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Ultrasonic scattering cross sections of shell-encapsulated gas bubbles immersed in a viscoelastic liquid: first and second harmonics

机译:浸入粘弹性液体中的壳包裹气泡的超声散射截面:一次和二次谐波

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The oscillations of gas bubbles, without shell, immersed in viscoelastic liquids and driven by an acoustic wave have been the subject of several investigations. They demonstrate that the viscosity coefficient and the spring constant of the liquid have significant influence on the scattering cross section of the gas bubble. For shell-encapsulated gas bubbles, the investigations have been concentrated to bubbles immersed in a pure viscous liquid. This present work computes the ultrasonic scattering cross section, first and second harmonics, of shell-encapsulated gas bubbles immersed in a viscoelastic liquid. The theoretical model of the bubble oscillation is based on the generalized Rayleigh-Plesset equation of motion of a spherical cavity immersed in a viscoelastic liquid represented by a three-parameter linear Oldroyd model. The scattering cross section is computed for Albunex((R)) type of bubble (shell thickness = 15 nm, shell shear viscosity = 1.77 Pa s, shell modulus of rigidity = 88.8 MPa) irradiated by a 3.5 MHz ultrasonic pressure wave with an amplitude of 30 kPa. The results demonstrate that encapsulated bubbles respond independently of the surrounding liquid being pure viscous or viscoelastic as long as the surrounding liquid shear viscosity is as low as 10(-3) Pa s. Nevertheless, for higher shear viscosities, the bubble responds differently if the surrounding liquid is pure viscous or viscoelastic. In general, the scattering cross sections of first and second harmonics are larger for the viscoelastic liquid. (C) 2003 Elsevier B.V. All rights reserved. [References: 17]
机译:浸没在粘弹性液体中并由声波驱动的无壳气泡的振荡已成为许多研究的主题。他们证明了液体的粘度系数和弹簧常数对气泡的散射横截面有重大影响。对于壳包裹的气泡,研究已经集中到浸入纯粘性液体中的气泡中。本工作计算了浸没在粘弹性液体中的壳封装气泡的超声散射截面(一次谐波和二次谐波)。气泡振荡的理论模型基于浸入由三参数线性Oldroyd模型表示的粘弹性液体中的球形空腔的广义Rayleigh-Plesset运动方程。计算通过3.5 MHz超声波压力波辐照的Albunex(R)型气泡(壳厚度= 15 nm,壳剪切粘度= 1.77 Pa s,壳刚性模量= 88.8 MPa)的散射截面。 30 kPa。结果表明,只要周围的液体剪切粘度低至10(-3)Pa s,封装的气泡就可以独立于周围的液体(纯粘性或粘弹性)做出响应。但是,对于较高的剪切粘度,如果周围的液体是纯粘性的或粘弹性的,气泡的响应会有所不同。通常,对于粘弹性液体,一次谐波和二次谐波的散射截面较大。 (C)2003 Elsevier B.V.保留所有权利。 [参考:17]

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