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Actas JP2011 - Universidad de La Laguna

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<strong>Actas</strong> XXII Jornadas <strong>de</strong> Paralelismo (<strong>JP2011</strong>) , <strong>La</strong> <strong>La</strong>guna, Tenerife, 7-9 septiembre 2011Statistical Mo<strong>de</strong>ling of Transmission Path Lossin Un<strong>de</strong>rwater Acoustic NetworksJesús Llor and Manuel Pérez Malumbres 1Abstract—Propagation conditions in an un<strong>de</strong>rwateracoustic channel are known to vary in time, causing thereceived signal strength to <strong>de</strong>viate from the nominal valuepredicted by a <strong>de</strong>terministic propagation mo<strong>de</strong>l. Tofacilitate large-scale system <strong>de</strong>sign in such conditions (e.g.power allocation), we <strong>de</strong>velop a statistical propagationmo<strong>de</strong>l in which the transmission loss is treated as a randomvariable. By repetitive computation of acoustic field usingray tracing for a set of varying environmental conditions(surface height, wave activity, small displacements oftransmitter and receiver around nominal locations), anensemble of transmission losses is compiled which is thenused to infer the statistical mo<strong>de</strong>l parameters. A reasonableagreement is found with log-normal distribution whosemean is taken as the nominal transmission loss, and whosevariance appears to be constant for a certain range ofinter-no<strong>de</strong> distances in a given <strong>de</strong>ployment location. Thestatistical mo<strong>de</strong>l is <strong>de</strong>emed useful for higher-level systemplanning, where simulation is nee<strong>de</strong>d to assess theperformance of candidate network protocols un<strong>de</strong>r variousresource allocation policies, i.e. to <strong>de</strong>termine the transmitpower and bandwidth allocation necessary to achieve a<strong>de</strong>sire.Keywords—Un<strong>de</strong>rwater acoustics, Acoustic channelmo<strong>de</strong>l, Wireless sensor networks, Network simulation.TI. INTRODUCTIONHE growing need for ocean observation and remotesensing has recently motivated a surge in researchpublications as well as several experimental efforts (e.g.[1]) in the area of un<strong>de</strong>rwater acoustic networks. Crucialto these <strong>de</strong>velopments is the un<strong>de</strong>rstanding ofpropagation conditions that <strong>de</strong>fine the time-varying andlocation-sensitive acoustic environment, not only fromthe viewpoint of small-scale, rapid signal fluctuationsthat affect the performance of the physical layertechniques, but also from the viewpoint of large-scale,slow fluctuations of the received signal power thataffect the performance of higher network layers. Thisfact has been gaining recognition in the researchcommunity, leading to an increased awareness about theneed for network simulators that take into account thephysics of acoustic propagation [1]-[4]. As a result, thefirst publicly available acoustic network simulators haveemerged [2], and more are likely to come.One of the challenges in the <strong>de</strong>sign of un<strong>de</strong>rwateracoustic networks is the allocation of power acrossdifferent network no<strong>de</strong>s. This task is exacerbated by the1 All authors are with the Dept. of Physics and Computer Engineeringat the Miguel Hernan<strong>de</strong>z University (Spain). E-mails: {jllor,mels}@umh.esspatial and temporal variation of the large-scaletransmission loss, and the lack of statistical mo<strong>de</strong>ls thatcapture these apparently random phenomena.While it is well known from field experiments that thereceived power varies in time around the nominal valuepredicted by a <strong>de</strong>terministic propagation mo<strong>de</strong>l, little isknown about the statistical nature of these variations.Literature on this topic is scarce; however, several recentreferences indicate that the received signal strengthobeys a log-normal distribution (e.g. [5][6]). A goodsystem <strong>de</strong>sign has to budget for signal strengthvariations in or<strong>de</strong>r to ensure a <strong>de</strong>sired level of networkperformance (e.g. connectivity), and the budgeting taskcan be ma<strong>de</strong> much easier if the statistics of theun<strong>de</strong>rlying process are known.In this paper, we analyze those random variations inthe large-scale transmission loss that are mainlygoverned by the environmental factors such as surfaceactivity (waves) for a particular network scenario. Webegin by employing a prediction mo<strong>de</strong>l based on theBellhop ray tracing tool [7]. Such a <strong>de</strong>terministic mo<strong>de</strong>lprovi<strong>de</strong>s accurate results for a specific geometry of thesystem, but does not reflect the changes that occur as thegeometry changes slightly due to either surface motionor transmitter/receiver motion. Fig.1 illustrates thissituation for a point-to-point link. It shows an ensembleof transmission losses calculated by the Bellhop mo<strong>de</strong>lfor a set of varying surface conditions, each slightlydifferent from the nominal.While it is possible in principle to run a <strong>de</strong>terministicpropagation mo<strong>de</strong>l for a large number of differentsurface conditions, the un<strong>de</strong>rlying computational<strong>de</strong>mands are high. In a large network, it is ineffective,and possibly not even feasible, to run a complexprediction mo<strong>de</strong>l for each packet transmission. Astatistical prediction mo<strong>de</strong>l then becomes necessary.The goal of our work is to employ an existing<strong>de</strong>terministic prediction mo<strong>de</strong>l (DPM) such as the raytracer [7] to generate an ensemble of channel responsescorresponding to varying propagation conditions in agiven network. Using the so-obtained values, we thenconduct a statistical analysis to obtain the probability<strong>de</strong>nsity function (pdf) of the large-scale transmissionloss. The result is a statistical prediction mo<strong>de</strong>l (SPM)that is easy to employ for network <strong>de</strong>sign and analysis.The rest of this paper is organized as follows. In Sec.IIwe outline a specific system example, and discuss thecomputational <strong>de</strong>mands of <strong>de</strong>terministic propagationmo<strong>de</strong>ling. In Sec.III, we present the results of<strong>de</strong>terministic mo<strong>de</strong>ling and <strong>de</strong>velop an un<strong>de</strong>rlying<strong>JP2011</strong>-391

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