Vertical dynamic response of a pile embedded in a poroelastic soil layer overlying rigid base

2020 ◽  
Author(s):  
Changjie Zheng ◽  
Shishun Gan ◽  
Lubao Luan ◽  
Xuanming Ding
2015 ◽  
Vol 77 ◽  
pp. 348-359 ◽  
Author(s):  
Zonghao Yuan ◽  
Changjie Xu ◽  
Yuanqiang Cai ◽  
Zhigang Cao

2004 ◽  
Vol 27 (5) ◽  
pp. 11850
Author(s):  
L David Suits ◽  
TC Sheahan ◽  
A Mandal ◽  
DK Baidya

2013 ◽  
Vol 2013 ◽  
pp. 1-13 ◽  
Author(s):  
Changjie Zheng ◽  
Hanlong Liu ◽  
Xuanming Ding ◽  
Qiang Fu

An analytical solution is developed in this paper to investigate the horizontal dynamic response of a large-diameter pipe pile in viscoelastic soil layer. Potential functions are applied to decouple the governing equations of the outer and inner soil. The analytical solutions of the outer and inner soil are obtained by the method of separation of variables. The horizontal dynamic response and complex dynamic stiffnesses of the pipe pile are then obtained based on the continuity conditions between the pile and the outer and inner soil. To verify the validity of the solution, the derived solution in this study is compared with an existing solution for a solid pile. Numerical examples are presented to analyze the vibration characteristics of the pile and illustrate the effects of major parameters on the stiffness and damping properties.


2021 ◽  
Vol 2 (2) ◽  
Author(s):  
Kan Han ◽  
Chunxiao Xue

In order to reduce the damage of liquefaction of aeolian sand along the Sichuan-Tibet railway, the dynamic response characteristics of saturated aeolian sand in the study area were discussed by using shaking table test. The results show that the macroscopic characteristics of saturated aeolian sand in the study area are subsidence, water flow and fracture. The displacement time history shows that the surface displacement increases with increasing the input ground motion acceleration. When the acceleration is small (0.1g), the vibration in the soil layer has an obvious tendency to enlarge continuously from bottom to top. With the increase of the acceleration (0.2g), the amplification trend basically disappeared. When the acceleration increases to 0.3g, the ground motion increases first and then decreases.


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