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Fourth Study Conference on BALTEX Scala Cinema Gudhjem

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- 92 -<br />

On Variability of the Riverine Waters in the Gulf of Gdansk - a Model<br />

<str<strong>on</strong>g>Study</str<strong>on</strong>g><br />

Andrzej Jankowski<br />

Institute of Oceanology of PAS., Powstańców Warszawy 55, 81-712 Sopot, Poland, e-mail: jankowsk@iopan.gda.pl<br />

1. Introducti<strong>on</strong><br />

A three−dimensi<strong>on</strong>al baroclinic σ-coordinate model was<br />

used to investigate the development and evoluti<strong>on</strong> of<br />

buoyant river plumes in the Gulf of Gdansk (Gdansk Basin).<br />

Situated in the southern part of the Gdansk Basin, the Gulf<br />

of Gdansk, is <strong>on</strong>e of the Baltic's open gulfs. Its<br />

hydrological regime is formed by atmospheric forcing and,<br />

due to wide and deep c<strong>on</strong>necti<strong>on</strong> with the open sea, under<br />

influence of the Baltic proper (Majewski 1990). Its surface<br />

waters are influenced by riverine inflows am<strong>on</strong>g which the<br />

greater significance has those of the Vistula River (with<br />

mean annual discharge about 1000 m3/s Cyberski 1997),<br />

the biggest river in the regi<strong>on</strong>. The mixed river waters can<br />

be observed at the open boundary of the Gulf of Gdansk or<br />

even futher after the str<strong>on</strong>g flood events. The inflow of<br />

riverine waters substantially modifies the envir<strong>on</strong>mental<br />

c<strong>on</strong>diti<strong>on</strong>s in the surface water of the Gulf by reducing its<br />

salinity as well as c<strong>on</strong>taminating it with their polluti<strong>on</strong> load<br />

(Andrulewicz 1996, Cyberska and Krzyminski 1988, 1996).<br />

The purpose of this study is to obtain more detailed<br />

informati<strong>on</strong> <strong>on</strong> fate of riverine water as it mixes and moves<br />

around with the currents and winds in the Gulf of Gdansk<br />

and to test the capabilities of the model to simulate the<br />

characteristic features of the spreading of the riverine waters<br />

during summer flood event.<br />

2. Model<br />

The model is based <strong>on</strong> the Princet<strong>on</strong> Ocean Model (POM) -<br />

code of Blumberg and Mellor 1987 adapted to the Baltic Sea<br />

c<strong>on</strong>diti<strong>on</strong>s (Jankowski 2002a). POM is based <strong>on</strong> a standard<br />

formulati<strong>on</strong> of the c<strong>on</strong>servati<strong>on</strong> equati<strong>on</strong>s for momentum<br />

and mass, utilizing the hydrostatic and the Boussinesq<br />

approximati<strong>on</strong>. The model uses Smagorinsky (1963)<br />

parameterizati<strong>on</strong> for the horiz<strong>on</strong>tal mixing (turbulent<br />

exchange). To calculate the vertical eddy viscosity and<br />

diffusi<strong>on</strong> coefficients a sec<strong>on</strong>d turbulence closure scheme<br />

(Mellor and Yamada 1974, 1982) is applied. The model<br />

domain comprises the whole Baltic Sea with the Gulf of<br />

Bothnia, the Gulf of Finland and the Gulf of Riga as well as<br />

the Danish Straits and Kattegat and Skagerrak. At the open<br />

boundary in the Skagerrak simplified radiati<strong>on</strong>-type<br />

boundary c<strong>on</strong>diti<strong>on</strong>s are applied. The bottom topography of<br />

the Baltic Sea used in the model is based <strong>on</strong> data from<br />

Seifert and Kayser (1995). A “C” numerical grid (Mesinger<br />

and Arakawa 1976) is applied. With a horiz<strong>on</strong>tal resoluti<strong>on</strong><br />

of ≈ 5 km and with 24 σ-levels in vertical, the model<br />

enables variability as well as mesoscale features of the order<br />

of 10 km of currents and thermohaline fields in the Baltic<br />

Sea to be investigated.<br />

To date, the model has been investigated to simulate major<br />

features of the coastal area of the Southern Baltic<br />

(Jankowski, 2002a, 2002b).<br />

3. Model experiments<br />

The climatological forcings were coupled to the model by<br />

means of the so-called method of ’relaxati<strong>on</strong> towards<br />

climatology’ ( cf. Lehmann 1995). Wind field is estimated<br />

from atmospheric surface pressure charts and surface heat<br />

fluxes at the sea surface are calculated with standard bulk<br />

formulae.<br />

In order to simulate the characteristic features of wind-<br />

and river inflow-induced variability of hydrodynamic<br />

c<strong>on</strong>diti<strong>on</strong>s in the Gdansk Basin, the prognostic hindcast<br />

calculati<strong>on</strong>s were performed for summer period of 1980<br />

(summer flood event in the Vistula catchment). Model<br />

runs, starting with climatological m<strong>on</strong>tly means of<br />

temperature and salinity were carried out for the period of<br />

1 st July to 31 st August 1980. For this simulati<strong>on</strong> the model<br />

was forced by realistic forcing estimated <strong>on</strong> 3-hourly<br />

atmospheric data (pressure, air temperature, relative<br />

humidity and the wind - field) taken from (BED, 2000)<br />

and by climatological forcings.<br />

A comparis<strong>on</strong> of computed and measured temperature and<br />

salinity shows that the model reproduces the vertical<br />

structure of seawater temperature and salinity in a good<br />

agreement to the in situ observati<strong>on</strong>s.<br />

Besides the realistic meteorological forcing the spatially<br />

uniform winds from 8 directi<strong>on</strong>s and without wind were<br />

also c<strong>on</strong>sidered. The winds from 8 directi<strong>on</strong>s: SE, S, SW,<br />

W, NW, N, NE and E, of c<strong>on</strong>stant speed over the whole<br />

Baltic area. The wind stress was assumed to be in a range<br />

from 0.025 to 0.1 N/m2.<br />

4. Results and comments<br />

The sea water salinity was used as a natural tracer for<br />

visualizati<strong>on</strong> of spreading of riverine waters in the Gulf of<br />

Gdansk. The numerical experiments visualize the<br />

patterns of weak saline surface water (riverine plume)<br />

propagati<strong>on</strong> <strong>on</strong> their way from the Vistula mouth toward<br />

the open boundary of the Gulf of Gdansk.<br />

The results show that local hydrodynamics near the river<br />

mouth, and c<strong>on</strong>sequently the spreading of the river plume,<br />

are highly dependent <strong>on</strong> the driving river discharge and<br />

wind field characteristics.<br />

In the absence of wind forcing the modeled river plumes<br />

typically c<strong>on</strong>sist of an offshore bulge and a al<strong>on</strong>gshore<br />

currents in the counterclockwise directi<strong>on</strong>.<br />

In the presence of wind forcing the favorable c<strong>on</strong>diti<strong>on</strong>s<br />

for offshore removal of coastal low-salinity waters include<br />

favorable wind stress and circulati<strong>on</strong> pattern highly<br />

dependent <strong>on</strong> open sea hydrodynamic c<strong>on</strong>diti<strong>on</strong>s.<br />

The results of simulati<strong>on</strong>s with space uniform winds<br />

showed that the surface water plume can be particularly<br />

sensitive to the wind stress because it is thin. Its extent<br />

is influenced by the wind stress and varied depending <strong>on</strong><br />

the orientati<strong>on</strong> of the wind stress.<br />

The values of area of mixing z<strong>on</strong>e (salinity < 7 PSU) vary<br />

from 1100-1200 km˛ (wind from E and NE) to 400-500<br />

km2 (winds from W and SW). Under str<strong>on</strong>ger winds the<br />

area of mixing z<strong>on</strong>e decrease almost twice. These findings<br />

and general resp<strong>on</strong>se of surface waters to river run-off<br />

and winds are in agreement with in situ measurements(e.g.

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