共查询到19条相似文献，搜索用时 125 毫秒
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基于广义Biot动力理论和Longuet-Higgins线性叠加模型,构建波浪-海床-管线动态响应的有限元计算模型,求解随机波作用下,多层砂质海床中管线周围土体孔隙水压力和竖向有效应力的分布。采用基于超静孔隙水压力的液化判断准则,得出液化区的最大深度及横向范围,从而判断海床土体液化情况。考虑海洋波浪的随机性,将海床视为多孔介质,海床动态响应计算模型采用u-p模式,孔隙水压力和位移视为场变量。并考虑孔隙水的可压缩性、海床弹性变形、土体速度、土体加速度以及流体速度的影响,忽略孔隙流体惯性作用。参数研究表明:土体渗透系数、饱和度以及有效波高等参数对海床土体孔隙水压力、竖向有效应力和液化区域分布有显著影响。 相似文献
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《中国海洋大学学报(自然科学版)》2017,(10)
本文以黄河三角洲粉质土为研究对象,开展了波致海床剪切破坏过程中孔压响应与土体强度变化的室内水槽试验研究,试验过程中,先后在模拟海床床上施加5、10、15cm波高的模拟波浪荷载,同步测量海床内不同深度处的孔压变化,并对海床进行贯入阻力测试和不排水抗剪强度测试。研究发现:海床中孔压响应过程的规律为孔压快速累积-孔压缓慢消散,在该过程中海床内最容易形成大幅度的孔压累积、孔压响应最强烈的位置,也是海床内土体强度的逐渐丧失以及土体剪切破坏是处开始发育的深度;波浪作用下粉质海床剪切破坏后会在海床内部一定深度处出现明显的弧形破坏界面,破坏土体沿界面随波浪作振荡运动,且破坏范围经历先扩展后回缩的过程,剪切破坏界面以下会有强度硬层的发育,强度硬层的形成与演化直接受剪切破坏过程控制,最终整个海床出现明显的强度非均质化;在孔压响应过程中孔压比即超孔压与上覆有效应力比值存在临界值K(本文水槽试验所得K=0.5),当超过K值时,土体贯入阻力和不排水抗剪强度降低,发生剪切破坏,这是波浪作用提供的剪切力以及超孔压累积导致海床内部抗剪强度降低共同作用的结果。 相似文献
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《海洋地质与第四纪地质》2014,(5)
黄河三角洲海床沉积物质为粉质土,在大的风暴浪作用下海底浅表粉质土能够发生液化,形成塌陷凹坑。以黄河三角洲粉质土铺设底床,进行液化粉质土形成塌陷的波浪水槽试验,在底床粉粒和砂粒不随水流脱离液化区的前提下,对形成塌陷量的贡献因素进行了分析。根据试验数据,估算了黏粒迁移析出与液化区底床密度增大对液化致塌陷凹坑的贡献度,得出黏粒迁移析出贡献一般大于55%。试验还发现在波浪作用下粉质土液化后黏粒发生迁移,原均质底床黏粒含量在垂向上出现2个分段特点的重新分布,分段点处于水土界面、底床液化最终界面和最大液化界面上,每段以上少下多分布。 相似文献
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《中国海洋大学学报(自然科学版)》2021,(10)
椭圆余弦波是一种常见的浅水非线性波,对近岸区海床的稳定性有重要影响。本文根据有限体积法原理,基于开源流体力学计算平台OpenFOAM,利用C++语言编制了波致无粘性土海床响应的数值计算程序,联合波浪数值模拟软件,对椭圆余弦波作用下海床的瞬态响应、累积响应及其渐进液化特征进行了分析。与线性波作用下海床响应计算结果的对比分析表明,椭圆余弦波会明显增大海床瞬态孔隙水压力和应力幅值,进而显著促进海床内孔隙水压力的累积和液化深度的发展。在近岸浅水区海床的响应分析尤其是海床累积响应的分析中,波浪的非线性效应不容忽视。 相似文献
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《中国海洋大学学报(自然科学版)》2017,(7)
波浪作用下海床的稳定性直接影响着海洋构筑物的安全。目前在波土相互作用的研究中,虽然较多地涉及到对海床液化或剪切破坏的分析,但缺乏不同海床计算厚度和饱和度等条件下二者破坏特征的对比研究。本文基于波浪作用下海床应力的解析解,对砂土海床的剪切破坏和瞬态液化破坏特征进行了详细研究和对比。结果分析表明,对于波浪作用下不同饱和度的砂土海床,其剪切破坏深度随海床计算厚度的增加表现为3种变化模式,而其液化深度随海床计算厚度的增加则只表现为1种变化模式。相比非饱和砂土海床,饱和砂土海床计算厚度较小时才可能发生液化,且其液化深度最小,但相同条件下对应的剪切破坏深度却最大。波浪作用下砂土海床存在一个最不稳定厚度,其数值约为(0.2~0.3)倍波长,此时海床最易发生破坏,且破坏深度较大。波浪作用下砂土海床的剪切破坏在波峰和波谷处均可能发生,而瞬态液化只发生在波谷位置,且其液化深度位于剪切破坏深度范围内。 相似文献
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波浪引起的海床不稳定性是海洋工程中需要考虑的重要问题。在对现有波致海床滑动稳定性计算方法进行分析的基础上,提出了一种波致海床滑动稳定性计算的全应力状态法,将其与现有计算方法进行了对比分析,并进一步研究了波致砂土海床和软土海床的滑动失稳特征。结果分析表明,全应力状态法在波致海床滑动稳定性分析中具有较好的适用性。对于砂土海床,其滑动稳定性受饱和度的影响较大,且当海床计算厚度约为0.2倍波长时对应的滑动深度最大。波浪作用下坡度不超过2°的均质软土海床,其最危险滑动面的位置仅与波长有关,其滑动深度约为0.21倍波长,滑动面半弦长约为0.33倍波长;海床表面的波压力数值只影响其安全系数的大小,而不影响其滑动深度。 相似文献
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《海洋通报(英文版)》2016,(1)
海床土对波浪响应以及波致海床液化失稳的问题,已经有很多研究成果,而波浪作用海床液化土波动压力的研究还未见报道。采用波浪水槽实验,在未液化和液化两种情况下,分别施加不同波高的波浪,对底床各层位采集土体土压力,进行分析。实验结果表明,液化前后总土压力变化不明显,液化后的土动压力比液化前增大几倍到十几倍,且沿着深度的衰减速度更快。根据试验获得结果,进一步分析,提出了在水槽试验条件下的土动压力与波浪要素之间的经验公式。同时指出,在工程设计中应注意因底床液化引起的土动压力的增加的现象。 相似文献
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Wave-induced liquefaction in a porous seabed around submarine pipeline may cause catastrophic consequences such as large horizontal displacements of pipelines on the seabed, sinking or floatation of buried pipelines. Most previous studies in relation to the wave and seabed interactions with embedded pipeline dealt with the wave-induced instaneous seabed response and possible resulting momentary liquefaction (where the soil is liquefied instantaneously during the passage of a wave trough), using theory of poro-elasticity. Studies for the interactions between a buried pipeline and a soil undergoing build-up of pore pressure and residual liquefaction have been comparatively rare. In this paper, this complicated process was investigated by using a new developed integrated numerical model with RANS (Reynolds averaged Navier–Stokes) equations used for governing the incompressible flow in the wave field and Biot consolidation equations used for linking the solid–pore fluid interactions in a porous seabed with embedded pipeline. Regarding the wave-induced residual soil response, a two-dimensional poro-elastoplastic solution with the new definition of the source term was developed, where the pre-consolidation analysis of seabed foundation under gravitational forces including the body forces of a pipeline was incorporated. The proposed numerical model was verified with laboratory experiment to demonstrate its accuracy and effectiveness. The numerical results indicate that residual liquefaction is more likely to occur in the vicinity of the pipeline compared to that in the far-field. The inclusion of body forces of a pipeline in the pre-consolidation analysis of seabed foundation significantly affects the potential for residual liquefaction in the vicinity of the pipeline, especially for a shallow-embedded case. Parametric studies reveal that the gradients of maximum liquefaction depth with various wave and soil characteristics become steeper as pipeline burial depth decreases. 相似文献
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The evaluation of the wave-induced liquefaction potential is particularly important for coastal engineers involved in the design of marine structures. Most previous investigations of the wave-induced liquefaction have been limited to two-dimensional non-breaking waves. In this paper, the integrated three-dimensional poro-elastic model for the wave-seabed interaction proposed by [Zhang, H., Jeng, D.-S., 2005. An integrated three-dimensional model of wave-induced pore pressure and effective stresses in a porous seabed: I. A sloping seabed. Ocean Engineering 32(5/6), 701–729.] is further extended to simulate the seabed liquefaction potential with breaking wave loading. Based on the parametric study, we conclude: (1) the liquefaction depth due to breaking waves is smaller than that of due to non-breaking waves; (2) the degree of saturation significantly affects the wave-induced liquefaction depth, and no liquefaction occurs in full saturated seabed, and (3) soil permeability does not only significantly affect the pore pressure, but also the shear stresses distribution. 相似文献
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The objectives of this study are carried out a series of controlled large wave flume experiments using fine-grained sediment from the Huanghe River Delta, exploring the complete sequence of sediment behavior in the bottom boundary layer(BBL) during wave-induced liquefaction. The results show that:(1) The BBL in silty seabed is exposed to a progressive wave, goes through a number of different stages including compaction before liquefaction, sediment liquefaction, and compaction after liquefaction, which determines the range and thickness of BBL.(2) With the introduction of waves, first, the sediment surface has settled by an amount S(S=1–2 cm) in the course of wave loadings with an insufficient accumulation of pore water pressure. And a thin high concentration layer formed the near-bed bottom.(3) Once the liquefaction sets in, the liquefied sediment with an ‘orbital motion' and the sub-liquefied sediment form a two-layer-sediment region. The range of BBL extends downwards and stopped at a certain depth, subsequently, develops upwards with the compaction process. Meanwhile, resuspended sediments diffuse to the upper water column.(4) During the dynamics process of the BBL beneath progressive waves, the re-suspended sediment increment ranked as sediment liquefaction erosion before liquefaction compaction after liquefaction. 相似文献
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波浪作用下埕岛海域海底土液化分区 总被引：1，自引：0，他引：1
根据埕岛海域表层沉积物特征,结合该区的波浪实测资料推算的波浪要素,利用动三轴实验得到研究区土体在循环荷载作用下孔隙水压力的增长与振动次数的关系,计算研究区内海底土层的液化可能性和液化所需的时间,并根据土体在不同水深情况下达到液化所需的时间对研究海域进行了液化分区。结果显示,7-8 m等深线之间的海底土体由于受到波浪破碎作用的影响,最易发生液化,液化影响深度也最深,自该海域向近岸和远海,液化可能性降低;土层埋深为2.5 m以浅时,研究区大部分区域液化可能性为高,而到埋深为4 m时土层液化可能性明显降低。 相似文献
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黄河水下三角洲的地质勘察揭示了海底浅表地层发生的各种灾害地质现象。本文以风暴浪导致海底土体液化观点,结合土体动力三轴试验、波浪水槽试验,对黄河水下三角洲浅表地层土体的液化发生条件、形成模式、液化土体运动以及地层发生的重新层化问题进行了分析,指出黄河水下三角洲的灾害地质由于风暴浪导致海底粉质土液化运动而形成,液化后土体运动形式与波浪运动一致,液化土体运动造成的土颗粒分异而使地层重新层化,并初步指出了风暴浪导致海底土体液化在地学、环境、工程等方面的研究问题。 相似文献
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近年来,在各种近海建筑物的建设中,桩基础被越来越广泛地应用。关于海床内桩基各层位对波浪动力响应相位差的研究,国内外学者研究的重点主要集中在海床内各层位孔隙水压力的相位变化。而关于波浪作用下海床各层位土体总压力相位的研究则很少。本研究采用波浪水槽实验,在土床未扰动和土床扰动液化两种工况下,分别施加不同波高的波浪,对底床各层位土体总压力的相位进行对比研究。实验结果表明,当土体未运动时,在渗透性和饱和度均匀的土体中,各层位土体之间不存在相位差。当底床液化后,土体出现显著分层现象,在液化土层和不动土层间存在显著的相位差。此时,总压力振幅呈现先增大后减小的现象,且在床面下-10cm处出现最大值。 相似文献
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辽河三角洲潮道沉积物为软弱淤泥质土，管桩在波流荷载作用下的弹性变形或振动，可以导致潮道软土强度衰减并发生变形位移，随着悬臂段加长和波流荷载振动作用，下部扮土会自上而下发生液化。简单管桩的抗倾验算可以按照波流力与被动土压力的作用力矩分析，并考虑到海底的冲刷淘空深度。管桩打入下卧高强度粉土时，在保证打入深度的同时，应适当增大管桩的强度，加大管桩自振周期与波浪周期的差值。 相似文献
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根据现场大风浪条件下的实测资料,粉质土海岸水体中的含沙量沿垂向具有上部均匀、近底突增的分布特点,即呈L型分布特征。利用黄河三角洲粉质土作为试验底床开展波浪水槽试验研究,揭示了底床粉质土在波浪作用下产生液化情况的水体含沙量沿垂向存在L型分布特征。根据试验现象以及悬沙粒度变化,分析认为底部高含沙层的形成主要受粉质土液化后细颗粒析出的影响,上部水体中悬沙由湍流脉动维持。对粉质土海岸大风天气期间水体含沙量剧烈增加采用波致粉质土液化的观点进行了初步解释。 相似文献
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The evaluation of seabed response under wave loading is important for prediction of stability of foundations of offshore structures. In this study, a stochastic finite element model which integrates the Karhunen-Loève expansion random field simulation and finite element modeling of wave-induced seabed response is established. The wave-induced oscillatory response in a spatially random heterogeneous porous seabed considering cross-correlated multiple soil properties is investigated. The effects of multiple spatial random soil properties, correlation length and the trend function (the relation of the mean value versus depth) on oscillatory pore water pressure and momentary liquefaction are discussed. The stochastic analyses show that the uncertainty bounds of oscillatory pore water pressure are wider for the case with multiple spatially random soil properties compared with those with the single random soil property. The mean pore water pressure of the stochastic analysis is greater than the one obtained by the deterministic analysis. Therefore, the average momentary liquefaction zone in the stochastic analysis is shallower than the deterministic one. The median of momentary liquefaction depth generally decreases with the increase of vertical correlation length. When the slope of the trend function increases, the uncertainty of pore water pressure is greatly reduced at deeper depth of the seabed. Without considering the trend of soil properties, the wave-induced momentary liquefaction potential may be underestimated. 相似文献