共查询到16条相似文献，搜索用时 203 毫秒
1.
根据豪斯纳尔（Housner）理论, 建立了考虑槽内水体与渡槽槽身流-固耦合的横向地震响应计算模型,分析了槽身断面深宽比变化对渡槽结构抗震的影响,并对某大型渡槽进行了多工况地震时程响应计算. 结果表明,在地震波作用下,渡槽槽内大质量水体对渡槽的横向地震响应有较大的影响, 但水体的晃荡作用有明显的TLD效应. 若将水体视为刚体, 质量全部附加到槽体上,将严重地夸大水的地震惯性力作用,且在渡槽槽身断面选择时应考虑深宽比对墩身地震响应的影响, 以减小地震力. 相似文献
2.
3.
大型三维矩形、U形渡槽地震响应对比分析 总被引：1，自引：1，他引：0
本文应用任意拉格朗日-欧拉(ALE)有限元方法对比分析大型三维排架支撑矩形、U形渡槽结构地震响应,以获得渡槽中动水压力资料。研究表明,渡槽中水体的晃动幅度十分显著,水体的大幅晃动显著地改变两种截面形式渡槽中水压力、槽体应力值及U形渡槽动水压力和应力分布,对矩形渡槽动水压力和应力分布规律影响不大。动应力分布的改变直接影响到大型预应力U形截面渡槽结构中预应力钢筋的有效性。在渡槽的抗震设计中,应充分考虑U形截面渡槽动水压力和动应力分布变化问题,动水压力应该作为一项主要的外荷载予以考虑。 相似文献
4.
随着我国经济的发展,大型渡槽的建设向西部高烈度山区快速推进,渡槽面临着严峻的地震风险。正确模拟渡槽中水体晃动性能,是渡槽抗震性能分析的关键技术难点。依托滇中引水工程中的松林渡槽,本文建立了大断面渡槽结构的精细化有限元模型,通过欧拉-拉格朗日耦合(coupled Eulerian-Lagrangian,简称“CEL”)分析建立了渡槽水体晃动的流固耦合分析模型,同时建立了经典的等效弹簧-质量模型(简称“SM模型”)作为对比,量化两种水体建模方法产生的结果差异。通过对松林渡槽中典型简支跨进行非线性动力时程分析,对比了两种建模方式下,槽身和墩柱混凝土损伤的发展情况,摩擦摆支座的竖向反力,并呈现了CEL分析得到的水体波动情况,阐释了两种分析方法的主要误差来源。在渡槽地震响应分析的基础上,论文建立了槽身的节段模型,研究了CEL方法和等效SM模型在不同槽身加速度和竖向分量下的动力分析结果异同,并提出了等效SM模型的适用范围。 相似文献
5.
6.
在深水桥墩及桩基础等结构地震反应中,地震激励下的水流动水压力对水中结构的作用以及结构位形变化对水体的反作用,属于典型的流固强界面耦合问题。以一顶端伸出水面的圆柱式结构为研究对象,基于任意拉格朗日-欧拉描述的Navier-stokes方程,建立了考虑水流-结构强耦合效应的水流-结构三维有限元模型。以正弦位移波输入,考察结构材料模量、水流流速和水位、激振频率和位移幅值等多种因素,分析了结构表面作用的动水压力反应特征以及水流动力效应,探讨了水流动力效应的主要影响因素。结果表明：考虑流固强耦合作用时,结构表面作用的动水压力及其分布具有强烈的频率依赖性,高频激励可显著增强动水压力作用;由于结构周围流体具有一定的粘滞性及动载作用下具有较强的辐射阻尼效应,水流动力效应对结构的位移、内力反应均有一定的抑制作用;激振频率、水流流速和水位以及结构材料模量等因素,对水流动力效应均有一定的影响。 相似文献
7.
大型渡槽结构模态分析 总被引：17，自引：0，他引：17
大型渡槽在南水北调水利工程中起着重要作用。本文根据大型渡槽的结构特点,考虑渡槽横向弯扭耦合振动、约束扭转变形、渡槽支架变形和盆式橡胶支座等胶地支座等对渡槽动力作用的影响,应用梁段有限元方法,对某大型渡槽的模态进行分析,研究了该渡槽设计水位、渡槽支架高度、渡槽支架截面尺寸、渡槽盆式橡胶支座刚度变化等对大型渡槽模态的影响,探讨了该大型渡槽的上述４种工况下的模态变化范围,所得结果可为大型渡槽的抗震设计提 相似文献
8.
首先介绍了钢筋混凝土渡槽结构在地震荷载作用下的分析理论,根据这些理论建立了渡槽结构的动力有限元分析模型,分别采用干模态法、附加质量法和ALE法考虑渡槽结构液固耦合作用,通过具体的工程算例,对钢筋混凝土渡槽结构进行了不同工况下的数值模拟研究,包括混凝土非线性材料分析、渡槽结构静水与动水响应分析、渡槽结构自振特性分析和槽墩的能力曲线分析。研究表明,考虑固液耦合作用的渡槽实体有限元模型能较好地模拟渡槽结构地震反应,并得到相应的渡槽结构地震反应规律。 相似文献
9.
为了研究槽墩高度对矩形渡槽结构系统的动力特性及水平地震动力响应的影响,本文采用Housner流-固耦合模型,提出了一种用于土-桩-渡槽-水体系统的有限元分析方法.以渡槽结构原理性拟动力试验结果为依据,对拟动力试验进行了有限元仿真计算,验证了本文所给出的计算模型的合理性.在此基础上,重点对不同槽墩高度的矩形渡槽结构系统进行了计算研究,结果表明:渡槽结构的基频随槽墩高变化显著,而其高阶模态频率则变化不大.在E1 Centro波及TAR波输入时,随着槽墩高的增大,渡槽结构关键部位的最大动应力等响应存在递减趋势;尤其在E1 Centro波输入时,递减趋势更为显著.人工波输入时,结构动力响应状况存在一定波动,但从总体而言志,矮墩渡槽的动力响应大于高墩渡槽的动力响应. 相似文献
10.
《地震工程与工程振动》2021,41(5)
地震动作用下,高烈度地区大型多跨渡槽槽间的相对错动直接关系到渡槽止水的安全,更有可能引起渡槽的倾覆性失稳。针对我国西南地区某一8跨渡槽,考虑了槽内水体与渡槽的动力相互作用,采用了可调节阻尼的等效双线性恢复力模型模拟了高阻尼支座的力学性能,建立了大型渡槽槽体-水体-支座-槽墩-地基的三维有限元整体模型,同时以拟合的3套符合场地特性的人工地震波和实测天津波作为输入,进行了大型渡槽结构的动力学分析,定量的给出了多跨渡槽槽间相对错动位移的大小并对其产生的机理进行了阐释,提出了槽间止水设计要点,以期促进待建和已建渡槽工程的实施与安全运营。 相似文献
11.
This paper reports on a semi‐analytical/numerical method to model sloshing water in an arbitrarily shaped aqueduct. The water motion is assumed to be inviscid, compressible, and linear (small displacement). The transverse sloshing fluid in an aqueduct is equivalently simplified as a fixed rigid mass M0 and a mass–spring system (M1, K1). According to a rule that the actual fluid (computed with finite element model) and its equivalent mechanical model have the same first sloshing frequency and acting effects on the aqueduct, the analytical solutions of the fixed (impulsive) mass M0, sloshing (convective) massM1, spring stiffness K1, and their locations in the aqueduct body are acquired by the least squares (curve fitting) algorithm. Applying this equivalent principle, the equivalent mechanical models are respectively obtained for the sloshing water in rectangular, semicircular, U‐shaped, and trapezoid aqueducts. The equivalent principle and fluid models are validated through comparison investigations involving rectangular and U‐shaped aqueducts. The dynamic properties and seismic responses of the original and equivalent systems are simulated, compared, and discussed for a U‐shaped aqueduct bridge. The main purpose of this paper is to provide a simplified model of sloshing fluid for the seismic/wind‐resistant computation of the support structures of the aqueduct bridge. Copyright © 2011 John Wiley & Sons, Ltd. 相似文献
12.
In this paper, a full-scale 3-D finite element model of the Jundushan cable-stayed aqueduct bridge is established with ANSYS Code. The shell, fluid, tension-only spar and beam elements are used for modeling the aqueduct deck, filled water, cables and support towers, respectively. A multi-element cable formulation is introduced to simulate the cable vibration. The dry (without water) and wet (with water) modes of the aqueduct bridge are both extracted and investigated in detail. The dry modes of the aqueduct bridge are basically similar to those of highway cable-stayed bridges. A dry mode may correspond to two types of wet modes, which are called the in-phase (with lower frequency) and out-of-phase (with higher frequency) modes. When the water-structure system vibrates in the in-phase/out-of-phase modes, the aqueduct deck moves and water sloshes in the same/opposite phase-angle, and the sloshing water may take different surface-wave modes. The wet modes of the system reflect the properties of interaction among the deck, towers, cables and water. The in-phase wet frequency generally decreases as the water depth increases, and the out-of-phase wet frequency may increase or decrease as the water depth increases. 相似文献
13.
渡槽中流体非线性晃动的边界元模拟 总被引：20，自引：0，他引：20
应用边界元法分析了流体非线性晃动及其对渡槽的作用效应,将所得结果与线性解析结果作了比较．数值计算表明：流体以较大幅度晃动时,线性模型结果与非线性边界元结果有较大偏差,计算有限幅流体晃动反应宜采用非线性模型． 相似文献
14.
Based on the theory of Housner, the transverse seismic response of beam aqueduct considering fluid-structure cou-pling is established. With the variation of aqueduct cross-section ratio of depth to width, the aqueduct transverse seismic response change. The transverse seismic response of a large-scale aqueduct in several work condition are calculated. It shows that the transverse seismic response is greatly influenced by the water mass in the aqueduct, but the shaking water play a TLD role. If the whole water is appended aqueduct body, it will magnify seismic iner-tia action. When aqueduct cross-section is selected, the influence of ratio of depth and width to pier seismic re-sponse should be considered in order to reduce seismic action. 相似文献
15.
This paper reports on the results of a study conducted on tanks partially filled with water, representing tuned liquid dampers (TLD), subjected to both 1D and 2D horizontal excitations. The sloshing response of the water in the tank is characterized by the free surface motion, the resulting base shear force, and evaluation of the energy dissipated by the sloshing water. A 1D non‐linear flow model capable of simulating a TLD equipped with damping screens is employed to model a 2D TLD. Application of this particular model requires the assumption that the response is decoupled and can be treated as the summation of two independent 1D TLDs. Results from the non‐linear flow model are compared with the 2D experimental shake table test results leading to a validation of the decoupled response assumption. This attractive decoupled response property allows square and rectangular tanks to be used as 2D TLDs, which can simultaneously reduce the dynamic response of a structure in two perpendicular modes of vibration. Copyright © 2005 John Wiley & Sons, Ltd. 相似文献
16.
Numerical simulations of a single‐degree‐of‐freedom (SDOF) structure, rigidly supporting a tuned liquid damper (TLD) and subjected to both real and artificially generated earthquake ground motions, show that a properly designed TLD can significantly reduce the structure's response to these motions. The TLD is a rigid, rectangular tank with shallow water in it. Its fundamental linear sloshing frequency is tuned to the structure's natural frequency. The TLD is more effective in reducing structural response as the ground excitation level increases. This is because it then dissipates more energy due to sloshing and wave breaking. A larger water‐depth to tank‐length ratio than previous studies suggested, which still falls within the constraint of shallow water theory, is shown to be more suitable for excitation levels expected in strong earthquake motions. A larger water‐mass to structure‐mass ratio is shown to be required for a TLD to remain equally effective as structural damping increases. Furthermore, the reduction in response is seen to be fairly insensitive to the bandwidth of the ground motion but is dependent on the structure's natural frequency relative to the significant ground frequencies. Finally, a practical approach is suggested for the design of a TLD to control earthquake response. Copyright © 2000 John Wiley & Sons, Ltd. 相似文献