共查询到18条相似文献,搜索用时 293 毫秒
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无挡板涡轮桨搅拌槽内湍流流动的分离涡模拟 总被引:1,自引:0,他引:1
采用分离涡模型对无挡板涡轮桨搅拌槽内的湍流流动进行了研究,重点分析了流场结构和速度分布,以检验该模型模拟搅拌槽内流体流动的有效性和正确性. 为了加快收敛,先采用标准k-e模型进行稳态流场计算,并以此结果为初始值进行分离涡模拟. 与现有文献大涡模拟及实验结果对比表明,分离涡模型能捕捉槽内流体的瞬时流动特征,获得的时均速度分布与大涡模拟及实验结果吻合较好,其中对切向速度分布的预测误差不超过7%,对径向速度分布的预测精度则低一些,局部误差接近12%. 分离涡模型适用于无挡板涡轮桨搅拌槽内湍流流动的模拟,能获得与大涡模拟相近的结果,且计算量更小(约为大涡模拟的1/3). 相似文献
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根据搅拌槽内的流动呈各向异性的特点 ,引入适用于强旋转流场的各向异性k -ε湍流模型 ,用改进的内外迭代法对有挡板的Rushton桨搅拌槽进行了整体数值模拟 .利用文献中对搅拌槽内流场测定结果 ,给出了适用于Rushton桨搅拌槽的各向异性湍流黏度系数值 .模拟计算得到了搅拌槽内的流场分布和脉动速度分布 ,并同标准k -ε湍流模型计算结果及文献数据进行比较 .结果表明 ,各向异性k -ε湍流模型能成功反映Reynolds应力、湍流动能等湍流特征量 ,明显优于标准k -ε湍流模型 . 相似文献
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为研究轴流桨搅拌槽内完全湍流状况,采用相位多普勒粒子分析仪(PDPA)对MK和ZHX搅拌器进行流场测试,得到不同工况下的时均速度场分布.应用渐近不变性方法,选取适当的特征尺度,给出挡板处壁面射流的轴向速度相似剖面,确定用于评定槽内完全湍流界限的轴向速度分布曲线,建立了搅拌雷诺数与搅拌槽内完全湍流流动达到的高度之间的线性关系.结果表明,非全槽完全湍流状态下,槽上部会出现过渡流区;随雷诺数的增大,搅拌槽内完全湍流流动达到的高度增大;不同型式搅拌器的完全湍流流场所需的雷诺数不同,单层桨搅拌槽内达到全槽完全湍流需要很大的搅拌功率. 相似文献
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各向异性k-ε湍流模型在Rushton桨搅拌槽三维流场整体数值模拟中的应用 总被引:2,自引:0,他引:2
根据搅拌槽内的流动呈各向异性的特点,引入适用于强旋转流场的各向异性k-ε湍流模型,用改进的内外迭代法对有挡板的Rushton桨搅拌槽进行了整体数值模拟.利用文献中对搅拌槽内流场测定结果,给出了适用于Rushton 桨搅拌槽的各向异性湍流黏度系数值.模拟计算得到了搅拌槽内的流场分布和脉动速度分布,并同标准k-e湍流模型计算结果及文献数据进行比较.结果表明,各向异性k-ε湍流模型能成功反映Reynolds应力、湍流动能等湍流特征量,明显优于标准k-ε湍流模型. 相似文献
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用粒子成像测速(PIV)技术对传统框式桨、传统框式组合桨和新型框式组合桨的流动特性进行研究,对比了三种框式桨在相同工况下搅拌槽内的速度、流型和湍动能。结果表明:传统框式桨搅拌槽内流体流动以水平环流为主,在框式桨上方和框式桨中间区域流体流动不充分;传统框式组合桨搅拌槽内框式桨上方由于二折叶桨的作用使得框式桨上部流体流速变大,槽内流体上下部的流动得到加强,但在框式桨中心区域依旧存在流动死区;新型框式组合桨搅拌槽内两层桨叶间的连接流得到了加强,框式桨底部和中间区域物质和能量的交换更加充分。在考察的三种框式桨中,新型框式组合桨的混合效果更好。研究结果可为新型框式组合桨应用于化工合成工业中提供参考。 相似文献
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Masanori Yoshida Yuma Wakura Kazuaki Yamagiwa Akira Ohkawa Shuichi Tezura 《Journal of chemical technology and biotechnology (Oxford, Oxfordshire : 1986)》2010,85(7):1017-1022
Liquid‐phase mixing is a common operation, often performed in vessels using mechanically rotating impellers. To enhance axial mixing the vessels are generally equipped with baffles; however, in industries where cleaning the vessel interior is a major concern, i.e. food and pharmaceuticals, and crystallization, where baffles can disturb particle growth, unbaffled vessels are preferred. One method of agitation in unbaffled vessels is an impeller that periodically changes either the direction or rate of rotation: so‐called unsteady rotation. For use in an enhanced agitation vessel, an agitation technology using an unsteady forward–reverse rotating impeller in an unbaffled vessel was investigated. Such unsteady agitation is expected to enhance mixing. However, knowledge of the liquid flows in such an apparatus remains elusive. Thus an aim of this work was to characterize the circulation flow in such a system. Circulation by a disk turbine impeller with six flat blades was studied through examination of tracer particle trajectories. Images showing flow patterns with the forward–reverse rotating impeller resembled those obtained with a unidirectionally rotating impeller in a baffled vessel. The pattern was characterized by a circulation loop whose pathway exits from the impeller rotational region and returns to that region past the wall and bottom of the vessel. Time‐series particle tracking velocimetry (PTV) images obtained during one forward–reverse rotation of the impeller showed that the flow near the vessel wall reduced the periodic fluctuation downstream and that a flow that was almost independent of time was induced near the vessel bottom. For the flow from the bottom to the impeller, unsteadiness was provided by proximity to the impeller. Based on the intensity distribution of the unsteady flow produced by this type of forward–reverse rotating impeller within the vessel, the unsteady flow was shown to have the potential to reach the region near the vessel wall. Copyright © 2010 Society of Chemical Industry 相似文献
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半圆管曲面涡轮搅拌槽内混合特性的数值模拟 总被引:4,自引:3,他引:1
在商业化软件ANSYS CFX 10.0平台上,采用多重参考系法来解决挡板与桨叶之间的相对转动问题,由标准k-ε模型对半圆管曲面涡轮搅拌槽内流动和混合过程进行了详细的数值模拟,本模拟所得的功率准数和设计值以及相关文献值吻合良好。结果表明:当搅拌桨离底距离由搅拌槽直径的1/2处变为1/3处时,搅拌槽内的流型均为典型的“双循环流型”,而当搅拌桨离底距离由搅拌槽直径的1/3处降低至1/6处时,槽内流型由典型的“双循环流型”转变为“单循环流型”;通过对不同时刻不同桨叶离底距离下的示踪剂浓度分布图分析表明槽内的混合过程与流动场密切相关;加料点位置对于最终的流场混合效果有着显著影响,对于混合时间数据的采集应注意不同加料位置时监测点的选取。CFD模拟结果表明本文所采用的模型可以很好的预测半圆管曲面涡轮搅拌槽内的混合特性,为进一步改进和优化半圆管曲面涡轮的设计提供了一定的参考。 相似文献
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对应用于聚乙烯聚合反应中的三叶后掠-HEDT组合桨的搅拌釜内流场进行了模拟研究,分析组合桨的离底距C 1、桨间距C 2以及转速N的变化对搅拌釜内流场的影响,利用PIV实验对模拟结果进行了验证;将该组合桨与三叶后掠-六直叶圆盘涡轮组合桨进行了模拟对比研究。结果表明:当桨间距与釜内径的比为0.35时,釜内桨叶间的流体流动效果最好,该条件下能够改善搅拌釜上层流体的速度分布;当离底距与釜内径的比值为0.29时,组合桨下方出现了整体的环流,有利于釜底流体的混合;桨叶转速N=90 r/min时釜内流体速度分布均匀,同时上层HEDT桨叶产生的射流方向趋于水平。两种组合桨的对比研究表明:二者流型相近,但前者搅拌功率能够得到明显降低。研究结果可为三叶后掠-HEDT组合桨在聚乙烯聚合反应釜中的工程应用提供参考。 相似文献
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P. Guiraud J. Costes J. Bertrand 《Chemical engineering journal (Lausanne, Switzerland : 1996)》1997,68(2-3)
An experimental approach is proposed for the measurement of the local behaviour of continuous and dispersed phases in a stirred suspension at low particle concentrations (0.5 vol.%). The basic principle involves the simultaneous measurement of the local velocity and particle size with a phase Doppler velocimeter and the separation of the data obtained from large particles (representing the dispersed phase) and very small particles (representing the motion of the continuous liquid phase).This technique was applied to the investigation of a fully baffled cylindrical vessel, with a flat bottom, stirred by an industrial axial propeller. The diameters of the vessel and the propeller and the vertical clearance were 0.3 m, 0.14 m and 0. l m respectively. The liquid was water and spherical glass particles were used as the dispersed phase.In the absence of particles, the circulation pattern created by the propeller in the middle plane between two baffles revealed a major circulation loop in the lower part of the vessel and a minor contra-rotative loop in the wall surface corner. The calculated pumping coefficient, circulation flow number, non-dimensional time of renewal and circulation time were 0.62, 0.89, 11.76 and 8.15 respectively. The tangential velocities remained at values of less than 15% of the impeller tip velocity in the plane of the measurements.Axial, radial and tangential mean and root-mean-square velocities for the carrier liquid phase and particles were measured in the two-phase flow, using particles with a mean diameter of 253 μm. These measurements showed that the particles lagged behind the liquid phase in the upward parts of the flow field, but were ahead in some downward parts. The root-mean-square axial velocities obtained for the particles were always greater than these obtained for the continuous phase. Non-homogeneities in the suspension were observed by the local mean diameter field. The effects of the stirring rate and size of the particles were also checked in the upward part of the flow in the vessel. 相似文献
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Computational fluid dynamics simulation is becoming an increasingly useful tool in the analysis and design of simultaneous
saccharification fermentation (SSF) and saccharification followed by fermentation process (SFF). To understand and improve
mixing and mass transfer in a highly viscous non-Newtonian system, it was necessary to simulate the flow behavior in this
bench scale bioreactor (BioFlo 3000). This study focused on designing a high concentration medium agitation system for such
a process using the commercial computational fluid dynamics package Fluent (V. 6.2.20) and its preprocessor Mixsim (V. 2.1.10).
The objective of this study is to compare performance of various designs of a bioreactor and identify the flow pattern and
related phenomena in the bench scale tank. The configuration of the physical model for simulating a mixing tank with a Rushton
impeller consists of an ellipsoidal cylindrical tank with four equally spaced wall mounted baffles extending the vessel bottom
to the free surface, stirred by a centrally located six-blade Rushton turbine impeller. Simulations were performed with the
original and a modified design in which the lower bottom shaft mounted a Lightnin A200 impeller. The results suggest that
there is a potential for slow or stagnant flow between top impellers and bottom of the tank region, which could result in
poor nitrogen and heat transfer for highly viscous fermentations. The results also show that the axial velocity was significantly
improved for the modified geometry in the bottom of the tank. 相似文献
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Rates of liquid‐solid mass transfer at a packed bed of Raschig rings fixed to the wall of a stirred tank were measured by a technique which involves the diffusion‐controlled dissolution of copper in acidified dichromate. Variables studied were impeller rotation speed, impeller geometry, Raschig ring diameter, bed thickness, presence of baffles, physical properties of the solution, and effect of superimposed flow. Mass transfer data for the batch reactor were correlated by a dimensionless equation. For a given set of conditions, the radial‐flow impeller was found to produce higher rates of mass transfer than the axial‐flow impeller. The presence of baffles increased the rate of mass transfer inside the bed. Applications of the suggested reactor in conducting different diffusion‐controlled liquid‐solid reactions were evaluated. 相似文献