Demonstration on the nonlinear scattering of crossed ultrasonic beams in presence of single bubble in water

Katherine A. Haas, M. Korman
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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...
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水中单泡存在时交叉超声波束的非线性散射论证
一种由开口薄壁透明丙烯酸矩形槽组成的装置,用于以nx=1, ny=1, nz=3模式对水的体积腔进行共振;这样一个毫米大小或更小的气泡可以悬浮在水箱的中心。作者将采用T.J. Asaki, P.L. Marston和E.H. Trinh[调制超声辐射压力驱动水中气泡的形状振荡:散射激光的观察和探测]提出的实验安排,JASA 93, p 706-713,(1993)。在这篇文章中,他们的实验装置包括对压电驱动器的描述,该驱动器与水箱底部耦合。接下来,演示了主要频率分量的交叉超声波束的非线性散射:f1=1.9 MHz, f2= 2.1 MHz;在组合频率f+ = 4.0 MHz处,与气泡非线性相互作用,在相互作用区域外产生非线性散射。接收4mhz换能器单元将测量非线性散射…
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