IEEE JOURNAL OF OCEANIC ENGINEERING, VOL. 38, NO. 4, OCTOBER 2013 701
Statistical Characterization and Computationally
Ef ficient Modeling of a Class of Underwater
Acoustic Communication Channels
Parastoo Qarabaqi, Student Member, IEEE, and Milica Stojanovic, Fellow, IEEE
Abstract—Underwater acoustic channel models provide a tool
for predicting the performance of communication systems before
deployment, and are thus essential for system design. In this paper,
we offer a statistical channel model which incorporates physical
laws of acoustic propagation (frequency-dependent attenuation,
bottom/surface reflections), as well as the effects of inevitable
random local displacements. Specifically, we focus on random
displacements on two scales: those that involve distances on the
order of a few wavelengths, to which we refer as small-scale
effects, and those that involve many wavelengths, to which we
refer as large-scale effects. Small-scale effects include scattering
and motion-induced Doppler shifting, and are responsible for
fast variations of the instantaneous channel response, while
large-scale effects describe the location uncertainty and changing
environmental conditions, and affect the locally averaged received
power. We model each propagation path by a large-scale gain and
micromultipath components that cumulatively result in a complex
Gaussian distortion. Time- and frequency-correlation properties
of the path coefficients are assessed analytically, leading to a
computationally efficient model for numerical channel simulation.
Random motion of the surface and transmitter/receiver displace-
ments introduce additional variation whose temporal correlation
is described by Bessel-type functions. The total energy, or the gain
contained in the channel, averaged over small scale, is modeled as
log-normally distributed. The models are validated using real data
obtained from four experiments. Specifically, experimental data
are used to assess the distribution and the autocorrelation func-
tions of the large-scale transmission loss and the short-term path
gains. While the former indicates a log-normal distribution with
an exponentially decaying autocorrelation, the latter indicates a
conditional Ricean distribution with Bessel-type autocorrelation.
Index Terms—Channel simulation, Doppler shifting, Doppler
spreading, frequency correlation, large-scale fading, scattering,
small-scale fading, statistical channel modeling, time correlation,
underwater acoustic (UWA) communications.
I. INTRODUCTION
U
NDERWATER ACOUSTIC (UWA) communication
systems have to be designed to operate in a variety
of conditions that differ from the nominal ones due to the
Manuscript received November 19, 2012; revised April 11, 2013; accepted
August 08, 2013. Date of publication September 30, 2013; date of current ver-
sion October 09, 2013. This work was supported by the U.S. Office of Naval Re-
search (ONR) Multidisciplinary University Research Initiative (MURI) under
Grant N00014-07-1-0738, by the ONR under Grant N00014-09-1-0700, and by
the National Science Foundation (NSF) under Grant CNS-1212999.
Associate Editor: J. Potter.
The authors are with the Department of Electrical and Computer Engineering,
Northeastern University, Boston, MA 02115 USA (e-mail: qarabaqi@ece.neu.
edu; millitsa@ece.neu.edu).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/JOE.2013.2278787
changes in system geometry and environmental conditions.
To allocate the appropriate resources (power, bandwidth)
before system deployment, as well as to design appropriate
signals and processing algorithms on both the physical link
layer and the higher network layers, it is necessary to have a
relatively accurate channel model. Beam tracing tools, such
as Bellhop [1], use ray theory to provide an accurate deter-
ministic picture of a UWA channel for a given geometry and
signal frequency, but they do not take into account random
channel variation. In recent years, there has been a growing
awareness of the need to develop statistical channel models
that will lead to computationally efficient tools for numerical
simulation. New tools have been developed that address this
need to some extent. For example, the Virtual Timeseries
EXperiment (VirTEX) code [2] was developed to simulate the
effect of channel variation in a manner that is computationally
more efficient than repeated application of the Bellhop beam
tracing. This algorithm operates by tracing multiple interre-
lated beams to assess the cumulative effect on the signal of
a given frequency. However, its computational complexity
may still be an issue. For example, simulating a channel
with a Doppler distortion on the order of 15 Hz requires at
least 30 channel realizations per second which amounts to a
total of 5400 Bellhop runs for simulating a system with two
transmitters and six receiver elements over a period of 15
s. The wave front model [3] offers a deterministic approach
which provides approximations to the ray theory to efficiently
model the effects of the curvature of the surface waves and the
amplitude and arrival time fluctuations that they introduce [4].
Numerous studies have also been conducted to model the
UWA channel stochastically, e.g., [5]–[16]. These studies are
usually based on the analyses of experimental acoustic data
collected in a particular location. Some authors find Ricean
fading [5], [7] or Rayleigh fading [6], [8], [13] to provide a good
match for their measurements, while others find log-normal
distribution [9], [10], the -distribution [11], [12], or a general
class of Ricean shadowed distribution [16] to be a better fit.
The variety of proposed statistical models is due to experi-
ment-specific properties, e.g., the deployment site and the type
of signals used for probing, as well as the time intervals during
which the channel is observed.
Statistical modeling of small-scale phenomena is a subject of
ongoing research, which points to different types of fading, and
no consensus exists yet on this topic. Modeling of large-scale
phenomena has also been addressed only to a very limited ex-
tent (see, e.g., [14], which shows some evidence of log-normal
fading), while a few attempts have been made at unifying the
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