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垂直管内油水两相流局部相分布特性实验研究 总被引:1,自引:0,他引:1
应用双头电导探针测量系统,对垂直上升管内油水两相分散流局部相分布特性进行了系统测量。得到了油水两相分散流的局部含油率分布类型图。研究结果表明低折算水速和低折算油速条件下,局部含油率在实验段截面上呈抛物线型局部分布特征,局部最大值出现在实验段中心区域。随折算油速增大,油滴受到横向力如升力的作用,逐渐向实验段壁面区域迁移,形成局部含油率的壁面峰值分布特性。当折算水速大于0.8 m/s时,局部含油率在实验段截面上呈均匀分布。 相似文献
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旋流两相流动的DSM—PDF两相湍流模型 总被引:1,自引:1,他引:0
本文提出了气相雷诺应力方程模型和颗粒概率密度输运方程模型相结合而构成的DSM—PDF两相湍流模型,并用该模型和k-ε-Kp模型模拟了文献中测量的旋流数为0.47的旋流突扩气粒两相流动.和测量结果的对照表明,两模型都能较好地模拟族流数不高的两相流动平均速度场,但DSM—PDF模型可以揭示出两相湍流的各向异性,因此有预报强旋两相流动的潜力. 相似文献
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本文用气粒两相流双流体模型,气相湍流的k-ε模型及颗粒湍能k_p输运方程模型,即k-ε-k_p模型,对大速差射流燃烧室内三维回流湍流气粒两相流动进行了模拟,给出了各纵剖面内气相及颗粒时均轴向速度分布、气粒两相各自的湍流强度分布、颗粒轴向质量流分布及各横截面内气粒两相时均周向速度分布。预报结果与激光多普勒仪测量结果定性上类似,特别是正确地预示出实验中观测到的流场某些区域内颗粒湍流度大于气相湍流度的现象,又一次表明,全面计及颗粒湍能输运过程的模型比经典的局部追随的颗粒湍能代数模型更合理。 相似文献
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本文提出了两相流气相湍流变动的双时间尺度耗散模型,包括气相耗散率的双时间尺度耗散模型和两相速度关联的双时间尺度各向异性耗散模型。用所提出封闭模型模拟了旋流数为0.47的气粒两相流动,发现所提出的湍流变动模型对气相脉动速度的预报结果比原有的单时间尺度模型的预报结果有明显的改进,但是颗粒尾涡的作用仍然需要进一步研究。 相似文献
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湍流两相流动及燃烧的模拟中常用的各个子模型,如k-8气相湍流模型,Hinze-Tchen颗粒湍流模型及EBU-Arrhenius湍流燃烧模型等,不能正确地反映旋转流与浮力流的各向异性,颗粒气体的湍流相互作用及有限反应率与湍流间相互作用,这些模型在性质上的不同造成理论上不协调和数值解法及程序编制上的不便,本文按作者及其同事们多年的研究经验,把单相湍流代数应力模型的思路推广于有反应两相流中,用统一的关联矩封闭方法处理气相湍流,颗粒湍流及气相湍流燃烧,以便更合理而经济地解决实际工程问题。 相似文献
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利用有机玻璃管、吸管、泡沫球等简易材料自制了演示流体压强与流速关系的实验装置。该装置有效地解决了小球随意滚动、吹气方向不固定等问题。实验用泡沫球代替乒乓球,并将其放置在玻璃管中放置,使实验过程不受外界空气影响,且较轻的泡沫球更易运动,实验效果更明显。利用该原理还自制了模拟非洲草原犬鼠洞穴的演示装置,有趣且直观地演示了犬鼠洞穴中的气体流向。 相似文献
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1引言圆柱绕流是流动与传热领域的基本流动现象,也是历史悠久的研究课题。“经过多年的努力,人们已经获得了圆柱绕流的基本图象,积累了相当丰富的实验及分析资料,但有许多问题至今仍然是不解之谜[1]。在这些问题中,亚临界绕流时的绕流阻力具有重要的意义。在能源、化工、环保等工业领域大量存在的圆管外绕流,其绕流雷诺数大多在104数量级,为典型的亚临界绕流工况。在该雷诺数范围内,圆柱绕流阻力系数Cd≈1.2,处于较高水平。降低亚临界绕流圆柱的流动阻力将产生工业上量大面广的节能效益。为探索实用的流动减阻技术,必须对亚临界… 相似文献
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A mathematical model was developed to simulate two-phase gas-dispersed flow moving through a pipe with axisymmetric sudden
expansion. In the model, the two-fluid Euler approach was used. The model is based on solving Reynolds-averaged Navier — Stokes
equations for a two-phase stream. In calculating the fluctuating characteristics of the dispersed phase, equations borrowed
from the models by Simonin (1991), Zaichik et al. (1994), and Derevich (2002) were used. Results of a comparative analysis
with previously reported experimental and numerical data on two-phase flows with separation past sudden expansion in a plane
channel and in a pipe are given.
This work was supported by the President of the Russian Federation through the Foundation for Young Candidates of Sciences
under Grant MK-186.2007.8 and by the Russian Foundation for Basic Research (Grants Nos. 05-08-33586 and 06-08-00967). 相似文献
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在Ma=3.0的超声速风洞中, 分别对上游边界层为超声速层流和湍流, 压缩角度为25°和28°的压缩拐角流动进行了实验研究. 采用纳米粒子示踪平面激光散射(NPLS)技术获得了流场整体和局部区域的精细结构, 边界层、剪切层、分离激波、回流区和再附激波等典型结构清晰可见, 测量了超声速层流压缩拐角壁面的压力系数. 从时间平均的流场结构中测量出分离激波、再附激波的角度和再附后重新发展的边界层的增长情况, 通过分析时间相关的流场NPLS图像, 可以发现流场结构随时间的演化特性. 实验结果表明: 在25°的压缩角度下, 超声速层流压缩拐角流动发生了典型的分离, 边界层迅速增长失稳转捩, 并引起一道诱导激波, 流场中出现了K-H涡、剪切层和微弱压缩波结构, 而超声速湍流压缩拐角流动没有出现分离, 湍流边界层始终表现为附着状态; 在28° 的压缩角度下, 超声速层流压缩拐角流动进一步分离, 回流区范围明显扩大, 诱导激波、分离激波向上游移动, 再附激波向下游移动, 分离区流动结构复杂, 相比之下, 超声速湍流压缩拐角流动的回流区范围明显较小, 边界层增长缓慢, 流场中没有出现诱导激波、K-H涡和压缩波, 流动分离区域的结构也相对简单, 但分离激波的强度则明显更强.
关键词:
压缩拐角
层流
湍流
流动结构 相似文献
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Langevin simulations are preformed on the depinning dynamics of fluid monolayer on a quenched substrate. With increase in the strength of the substrate, we find for the first time a crossover from elastic crystal to smectic flows as well as a crossover from smectic to plastic flows above the depinning. A power-law scaling relationship can be derived between the drift velocity and the driving force for both the elastic crystal and smectic flows, but fails to be obtained for the plastic flow. The power-law exponents are found to be no larger than 1 for the elastic crystal flow and larger than 1 for the smeetic flow. The critical driving force and the averaged intensity of Bragg peaks remain invariant basically in the regime of smectic flow. A sudden increase in the critical driving force is observed within the crossover from the smeetic to plastic flows, and the averaged intensity of Bragg peaks shows sudden decreases within the crossovers both from the elastic crystal to smectic flows and from the smectic to plastic flows. The results are helpful for understanding the slip dynamics of fluids on a molecular level. 相似文献
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Langevin simulations are preformed on the depinning dynamics of fluidmonolayer on a quenched substrate. With increase in the strength of thesubstrate, we find for the first time a crossover from elastic crystal tosmectic flows as well as a crossover from smectic to plastic flows above thedepinning. A power-law scaling relationship can be derived between the driftvelocity and the driving force for both the elastic crystal and smecticflows, but fails to be obtained for the plastic flow. The power-lawexponents are found to be no larger than 1 for the elastic crystal flow andlarger than 1 for the smectic flow. The critical driving force and theaveraged intensity of Bragg peaks remain invariant basically in the regimeof smectic flow. A sudden increase in the critical driving force is observedwithin the crossover from the smectic to plastic flows, and the averagedintensity of Bragg peaks shows sudden decreases within the crossovers bothfrom the elastic crystal to smectic flows and from the smectic to plastic flows.The results are helpful for understanding the slip dynamics of fluids on a molecular level. 相似文献
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以Taitel 和Barnea(1998,1999)提出的段塞流跟踪模型为基础,进一步考虑加速压降的影响,建立了新的瞬态段塞流跟踪模型,并采用面向对象技术编制了数值模拟软件,实现了数值跟踪。计算结果与King等的段塞流气体流量瞬变实验数据对比表明,瞬态跟踪模型较好地预测了气体流量上升造成的段塞流压力“过升”现象,以及长液塞的出现;当气体流量下降时出现的压力“过降”现象和短暂分层流现象也由模型准确预测,分析认为,由于段塞流压降远高于分层流型,因此大部分液塞消失而出现的短暂分层流导致了压力过降。 相似文献