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三维粒子成像测速(PIV)中粒子像斑定位的透视成像原理,方法及其可确定性 总被引:4,自引:1,他引:3
在三维粒子成像测速(PIV)方面,可运用体积光照明同时从不同光轴用多个照相机获得PIV图像,如何根据这些不同光轴获得的PIV图像确定出粒子物点的空间位置是实现三维粒子成像测速的前提。基于此,本文提出了根据多幅不同光轴的PIV图像的粒子像斑实现粒子物点三维定位的透视成像定位原理和方法,精确确定透视平面与透视中心在空间的位置是实现粒子物点三维定位的关键,直接测定透视中心(照相机的光学中心)和透视平面在 相似文献
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基于BICC算法的PIV技术 总被引:12,自引:0,他引:12
对基于BICC(BinaryImageCross-Correlation)算法的PIV(ParticleImageVelocimetry)技术的原理进行了较详细的介绍.以封闭的正方形容器内的旋转流场为例,用计算机模拟检验了BICC算法的可靠性,最后利用PIV技术对阀腔内真实流场进行了测量.结果表明,BICC算法能有效地进行图像粒子的识别,利用该算法可以得到精确的PIV测量结果. 相似文献
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基于双流体模型,采用跟踪法处理火焰内边界,TVD格式计算气相激波,MacCo-mack格式计算颗粒相流场,对两相可燃介质中火焰诱导激波现象进行了理论分析与实验模拟,研究了颗粒相参数对火焰诱导激波现象的影响。 相似文献
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强旋湍流气-固两相流动的颗粒随机轨道法模拟 总被引:4,自引:1,他引:4
应用颗粒随机轨道模型,并与一种新的代数Reynolds应力模型相结合,对新型煤粉涡旋燃烧炉内强旋湍流气。固两相流动进行了数值模拟。得到了与实验相符合的颗粒相密度分布和质量流分布。计算结果表明,在涡旋燃烧炉内的强旋湍流流场中,外壁附近颗粒浓度最高,颗粒停留时间加长,气-固两相间滑移速度增大。 相似文献
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方管内气固两相流动速度的LDV测量 总被引:1,自引:0,他引:1
介绍了气固两相流动的LDV测试方法和有关技术,并给出了方管内网栅后气固两相流动的部分测试结果与分析。对于气相,给出了纯净气流(α=0)、平均粒径dp=350μm的颗粒(α=0.12%、0.21%、0.335%)存在时的气流在管内不同断面上时均速度分布情况及不同颗粒浓度时气流速度结构的比较;对于固相,给出了三种不同固相浓度时颗粒在管内不同断面上时均速度的分布情况,并对三种固相浓度时颗粒与气相的速度分布进行了比较。 相似文献
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在IPSAR算法基础上推导了适用于考虑液度变化影响的密相液固两相湍流流动数值计算的DIPSAR算法,并采用低雷诺数模型,对竖直上升管中密相液固两相湍流分别采用IPSAR算法和DIPSAR算法进行了数值计算,计算值与实测值较符合,计算结果的比较表明DIPSAR算法能更有效地预测密相液固两相湍流流动 相似文献
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旋转,弯曲,扩散流道中流固两相流场的数值模拟及其分析 总被引:1,自引:0,他引:1
本文简要介绍了旋转,弯曲,扩散流道中,液-固两相流流数值计算结果,进而从理论上分析了泵叶轮压力面遭受磨损和输送两相流时扬程度降低的原因。 相似文献
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Particle dispersion in a single-sided backward-facing step flow 总被引:8,自引:0,他引:8
The paper describes the particle dispersion in a single-sided backward-facing step flow. Particles of well-known sizes in the diameter range from 1 to 70 μm were suspended in an air flow and the particle motion over a step was measured by mean of a laser-Doppler anemometer. Thus, the local and integral flow quantities, i.e. the mean and turbulent velocity data could be measured precisely. In the experiments, monodispersed particle size distributions were used to exclude particle size related information ambiguity, known as triggering effects or size bias. The results of this study show qualitatively and quantitatively the difference in time-averaged particle dynamics for selected particle sizes in a backward-facing step flow. The experiments show, for different sizes, the changes in the particle velocity field in comparison with the velocity field of the continuous phase deduced from the 1 μm particles, and also imply the strong influences which different particle sizes have on flow data evaluation when size effects are not taken into account with particle-related optical measuring techniques. 相似文献
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The asymptotic and numerical investigations of shock-induced boundary layers in gas-particle mixtures are presented.The Saffman lift force acting on a particle in a shear flow istaken into account.It is shown that particle migration across the boundary layer leads tointersections of particle trajectories.The corresponding modification of dusty gas model isproposed in this paper.The equations of two-phase sidewall boundary layer behind a shock wave moving at aconstant speed are obtained by using the method of matched asymptotic expansions.Themethod of the calculation of particle phase parameters in Lagrangian coordinates isdescribed in detail.Some numerical results for the case of small particle concentration aregiven. 相似文献
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The interaction of a planar shock wave with a loose dusty bulk layer has been investigated both experimentally and numerically.
Experiments were conducted in a shock tube. The incident shock wave velocity and particle diameters were measured with the
use of pressure transducers and a Malvern particle sizer, respectively. The flow fields, induced by shock waves, of both gas
and granular phase were visualized by means of shadowgraphs and pulsed X-ray radiography with trace particles added. In addition,
a two-phase model for granular flow presented by Gidaspow is introduced and is extended to describe such a complex phenomenon.
Based on the kinetic theory, such a two-phase model has the advantage of being able to clarify many physical concepts, like
particulate viscosity, granular conductivity and solid pressure, and deduce the correlative constitutive equations of the
solid phase. The AUSM scheme was employed for the numerical calculation. The flow field behind the shock wave was displayed
numerically and agrees well with our corresponding experimental results.
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A three-dimensional particle tracking velocimeter (3-D PTV) was applied to air-flow measurement in a strongly curved U-bend
of a square cross-section. He-filled neutral-buoyant soap bubbles were employed as a flow tracer, and turbulent statistics
including all Reynolds stress components were measured. The pressure-induced secondary flow, of which magnitude reached about
30% of the bulk mean velocity, was observed. The present experimental result is mostly in good agreement with the LDA data
at higher bulk-mean Reynolds number taken by Chang et al. The effect of the secondary flow on the production mechanism of
turbulent kinetic energy as well as on the distributions of the invariants of stress anisotropy tensor was examined in detail.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
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The turbulent fluid and particle interaction in the turbulent boundary layer for cross flow over a cylinder has been experimentally
studied. A phase-Doppler anemometer was used to measure the mean and fluctuating velocities of both phases. Two size ranges
of particles (30μm–60μm and 80μm–150μm) at certain concentrations were used for considering the effects of particle sizes
on the mean velocity profiles and on the turbulent intensity levels. The measurements clearly demonstrated that the larger
particles damped fluid turbulence. For the smaller particles, this damping effect was less noticeable. The measurements further
showed a delay in the separation point for two phase turbulent cross flow over a cylinder.
The project supported by the National Natural Science Foundation of China 相似文献
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N. Angarita-Jaimes E. McGhee M. Chennaoui H. I. Campbell S. Zhang C. E. Towers A. H. Greenaway D. P. Towers 《Experiments in fluids》2006,41(6):881-891
We present the application of wavefront sensing to particle image velocimetry for three-component (3C), three-dimensional (3D) flow measurement from a single view. The technique is based upon measuring the wavefront scattered by a tracer particle and from that wavefront the 3D tracer location can be determined. Hence, from a temporally resolved sequence of 3D particle locations the velocity vector field is obtained. Two approaches to capture the data required to measure the wavefronts are described: multi-planar imaging using a distorted diffraction grating and an anamorphic technique. Both techniques are optically efficient, robust and compatible with coherent and incoherent scattering from flow tracers. The depth (range) resolution and repeatability have been quantified experimentally using a single mode fiber source representing a tracer particle. The anamorphic approach is shown to have the greatest measurement range and hence was selected for the first proof of principle experiments using this technique for 3D particle imaging velocimetry (PIV) on a sparsely seeded gas phase flow. 相似文献