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1.
考虑横向效应饱和黏弹性土层中桩的纵向振动   总被引:1,自引:0,他引:1  
杨骁  蔡雪琼 《岩土力学》2011,32(6):1857-1863
由于饱和土中土体颗粒与孔隙水的相互作用以及桩与土体的不同渗透率,饱和土体中桩基的力学行为与单相土中桩基力学行为有很大的差别。基于饱和多孔介质理论,考虑桩纵向振动时的横向变形及惯性效应,将桩等效为Rayleigh-Love杆,在频率域中研究了饱和黏弹性土层中端承桩纵向振动的动力特性,给出了饱和黏弹性土层和桩纵向振动时动力响应的解析解及桩头复刚度的解析表达式。通过数值计算,给出了桩头动刚度因子和阻尼随激励频率的响应,考察了饱和土物性参数、桩土模量比、桩长径比、泊松比等参数对桩头刚度因子和阻尼的影响。研究表明,对于大直径桩,当外载荷激励频率较大时桩横向效应对桩头刚度因子和阻尼有显著的影响  相似文献   

2.
成层饱和土中考虑横向惯性的单桩纵向振动   总被引:2,自引:0,他引:2  
杨骁  唐洁 《岩土力学》2013,34(6):1560-1566
基于饱和多孔介质理论,研究了成层饱和黏弹性土层中端承桩的纵向振动特性。首先利用Novak薄层法,得到了土层对纵向振动桩的动力阻抗。其次,将桩等效为Rayleigh-Love杆,给出了成层饱和黏弹性土中端承桩纵向振动的一般分析方法和桩头动力复刚度的解析表达式。具体分析了两层饱和黏弹性土中端承桩的纵向振动特性,得到了桩头动刚度因子和等效阻尼随频率的响应特征,讨论了物理和几何等参数对动刚度因子和等效阻尼的影响。结果表明:桩长径比、土层模量比以及桩土模量比等对桩头动刚度因子和等效阻尼有显著的影响。相比于均质土层中的桩,上层土越硬或下层为软弱土层,桩的动刚度因子和等效阻尼振动幅值增大,其周期随长径比显著变化,且对于大直径桩,动刚度因子和等效阻尼随频率呈振动变化。同时,土体与孔隙水相互作用系数和桩泊松比等的影响相对较小。其结果可作为桩基动力基础设计和动力检测等基础数据。  相似文献   

3.
饱和黏弹性地基土中管桩纵向振动研究   总被引:1,自引:0,他引:1  
应跃龙  罗海亮  闻敏杰 《岩土力学》2013,34(Z1):103-108
用解析方法在频率域内研究考虑质量耦合效应的饱和黏弹性地基土中管桩的纵向振动特性。基于Biot理论,采用薄层法,推导得到饱和黏弹性地基土的位移、应力等的表达式。将管桩等效为一维弹性杆件处理。根据界面连续性条件,给出饱和黏弹性地基土中管桩的纵向振动一般分析方法和桩顶动力复刚度的表达式。在该基础上,对比分析饱和地基土中实心桩和管桩纵向振动特性。通过算例分析,考察桩周土和桩芯土的力学参数对桩顶刚度因子和等效阻尼的影响。研究表明,饱和黏弹性地基土中实心桩和管桩的纵向振动有明显的差异。  相似文献   

4.
胡安峰  肖志荣  宋桂亭  刘洋 《岩土力学》2006,27(Z2):837-840
基于动力Winkler模型,采用与频率相关的刚度系数和阻尼系数来模拟土对桩的动反力,得到了黏弹性地基中考虑桩顶附加质量时的单桩水平动力响应解析解。研究了桩土模量比、桩体长径比以及激振频率对桩基动力响应的影响。分析表明,当考虑桩顶附加质量时,桩体位移总体上有减小的趋势;无量纲频率对桩体水平位移的影响程度要远远大于不考虑桩顶附加质量时的情况。  相似文献   

5.
秦世伟  莫泷  史蕙质 《岩土力学》2013,34(4):987-995
将地震液化场地土层分为非液化表层土、中部的液化土层和底部的基层,基于饱和多孔介质理论和Novak薄层法,研究轴向压力作用下液化黏弹性土层中端承桩的水平动力特性。利用Helmholtz分解和变量分离法,得到液化土层对桩水平振动的阻抗。利用矩阵传递法,在频率域得到轴力作用下液化土层中端承桩简谐振动的解析解和桩头复刚度的表达式,并进行参数研究,分析轴力、桩-土模量比、桩长径比、液-固耦合系数等对桩头动力刚度和阻尼的影响。结果表明,在轴力作用下,不同长径比、桩-土模量比、液-固耦合系数时的动力刚度绝对值均比无轴力作用时减小,但随频率的变化趋势相同;轴力对桩水平振动的动力阻抗影响显著,随着轴力的增加,桩的水平振动动力刚度因子的绝对值减小,若轴力继续增大,其绝对值趋近于0,桩发生失稳破坏;桩长径比和桩土模量比对桩的水平振动动力阻抗有显著的影响,而液-固耦合系数的影响较小。  相似文献   

6.
基于Biot波动理论提出了一种桩底饱和虚土桩模型,同时考虑桩周、桩底土体三维波动效应及饱和特性,建立了三维饱和黏弹性土、虚土桩和实体桩完全耦合振动定解问题。采用势函数求解得出饱和土体位移解,并利用饱和土-桩界面耦合条件,求解得出桩顶纵向振动动力阻抗解析解答。将所得解退化到已有解析解进行对比验证,并在此基础上对浮承桩纵向振动特性进行参数化分析,计算结果表明:桩底饱和土层厚度越大,桩顶动刚度和动阻尼曲线振幅及共振频率越小,且当桩底饱和土层厚度增大到一定程度后,振幅呈现大、小峰值交替现象;桩周饱和土体孔隙率仅对桩顶动力阻抗曲线振幅产生明显影响,而桩底饱和土体孔隙率对桩顶动力阻抗曲线共振幅值和共振频率均影响显著;随桩周、桩底饱和土体剪切模量的增加,桩顶动力阻抗曲线共振幅值水平均明显降低,且受桩周饱和土体剪切模量影响更为突出。  相似文献   

7.
黏弹性地基中PCC桩扭转振动响应解析方法研究   总被引:2,自引:0,他引:2  
考虑土体材料的黏性阻尼和桩-土扭转耦合振动,把桩看作一维杆,将土体视作三维轴对称黏弹性介质,对黏弹性地基中现浇混凝土大直径管桩(简称PCC桩)扭转振动频域特性进行了理论研究,采用Laplace变换和分离变量的方法求得了桩顶扭转频域响应解析解。将所得解完全退化到实心桩的解,并与经典平面应变解进行对比,验证了解析解的合理性。分析了桩长以及土体黏性阻尼系数对桩顶速度导纳和复动刚度的影响,得到了各参数对桩扭转振动特性影响的规律。分析表明:桩周土黏性阻尼系数增大可以显著提高桩顶扭转复动刚度和减小速度导纳振荡幅值,而桩芯土黏性阻尼系数的影响不明显;桩长越长,桩顶复动刚度越大,速度导纳振荡幅值越小,但当桩长增大到一定程度时,再继续增加桩长,桩顶复动刚度基本没有改变。  相似文献   

8.
丁选明  刘汉龙 《岩土力学》2008,29(12):3353-3359
考虑土体材料的黏性阻尼和桩-土纵向耦合振动,建立了轴对称均匀黏弹性地基中现浇薄壁管桩管桩纵向振动的定解问题,采用Laplace变换的方法求得了解析解。对一算例进行了分析,将计算结果与实测波形和有限元进行了对比,三者吻合较好。进一步分析了桩周土和桩芯土黏性阻尼系数对桩顶速度导纳和复动刚度的影响以及桩底土阻尼系数对桩顶速度导纳的影响,得到了各参数对桩纵向振动特性影响的规律  相似文献   

9.
杨冬英  丁海平 《岩土力学》2014,35(Z1):311-318
根据桩端土应力扩散的规律,建立了桩端扩散虚土桩模型。基于该模型对非均质土中桩-土纵向耦合振动进行研究。利用复刚度传递多圈层平面应变模型,得到桩与虚土桩桩侧土的剪切复刚度。结合边界条件、初始条件和连续条件,对扩散虚土桩和实体桩动力方程从底层往顶层逐层进行求解,得到桩顶动力响应的频域解析解和时域半解析解。通过对桩端扩散虚土桩扩散角、扩散层厚度、桩侧土非均质性和桩长的影响进行计算分析,得到基于扩散虚土桩法桩-土纵向振动响应特性。研究结论可为桩基础动力设计和动态检测提供理论依据。  相似文献   

10.
沈纪苹  陈蕾 《岩土力学》2016,37(10):2810-2816
在考虑土体分层特性的基础上,分别建立了管桩桩周土体和桩芯土体的水平振动控制方程。通过引入势函数并考虑桩周土和桩芯土径向位移和环向位移的边界条件及其奇偶性,求得了管桩-土动力相互作用的刚度系数和阻尼系数。将土体模拟为连续分布的弹簧-阻尼器,并考虑桩芯土和桩周土的作用,建立了层状土中管桩的水平振动方程。借助初参数法和传递矩阵法求解了管桩的水平振动,得到了管桩桩顶的水平动力阻抗。通过数值分析,得到了土层剪切模量、管桩壁厚、桩周土和桩芯土剪切模量比、土层厚度等对管桩桩顶动力阻抗的影响规律。土层剪切模量、管桩壁厚、桩周土和桩芯土剪切模量比对层状土中管桩水平振动的影响主要在低频处,土层厚度在较宽的频率范围内对管桩水平振动有影响;管桩壁越厚,桩周土的剪切模量越大时,管桩水平动力阻抗的绝对值越大。  相似文献   

11.
被动桩中土拱效应问题的数值分析   总被引:47,自引:6,他引:41  
被动桩对侧向位移的土层起到遮拦作用的机理主要是土拱效应。采用有限元软件Plaxis 8.1,详细地研究了被动桩中土拱效应的产生机理,分析了导致侧向位移的荷载大小、土体性质、群桩以及桩土接触面性质等影响因素对土拱效应性态和桩土应力分担比的影响,分析表明,桩间距是影响土拱效应的最主要因素。  相似文献   

12.
The pile-to-pile interaction was obtained for vertically loaded piles embedded in homogeneous poroelastic saturated soil. Deduced from Biot’s theory, the fundamental functions of the quasi-static development for the force, displacement and pore pressure were acquired in cylindrical coordinates. The pile–soil system was decomposed into extended soil and fictitious piles, and the compatibility condition was set up between the axial strain of the fictitious piles and the corresponding average strain over the extended soil. This approach results in the governing equations, which consist of the Fredholm integral equations of the second kind and the basic unknowns of the axial forces along the fictitious pile shaft. The axial force and settlement along the pile shaft were calculated based on the axial forces of the fictitious piles. The interaction between the piles was investigated under different consolidation conditions through a two-pile model, and two pile interaction factors were obtained. Stemming from the two-pile analysis, numerical analyses on the settlement of the pile groups were conducted to probe pile interaction with consolidation. The conventional solutions for the single-phase soil-pile problem seem to underestimate the interaction factor if the consolidation effect is taken into account as pile settlement continues. The pile-to-pile interaction can also aggravate the percentage of consolidation settlement (PCS), and as the pile number increases, the value of the PCS will also increase. Several key factors, such as the pile stiffness, pile slenderness ratio and pile spacing, are investigated to better understand the impact of consolidation on pile analysis.  相似文献   

13.
This paper presents an analytical solution for determining the dynamic characteristics of axially loaded piles embedded in elastic-poroelastic layered soil of finite thickness. The interface between the elastic and poroelastic soil coincides with the groundwater table level, which is explicitly taken into account in the solution. The pile is modelled as elastic one-dimensional rod to account for the effect of its dynamic characteristics on the response of the soil-pile system. The solution is based on Biot's poroelastodynamic theory and the classical elastodynamic theory, which we use to establish the governing equations of the soil and pile. Accordingly, the pile base resistance, shaft reaction, and the complex impedance of soil-pile system are obtained using the method of Hankel integral transformation. Following the validation of the derived solution, we identify the main parameters affecting the vertical dynamic impedance of the pile via a parametric study. The presented method poses as an efficient alternative for quickly estimating the dynamic characteristics of axially loaded piles, without having to resort to complex numerical analyses.  相似文献   

14.

Physical-scaled model testing under 1 g conditions is carried out in obtaining the vertical response of fixed head floating-inclined single piles embedded in dry sand. Practical pile inclinations of 5° and 10° besides a vertical pile (0°) subjected to static and dynamic vertical pile head loadings are considered. To account for the effects of soil nonlinearity as well as the soil–pile interface nonlinearity on the response of piles, a range of low-to-high magnitude of pile head displacements is considered for the static case while a varying amplitude of harmonic accelerations for a wide range of frequencies is considered for the dynamic case. Experimental results are obtained in the form of pile head stiffnesses and strains generated in the pile under both the static and dynamic loadings. Results suggest that the nonlinear behavior of soil as well as the nonlinearity generated at the interface between the soil and the pile as the result of applied loading considerably affect the response of piles. The soil–pile interface nonlinearity that governs the slippage of pile shows a clear influence on the pile head stiffnesses by providing two distinct values of stiffnesses corresponding to the push and the pull directional movement of piles; the two values are significantly different. Axial and bending strains generated in the piles show expected dependency on the amplitude of applied loading; the pile head-level bending strain increases almost linearly with the increase in the angle of pile inclination.

  相似文献   

15.
基于虚土桩模型,分析了层状地基中桩端土性对单桩沉降特性的影响。首先,以虚土桩扩散角反映桩端土层应力扩散效应,将桩端一定锥角范围内由桩端至基岩面的土体视为虚土桩,并根据其变截面特性,将虚土桩沿纵向划分为有限个微元段。然后,对桩及虚土桩桩侧土体采用理想弹塑性荷载传递模型,利用荷载传递法,推导了层状地基中以桩侧土塑性发展深度为变量的单桩荷载-沉降递推计算方法,并进一步得到了桩身轴力及桩侧摩阻力递推计算式。在此基础上,给出了荷载传递模型参数选取方法,并分析了虚土桩临界深度的影响因素及由实测荷载-沉降曲线反演虚土桩扩散角的可行性。最后,利用该方法分析了桩端沉渣和软弱下卧层对荷载-沉降曲线的影响。结果表明,考虑桩端土层应力扩散效应时,通过计算得到的桩顶及桩端荷载-沉降曲线与实测曲线吻合较好;当桩端存在沉渣或软弱下卧层时,采用虚土桩模型的单桩沉降计算方法可以在一定程度上反映沉渣特性及软弱下卧层埋深等因素对桩顶荷载-沉降曲线的影响。  相似文献   

16.
马蒙  刘建磊  孙宁  柯在田  李林杰 《岩土力学》2015,36(7):1939-1944
动刚度是桩基动测分析中一个重要指标,研究动刚度的影响因素有着现实的工程意义。为了分析完整桩和缺陷桩单桩动刚度的变化规律和影响因素,推导并求解了竖向简谐荷载作用下考虑两个变截面桩的导纳响应解析解。利用测试数据验证了该模型能有效计算导纳共振频率值和动刚度值。同时,对513根相同型式桥桩进行机械阻抗法测试,并对其动刚度进行统计分析。研究表明:(1)桩端支撑刚度和桩长对动刚度影响较大,端承桩动刚度随桩长增加而降低,纯摩擦桩情况与之相反。摩擦桩在桩长较长时其动刚度可能大于端承桩。(2)桩身缺陷体积改变量与动刚度变化成正相关。(3)动刚度对桩身缩颈缺陷敏感度较高,在一定程度上可以用于判断桩身完整性和承载能力。  相似文献   

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