共查询到20条相似文献,搜索用时 125 毫秒
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构造了一个特殊的弹性力学平面问题比拟不可压平面无黏流动, 从而使这类流体力学问题可
以采用固体力学软件ANSYS计算. 算例说明了比拟关系的正确性, 同时说明这样的比拟计算
与直接使用流体力学软件Fluent计算相比, 可以得到更精确的结果. 相似文献
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微流控器件中的多相流动 总被引:3,自引:0,他引:3
微流控技术及微流控器件是近年来发展迅速的多学科交叉研究领域.相比于传统方法, 微流控技术能够实现对微量多相流体的精准操控, 可应用于化学分析、先进材料合成、蛋白质结晶、单细胞培育及检测、信息处理等领域. 该文回顾微流控器件中的多相流动现象, 概述其所涉及的流体力学机理,阐述实现多相微流控的各种方法, 并分析多相微流控技术的应用现状及面临的挑战, 最后总结针对多相微流动问题的数值模拟方法和实验测量技术, 展望多相微流控器件的研究方向及应用前景. 相似文献
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<正> 1 引言 90年代的开始,正是对工业和环境流体力学进行综述的适当时候,因为在这10年里,将有许多流体流动问题有待解决,这些问题就是全世界都在关注的经济发展问题,人民生活质量问题,以及全球环境问题。此外,很可能,流体力学研究及其应用的方向,同其他科学和技术一样,由军事装备的设计及其在战争中的使用而引起的问题,将趋于减少;军事技术方面取得的进展,可能在许多场合应用于工业和环境流体力学(IEFM)提出的重要问题。 相似文献
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以压力为基本求解变量数值模拟粘性超、跨音速流动 总被引:1,自引:0,他引:1
应用以压力为基本求解变量的SIMPLE方法 ,对一双喉喷管中的层流超音速流动和一扩压器中的紊流跨音速流动进行了数值计算。计算结果显示 ,本文的计算结果与文献数据及实验结果相符很好。表明本文方法对可压缩流动有很高的模拟精度。进而表明经过可压缩推广的SIMPLE方法适用于任何马赫数的流动计算 相似文献
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流体力学在制浆造纸工程中的应用 总被引:3,自引:0,他引:3
造纸工业是流体力学的应用领域之一.本文从纸浆流动机理、湍流理论在纸页成形中的作用,中浓纸浆的流体化及涂料流变学等几方面讨论了流体力学在轻工业中的应用. 相似文献
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数值模拟方法在体液流动研究中的应用与展望 总被引:3,自引:0,他引:3
计算流体力学的数值模拟技术产生于20世纪60年代,现已成功地应用到众多科学研究与工程设计领域. 从20世纪80年代开始,虽已有不少研究工作开始利用CFD方法与计算机技术对人体的血流、气管中的气流、胆汁流等流动进行数值模拟与分析,但并没有与器官功能分析和病理分析及临床应用紧密联系. 近十几年来,这方面的工作已经取得了长足的进步和发展,模拟出了譬如脑血管、颈动脉、心血管等复杂血管流动,甚至整个肺泡的活动,得到了非常有病理意义和临床价值的图像.本文介绍和评述计算人体流体动力学的历史,发展和已经取得的成果. 相似文献
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二维轴对称耦合流动问题的解析解及应用 总被引:4,自引:0,他引:4
耦合流动问题与矿井开采中许多重要工程问题有密切联系:基于 Biot 三维固结理论导出了平面轴对称耦合流动与非耦合流动的场方程,得到了给定势问题的解析解.对耦合和非耦合两种情况进行了比较,并介绍了其在采矿工程中的应用. 相似文献
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The temperature and the flow field of thermo-convective liquid flows are visualized using cholesteric liquid crystal material as tracer particles. This type of tracers offers the scientifically valuable feature of measuring the flow and the temperature field simultaneously. Three thermoconvective flow configurations have been investigated successfully using liquid crystals. The results are discussed in some detail. It turns out that the liquid crystal technique is a valuable tool for thermo-convective liquid flow analysis. 相似文献
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This paper presents a control-volume-based finite difference method in non-orthogonal curvilinear coordinates on a local basis in which the vectors and tensors are all based on the general curvilinear coordinates for buoyant flow calculations in arbitrary three-dimensional geometries. The governing equations are transformed from Cartesian co-ordinates into generalized curvilinear co-ordinates. After integrating the set of equations for the control volumes, the finite difference equations are then formulated by a proper treatment of the heat flux and stress tensors and by incorporating the QUICK scheme for the convective terms. The solution procedure then follows the one for three-dimensional Cartesian co-ordinates. Examples are given in problems of natural convection in such three-dimensional enclosures as parallelepiped enclosures and horizontal closed cylinders with differentially heated ends. In the latter case, important applications have been found in crystal growth by means of chemical vapour deposition in a cylindrical ampoule, in which uniform heat fluxes along the two ends are required in order to produce high-quality crystals. Special attention is given to the insertion of baffles in the cylinder to improve the recirculating flow patterns near the two ends. 相似文献
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Viscous effects in liquid encapsulated liquid bridges 总被引:3,自引:0,他引:3
An analytical derivation of the surface deflections and the streamfunctions for the flow inside a liquid encapsulated liquid bridge has been derived using an asymptotic expansion about a small capillary number. The model assumes an initially flat and cylindrical interface under the assumption that the densities of both fluids are equal. To simplify the analysis, the top and bottom walls are assumed to be stress-free and the Reynolds number is assumed to be negligible. Flow is generated either by a moving outer wall (shear-driven flow) or by applying a temperature difference across the top and bottom walls (Marangoni-driven flow). The resulting equations show that for the shear-driven flow, as the viscosity ratio increases, the surface deflections increase monotonically. For the Marangoni-driven flow there exist values of the viscosity ratio where the surface deflections reach a minimum and then switch signs. This investigation shows that it may be possible in more realistic systems to use an outer encapsulating liquid of the proper viscosity ratio to stabilize the liquid–liquid interface during float zone crystal growth. 相似文献
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The effect of convective flow on a spherical crystal growth in the undercooled melt with a moderate far field flow is studied. The asymptotic solution of the evolution of the interface of the spherical crystal growth is obtained by the matched asymptotic expansion method. The analytic result shows that the convective flow in the undercooled melt has a strong effect on the evolution of spherical crystal growth. The convective flow induced by the far field flow makes the interface of the growing spherical crystal enhance its growth velocity in the upstream direction of the far field flow and inhibit growth in the downstream direction, and the interface of the decaying spherical crystal further decay in the upstream direction and inhibit decay in the downstream direction. The maximum growth velocity of the interface of the spherical crystal influenced by the far field flow is obtained. 相似文献
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数值分析结果表明,外加磁场可以改变熔融半导体中的流型,几千高斯的磁场可以显著地减小熔体的流动,但对温度场影响不大。 相似文献
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数值分析结果表明,外加磁场可以改变熔融半导体中的流型,几千高斯的磁场可以显著地减小熔体的流动,但对温度场影响不大。 相似文献
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It has been known for decades that crystal stress directions move toward the vertices of the single crystal yield surface (SCYS) during plastic flow of polycrystalline solids to satisfy the deformation compatibility among crystals. The alignment of crystal stress with a SCYS vertex is affected not only by plastic anisotropy, but also by other factors such as elastic anisotropy, loading direction, and grain interactions. Among the factors contributing to the degree of alignment, the effect of phase interactions on the crystal stress evolution during plastic flow has not been extensively investigated. In this research, the effect of phase interactions on the crystal stress direction evolution is investigated using simulations of an elastoplastically deforming two-phase (Cu/Fe) polycrystalline solid calibrated to a neutron diffraction experiment. By mapping the simulated crystal stresses over the crystal orientation space, crystal-orientation-dependent nonuniform partitioning of the crystal stress between phases can be observed. An analysis of the distribution of angles between the SCYS vertex and the crystal stress based on the simulation of the two-phase material shows that the crystal stress evolution pattern during plastic flow is strongly affected by phase interactions. These interactions result in low alignment and greater dispersion angles between the crystal stresses and SCYS vertices, particularly in the strong phase. 相似文献
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Both a real time optical interferometric experiment and a numerical simulation of two-dimension non-steady state model were employed to study the growth process of aqueous sodium chlorate crystals. The parameters such as solution concentration distribution, crystal dimensions, growth rate and velocity field were obtained by both experiment and numerical simulation. The influence of earth gravity during crystal growth process was analyzed. A reasonable theory model corresponding to the present experiment is advanced. The thickness of concentration boundary layer was investigated especially. The results from the experiment and numerical simulation match well. 相似文献
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Experiments are reported in which the heat flux distribution near a single circular, sonic transverse jet on a flat plate
exposed to a hypersonic (Mach 6.7) freestream flow was quantitatively measured using thermochromic liquid crystals. The freestream
conditions were such that the boundary layer growth on the plate ahead of the jet was laminar. The results indicate that the
interaction of the jet with the freestream flow created a complex flowfield with regions of separation and reattachment which
caused localised enhancements to the heat flux upstream and to the side of the jet, the magnitudes of which were sensitive
to both jet plenum pressure and jet gas composition.
Received 28 August 1996 / Accepted 6 June 1997 相似文献