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Hans Burchard 1,2 , Joanna Staneva 3 , Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5 1. Baltic Sea Research Institute Warnemünde, Germany 2. Bolding & Burchard Hyrodynamics, Rostock, Germany 3. ICBM, University of Oldenburg, Germany 4. GKSS Research Centre, Geesthacht, Germany 5. Institute of Physics, University of Oldenburg, Germany [email protected] Impact of density gradients on net sediment transport into the Wadden Sea

Hans Burchard 1,2 , Joanna Staneva 3 , Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

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Impact of density gradients on net sediment transport into the Wadden Sea. Hans Burchard 1,2 , Joanna Staneva 3 , Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5 1. Baltic Sea Research Institute Warnemünde, Germany 2. Bolding & Burchard Hyrodynamics, Rostock, Germany - PowerPoint PPT Presentation

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Page 1: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Hans Burchard1,2, Joanna Staneva3, Götz Flöser4, Rolf Riethmüller4,

and Thomas Badewien5

1. Baltic Sea Research Institute Warnemünde, Germany2. Bolding & Burchard Hyrodynamics, Rostock, Germany

3. ICBM, University of Oldenburg, Germany4. GKSS Research Centre, Geesthacht, Germany

5. Institute of Physics, University of Oldenburg, Germany

[email protected]

Impact of density gradients on net sediment transport

into the Wadden Sea

Page 2: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Observation 1:

Suspended matter

concentrations

are substantially

increased in the

Wadden Sea of the

German Bight.

Total suspended matter from MERIS/ENVISAT on August, 12, 2003.

Page 3: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

The areal view shows

locations of five automatic

monitoring poles in the

Wadden Sea of the

German Bight, operated by

GKSS and University

of Oldenburg. They record

Several parameters in the

water column, such as

temperature and salinity.

Page 4: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Salinity difference HW-LW

Page 5: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Temperature difference HW-LW

Page 6: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Density difference HW-LW

Page 7: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Observation 2:

In winter, salinity is

significantly (1-2 psu)

higher during high water

than during low water.

In summer, temperature

is significantly (1-2 deg)

lower during high water than during low water.

Spiekeroog data

Page 8: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Conclusion 1:

The Wadden Sea water is generally less dense

than the open sea water. Thus, the presence of a

horizontal density gradient has to be assumed

for most of the time.

Page 9: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Hypothesis: This must have a dynamic impact on tidal flow and SPM transport, see the theory of Jay and Musiak (1994) below.

Page 10: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Flood and ebb profilesof current velocity,salinity, eddy diffusivity and SPM concentrationat 3 psu vertical meanSalinity.

Flat bottom Elbeestuary simulation:

Burchard & Baumert 1998

Page 11: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

SPM concentration and

salinity contours

(2,4,6, … 30 psu) for an

idealised Elbe simulation.

Burchard & Baumert 1998

Flat bottom Elbeestuary simulation:

Page 12: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Online since 1999, 50000 logins, mostly from Canada & US

Page 13: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Testing with GOTM supports hypothesis:

Residualonshorenear-bedcurrent

Along-tidesalinity gradientprescribed

Bottom-surface salinity

Page 14: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

3D simulations with GETM for the Sylt-Rømø bight

Approach:

Simulating a closed Wadden Sea basin (Sylt-Rømø bight)

with small freshwater-runoff and net precipitation.

Spin up model with variable and with constant density

until periodic steady state.

Then initialise both scenarios with const. SPM concentration.

Quantify SPM content of fixed budget boxes.

GETM – General Estuarine Transport Model – www.getm.eu

Page 15: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Present GETM characteristics ... physics ...

Solves three-dimensional primitive equations withhydrostatic and Boussinesq approximations.

Based on general vertical coordinates.

Options for Cartesian, spherical and curvilinear coordinates.

Fully baroclinic with tracer equations for salinity, temperature,suspended matter and ecosystem (from GOTM bio module).

Two-equation turbulence closure models with algebraicsecond-moment closures (from GOTM turbulence module).

Wetting and drying of intertidal flats is supported also inbaroclinic mode.

Page 16: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Present GETM characteristics ... numerics ...

Consistent explicit mode splitting into barotropic and baroclinic mode.

High-order positive-definite TVD advection schemes withdirectional split.

Choice of different schemes for internal pressure gradientcalculation.

Consistent treatment of zero-velocity bottom boundary condition for momentum.

Positive-definite conservative schemes for ecosystem processes (in GOTM bio module).

Page 17: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

The Sylt-Rømø bight

Page 18: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Bottom salinity at high and low water during periodically steady state.

Page 19: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Vertically averaged current velocity during full flood and full ebb.

Page 20: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Cross-sectionaldynamics

Page 21: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Tidal periods# 46-55

Page 22: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total water volume and SPM unit mass in budget boxes

Case with density differences, tidal periods # 46-55

Page 23: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total excess SPM mass in budget boxes

Case with density differences, tidal periods # 46-55

Page 24: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total water volume and SPM unit mass in budget boxes

Case with no density differences, tidal periods # 46-55

Page 25: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total excess SPM mass in budget boxes

Case with no density differences, tidal periods # 46-55

Page 26: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total excess SPM mass in budget boxes, slow settling

Case with density differences, tidal periods # 46-55

Page 27: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Total excess SPM mass in budget boxes, slow settling

Case with no density differences, tidal periods # 46-55

Page 28: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

Conclusions:

The hypothesis is strongly supported.

Other mechanisms than density differences

which are also reproduced by the model system

(such as settling lag and barotropic tidal asymmetries)

do not play a major role in this scenario.

Now, targeted field studied are needed

for further confirming the hypothesis.

Page 29: Hans Burchard 1,2 , Joanna Staneva 3 ,  Götz Flöser 4 , Rolf Riethmüller 4 , and Thomas Badewien 5

River Warnow mouth in Warnemünde