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受限和非受限气泡对碎石机冲击波脉冲的响应。

Response of constrained and unconstrained bubbles to lithotripter shock wave pulses.

作者信息

Ding Z, Gracewski S M

机构信息

Department of Mechanical Engineering, University of Rochester, New York 14627.

出版信息

J Acoust Soc Am. 1994 Dec;96(6):3636-44. doi: 10.1121/1.410582.

Abstract

The Gilmore formulation for spherical bubble dynamics [F. R. Gilmore, The Growth or Collapse of a Spherical Bubble in a Viscous Compressible Liquid (California Institute of Technology, Pasadena, CA, 1952), Rep. No. 26-4] is used to investigate the response of air bubbles to a variety of lithotripter shock waveforms. A modification of the Gilmore model is proposed to account for partial constraint of the bubble expansion that can be caused by bubble coatings (such as in echo contrast agents) and by tissues or vessels surrounding bubbles in vivo. In the modified formulation, a viscoelastic membrane is assumed to exist at the bubble interface to include the possible effects of the nonlinear elasticity and strain rate dependent viscosity on the bubble response. The stress induced in the membrane is assumed to be an exponential function of the bubble radius, which tends to restrict the bubble expansion. The viscosity is assumed to increase with the strain rate. In the absence of the membrane, the maximum bubble wall pressure induced by a negative (tensile) pulse is much larger than that induced by a positive (compressive) pulse of the same pressure waveform and amplitude. This difference increases with decreasing initial bubble radius. The addition of the viscoelastic membrane significantly decreases the predicted maximum bubble pressure and the difference in response between the positive and negative pulses. The effect of the time delay between double pulses (positive followed by negative or negative followed by positive) is also investigated for unconstrained bubbles.

摘要

吉尔摩球形气泡动力学公式[F. R. 吉尔摩,《粘性可压缩液体中球形气泡的生长或坍塌》(加利福尼亚理工学院,帕萨迪纳,加利福尼亚,1952年),报告编号26 - 4]被用于研究气泡对各种碎石机冲击波波形的响应。提出了吉尔摩模型的一种修正形式,以考虑气泡膨胀的部分约束,这种约束可能由气泡涂层(如超声造影剂中的涂层)以及体内气泡周围的组织或血管引起。在修正后的公式中,假设在气泡界面存在一个粘弹性膜,以纳入非线性弹性和应变率相关粘度对气泡响应的可能影响。假设膜中产生的应力是气泡半径的指数函数,这倾向于限制气泡膨胀。假设粘度随应变率增加。在没有膜的情况下,由负(拉伸)脉冲引起的最大气泡壁压力比由相同压力波形和幅度的正(压缩)脉冲引起的大得多。这种差异随着初始气泡半径的减小而增大。添加粘弹性膜显著降低了预测的最大气泡压力以及正负脉冲响应之间的差异。还对无约束气泡研究了双脉冲(正脉冲后跟负脉冲或负脉冲后跟正脉冲)之间时间延迟的影响。

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