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微载体培养转瓶中的流体动力学研究:粒子跟踪测速法

Study of hydrodynamics in microcarrier culture spinner vessels: A particle tracking velocimetry approach.

作者信息

Venkat R V, Stock L R, Chalmers J J

机构信息

Department of Chemical Engineering, The Ohio State University, 140 W. 19th Avenue, Columbus, Ohio 43210-1180.

出版信息

Biotechnol Bioeng. 1996 Feb 20;49(4):456-66. doi: 10.1002/(SICI)1097-0290(19960220)49:4<456::AID-BIT13>3.0.CO;2-8.

DOI:10.1002/(SICI)1097-0290(19960220)49:4<456::AID-BIT13>3.0.CO;2-8
PMID:18623601
Abstract

Three-dimensional particle tracking velocimetry (3-D PTV), a modern, quantitative, visualization tool, has been applied to the characterization of the flow field in the impeller region of cell culture reactor vessels. The experimental system used here is a 250-mL microcarrier spinner vessel. The studies were conducted at three different agitation rates, 90, 150, and 210 rpm, corresponding to healthy, mildly damaging, and severely damaging shear intensities, respectively. The flow can be classified into three regions: a predominantly tangential (azimuthal) flow generated by the impeller; a trailing vortex region coming off the impeller tip; and a converging flow region close to the center of the vessel. The latter two are the regions of highest velocity gradients. Energy dissipation rates due to mean velocity gradients were also calculated to characterize the impeller stream. Local specific energy dissipation rates > 10,000 erg/(cm(3)sec) . have been measured. It is proposed that the critical regions for microcarrier culture damage due to impeller hydrodynamics are the trailing vortex region and the high energy converging flow region. Graphical representation of the mean velocity flow fields and the distribution of energy dissipation rates in the impeller region are also presented here. The merits of using the dissipation function (measure of specific energy dissipation rate) as a possible scale-up parameter are also discussed. (c) 1996 John Wiley & Sons, Inc.

摘要

三维粒子跟踪测速技术(3-D PTV)是一种现代的、定量的可视化工具,已被应用于表征细胞培养反应器容器叶轮区域的流场。这里使用的实验系统是一个250毫升的微载体旋转培养容器。研究在三种不同的搅拌速率下进行,分别为90、150和210转/分钟,对应于健康、轻度损伤和重度损伤的剪切强度。流动可分为三个区域:由叶轮产生的主要为切向(方位角)流动;从叶轮尖端流出的尾涡区域;以及靠近容器中心的汇聚流动区域。后两个区域是速度梯度最高的区域。还计算了由于平均速度梯度引起的能量耗散率,以表征叶轮流。已测量到局部比能量耗散率>10,000尔格/(立方厘米·秒)。有人提出,由于叶轮流体动力学导致微载体培养损伤的关键区域是尾涡区域和高能量汇聚流动区域。这里还给出了叶轮区域平均速度流场的图形表示以及能量耗散率的分布。还讨论了使用耗散函数(比能量耗散率的度量)作为可能的放大参数的优点。(c)1996约翰·威利父子公司

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