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二维鼓泡床内气泡尺寸分布的实验与CFD模拟 总被引:3,自引:2,他引:1
在有机玻璃制成的二维鼓泡床(0.20m×0.02m×2.00m)内,采用摄像法对空气-自来水的气液两相体系的气泡尺寸分布进行了考察。以商业计算流体力学软件ANSYS CFX 10.0为平台,在双流体模型的基础上,采用k-ε湍流模型和GRACE曳力模型对气液鼓泡床内流体动力学行为进行了多相流CFD数值模拟。结果表明 MUSIG(Multiple Size Group)模型实现了对多气泡体系内气泡尺寸分布特性的考察,气泡尺寸分布的模拟结果与实验结果吻合得较好,从而说明了考虑了气泡聚并破碎的MUSIG模型能很好地反映出鼓泡床内气泡尺寸分布特性。 相似文献
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引言 鼓泡床是一种重要的气液或气液固多相反应器.液体循环流动是鼓泡床的一个重要流体力学特征,从20世纪50年代人们就开始对此进行了比较系统的实验研究[1-6].这个特征对鼓泡床的流体返混行为、气含率、气液界面积以及传热传质系数都有很大影响,特别是液体返混行为可以由液体循环特性直接决定.如何准确地描述和预测鼓泡床中的液体流速沿径向的分布,关系到鼓泡床反应器的设计、放大和优化.因此,许多年来它一直是人们致力探讨的重要课题之一[7-8]. 相似文献
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本文分析了锥形鼓泡床内流型过渡、平均气含率及气含率轴向分布特性,考察了入口气体速度、静止液体(或淤浆)高度及淤浆浓度的影响,比较了与圆柱床的差异,结果表明对于鼓泡床内气体体积收缩的反应,用锥形床的冷态试验可以较精确地模拟其实际结果。 相似文献
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本文比较了目前常用的几种分布器,通过照像法观察了三种分布器(单孔板、多孔板和烧结金属板)上的气泡形成过程,然后测定了这三种分布器的干板压降和湿板压降,并就它们对水力学条件的影响进行了考察。其结果对鼓泡床内分布器的设计具有一定的参考价值。 相似文献
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能量最小多尺度(energy-minimization multi-scale,EMMS)方法已经被应用于气液体系中群平衡(population balance model,PBM)模型的改进。EMMS模型可计算气泡破碎聚并过程的能量,进而获得聚并速率的修正因子。应用这一模型对高气速鼓泡塔进行了模拟计算,并进一步对比了均一尺径模型、CFD-PBM模型以及CFD-PBM-EMMS模型的模拟结果与实验数据。结果表明,在高表观气速条件下,基于EMMS方法的群平衡模型可以更加准确地预测鼓泡塔中不同高度的气泡尺径分布和轴向液速,同时提高了对整体气含率和局部气含率的模拟准确性。在表观气速为0.16 m·s-1和0.25 m·s-1时,CFD-PBM-EMMS模型对气泡尺径分布的预测精度更高,同时整体气含率模拟的相对误差下降为5%和15%,局部气含率模拟平均相对误差下降为8%和17%。 相似文献
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对圆柱形鼓泡塔反应器内的气液两相流动进行了三维瞬态数值模拟,模拟的表观气速范围为0.02~0.30 m8226;s-1; 模拟采用了双流体模型,并耦合了气泡界面密度单方程模型预测气泡尺寸,该模型考虑了气泡聚并与破碎对气泡尺寸的影响。液相湍流采用考虑气相影响的修正k-ε模型,两相间的动量传输仅考虑曳力作用。模拟获得了轴向气/液相速度分布、气含率分布、湍流动能分布以及气泡表面面积密度等,对部分模拟结果与实验值进行了定量比较,结果表明模拟结果与实验结果吻合较好。 相似文献
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采用CFD-PBM耦合方法,对高表观气速下的气?液鼓泡塔进行模拟,得到气含率、轴向液速及气泡尺寸。系统性对比求解群平衡方程(PBE)的不同方法:离散法(20 bins)和QMOM(包括四阶QMOM和六阶QMOM)。模拟结果与文献中的实验数据的对比结果表明,离散法和QMOM均能合理预测气含率、轴向液速、平均气泡大小和气泡尺寸分布。但QMOM比离散法节约2~3倍的计算成本。对于QMOM,使用四个矩能准确描述气相的演化。使用四阶QMOM和六阶QMOM得到的结果非常相似。利用QMOM的低阶矩可以快速有效地重构出单峰气泡尺寸分布。 相似文献
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This article presents the distribution of the local void fraction (α) in a mock-up bisectional bubble column with a diameter of 0.63 m. Owing to the lack of such data in the literature, α was investigated experimentally using a microresistivity (R) probe and a phase discrimination procedure based on the probe signal. The two-phase mixture that consisted of air and tap water was measured at 342 nodes in the vertical half-section plane of the column. Relatively small differences between the volume-integrated local values of α and the measured total gas holdups showed reasonably good agreement under all conditions. Experimental data were used for validation of a bubble column numerical model for a low hydrodynamic regime with commercial computational fluid dynamics (CFD) code. The difference between the CFD calculated total gas holdup and the experimentally measured mean value is 8.8%, while some differences in the local void fraction distributions were found in the lower part of the column. © 2019 American Institute of Chemical Engineers AIChE J, 65: 1186–1197, 2019 相似文献
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Knowledge of bubble size distribution (BSD) is critical for controlling mass transfer and reaction in bubble column reactors. Installation of internals further complicates this issue. The effects of internals on BSD were systematically investigated through experiments and computational fluid dynamics-population balance model simulations. The experiments show a bimodal distribution of the volume-based BSD except at low superficial gas velocity of 0.01 m/s. Addition of 20% internals increases the small-bubbles fraction, making the first BSD peak more evident. Correspondingly, the simulation reveals a prominent decrease of turbulent dissipation rate and turbulent kinetic energy. Moreover, while the unresolved turbulent kinetic energy dominates in the empty columns, the resolved portion becomes the major component in the presence of internals. This suggests that internals may redistribute turbulent kinetic energy in each scale, which provides more insights into the complex flow characteristics in the presence of internals and process intensification. 相似文献
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Performance of an ejector system in a two-phase downflow bubble column has been evaluated with respect to the energy dissipation during coaxial flow of liquid and gas in a parallel throat and divergent diffiser and during gas—liquid mixing in the column. Experiments were carried out in a 51.6 mm i.d. column with five different nozzles. Three systems, namely air—water, air-kerosene and air—paraffin were used. Correlations have been developed for predicting the ejector loss coefficient as well as mixing loss coefficient as a function of different physical and dynamic variables of the system. 相似文献