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Using X-ray computed tomography to measure local gas holdup in a stirred tank reactor.

机译:使用X射线计算机断层摄影术测量搅拌釜反应器中的局部气体滞留量。

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Gas holdup is one of the most important hydrodynamic parameters needed for reliable design, performance estimation, and scale-up of stirred tank reactors (STRs). In the present work, local gas holdup is measured in an acrylic stirred tank reactor equipped with a Rushton impeller using X-ray computed tomography (CT) for many different operating conditions. Power consumption for different operating conditions is determined to identify various STR flow regimes. The gas holdup results obtained by X-ray CT imaging are presented as: (i) profiles along all 3 axes, (ii) plots of local gas holdup along the x-axis, (iii) average gas holdup for z-slice, and (iv) overall gas holdup for the imaging region. The high resolution of the X-ray CT system allows for the visualization of minor details such as recirculation zones behind the baffles. The results show that there are dramatic differences in gas dispersion depending on the flow regime. Completely dispersed conditions have a relatively constant holdup profile while flooded conditions have a parabolic shape with an increase in gas holdup towards the center of the tank. The CT slices show that there is very little visual difference between scans taken in the same operating regime, even though there are differences in impeller speed and gas flow rate. Average z-slice holdup values increase with increasing height from the impeller for the flooded condition, while the opposite occurs for the loaded and completely dispersed conditions. Local gas holdup conditions are sensitive to tank design, which are shown by differences in the x- and y-slices. Overall holdup values for the image region are determined and shown to increase as the impeller speed increases while holding Qg constant.
机译:气体滞留率是搅拌釜反应器(STRs)可靠设计,性能评估和按比例放大所需的最重要的流体力学参数之一。在本工作中,对于许多不同的操作条件,使用X射线计算机断层扫描(CT)在配备Rushton叶轮的丙烯酸搅拌釜反应器中测量局部气体滞留量。确定不同工作条件下的功耗以识别各种STR流量状态。通过X射线CT成像获得的气体滞留率结果表示为:(i)沿所有三个轴的分布图;(ii)沿x轴的局部气体滞留率图;(iii)z切片的平均气体滞留率;以及(iv)成像区域的整体气体滞留率。 X射线CT系统的高分辨率允许可视化较小的细节,例如挡板后面的回流区。结果表明,根据流态的不同,气体扩散存在巨大差异。完全分散的条件具有相对恒定的滞留曲线,而溢流条件则呈抛物线形状,朝向储罐中心的气体滞留率增加。 CT切片显示,即使叶轮速度和气体流速存在差异,在相同的工作方式下进行的两次扫描之间的视觉差异也很小。在满水情况下,平均z切片滞留值随叶轮高度的增加而增加,而在负载和完全分散的情况下则相反。局部气体滞留条件对气罐设计很敏感,这通过x切片和y切片的差异来显示。确定图像区域的总体保持率值,并显示其随着叶轮速度的增加而增加,同时保持Qg不变。

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