Turbulent flow due to the interaction of two mutually perpendicular crossed turbulent streaming jets in water

Jenna Cartron, M. Korman
{"title":"Turbulent flow due to the interaction of two mutually perpendicular crossed turbulent streaming jets in water","authors":"Jenna Cartron, M. Korman","doi":"10.1121/2.0000884","DOIUrl":null,"url":null,"abstract":"The food industry has studied turbulent streaming from an ultrasonic horn reactor, where the turbulent flow field can be modelled by a laminar jet flow that has a turbulent eddy viscosity [M. J. Lighthill, “Acoustic streaming,” J. Sound Vib. 61 (3), (1978) 391–418]. Work by Kumar (2006), Trujillo (2009) and others successfully compared the results with CFD models, have sparked interest in revisiting turbulent streaming by an ultrasonic horn, resulting in this presentation. Our demonstration studies the turbulent flow generated by the interaction between two mutually perpendicular crossed streaming jets – which both exhibit turbulent behavior. We are specifically interested in the flow field in the forward and backward directions defined by the bisecting line segment ±45 degrees from the axis of each streaming jet, with the line segment located in the plane shared by the jet axes. The apparatus consists of two Langevin ultrasonic transducers (125 kHz) that are both equipped with a half-wavelength exponential horn. The horns are slightly submerged in an open acrylic water tank to allow for viewing of the flow field. A particle image velocimeter (PIV) will be used to measure the turbulent flow velocity field in the plane of the interaction region aforementioned.The food industry has studied turbulent streaming from an ultrasonic horn reactor, where the turbulent flow field can be modelled by a laminar jet flow that has a turbulent eddy viscosity [M. J. Lighthill, “Acoustic streaming,” J. Sound Vib. 61 (3), (1978) 391–418]. Work by Kumar (2006), Trujillo (2009) and others successfully compared the results with CFD models, have sparked interest in revisiting turbulent streaming by an ultrasonic horn, resulting in this presentation. Our demonstration studies the turbulent flow generated by the interaction between two mutually perpendicular crossed streaming jets – which both exhibit turbulent behavior. We are specifically interested in the flow field in the forward and backward directions defined by the bisecting line segment ±45 degrees from the axis of each streaming jet, with the line segment located in the plane shared by the jet axes. The apparatus consists of two Langevin ultrasonic transducers (125 kHz) that are both equipped with a half-wavelength exponenti...","PeriodicalId":20469,"journal":{"name":"Proc. Meet. Acoust.","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2018-10-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proc. Meet. Acoust.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1121/2.0000884","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

The food industry has studied turbulent streaming from an ultrasonic horn reactor, where the turbulent flow field can be modelled by a laminar jet flow that has a turbulent eddy viscosity [M. J. Lighthill, “Acoustic streaming,” J. Sound Vib. 61 (3), (1978) 391–418]. Work by Kumar (2006), Trujillo (2009) and others successfully compared the results with CFD models, have sparked interest in revisiting turbulent streaming by an ultrasonic horn, resulting in this presentation. Our demonstration studies the turbulent flow generated by the interaction between two mutually perpendicular crossed streaming jets – which both exhibit turbulent behavior. We are specifically interested in the flow field in the forward and backward directions defined by the bisecting line segment ±45 degrees from the axis of each streaming jet, with the line segment located in the plane shared by the jet axes. The apparatus consists of two Langevin ultrasonic transducers (125 kHz) that are both equipped with a half-wavelength exponential horn. The horns are slightly submerged in an open acrylic water tank to allow for viewing of the flow field. A particle image velocimeter (PIV) will be used to measure the turbulent flow velocity field in the plane of the interaction region aforementioned.The food industry has studied turbulent streaming from an ultrasonic horn reactor, where the turbulent flow field can be modelled by a laminar jet flow that has a turbulent eddy viscosity [M. J. Lighthill, “Acoustic streaming,” J. Sound Vib. 61 (3), (1978) 391–418]. Work by Kumar (2006), Trujillo (2009) and others successfully compared the results with CFD models, have sparked interest in revisiting turbulent streaming by an ultrasonic horn, resulting in this presentation. Our demonstration studies the turbulent flow generated by the interaction between two mutually perpendicular crossed streaming jets – which both exhibit turbulent behavior. We are specifically interested in the flow field in the forward and backward directions defined by the bisecting line segment ±45 degrees from the axis of each streaming jet, with the line segment located in the plane shared by the jet axes. The apparatus consists of two Langevin ultrasonic transducers (125 kHz) that are both equipped with a half-wavelength exponenti...
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
湍流由于两个相互垂直的交叉湍流射流在水中相互作用而产生的湍流
食品工业已经研究了超声波喇叭反应器中的湍流流,其中湍流流场可以通过具有湍流涡流粘度的层流射流来模拟[M]。李志强,“声学流”,声学学报,(1978):391-418。库马尔(2006)、特鲁希略(2009)等人的工作成功地将结果与CFD模型进行了比较,激发了人们重新研究超声喇叭湍流流的兴趣,从而产生了这次演讲。我们的演示研究了两个相互垂直的交叉流射流相互作用产生的湍流,这两个射流都表现出湍流行为。我们特别感兴趣的是向前和向后方向的流场,由与每个流射流轴±45度的平分线段定义,线段位于射流轴共享的平面上。该装置由两个125千赫的朗格万超声换能器组成,这两个换能器都配备了一个半波长指数喇叭。角被稍微淹没在一个开放的丙烯酸水箱,以允许观看流场。粒子图像测速仪(PIV)将用于测量上述相互作用区域平面上的湍流速度场。食品工业已经研究了超声波喇叭反应器中的湍流流,其中湍流流场可以通过具有湍流涡流粘度的层流射流来模拟[M]。李志强,“声学流”,声学学报,(1978):391-418。库马尔(2006)、特鲁希略(2009)等人的工作成功地将结果与CFD模型进行了比较,激发了人们重新研究超声喇叭湍流流的兴趣,从而产生了这次演讲。我们的演示研究了两个相互垂直的交叉流射流相互作用产生的湍流,这两个射流都表现出湍流行为。我们特别感兴趣的是向前和向后方向的流场,由与每个流射流轴±45度的平分线段定义,线段位于射流轴共享的平面上。该装置由两个Langevin超声波换能器(125 kHz)组成,这两个换能器都配备了半波长指数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
Different origins of acoustic streaming at resonance Clinical studies of biceps anisotropy, relaxation and nonlinearity with a medical device for ultrasonic imaging Prospective medical applications of Nonlinear Time Reversal Acoustics Nonlinear relaxation in geomaterials: New results Numerical investigation of self-focused Lamb waves in anisotropic media
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1