{"title":"水中单泡存在时交叉超声波束的非线性散射论证","authors":"Katherine A. Haas, M. Korman","doi":"10.1121/2.0000911","DOIUrl":null,"url":null,"abstract":"An apparatus consisting of an open thin-wall clear acrylic rectangular tank is used to resonate the volume cavity of water in an nx=1, ny=1, nz=3 mode; such that a mm sized bubble or less can be levitated in the center of the tank. The authors will utilize the experimental arrangement suggested by T.J. Asaki, P.L. Marston, and E.H. Trinh [“Shape oscillations of bubbles in water driven by modulated ultrasonic radiation pressure: Observations and detection with scattered laser light,” JASA 93, p 706-713, (1993)]. In which, their experimental apparatus involves a description of their piezoelectric driver, which couples into the bottom of the tank. Next, the demonstration consists of the nonlinear scattering of crossed ultrasonic beams of primary frequency components: f1=1.9 MHz, f2= 2.1 MHz; which, interact nonlinearly with the bubble to produce nonlinear scattering outside the interaction region at the combination frequency f+ = 4.0 MHz. The receiving 4 MHz transducer unit will measure the nonlinear scatter...","PeriodicalId":20469,"journal":{"name":"Proc. Meet. Acoust.","volume":"3 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2018-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Demonstration on the nonlinear scattering of crossed ultrasonic beams in presence of single bubble in water\",\"authors\":\"Katherine A. Haas, M. Korman\",\"doi\":\"10.1121/2.0000911\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"An apparatus consisting of an open thin-wall clear acrylic rectangular tank is used to resonate the volume cavity of water in an nx=1, ny=1, nz=3 mode; such that a mm sized bubble or less can be levitated in the center of the tank. The authors will utilize the experimental arrangement suggested by T.J. Asaki, P.L. Marston, and E.H. Trinh [“Shape oscillations of bubbles in water driven by modulated ultrasonic radiation pressure: Observations and detection with scattered laser light,” JASA 93, p 706-713, (1993)]. In which, their experimental apparatus involves a description of their piezoelectric driver, which couples into the bottom of the tank. Next, the demonstration consists of the nonlinear scattering of crossed ultrasonic beams of primary frequency components: f1=1.9 MHz, f2= 2.1 MHz; which, interact nonlinearly with the bubble to produce nonlinear scattering outside the interaction region at the combination frequency f+ = 4.0 MHz. The receiving 4 MHz transducer unit will measure the nonlinear scatter...\",\"PeriodicalId\":20469,\"journal\":{\"name\":\"Proc. Meet. Acoust.\",\"volume\":\"3 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-11-01\",\"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/10.1121/2.0000911\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proc. Meet. Acoust.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1121/2.0000911","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Demonstration on the nonlinear scattering of crossed ultrasonic beams in presence of single bubble in water
An apparatus consisting of an open thin-wall clear acrylic rectangular tank is used to resonate the volume cavity of water in an nx=1, ny=1, nz=3 mode; such that a mm sized bubble or less can be levitated in the center of the tank. The authors will utilize the experimental arrangement suggested by T.J. Asaki, P.L. Marston, and E.H. Trinh [“Shape oscillations of bubbles in water driven by modulated ultrasonic radiation pressure: Observations and detection with scattered laser light,” JASA 93, p 706-713, (1993)]. In which, their experimental apparatus involves a description of their piezoelectric driver, which couples into the bottom of the tank. Next, the demonstration consists of the nonlinear scattering of crossed ultrasonic beams of primary frequency components: f1=1.9 MHz, f2= 2.1 MHz; which, interact nonlinearly with the bubble to produce nonlinear scattering outside the interaction region at the combination frequency f+ = 4.0 MHz. The receiving 4 MHz transducer unit will measure the nonlinear scatter...