三维横向流体诱发直管振动的数值研究

基于计算流体力学和计算结构动力学,并考虑流体-结构两个物理场之间的相互作用,利用有限体积法及LES方法离散非稳态、粘性、不可压缩湍流流场;采用有限元方法离散结构动力学方程,结合动网格控制技术,建立了横向流体作用下传热管流致振动计算的三维仿真模型。首先,基于建立的模型得到了横流作用下传热管的振动响应,并通过与已有的文献数据进行比较发现,两者趋势一致、数值上吻合较好,证明了本文模型的合理性;其次,在较宽的折减速度和频率比范围内,研究了直管的响应、流体力系数、涡脱落频率,并通过管表面压力分布、尾流区的时均速度等分析了时均流场特性;第三,研究了两种折减速度的归一化方法,指出对于三维弹性管的流体诱发振动问题,采用通用的折合速度来表示响应图能清晰地表征其响应特征;最后,比较分析了弹性支撑刚性管与弹性管的流体诱发振动特性。结果表明,对于三维弹性管的流体诱发振动计算应考虑结构的弹性变形与流体流动间的相互作用。     

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采用两相流的流动换热理论,建立二维几何模型,运用FLUENT对稳定入口流速下注入气体的铅铋流动段作了模拟。模拟研究注入气体的体积份额或速度改变对压力和铅铋与注入气体之间换热与影响,得到了不同条件下的温度与压力分布。分析结果发现,体积份额减小,铅铋流体的径向温度分布更加均匀,中心温度更低;随着体积份额的减小,铅铋的总压呈现出一种下降的趋势。注入气体速度不同对铅铋整体的换热影响不大;中心处的动压有较大增加,总压改变甚微。     

All-optical modulator based on a ferrofluid core metal cladding waveguide chip

We propose a novel optical intensity modulator based on the combination of a symmetrical metal cladding optical waveguide （SMCW） and ferrofluid, where the ferrofluid is sealed in the waveguide to act as a guiding layer. The light matter interaction in the ferrofluid film leads to the formation of a regular nanoparticle pattern, which changes the phase match condition of the ultrahigh order modes in return. When two lasers are incident on the same spot of the waveguide chip, experiments illustrate all-optical modulation of one laser beam by adjusting the intensity of the other laser. A possible theoretical explanation may be due to the optical trapping and Soret effect since the phenomenon is considerable only when the control laser is effectively coupled into the waveguide.     

Effects of transpiration on unsteady MHD flow of an upper convected Maxwell （UCM） fluid passing through a stretching surface in the presence of a first order chemical reaction

The aim of this article is to present the effects of transpiration on the unsteady two-dimensional boundary layer flow of non-Newtonian fluid passing through a stretching sheet in the presence of a first order constructive/destructive chemical reaction. The upper-convected Maxwell （UCM） model is used here to characterize the non-Newtonian behavior of the fluid. Using similarity solutions, the governing nonlinear partial differential equations are transformed into ordinary ones and are then solved numerically by the shooting method. The flow fields and mass transfer are significantly influenced by the governing parameters. The fluid velocity initially decreases as the unsteadiness parameter increases and the concentration decreases significantly due to the increase in the unsteadiness. The effect of increasing values of transpiration （suction） and the Maxwell parameter is to suppress the velocity field; however, the concentration is enhanced as transpiration （suction） and the Maxwell parameter increase. Also, it is found that the fluid velocity decreases as the magnetic parameter increases; however, the concentration increases in this case.     

氢分子团簇的研究进展及其应用

氢分子是宇宙中结构最简单、数量最多的分子,氢分子团簇是分子团簇结构和动力学的研究原型。同时,作为激光核聚变和托克马克受控热核聚变的原料,氢分子团簇对聚变的效率有很大的影响。本文介绍了氢分子团簇在基础研究、超流体研究、托克马克研究和激光核聚变研究中的研究意义、研究内容和研究现状。     

基于流体模型和非平衡态电子能量分布函数的高功率微波气体击穿研究

用流体模型研究高功率微波气体击穿时, 电子能量分布函数常被假设为麦克斯韦分布形式, 此假设可能将给模拟结果带来较大的误差. 通过求解玻尔兹曼方程, 得到非平衡状态下的电子能量分布函数. 分别将上述两类分布函数引入到流体模型中, 对氩气击穿进行了数值模拟. 结果表明, 基于非平衡分布函数得到的击穿时间与粒子模拟结果符合得很好, 而当平均电子能量较低时, 麦克斯韦分布函数的高能尾部导致了较短的击穿时间. 最后, 采用非平衡分布函数计算了不同压强下的氩气击穿阈值, 发现其与实验结果基本符合. 关键词： 微波气体击穿 电子能量分布函数 流体模型 玻尔兹曼方程     

利用格子Boltzmann方法模拟矩形腔内纳米流体Raleigh-Benard对流

利用格 子 Boltzmann方法模拟矩形腔内纳米流体Rayleigh-Benard对流, 得到温度场和流线分布, 比较分析不同Ra数、体积分数、粒径下纳米流体对流换热的变化情况. 结果表明: 在相同的Ra 数和体积分数下, 纳米流体的对流换热随着粒径的增大而减弱; 在相同的Ra数和粒径下, 纳米流体的对流换热随着体积分数增大而增强. 关键词： 纳米流体 Raleigh-Benard 多相流 格子Boltzmann方法     

微细通道纳米与非纳米流体传热和压降对比研究

分别以0.2%、0.5%、1%质量分数的Al2O3-H2O纳米流体和去离子水为实验工质,在高2mm,宽1mm的矩形微细通道内进行纳米流体与非纳米流体两相沸腾传热和压降对比研究。实验结果表明:增加质量通量对两种工质换热系数影响都较小,但增加热流密度可提高换热系数;在相同工况下,与水基液相比,采用Al2O3-H2O纳米流体换热系数明显增大,且随着纳米流体质量分数的增加而增加,对于该实验换热系数可提高8%～17%;随着纳米颗粒质量分数和质量通量的增加,两相摩擦压降显著增大。     

由雁阵引出的一些话题

编者按:欢迎就"雁陈现象"作进一步的分析、讨论."蜃楼百尺横苍海,雁字一行书绛霄","九秋惊雁序,万里狎渔翁","雁阵惊寒,声断衡阳之浦","碧云天,黄花地,西风紧,北雁南翔"……秋霄雁阵,总能给人以或壮丽、或凄婉、或温馨……不尽的     

FINITE ELEMENT METHODS FOR THE NAVIER-STOKES EQUATIONS BY H（div） ELEMENTS

We derived and analyzed a new numerical scheme for the Navier-Stokes equations by using H（div） conforming finite elements. A great deal of effort was given to an establishment of some Sobolev-type inequalities for piecewise smooth functions. In particular, the newly derived Sobolev inequalities were employed to provide a mathematical theory for the H（div） finite element scheme. For example, it was proved that the new finite element scheme has solutions which admit a certain boundedness in terms of the input data. A solution uniqueness was also possible when the input data satisfies a certain smallness condition. Optimal-order error estimates for the corresponding finite element solutions were established in various Sobolev norms. The finite element solutions from the new scheme feature a full satisfaction of the continuity equation which is highly demanded in scientific computing.