M. Cicolin, S. Chellini, B. Usherwood, B. Ganapathisubramani, Ian P. Castro
{"title":"多孔平板后的涡流脱落与流动方向一致","authors":"M. Cicolin, S. Chellini, B. Usherwood, B. Ganapathisubramani, Ian P. Castro","doi":"10.1017/jfm.2024.300","DOIUrl":null,"url":null,"abstract":"This work examines the influence of body porosity on the wake past nominally two-dimensional rectangular plates of fixed width \n \n \n $D$\n \n in the moderate range of Reynolds numbers \n \n \n $Re = UD/\\nu$\n \n (with \n \n \n $U$\n \n the incoming velocity and \n \n \n $\\nu$\n \n the kinematic viscosity) between 15 000 and 70 000. With porosity \n \n \n $\\beta$\n \n defined as the ratio of open to total area of the plate, it is well established that as porosity increases, the wake shifts from the periodic von Kármán shedding behaviour to a regime where this vortex shedding is absent. This change impacts the fluid forces acting on the plate, especially the drag, which is significantly lower for a wake without vortex shedding. We analyse experimentally the transition between these two regimes using hot-wire anemometry, particle-image velocimetry and force measurements. Coherence and phase measurements are used to determine the existence of regular, periodic vortex shedding based on the velocity fluctuations in the two main shear layers on either side of the wake. Results show that, independent of \n \n \n $Re$\n \n , the wake exhibits the classical Kármán vortex shedding pattern for \n \n \n $\\beta <0.2$\n \n but this is absent for \n \n \n $\\beta >0.3$\n \n . In the intermediate range, \n \n \n $0.2<\\beta <0.3$\n \n , there is a transitional regime that has not previously been identified; it is characterised by intermittent shedding. The flow alternates randomly between a vortex shedding and a non-shedding pattern and the total proportion of time during which vortex shedding is observed (the intermittency) decreases with increasing porosity.","PeriodicalId":505053,"journal":{"name":"Journal of Fluid Mechanics","volume":"1 9","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-04-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Vortex shedding behind porous flat plates normal to the flow\",\"authors\":\"M. Cicolin, S. Chellini, B. Usherwood, B. Ganapathisubramani, Ian P. Castro\",\"doi\":\"10.1017/jfm.2024.300\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This work examines the influence of body porosity on the wake past nominally two-dimensional rectangular plates of fixed width \\n \\n \\n $D$\\n \\n in the moderate range of Reynolds numbers \\n \\n \\n $Re = UD/\\\\nu$\\n \\n (with \\n \\n \\n $U$\\n \\n the incoming velocity and \\n \\n \\n $\\\\nu$\\n \\n the kinematic viscosity) between 15 000 and 70 000. With porosity \\n \\n \\n $\\\\beta$\\n \\n defined as the ratio of open to total area of the plate, it is well established that as porosity increases, the wake shifts from the periodic von Kármán shedding behaviour to a regime where this vortex shedding is absent. This change impacts the fluid forces acting on the plate, especially the drag, which is significantly lower for a wake without vortex shedding. We analyse experimentally the transition between these two regimes using hot-wire anemometry, particle-image velocimetry and force measurements. Coherence and phase measurements are used to determine the existence of regular, periodic vortex shedding based on the velocity fluctuations in the two main shear layers on either side of the wake. Results show that, independent of \\n \\n \\n $Re$\\n \\n , the wake exhibits the classical Kármán vortex shedding pattern for \\n \\n \\n $\\\\beta <0.2$\\n \\n but this is absent for \\n \\n \\n $\\\\beta >0.3$\\n \\n . In the intermediate range, \\n \\n \\n $0.2<\\\\beta <0.3$\\n \\n , there is a transitional regime that has not previously been identified; it is characterised by intermittent shedding. The flow alternates randomly between a vortex shedding and a non-shedding pattern and the total proportion of time during which vortex shedding is observed (the intermittency) decreases with increasing porosity.\",\"PeriodicalId\":505053,\"journal\":{\"name\":\"Journal of Fluid Mechanics\",\"volume\":\"1 9\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-04-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Fluid Mechanics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1017/jfm.2024.300\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Fluid Mechanics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1017/jfm.2024.300","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Vortex shedding behind porous flat plates normal to the flow
This work examines the influence of body porosity on the wake past nominally two-dimensional rectangular plates of fixed width
$D$
in the moderate range of Reynolds numbers
$Re = UD/\nu$
(with
$U$
the incoming velocity and
$\nu$
the kinematic viscosity) between 15 000 and 70 000. With porosity
$\beta$
defined as the ratio of open to total area of the plate, it is well established that as porosity increases, the wake shifts from the periodic von Kármán shedding behaviour to a regime where this vortex shedding is absent. This change impacts the fluid forces acting on the plate, especially the drag, which is significantly lower for a wake without vortex shedding. We analyse experimentally the transition between these two regimes using hot-wire anemometry, particle-image velocimetry and force measurements. Coherence and phase measurements are used to determine the existence of regular, periodic vortex shedding based on the velocity fluctuations in the two main shear layers on either side of the wake. Results show that, independent of
$Re$
, the wake exhibits the classical Kármán vortex shedding pattern for
$\beta <0.2$
but this is absent for
$\beta >0.3$
. In the intermediate range,
$0.2<\beta <0.3$
, there is a transitional regime that has not previously been identified; it is characterised by intermittent shedding. The flow alternates randomly between a vortex shedding and a non-shedding pattern and the total proportion of time during which vortex shedding is observed (the intermittency) decreases with increasing porosity.