <strong>the</strong> <strong>piles</strong> are closely spaced. The <strong>stiffness</strong> matrix presented herein (Equation(2.1)) yields close approximations <strong>of</strong> both <strong>dynamic</strong> pile-cap <strong>stiffness</strong> and kinematicdisplacement factors. This idealization <strong>of</strong> <strong>grouped</strong> <strong>piles</strong> as a single equivalent uprightbeam and <strong>the</strong> concept <strong>of</strong> <strong>the</strong> active pile length have facilitated <strong>the</strong> derivation <strong>of</strong> a <strong>simple</strong><strong>expression</strong> <strong>of</strong> pile-cap <strong>stiffness</strong> in terms <strong>of</strong> frequency-independent mass, damping and<strong>stiffness</strong> parameters (Equations (2.29a)-(2.29c)). This <strong>expression</strong> is valid irrespective <strong>of</strong>pile and soil parameters as long as <strong>the</strong> pile group exhibits a “flexible” nature with itsactive-pile-length ratio, L0 / L, kept less than 0.3. The present <strong>simple</strong> <strong>expression</strong> <strong>of</strong>pile-cap <strong>stiffness</strong> also allows <strong>the</strong> effects <strong>of</strong> overall site non-linearity to be reflected bysimply replacing <strong>the</strong> shear modulus <strong>of</strong> <strong>the</strong> intact soil, µ , with <strong>the</strong> complex modulus,µ'( 1+ iD ) , which describes equivalent-linear features <strong>of</strong> <strong>the</strong> soil experiencing <strong>the</strong>seismic motion.A similar <strong>expression</strong> must also be derived for <strong>the</strong> <strong>dynamic</strong> <strong>stiffness</strong> <strong>of</strong> <strong>grouped</strong> <strong>piles</strong> inrocking motion and for <strong>the</strong> coupled <strong>stiffness</strong> between lateral sway and rocking motions.Moreover, <strong>the</strong>re is fur<strong>the</strong>r scope to extend this study for inhomogeneous soil-pr<strong>of</strong>ile and<strong>the</strong> local non-linearity <strong>of</strong> soil that develops in <strong>the</strong> vicinity <strong>of</strong> <strong>piles</strong>. In <strong>the</strong>se extensionsalso, active pile length, if rationally estimated, would allow pile-cap <strong>stiffness</strong> to beapproximately described in a similar manner. This will be discussed in futurepublications.REFERENCESFan, K., Gazetas, G., Kanya, A., Kausel, E. and Ahmad, S. [1991] “Kinematic SeismicResponse <strong>of</strong> Single Piles and Pile Groups,” Jour., Geotechnical Engineering, ASCE,117(12), 1860-1879.Gazetas, G. and Dobry, R. [1984] “Horizontal Response <strong>of</strong> Piles in Layered Soils,” Journal <strong>of</strong>Geotechnical Engineering, ASCE, 110(1), 20-40.Kanya, A. and E. Kausel [1982] “Dynamic Stiffness and Seismic Response <strong>of</strong> Pile Groups,”NSF report, NSF/CEE-82023.Konagai, K. and Maehara, M. [1992] “Study on Hypo<strong>the</strong>ses for Simple Numerical Evaluation<strong>of</strong> Soil-Embedded Structure Interaction,” Bull., Earthquake Resistant Structure ResearchCenter, 25, 39-60.Konagai, K. and T. Nogami [1998a] “Analog circuit to simulate <strong>dynamic</strong> soil-structureinteraction in shake table test,” International Journal <strong>of</strong> Soil Dynamics and EarthquakeEngineering, 17(5), 279-287.Konagai, K., A. Mikami and T. Nogami [1998b] “Simulation <strong>of</strong> Soil-Structure InteractionEffects in Shaking Table Tests,” Geotechnical Earthquake Engineering and Soil Dynamics

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