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Dept. of Oceanology and Environmental Geophysics |
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A 3D Graphical Visualization |
Paolo SCARAZZATO, Osservatorio
Geofisico Sperimentale - Trieste
Summary The
time and space evolution of the Levantine Intermediate Water (LIW) in the
area of the Strait of Otranto during 1994/1995 is shown by means of a graphical
interpolative and displaying technique. The study reveals both a seasonal
and an interannual variability which appears in LIW volume, position and
salinity maximum. Comparison were also made with data measured in the same
area during some POEM cruises performed in the period 1985-1987.
Introduction
The Otranto Strait connects the Adriatic Sea with
the Ionian and consequently with the entire Mediterranean Sea and therefore
plays an important role in the water exchange processes between the two
basins, as revealed by the results of some studies performed in the past
decades (Wust, 1961; Ovchinnikov, 1966; Zore-Armanda, 1969, Orlic et al.,
1992). However, as they were rather occasional than systematical, a more
intense and detailed study (Otranto Project) was recently carried out over
the strait area, with six seasonal oceanographic cruises in 15 months and
about 20 months of eulerian current measurements by means of moored instruments
at 4 to 6 stations across the strait.
The main results are reported by Gacic et al., 1996; however a brief description of the water masses properties which are found in the strait zone will be given here.
In the surface layer the flow through the strait appears to be subject to seasonal fluctuations due to both meteorological factors and thermohaline differences between the Adriatic and Ionian Surface Waters (ASW and ISW). In winter, when the Adriatic waters are denser than the Ionian and south-easterly winds prevail over the region, an inflow (into the Adriatic) of ISW occurs along the Albanian coast and in the central part of the strait, while an outflow of ASW is found along the western side. In summer, when the meteo-oceanographic conditions reverse, outflow predominates along the Italian coast and in the central part of the strait, while the ISW inflow is concentrated in a narrow coastal band on the eastern side.
In the intermediate layer, there is an outflow of Adriatic water along the Italian shelf and slope, while an inflow of highly saline Levantine Intermediate Layer (LIW) occurs in the remaining part of the strait, its main nucleus being centered at about 300 m depth.
Finally, in the bottom layer, the deep water formed
in the Adriatic outflows into the northwestern Ionian basin, and subsequently
spreads towards and throughout the bottom layer of the Levantine Basin.
This water mass, the Adriatic Bottom Water (ABW), was found to be the main
component of the Eastern Mediterranean Deep Water (EMDW) (Pollak, 1951).
The aim of the present paper is to follow the temporal
and spatial evolution of the LIW, defined as the water with salinity equal
or higher than 38.75, during the time interval covered by the Otranto Project.
by means of a spatial interpolation technique of the salinity field coupled
with a three-dimensional visualization, employing UNIRAS software for gridding,
interpolations and displaying.
Experimental

The grid of the hydrological stations occupied during
the six oceanographic cruises is shown in
Figure 1. The cruises calendar
was as follows:
Cruise Otranto1 Otranto2 Otranto3 Otranto4 Otranto5 Otranto6 From 22/02/94 17/05/94 06/08/94 31/10/94 07/02/95 19/05/95 To 05/03/94 22/05/94 16/08/94 05/11/94 13/02/95 24/05/95
The ships employed were R/V Urania of the Italian Consiglio Nazionale delle ricerche, R/V Aegaeo of the National Centre for Marine Research of Athens, ITS Magnaghi of the Istituto Idrografico della Marina and R/V Alliance of the NATO SACLANT Undersea Research Centre.
The thermohaline measurements were performed by means of a CTD SeaBird 911 (cruises 1 to 5) and a CTD N.Brown Mk3C (cruise Otranto 6), coupled with a 24-bottles Rosette for water sampling. The sensors were calibrated before each cruise and controlled by means of SIS reversing thermometers and frequent discrete salinity determinations by means of an Autosal salinometer.
The CTD data were collected only during the downcast,
at a sampling frequency of 24 Hz, while the instrument was lowered through
the water mass at a rate of about 1 m/s. The first data processing was
carried on board: the data were cleaned to eliminate spikes and misrecordings
and subsequently averaged over 1 dbar pressure intervals. Salinity was
computed from pressure, temperature and conductivity averaged values, according
to the UNESCO (1983) algorithm. The final adjustment of temperature and
salinity values was performed on land, after having analized the data sets
coming from thermometers readings as well as from salinity determinations.
Figure 1. shows also the area in which the temporal and spatial evolution of LIW was studied; it is delimited by a rectangular grid which was chosen taking into account the following criteria:
According to these criteria, the grid was designed with the following features:
- spatial extension:

From the salinity data measured at sea the salinity
field was subsequently estimated at the locations where the grid lines
intersect. This grid fitting was made employing the software (UNIRAS, 1988a)
AGL/Interpolations, which is a library of several FORTRAN subroutines that
together act as a package for gridding and interpolation of mapping data.
Since the LIW layer reaches the maximum depth of about 700 m, this procedure
was repeated from the surface layer down to this depth, with a vertical
step of 20 m. In this way a 3-dimensional grid of 2592 nodes was obtained,
with a total volume of 3703 km3, being 3264 of which occupied
by the sea, owing to the bottom topography
(see Figure 2).
To visualize the 3-dimensional salinity field so
obtained, the AGL/Blocks (UNIRAS, 1988b) software was employed, i.e. a
library of FORTRAN subroutines which allow a graphical presentation of
spatially varying phenomena using block diagrams. All the maps of the present
paper show the resulting "cube" as seen from South-East, as indicated
by the arrow of
Figure 1.
Results and discussion

The LIW pattern during the investigated period
(Figure 3)
shows not only a seasonal variability but also an interannual one, with
the features of the sixth Otranto cruise (May 1995) quite different from
the previous five ones. In fact, the situations met during these cruises
do not show remarkable differences: the layer of maximum salinity (from
38.80 to 38.85) is located at a depth ranging from 200 (Otranto 3) to 250
meters (Otranto 5) and occupies the eastern face of the cube or only its
south-eastern corner (Otranto 2), while only during the autumn cruise Otranto
4 this layer is restricted to few "spots". On the other hand
the maximum thickness of the LIW layer varies from a minimum of 220 m to
a maximum of about 300 m (cruises Otranto 2 and 5, both performed during
the winter period), while it does not reach the western side of the cube
again during the cruise Otranto 4, which appears to be the poorest in LIW.
The LIW features met during the last Otranto cruise
show, on the contrary, a sudden change from the previous situations, from
three points of view: the salinity maximum value, its position and the
volume occupied. In fact the salinity reaches values as high as 38.92,
which were never found before, and the depth of this maximum rises to 150
m. At the same time the LIW layer shows a maximum thickness of about 500
m, the volume occupied increases and it appears compressed against the
eastern side of the cube.

A better and more immediate understanding of the
LIW evolution may be easily reached employing an interesting facility offered
by the graphical displaying software. It consists in making visible the
inner part of the studied volume simply setting to "undefined"
all the grid nodes of the external part: this will make the cells transparent
when the grid is countured.
Figure 4
shows the inner structure of the six
cubes, which were made partially transparent to evidentiate the level of
the salinity maximum and the peculiar features found during the sixth cruise.

With this simple contrivance it is also possible
to display only the LIW body, setting to "undefined" all the
grid nodes where the salinity is less than 38.75. The results are shown
in
Figure 5, where again the different situation of the May 1995 cruise
is evident as well as the minimum LIW volume of the autumn 1994 cruise.

As in the Otranto Strait area several previuos cruises
were carried out, mainly in the frame of the POEM program, this kind of
technique was employed on these data too, to look at the LIW pattern in
previous years. The results are reported in
Figure 6, which shows the situations
met during the POEM cruises 1 (October 1985), 2 (March 1986) and 5 (August
1987). One can easily see that the LIW amount was always larger than during
the Otranto survey, also if the maximum salinity did never reach the high
values measured during the May 1995 cruise. On the other hand the LIW layer
always reached the westernmost side of the cube, also if during the POEM
2 cruise it was limited to a thin vertical layer facing the southern (Ionian)
face of the cube.

Finally, the technique of the "undefined"
setting value of the non-LIW grid nodes, allows to compute the LIW percentage
simply by evaluating the ratio between the not modified and the total grid
nodes number, after having subtracted from the latter one the number of
the nodes occupied by the bottom, as shown in
Figure 2. The results, summarized
in
Figure 7, indicate that the LIW amount found during the period covered
by the cruises Otranto 1 to 5 (February 1994 - February 1995) ranged with
small oscillations from 15 to 22%, while during the second half of the
eighties its mean value was higher, ranging from 38 to 49%. On the other
hand there are no data enough up to now to state wether the value of 29%
found during the last Otranto cruise of May 1995 indicates the beginning
of a new period of increase of LIW amount or not.
As a conclusion, it is possible to state that the
variability of the Levantine Intermediate Water in the area of the Otranto
Strait is both spatial and temporal, the latter being both of seasonal
and interannual nature. The variations can be easily followed in terms
of LIW volume, position and also maximum salinity value and depth by means
of the three-dimensional representation of the salinity field. This technique
allows to get an immediate and comprehensive idea both of the field extension
and of its structure at any level and/or at any vertical section, making
easy the individuation of the water
Acknowledgements
This work was supported by the European Community,
under the contract MAS2-CT93-0068 for the project "Hydrodynamics and
Geochemical Fluxes in the Strait of Otranto" and by the Italian Consiglio
Nazionale delle Ricerche (CNR), contracts 86.00194.02 and 87. 1103.02 for
the POEM project.
References
Gacic M., V. Kovacevic, B. Manca, E. Papageorgiou,
P.M. Poulain, P. Scarazzato and A. Vetrano (1996): Thermohaline properties
and circulation in the Strait of Otranto. Dynamics of Mediterranean Straits
and Channels, Bull. Inst. oceanogr., Monaco, n. special 17, CIESM Science
Series n. 2, F. Briand Ed., 117-145.
Pollak M.I., 1951: The sources of deep water in the Eastern Mediterranean Sea. J. Mar. Res., 10, 128-15
Orlic M., M. Gacic and P. La Violette, 1992: The currents and circulation of the Ariatic Sea. Oceanol. Acta, 15, 2, 109-124.
Ovchinnikov I.M., 1966: Circulation in the surface and intermediate layers of the Mediterranean. Oceanology, 6, 48-59.
UNESCO, 1983: Algorithms for computation of fundamental properties of seawater. Unesco technical papers in marine science n. 44.
UNIRAS, 1988a: AGL/Interpolations, Version 6, User Guide and Reference Manual, Uniras A/S, Denmark, 80 pp.
UNIRAS, 1988b:AGL/Blocks, Version 6, User Guide and Reference Manual, Uniras A/S, Denmark, 99 pp.
Wust, G., 1961: On the vertical circulation of the Mediterranean Sea. J. Geoph. Res., 66, 3261-3271.
Zore-Armanda M., 1969: Water exchange between the Adriatic and the Eastern Mediterranean. Deep-Sea Res., 16, 171-178.
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