Abstract:Summary
This paper presents results of one‐g shake‐table tests on scoured pile‐group‐supported bridge models in saturated (liquefiable) and dry (nonliquefiable) sands. The primary objective is to reveal the influence of liquefaction on seismic demands and failure mechanism of scoured bridges. To this end, two identical models, each consisting of a 2 × 2 reinforced concrete pile‐group with a center‐to‐center spacing of 3 times pile diameter, a cap and a single pier with a lumped iron block, were constructed and… Show more
“…Large‐scale shaking table tests were conducted on a reinforced concrete (RC) bridge pier model supported by pile group in a liquefiable ground to examine the soil–pile group–superstructure interaction via comparing the acceleration of the ground, the pier, and the pile as well as the bending moment along the pile 9 . Shaking table tests were performed on a scoured RC bridge pier model in liquefiable and nonliquefiable soils respectively to demonstrate the difference in ground response, system dynamic characteristics, and curvature distribution of the pile 10 …”
Section: Introductionmentioning
confidence: 99%
“…9 Shaking table tests were performed on a scoured RC bridge pier model in liquefiable and nonliquefiable soils respectively to demonstrate the difference in ground response, system dynamic characteristics, and curvature distribution of the pile. 10 The soil container is important for geotechnical physical model tests, including tests on the pile foundation because it should be able to reasonably simulate the characteristics of the ground. To this end, the laminar shear box was used in many of the mentioned shaking table tests.…”
To investigate the seismic response of a pile group during liquefaction, shaking table tests on a 1/25 scale model of a 2 × 2 pile group were conducted, which were pilot tests of a test project of a scale-model offshore wind turbine with jacket foundation. A large laminar shear box was utilized as the soil container to prepare a liquefiable sandy ground specimen. The pile group model comprising four slender aluminum piles with their pile heads connected by a rigid frame was designed with similitude considerations focusing on soil-pile interaction. The input motions were 2-Hz sinusoids with various acceleration amplitudes. The excess pore water pressure generation indicated that the upper half of the ground specimen reached initial liquefaction under the 50-gal-amplitude excitation, whereas in the 75-gal-amplitude test, almost entire ground was liquefied. Accelerations in soil, on the movable frames composing the laminar boundary of the shear box, and along the pile showed limited difference at the same elevation before liquefaction. After liquefaction, the soil and the movable-frame accelerations that represented the ground response considerably reduced, whereas both the movable frames and the piles exhibited high-frequency jitters other than 2-Hz sinusoid, and meantime, remarkable phase difference between the responses of the pile group and the ground was observed, all probably due to the substantial degradation of liquefied soil. Axial strains along the pile implied its double-curvature bending behavior, and the accordingly calculated moment declined significantly after liquefaction. These observations demonstrated the interaction between soil and piles during liquefaction.
“…Large‐scale shaking table tests were conducted on a reinforced concrete (RC) bridge pier model supported by pile group in a liquefiable ground to examine the soil–pile group–superstructure interaction via comparing the acceleration of the ground, the pier, and the pile as well as the bending moment along the pile 9 . Shaking table tests were performed on a scoured RC bridge pier model in liquefiable and nonliquefiable soils respectively to demonstrate the difference in ground response, system dynamic characteristics, and curvature distribution of the pile 10 …”
Section: Introductionmentioning
confidence: 99%
“…9 Shaking table tests were performed on a scoured RC bridge pier model in liquefiable and nonliquefiable soils respectively to demonstrate the difference in ground response, system dynamic characteristics, and curvature distribution of the pile. 10 The soil container is important for geotechnical physical model tests, including tests on the pile foundation because it should be able to reasonably simulate the characteristics of the ground. To this end, the laminar shear box was used in many of the mentioned shaking table tests.…”
To investigate the seismic response of a pile group during liquefaction, shaking table tests on a 1/25 scale model of a 2 × 2 pile group were conducted, which were pilot tests of a test project of a scale-model offshore wind turbine with jacket foundation. A large laminar shear box was utilized as the soil container to prepare a liquefiable sandy ground specimen. The pile group model comprising four slender aluminum piles with their pile heads connected by a rigid frame was designed with similitude considerations focusing on soil-pile interaction. The input motions were 2-Hz sinusoids with various acceleration amplitudes. The excess pore water pressure generation indicated that the upper half of the ground specimen reached initial liquefaction under the 50-gal-amplitude excitation, whereas in the 75-gal-amplitude test, almost entire ground was liquefied. Accelerations in soil, on the movable frames composing the laminar boundary of the shear box, and along the pile showed limited difference at the same elevation before liquefaction. After liquefaction, the soil and the movable-frame accelerations that represented the ground response considerably reduced, whereas both the movable frames and the piles exhibited high-frequency jitters other than 2-Hz sinusoid, and meantime, remarkable phase difference between the responses of the pile group and the ground was observed, all probably due to the substantial degradation of liquefied soil. Axial strains along the pile implied its double-curvature bending behavior, and the accordingly calculated moment declined significantly after liquefaction. These observations demonstrated the interaction between soil and piles during liquefaction.
“…In the past, many tests have studied the SSI effects and seismic behavior of pile-supported piers with a concentrated oscillation mass or even neglecting an oscillation mass in different soils (Makris et al 1997, Yao et al 2004, Rollins et al 2005, Tokimatsu et al 2005, Cubrinovski et al 2006, Dungca et al 2006, Chau et al 2009, Motamed and Towhata 2010, Gao et al 2011, Haeri et al 2012, Chang and Hutchinson 2013, Motamed et al 2013, Goit and Saitoh 2014, Durante et al 2015, Wang et al 2015, Durante et al 2016, Su et al 2016, Durante et al 2017, Liu et al 2017, Wang et al 2019). The research work validated experimentally the Winkler foundation model using the displacement transfer function and strain spectrum of a SDOF superstructure supported by a single pile (Makris et al 1997).…”
Section: Introductionmentioning
confidence: 99%
“…Liu et al (2017) presented test results of a 2×2 pile-group behind a quay wall that evident pile group effects were observed by comparing the bending moment between piles. Wang et al (2019) investigated the inertial and kinematic effects on the curvature of the pile using shaking table tests on pile-soil-pier models in liquefiable and dry sand. Results indicated the near pile in liquefiable sand behaving more significant dilation tendency compared to the far-field.…”
This research is to assess the influences of the inertial mass from the girder on the dynamic characteristic, dynamic response, and structure-soil interaction of a pile-soil-pier subsystem in a scale-model of a cable-stayed bridge. Therefore, both connection configurations between the pile-soil-pier and girder, including the sliding and fixed connections, were designed to present various inertial mass from the superstructure delivered to the pile-soilpier. The pile-soil-pier supported by a 3×3 pile-group in mixed soil placed in a shear box was tested using shaking tables. The dynamic characteristics, seismic responses, inertial interactions, and pile group effects of the pile-soilpier between the sliding and fixed connections were analyzed under three input motions with different shaking amplitudes. These results showed that more inertial mass from the girder significantly increased the reinforcement strain and bending moment at the column bottom and pile top, displacement at the column top, inertial interaction effects, and pile group effects of the pile-soil-pier due to the sliding connection changing to the fixed connection.The inertial mass increment from the girder noticeably decreased the peak accelerations of the column of the pilesoil-pier when subjected to three input motions with different amplitudes. However, the inertial mass insignificantly affected the accelerations of the pile and free-soil. Therefore, the corresponding kinematic interaction effects were almost unaffected by the inertial mass. Additionally, the evident pile group effects were observed in the sliding and 2 fixed connections between the pile-soil-pier and girder. The numerical model could approximately reproduce the macroscopic seismic responses of the pile-soil-piers with sliding and fixed connections and capture the typical response variations induced by the connection configuration change.
“…Compared with the land environment [2], coastal and offshore bridge foundations can obstruct current flow in the offshore environment [3], which can induce a downward flow and create complex vortexes [4] and finally result in local scour of sediments around the foundations [5]. Local scour reduces not only the embedded depth, but also the stability and vibration frequency of bridge foundations, and hence affects the safety of structures [6][7][8].…”
Local scour around caissons under currents has become one of the main factors affecting the safety of foundation construction and operation in coastal and offshore bridge engineering. Local scour occurs not only in the operation stage, when the caisson has settled into the sediment, but also in the construction stage, when the caisson is suspended in water. In this study, the local scour induced by unidirectional and tidal currents around settled caissons with different cross-sections (circular, square, and diamond) was experimentally investigated. Circular and square caissons were selected to investigate the difference in local scour of suspended caissons under unidirectional and tidal currents. The main findings from the experimental results were: (1) the temporal development of scour under tidal current was slower than that of unidirectional current; (2) the effect of current type can significantly influence the size and location of maximum scour depth around circular and square caissons; (3) the appropriate choice of cross-section could reduce the maximum scour depth around the settled caisson; (4) the maximum scour depth of tidal current was smaller than that of unidirectional current when the caisson was settled into the sediment, while the opposite effect occurred when the caisson was suspended in water.
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