Abstract:A substructuring method has been implemented for the seismic analysis of bridge piers founded on vertical piles and pile groups in multi-layered soil. The method reproduces semi-analytically both the kinematic and inertial soil-structure interaction, in a simple realistic way. Vertical S-wave propagation and the pile-to-pile interplay are treated with sufficient rigor, within the realm of equivalent-linear soil behaviour, while a variety of support conditions of the bridge deck on the pier can be studied with … Show more
“…The method of analysis (Mylonakis et al, 1997) is schematically illustrated in Fig 5. As previously mentioned, the mass of the superstructure is concentrated at the top of the pier, and the pier is modeled as a beam. The soilcaisson interaction is reproduced through the dynamic impedances computed in the previous subsection.…”
An analytical method to study the seismic response of a bridge pier supported on a rigid caisson foundation embedded in a deep soil stratum underlain by a homogeneous half space is developed. The method reproduces the kinematic and inertial responses, using translational and rotational distributed Winkler springs and dashpots to simulate the soil-caisson interaction. Closed-form solutions are given in the frequency domain for vertical harmonic S-wave excitation. Comparison with results from fi nite element (FE) analysis and other available solutions demonstrates the reliability of the model. Results from parametric studies are given for the kinematic and inertial responses. The modifi cation of the fundamental period and damping ratio of the bridge due to soil-structure interaction is graphically illustrated.
“…The method of analysis (Mylonakis et al, 1997) is schematically illustrated in Fig 5. As previously mentioned, the mass of the superstructure is concentrated at the top of the pier, and the pier is modeled as a beam. The soilcaisson interaction is reproduced through the dynamic impedances computed in the previous subsection.…”
An analytical method to study the seismic response of a bridge pier supported on a rigid caisson foundation embedded in a deep soil stratum underlain by a homogeneous half space is developed. The method reproduces the kinematic and inertial responses, using translational and rotational distributed Winkler springs and dashpots to simulate the soil-caisson interaction. Closed-form solutions are given in the frequency domain for vertical harmonic S-wave excitation. Comparison with results from fi nite element (FE) analysis and other available solutions demonstrates the reliability of the model. Results from parametric studies are given for the kinematic and inertial responses. The modifi cation of the fundamental period and damping ratio of the bridge due to soil-structure interaction is graphically illustrated.
“…Notwithstanding the sharp soil stiffness contrast at the level of the clay-sand interface (z = 6 m), the peak bending moment occurs close to the pilehead. This should be attributed to inertial loading transmitted directly to the single pile foundation as a shear force and bending moment during superstructure oscillations (Mylonakis et al 1997;Wilson 1998). Note also that the depth where the maximum bending moment occurs increases with increasing peak base acceleration.…”
Section: Typical Sets Of Recorded and Computed Responsementioning
Seismic soil-pile interaction is evaluated in this study based on back-calculated p-y loops constructed from sampled data of pile bending moments. Fundamental properties of p-y loops are implemented to derive distributed springs and dashpots, thereby quantifying soil-pile interaction in the realm of a Beam on Dynamic Winkler Foundation modeling. The procedure is validated by means of well-documented centrifuge tests of a single pile supported structure founded on a two-layer soil profile that comprises of soft clay overlying dense sand. Two shaking levels of a real earthquake motion applied at the base of the soil profile were examined and the generated seismic p-y loops were compared to cyclic p-y curves commonly used in pile design practice. The results demonstrate the strong influence of intensity of the input motion on seismic p-y loops while cyclic p-y curves established for soft clays tend to overestimate soil stiffness under strong excitation. Typical sets of recorded and computed structural response are presented, denoting the ability of the BDWF model related to p-y loops in reproducing adequately fundamental aspects of seismic soil-pile interaction.
“…In principle, kinematic interaction accounts for the scattering of the incoming waves by the foundation as the result of its inability to conform to the displacement profile imposed by the vibration of the soil. In such a case, the displacement of the pile head (or the cap of the pile group) U 11 冒0脼 is related to that of the free-field surface U ff 冒0脼 through the kinematic interaction factor C, which is a measure of the effect of the foundation presence on dynamic soil response [15]:…”
Section: Asynchronous Excitation and Kinematic Interaction Analysismentioning
confidence: 99%
“…) is close to zero [14], hence naturally, the potential effect of rotational excitation is negligible [15]. Recent has revealed cases [14] where the rotation of the pile group, might have a considerable effect on the seismic demand of the superstructure, particularly in cases of inhomogeneous soil formations.…”
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