140th Meeting of the Acoustical Society of America


Session 2aBB-Dectection and Characterization of Bubbles, Acoustic Cavitation, and Associated Physical Effects I



2aBB9. Acoustic scattering from an elastic tube filled with bubbly fluid.

A complete model describing broadband sea surface scattering at high wind speeds has not been developed. One difficulty is accounting for scattering from near surface bubble clouds. This problem has been addressed in the literature for low frequencies. To first order, an acoustically compact bubble cloud can be modeled as a compressible sphere, where the scattering strength depends only on spherical cloud volume and mean void fraction, not the bubble size distribution or cloud shape. This hypothesis has been experimentally tested using freely rising artificial bubble clouds [J. Acoust. Soc. Am. 92, 2993--2996 (1992)]. The measured low frequency monopole target strength of the cloud agreed with theory but higher frequency results did not. To further understand scattering from these objects, laboratory scattering experiments are underway using geometrically well-characterized bubbly fluid targets. Initial measurements of scattering from a bubbly-fluid-filled latex tube are presented and compared to an effective medium theory. These initial results lack independent void fraction determination but good qualitative agreement is found, even above the monopole resonance frequency. A new method used in these experiments to generate large volumes of nearly monodisperse bubbly fluid samples will also be described. [Work supported by ONR.]


Preston S. Wilson, Ronald A. Roy and William M. Carey

Department of Aerospace and Mechanical Engineering, Boston University, Boston MA 02215


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Table of Contents

Acoustic scattering from an elastic tube filled with bubbly fluid.

Motivation for Work

Overview of Theoretical Approach

Theoretical Scattering Model

Mass Production of Microbubbles

Experimental Setup and Laser Alignment System

Schematic of Experiment (side view)

Experimental Results: Typical Pressure Signature ñ 12 kHz

Preliminary Model: CW Plane Wave, Infinite Fluid Cylinder, No Shell

A More Realistic Model: Account for Elastic Shell

A More Realistic Model: Account for Elastic Shell

Even Better: Account for Finite Pulse Length Convolve Incident Pulse with Scattering Response

Accounting for Shell and Finite Pulse Length Reduces High Void Fraction Error

Overview of Experimental Results Effect of Void Fraction on Scattering Strength

Summary / Future Work

Comments or questions: psw@bu.edu

Bubbly Fluids Main Page

Download Slides: 2aBB9.pdf (372 K)