Ocean Acoustic Observatories:
Data Analysis and Interpretation
A Collaborative Project Conducted by
Peter F. Worcester
Scripps Institution of Oceanography, University of California at San Diego
La Jolla, CA 92093-0225
phone: (619) 534-4688 fax: (619) 534-6251 email: pworcester@ucsd.edu
Award: N00014-95-1-0589
James A. Mercer and Robert C. Spindel
Applied Physics Laboratory, College of Ocean and Fishery Sciences
University of Washington
Seattle, WA 98105-6698
phone: (206) 543-1361 fax: (206) 543-678 email: mercer@apl.washington.edu
phone: (206) 543-1310 fax: (206) 543-3521 email: spindel@apl.washington.edu
Award #: N00014-95-1-0800
LONG-TERM GOAL
The ultimate limits to the coherence of long-range acoustic transmissions are imposed by ocean
processes, including internal waves, mesoscale variability, interior ocean boundaries (fronts), and
bathymetric scattering. An understanding of the effects of these processes on acoustic signals is crucial
to the use of acoustic remote sensing methods for a broad range of purposes, including undersea
surveillance, ocean acoustic tomography, and large-scale acoustic thermometry. The long-term goals of
this research are to enhance our understanding of the ocean processes that ultimately determine the
limits of useful long-range acoustic transmissions and to improve our capability to both generate and
detect very long-range transmissions.
OBJECTIVES
Theoretical considerations suggest that acoustic scattering due to internal-wave-induced sound-speed
perturbations will be small at very-low frequencies, i.e., below about 30 Hz, even at multi-megameter
ranges. The objective of this research is to understand the frequency dependence of scattering from
internal waves and other oceanographic features at multi-megameter ranges.
APPROACH
A short term transmission test, the Alternate Source Test (AST), was conducted during June-July 1996
to compare broadband transmissions at 28 Hz and 84 Hz (phase-locked coherent signals, each with a
10-Hz bandwidth). An HLF-6A acoustic source was suspended from shipboard near Pioneer Seamount
off central California and transmitted to two autonomous vertical line array (AVLA) receivers and to
ten horizontal line array (HLA) receivers, at ranges from 150 km to about 5 Mm. The combination of
temporal and spatial resolution makes it possible to isolate individual rays and, at the AVLA receivers,
low order modes, in order to elucidate the basic scattering physics. The data collected on the AVLA
and HLA receivers will be used to compare a variety of measures of the scattering at the two
frequencies, including travel time variance, and spread, scintillation index, coherences in time,
frequency, and space, emphasizing the unique capabilities of the AVLAs to provide information on
vertical coherence and modal structure and of the HLAs to provide information on the horizontal
coherence and spatial variability of the scattering. The computed statistics will be compared with
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1998
00-00-1998 to 00-00-1998
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Ocean Acoustic Observatories: Data Analysis and Interpretation
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University of California at San Diego,Scripps Institution of
Oceanography,La Jolla,CA,92093
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theoretical predictions. SIO investigators will play the leading role in analyzing the data from the
AVLA receivers, while APL/UW investigators will take the lead in analyzing the data from the HLA
receivers.
WORK COMPLETED
Analysis of the data continued throughout FY98. Signal processing of the dual-frequency receptions
has been completed and routine clock and mooring motion corrections have been applied to the AVLA
data (receivers at ranges of approximately 3500 km and 5100 km). Data from the AVLAs and two of
the HLAs (at approximately 150 and 700 km) have been analyzed.
The dual-frequency AVLA data have been used to test a modified vertical beamformer that explicitly
takes account of the depth dependence of the sound-speed profile, using a local WKBJ approximation.
The modified beamformer, called a turning-point filter, permits a uniform treatment of the arrival
pattern, from the early ray-like arrivals to the late mode-like arrivals.
RESULTS
Results indicate that internal-wave-induced acoustic scattering is less important at 28 Hz than at 84 Hz.
Processing of vertical line array data shows that the 28-Hz data has a more stable arrival pattern
compared to the 84-Hz data. This comparison holds for both the early ray arrivals and late mode
arrivals. Interpretation of the arrival pattern via a “turning point filter” has allowed a unified framework
for comparison of both regions. In simulations without internal waves the turning-point filter collapses
the acoustic arrival pattern at low vertical angles into a single energy-containing curve in vertical arrival
angle – travel time coordinates, where vertical arrival angle can be interpreted in terms of ray and mode
turning point depths. Using real data the arrival pattern does not collapse at low angles, however,
suggesting that internal-wave-induced scattering is still non-negligible even at 28 Hz. A paper
describing the turning point filter results is in preparation.
The horizontal line array data obtained on a receiver below the sound channel approximately 700 km
west of the source gave rms travel time fluctuations for one resolved “ray” arrival of 7.8 ms at 28 Hz
and 10.2 ms at 84 Hz, in the range of expected values. However the predicted ray arrivals turn above
the receiver, and we do not understand the associated propagation; explanations for this behavior (also
observed in other experiments with different ranges and frequencies) is being sought. The scintillation
index is approximately 0.11 at 28 Hz and 0.65 at 84 Hz, indicating much more stable amplitudes at the
lower frequency. Travel time spread is near zero for both frequencies. For the 150-km receiver there
were no single resolved ray arrivals; the arrival peak analyzed had two predicted ray arrivals separated
by 15 ms. In this case the rms travel time fluctuations were much large then one would expect for a
single ray at this range because of interference effects (order 14 ms for both frequencies compared to a
few milliseconds expected for a single ray). The scintillation index, though was 0.26 at 28 Hz and 0.64
at 84 Hz. While these scintillation estimates are contaminated by the two rays interfering with one
another, the trend also reflects the improvement (less fluctuation) at lower frequency.
The path integral theory of internal-wave-induced scattering in the ocean predicts that travel time bias is
proportional to the logarithm of the acoustic frequency. The dual frequency AST data should therefore
give information on the relative bias at the two frequencies. In preliminary calculations using the AVLA
data (Hawaii AVLA at 3500 km), the differences in travel times for simultaneous transmissions at 28 Hz
and 84 Hz are found to be of order 50 ms. For comparison, simulations by Colosi and Flatté give biases
that are less than 50 ms at 3 Mm range. For the two HLAs, the difference in travel time between the
two frequencies is 18 ms (150 km) and 31 ms (700 km), with the 28 Hz signal arriving later than the 84
Hz signal. At this point we can only say that the measurements are roughly in agreement with
predictions; a more quantitative comparison is in progress.
IMPACT/APPLICATIONS
Existing systems, whether active or passive, are not anywhere near the limits of what can be done in
underwater acoustics. A full understanding of the ultimate limits to acoustic coherence at long range in
the ocean is essential to the design of any acoustic system for remote sensing of the ocean interior,
whether it be for measurement of ocean temperatures, tracking of whales, detection of submarines, or
the study of volcanic processes at mid-ocean ridges. At the conclusion of our analyses we expect to
have a much fuller understanding of the frequency dependence of acoustic scattering from ocean
features at multi-megameter ranges, and of the potential for exploiting the anticipated reduction in
scattering, and corresponding increase in coherence, at very low frequencies.
TRANSITIONS
None.
RELATED PROJECTS
This work has been closely coordinated with, and partly supported by, the Acoustic Thermometry of
Ocean Climate (ATOC) project and the ONR North Pacific Acoustic Laboratory (NPAL) project. We
continue to collaborate very closely with J. Colosi (WHOI) and S. Flatté (UCSC).
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