{"title":"Flow Past Large Obstructions Between Corotating Disks in Fixed Cylindrical Enclosures","authors":"Hiroshi Suzuki, J. Humphrey","doi":"10.1115/1.2819272","DOIUrl":null,"url":null,"abstract":"\n Numerical calculations have been performed for isothermal, laminar, three-dimensional flow past one or two fixed obstructions radially aligned and symmetrically located between a pair of disks corotating in a fixed cylindrical enclosure. The single-obstruction cases respectively model the influence on the flow of (a) a magnetic head arm support and (b) an air lock. The dual-obstruction cases model the simultaneous presence of these two objects. The air lock produces an interdisk cross-stream plane blockage of 62% while the two head arm supports produce blockages of 31% and 62%, respectively. For the cases with the air lock and arm support simultaneously present, the circumferential angle between them is fixed to 40° or 80°. Velocity, pressure, shear stress and the disk torque coefficient are predicted mostly for a Reynolds number (Re = Ω R22/v) corresponding to 10,000, approximately, where R2, Ω, and v are the disk radius, the disk angular velocity in rad/s, and the kinematic viscosity of air at 300 K, respectively. The calculations show that a large blockage significantly alters the interdisk flow characteristics by markedly raising the pressure ahead of an obstruction and accelerating the flow through the empty space around it. This induces a detached reversed flow region ahead of the obstruction quite distinct from that in its wake. The disk surface pressure distributions point to a potential source of dynamical instability in rotating disk flows with obstructions. The variations of the disk torque coefficient with Re and geometry generally agree with the theoretical expression of Humphrey et al. (1992). It is shown that the bulk of the drag on an obstruction is form drag as opposed to friction drag.","PeriodicalId":231650,"journal":{"name":"7th International Symposium on Information Storage and Processing Systems","volume":"2169 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1996-11-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"15","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"7th International Symposium on Information Storage and Processing Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1115/1.2819272","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 15
Abstract
Numerical calculations have been performed for isothermal, laminar, three-dimensional flow past one or two fixed obstructions radially aligned and symmetrically located between a pair of disks corotating in a fixed cylindrical enclosure. The single-obstruction cases respectively model the influence on the flow of (a) a magnetic head arm support and (b) an air lock. The dual-obstruction cases model the simultaneous presence of these two objects. The air lock produces an interdisk cross-stream plane blockage of 62% while the two head arm supports produce blockages of 31% and 62%, respectively. For the cases with the air lock and arm support simultaneously present, the circumferential angle between them is fixed to 40° or 80°. Velocity, pressure, shear stress and the disk torque coefficient are predicted mostly for a Reynolds number (Re = Ω R22/v) corresponding to 10,000, approximately, where R2, Ω, and v are the disk radius, the disk angular velocity in rad/s, and the kinematic viscosity of air at 300 K, respectively. The calculations show that a large blockage significantly alters the interdisk flow characteristics by markedly raising the pressure ahead of an obstruction and accelerating the flow through the empty space around it. This induces a detached reversed flow region ahead of the obstruction quite distinct from that in its wake. The disk surface pressure distributions point to a potential source of dynamical instability in rotating disk flows with obstructions. The variations of the disk torque coefficient with Re and geometry generally agree with the theoretical expression of Humphrey et al. (1992). It is shown that the bulk of the drag on an obstruction is form drag as opposed to friction drag.