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1.
具有弹性支座杆件的动力稳定性研究   总被引:3,自引:0,他引:3  
孙强 《力学与实践》2004,26(1):29-31
研究了杆件具有弹性支座时直杆的动力稳定性问题,推导出了杆件的临界频率和动力不稳定边界,分析了弹簧刚度和阻尼对杆件动力稳定性的影响,研究表明杆件的侧向刚度愈大其结构的动力稳定性愈好,阻尼对杆的振动起有利作用,并提出了在实际工程中减小杆件振动的一些措施.  相似文献   

2.
钢筋混凝土空间杆件精细非线性分析模型   总被引:1,自引:0,他引:1  
针对现有钢筋混凝土空间杆件非线性分祈模型进行了评还,应用结构力学方法推导得到了沿秆长配筋分布均匀的钢筋混凝土空间杆件的非线性单元刚度矩阵,建立了应用高斯积分点所在截面的非线性性质描述钢筋混凝土空间杆件非线性的计算过程。对于沿杆长配筋分布不均匀的杆件,根据其实际情况,将其细分为两段或三段沿杆长配筋分布均匀的杆段,以沿杆长配筋分布均匀的钢筋混凝土空间杆件非线性分析模型为基础,建立了沿杆长配筋分布不均匀的空间杆件的非线性分析模型。最后,给出了两个算例。就本文方法及程序的计算结果与模型结构振动台试验结果、常规非线性杆件模型的计算结果进行了比较。  相似文献   

3.
压弯杆件的动荷性能分析   总被引:1,自引:0,他引:1  
研究了在轴向动力荷载作用下压弯构件的动力特征,根据压弯构件的动力平衡方程,导出了不同横向荷载形式下的振幅计算公式,分析了横向荷载对杆件动力性能的影响,根据理论研究成果提出了在实际工程中减小杆件振幅的一些措施.  相似文献   

4.
针对增量形式的流体饱和两相多孔介质弹塑性波动方程组,运用基于显式逐步积分格式的时域显式有限元方法对该波动方程组进行求解,并应用基于SMP破坏准则的弹塑性动力本构模型描述两相介质的动力反应性质,对两相介质在输入地震波作用下的弹塑性动力反应进行计算和分析,将计算结果与相应的弹性动力反应的计算结果进行对比;对本文应用的弹塑性...  相似文献   

5.
熊辉 《计算力学学报》2016,33(5):689-696
提出一种群桩-土弹塑性模型,结合动力文克尔理论,推导出了与桩(筏)-土属性及SSI体系频率相关的各项弹簧-阻尼单元动力阻抗,建立了三维框架土-结构相互作用有限元简化分析模型。针对不同地震激励,在不同桩-土条件下对模型进行了动力非线性时程分析,结果表明,在某些地震动和土-基础条件下,上部结构非线性作用效应结果可能大于固基假定情形,且桩-土弹塑性模型对上部结构柔弱层位置产生影响。应用本文简化方法可以快速、较准确有效地进行复杂的上下部结构动力时程分析及抗震评估。  相似文献   

6.
纤维杆元模型在框架结构非线性分析中的应用   总被引:4,自引:0,他引:4  
本文基于Fiber模型,结合分段变刚度概念,推导建立了便于框架结构非线性分析应用的纤维杆元模型,即由杆件两端弹塑性区的纤维子单元及杆件中部弹性区的弹性子单元组成。弹塑性区由于受力较大,采用精细的纤维子单元模拟,中间弹性区受力相对较小,直接采用弹性子单元代替;同时,应用增分理论,分别推导了三维纤维子单元及弹性子单元的单刚矩阵,并采用静力凝聚方法,集成了三维纤维杆元模型的刚度矩阵。另外,直接应用混凝土及钢筋的本构关系,利用该计算模型对一栋12层框架结构进行了时程非线性分析,计算结果与振动台试验结果进行了比较,比较结果表明两者在结构动力特性,位移响应方面等均吻合较好,验证了该模型的有效性,可为推广使用提供参考。  相似文献   

7.
利用ANSYS/LS-DYNA 有限元程序,考虑几何非线性和材料非线性效应,开展单层椭圆抛物面网壳结构在撞击荷载作用下的动力稳定性研究.分析了该类网壳在以一定高度的自由落体撞击作用下的撞击力响应(撞击力、节点位移、杆件轴力和能量)及网壳失稳模态,进一步根据产生的动力响应对其在撞击作用下的弹塑性动力稳定问题进行了判定.结果表明:网壳结构在撞击作用下失稳时,撞击力时程曲线形状基本上呈陡峭的三角形脉冲荷载形式,其最大峰值和脉宽与撞击冲量及网壳所处变形阶段的刚度性能相关;特征节点的位移响应突然增大,失稳部位杆件的轴力大幅减小,结构的变形能和总能量也突然增大,整个结构变形形状发生突变;节点的残余位移、撞击力和持时等特征参数都产生一致性突变.  相似文献   

8.
为模拟地震作用时杆件在变动轴力和双向弯曲的耦合特点,基于简化纤维模型的多弹簧单元模型近年被广泛应用。本文作者在相关论文中提出了考虑剪切变形弹塑性刚度影响的多弹簧模型空间梁柱单元,杆件的计算模拟精度除了取决于单元模型之外,还决定于两个重要参数:弹簧位置及个数布置、塑性区长度,本文将针对其进行参数分析并提出合理建议取值。本文最后还提出了模拟杆件残余应力的合理弹簧布置方式。  相似文献   

9.
基于多弹簧模型的空间梁柱单元(Ⅱ):参数分析   总被引:1,自引:0,他引:1  
为模拟地震作用时杆件在变动轴力和双向弯曲的耦合特点,基于简化纤维模型的多弹簧单元模型近年被广泛应用.本文作者在相关论文中提出了考虑剪切变形弹塑性刚度影响的多弹簧模型空间梁柱单元,杆件的计算模拟精度除了取决于单元模型之外,还决定于两个重要参数:弹簧位置及个数布置、塑性区长度,本文将针对其进行参数分析并提出合理建议取值.本文最后还提出了模拟杆件残余应力的合理弹簧布置方式.  相似文献   

10.
本文推导了考虑 P-Δ效应的带刚臂单杆件弹塑性刚度矩阵。在推导过程中,考虑了轴向变形、弯曲变形和剪切变形。可用于杆系结构的静力分忻、动态分析和弹塑性稳定计算。按照本文的推导结果,巳编成高层建筑弹塑性动态分析程序并在高层建筑工程中运用。本文的成果把 K.I.Majid和 M.F.Giberson 的工作推进了一步。高层建筑和大跨度结构的弹塑性动态分析是当前工程抗震方面的一个重要研究课题。本文的工作是应这一需要而展开的。  相似文献   

11.
In this paper, a numerical model is developed to predict the cryogenic chilldown process of a vertical tube for both terrestrial and microgravity conditions. The flow field is covered by four distinct regions, which are single-phase vapor region, dispersed flow region, inverted annular flow region, and single-phase liquid region. Heat transfer mechanisms are dictated by the flow patters. A two-fluid model is employed to analyze the dispersed flow region and the inverted annular film boiling region. Gravity effect on the chilldown process is also investigated. Model results indicate that film boiling heat transfer decreases with decreasing gravity level for the bottom flooding condition. The model results show a good agreement with the experimental data.  相似文献   

12.
为提高聚合物熔体剪切黏度模型的描述精度,提出了一个基于二次Bezier 曲线的黏度模型. 模型采用分段函数描述,在对数坐标系中,低剪切速率时的牛顿区和高剪切速率时的幂律区采用线性函数,介于二者之间的过渡区采用二次Bezier 曲线. 通过牛顿区和幂律区的直线延长线构造Bezier 曲线的控制多边形,从而保证三段曲线的光滑过渡. 模型可以明确给出任意温度下低剪切速率时牛顿区的结束点,以及高剪切速率时幂律区的开始点. 拟合算例表明,所提出模型的拟合精度明显高于Cross-Arrhenius 黏度模型.  相似文献   

13.
多孔材料填充薄壁结构吸能的相互作用效应   总被引:9,自引:1,他引:8  
研究多孔材料填充薄壁结构的相互作用效应产生的机理,并建立了表征模型. 以泡沫 铝填充帽形结构为例,发现压溃的填充物分为致密区、过致密区和未变形区3个区域. 基于 理想可压缩假设建立了填充多孔材料分析模型,获得各区域体积变化和等效应变等关系;结 合薄壁结构超叠缩单元模型,对填充结构各组分的能量吸收进行了拆分. 研究表明,薄壁结 构的吸能略有增加,多孔材料的吸能增加40{\%}左右. 过致密区的形成是相互作用效应的 主要原因.  相似文献   

14.
A computational method (CADD) is presented whereby a continuum region containing dislocation defects is coupled to a fully atomistic region. The model is related to previous hybrid models in which continuum finite elements are coupled to a fully atomistic region, with two key advantages: the ability to accomodate discrete dislocations in the continuum region and an algorithm for automatically detecting dislocations as they move from the atomistic region to the continuum region and then correctly “converting” the atomistic dislocations into discrete dislocations, or vice-versa. The resulting CADD model allows for the study of 2d problems involving large numbers of defects where the system size is too big for fully atomistic simulation, and improves upon existing discrete dislocation techniques by preserving accurate atomistic details of dislocation nucleation and other atomic scale phenomena. Applications to nanoindentation, atomic scale void growth under tensile stress, and fracture are used to validate and demonstrate the capabilities of the model.  相似文献   

15.
The “double-buffer problem” has been regarded as a crucial concern for the strategy behind the hybrid large eddy simulation (LES)/Reynolds-averaged Navier–Stokes (RANS) model (or HLR model, for short). Such models are likely to show unphysical mean-velocity distributions in the LES–RANS interface region, where “super-streak structures” also appear that look like low-speed streaks generated in the near-wall region of wall turbulence. To overcome this difficulty, the stochastic backscatter model, in which the vortex structures in the interface region are divided into smaller scales, holds promise due to the effect of random source term imposed in the momentum equation. Although this method is effective, several parameters must be prescribed and their specification process is arbitrary and ambiguous. An alternative advanced HLR model has been proposed, in which an anisotropy-resolving subgrid-scale (SGS) model was adopted in the LES region as well as a one-equation nonlinear eddy viscosity model in the RANS region. Previous investigations indicated that this HLR model did not exhibit or, at least, largely reduced the “double-buffer problem” in the mean-velocity distribution, with no special treatment being applied. The main purpose of the present study is to reveal why this HLR model improves the predictive performance in the LES–RANS interface region. Specifically, we focus on the role of the extra anisotropic term introduced in the SGS model, finding that it plays an important role in enhancing vortex structures in the interface region, leading to a considerable improvement in model performance.  相似文献   

16.
An ice failure model with large force contact region is presented. This model is based on survey and analysis of field and experimental observations and assumes the existence of a quasiregular failure structure in the contact region, where the failure nucleus can move on the contact surface (scan it). The character of motion is determined by the conditions of the failure nucleus displacement and the failure product extrusion from the contact region. The mechanism ensuring the average stress decrease as the contact region increases is explained.  相似文献   

17.
非晶态高聚物裂尖银纹损伤场   总被引:7,自引:0,他引:7  
在非晶态高聚物裂端塑性区引入银纹损伤,提出了一个修正的Dugdale模型,并由它确定塑性区的大小,算例表明,银纹损伤导致了塑性区深度的增加。此外,在Dugdale模型下研究了稳态扩展的端塑性区,在裂纹缓慢扩展、小范围银纹化以及材料为线粘弹性等假定下,由能量原理得到了控制裂纹生长的一个非线性微分一积分方程,从中看到银纹损伤的影响十分显著。  相似文献   

18.
A new lattice model of traffic flow based on Nagatani’s model is proposed by taking the effect of driver’s memory into account. The linear stability condition of the extended model is obtained by using the linear stability theory. The analytical results show that the stabile area of the new model is larger than that of the original lattice hydrodynamic model by adjusting the driver’s memory intensity parameter p of the past information in the system. The modified KdV equation near the critical point is derived to describe the traffic jam by nonlinear analysis, and the phase space could be divided into three regions: the stability region, the metastable region, and the unstable region, respectively. Numerical simulation also shows that our model can stabilize the traffic flow by considering the information of driver’s memory.  相似文献   

19.
Large eddy simulation (LES) is combined with the Reynolds-averaged Navier–Stokes (RANS) equation in a turbulent channel-flow calculation. A one-equation subgrid-scale model is solved in a three-dimensional grid in the near-wall region whereas the standard k–ε model is solved in a one-dimensional grid in the outer region away from the wall. The two grid systems are overlapped to connect the two models smoothly. A turbulent channel flow is calculated at Reynolds numbers higher than typical LES and several statistical quantities are examined. The mean velocity profile is in good agreement with the logarithmic law. The profile of the turbulent kinetic energy in the near-wall region is smoothly connected with that of the turbulent energy for the k–ε model in the outer region. Turbulence statistics show that the solution in the near-wall region is as accurate as a usual LES. The present approach is different from wall modeling in LES that uses a RANS model near the wall. The former is not as efficient as the latter for calculating high-Reynolds-number flows. Nevertheless, the present method of combining the two models is expected to pave the way for constructing a unified turbulence model that is useful for many purposes including wall modeling. Received 11 June 1999 and accepted 15 December 2000  相似文献   

20.
This study develops a one-group interfacial area transport equation (IATE) for vertical-upward-to-horizontal air–water bubbly two-phase flows through a 90° elbow with a non-dimensional centerline radius of curvature of three. In order to develop the model, an extensive database is established by acquiring local two-phase flow parameters using a four-sensor conductivity probe upstream and downstream of the elbow. The data show there exist three characteristic regions in void distribution, including a bimodal-to-bimodal region, a bimodal-to-single-peaked region, and a developed horizontal flow region with void accumulated at the top of the pipe cross-section. Using the database, the preliminary dissipation length model developed by Yadav et al. (2014b) is improved by including the transition region near the exit of the elbow in addition to the dissipation region. To close the IATE model, the bubble velocity advection term and bubble interaction terms in the IATE are correlated with the parameter characterizing the “elbow-strength”. The two-phase pressure drop across the elbow is modeled using the modified Lockhart–Martinelli correlation which takes into account the minor loss effect. The closed IATE model is implemented to predict interfacial area transport in vertical-upward-to-horizontal two-phase flow. It is found that the developed model is capable of predicting interfacial area concentration with an average percent difference of less than ±6%.  相似文献   

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