Simulation of an Underwater Acoustic Communication Channel Characterized by Wind-Generated Surface Waves and Bubbles

Sea-surface scattering by wind-generated waves and bubbles is regarded to be the main nonplatform related cause of the time variability of shallow acoustic communication channels. Simulations for predicting the quality of acoustic communication links in such channels thus require adequate modeling of these dynamic sea-surface effects. For frequencies in the range of 1-4 kHz , there is an important effect of bubbles on sea-surface reflection loss due to refraction, which can be modeled with a modified sound-speed profile (SSP) accounting for the bubble void fraction in the surface layer. The bubble cloud then acts as an acoustic lens, enhancing the rough-surface scattering by the resulting upward refraction. It is shown here that, for frequencies in the considered range of 4-8 kHz, bubble extinction, including both the effects of bubble scattering and absorption, provides a significant additional contribution to the surface loss. Model-based channel simulations are performed by applying a ray tracer, together with a toolbox for generation of rough sea-surface evolutions. This practical simulation framework is demonstrated to provide realistic results for both stationary and mobile communication nodes by capturing specific features observed in experiments, such as time variability, fading reverberation tails, and wind-speed dependence of the Doppler power spectrum.

[1]  W. Pierson,et al.  A proposed spectral form for fully developed wind seas based on the similarity theory of S , 1964 .

[2]  J. Ewing,et al.  Directional Wave Spectra Observed during JONSWAP 1973 , 1980 .

[3]  O. Hastrup Some Bottom-Reflection Loss Anomalies near Grazing and Their Effect on Propagation in Shallow Water , 1980 .

[4]  S. Thorpe,et al.  On the clouds of bubbles formed by breaking wind-waves in deep water, and their role in air-sea gas transfer , 1982, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[5]  M. Porter,et al.  Gaussian beam tracing for computing ocean acoustic fields , 1987 .

[6]  D. E. Weston,et al.  Wind effects in shallow‐water acoustic transmission , 1989 .

[7]  Marshall V. Hall,et al.  A comprehensive model of wind‐generated bubbles in the ocean and predictions of the effects on sound propagation at frequencies up to 40 kHz , 1989 .

[8]  T. Leighton The Acoustic Bubble , 1994 .

[9]  G. Norton,et al.  The impact of the background bubble layer on reverberation‐derived scattering strengths in the low to moderate frequency range , 1995 .

[10]  Reflection and transmission coefficients for a layered fluid sediment overlying a uniform solid substrate , 1996 .

[11]  Igor Rychlik,et al.  WAFO - A Matlab Toolbox For Analysis of Random Waves And Loads , 2000 .

[12]  G. Norton,et al.  On the relative role of sea-surface roughness and bubble plumes in shallow-water propagation in the low-kilohertz region , 2001 .

[13]  C. Tindle,et al.  Wavefronts and waveforms in deep-water sound propagation. , 2002, The Journal of the Acoustical Society of America.

[14]  M. Trevorrow,et al.  Measurements of near-surface bubble plumes in the open ocean with implications for high-frequency sonar performance. , 2003, The Journal of the Acoustical Society of America.

[15]  G. Deane,et al.  Surface wave focusing and acoustic communications in the surf zone , 2004 .

[16]  M. Ainslie Effect of wind-generated bubbles on fixed range acoustic attenuation in shallow water at 1–4kHz , 2005 .

[17]  M. Porter,et al.  Modeling broadband ocean acoustic transmissions with time-varying sea surfaces. , 2008, The Journal of the Acoustical Society of America.

[18]  Paul A. van Walree,et al.  A Discrete-Time Channel Simulator Driven by Measured Scattering Functions , 2008, IEEE Journal on Selected Areas in Communications.

[19]  Timothy G Leighton,et al.  Review of scattering and extinction cross-sections, damping factors, and resonance frequencies of a spherical gas bubble. , 2011, The Journal of the Acoustical Society of America.

[20]  Paul van Walree,et al.  Channel sounding for acoustic communications : techniques and shallow-water examples , 2011 .

[21]  Marcia J. Isakson Principles of Sonar Performance Modeling (Springer Praxis Books/Geo Sciences) , 2011 .

[22]  Robbert van Vossen,et al.  The effect of wind-generated bubbles on sea-surface backscattering at 940 Hz. , 2011, The Journal of the Acoustical Society of America.

[23]  Modulation of a high-frequency shallow-water acoustic channel by sea surface waves: 3-D PE-based modeling , 2011, OCEANS 2011 IEEE - Spain.

[24]  Kevin B. Smith,et al.  Coherent reflection from surface gravity water waves during reciprocal acoustic transmissions. , 2012, The Journal of the Acoustical Society of America.

[25]  Mohsen Badiey,et al.  The Effects of Surface Gravity Waves on High-Frequency Acoustic Propagation in Shallow Water , 2012, IEEE Journal of Oceanic Engineering.

[26]  Trond Jenserud,et al.  Erratum to “Validation of Replay-Based Underwater Acoustic Communication Channel Simulation” [R. Otnes, P. A. van Walree, T. Jenserud, IEEE J. Ocean. Eng., DOI: 10.1109/JOE.2013.2262743] , 2013 .

[27]  Henry Dol,et al.  Validation of simulations of an underwater acoustic communication channel characterized by wind-generated surface waves and bubbles , 2013 .

[28]  James C. Preisig,et al.  The Suspension of Large Bubbles Near the Sea Surface by Turbulence and Their Role in Absorbing Forward-Scattered Sound , 2013, IEEE Journal of Oceanic Engineering.