ESTIMATING CLIMATIC TEMPERATURE-CHANGE IN THE OCEAN WITH SYNTHETIC ACOUSTIC APERTURES

Citation
Al. Fabrikant et al., ESTIMATING CLIMATIC TEMPERATURE-CHANGE IN THE OCEAN WITH SYNTHETIC ACOUSTIC APERTURES, IEEE journal of oceanic engineering, 23(1), 1998, pp. 20-25
Citations number
24
Categorie Soggetti
Oceanografhy,"Engineering, Civil","Engineering, Eletrical & Electronic","Engineering, Marine
ISSN journal
03649059
Volume
23
Issue
1
Year of publication
1998
Pages
20 - 25
Database
ISI
SICI code
0364-9059(1998)23:1<20:ECTITO>2.0.ZU;2-T
Abstract
An acoustic tomography simulation is carried out in the eastern North Pacific ocean to assess whether climate trends are better detected and mapped with mobile or fixed receivers, In both cases, acoustic signal s from two stationary sources are transmitted to ten receivers, Natura l variability of the sound-speed field is simulated with the Naval Res earch Laboratory (NRL) layered-ocean model, A sequential Kalman-Bucy f ilter is used to estimate the sound speed field, where the apriori err or covariance matrix of the parameters is estimated from the NRL model , A spatially homogeneous climate trend is added to the NRL fluctuatio ns of sound speed, but the trend is not parameterized in the Kalman fi lter, Acoustic travel times are computed between the sources and recei vers by combining sound speeds from the NRL model with those from the unparameterized climate trend, The effects of the unparameterized clim ate trend are projected onto parameters which eventually drift beyond acceptable limits, At that time, the unparameterized trend is detected , Mobile and fixed receivers detect the trend at about the same time, At detection time, however, maps from fixed receivers are less accurat e because some of the unparameterized climate trend is projected onto the spatially-varying harmonics of the sound-speed field, With mobile receivers, the synthetic apertures suppress the projection onto these harmonics, Instead, the unparameterized trend is correctly projected o nto the spatially homogeneous portion of the parameterized sound speed field.