die dynamik von trübungszonen in gezeitenästuaren - iow · 0.5 setgra y0 0.5 setgra y1 die...

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0.5 setgray0 0.5 setgray1 Die Dynamik von Trübungszonen in Gezeitenästuaren Hans Burchard [email protected] Institut f ¨ ur Ostseeforschung Warnem ¨ unde FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 1/23

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Die Dynamik von Trübungszonenin Gezeitenästuaren

Hans [email protected]

Institut fur Ostseeforschung Warnemunde

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 1/23

Program of the talk

• Phenomenology• Conceptual models• Numerical simulations (historical)• Numerical simulations (recent)• Conclusions

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 2/23

Map of the tidal Elbe

9°00' 10' 20' 30' 40' 50' 50' 40' 30' 10°00'

54°00'

53°30' 0 10km

53°40'

53°50'

20' 8°10'

54°10'

Scharhörn

Gr. Knechtsand

Neuwerk

Cuxhaven

Friedrichskoog

Oste

Nord-

Ost

see-

Kana

l

Stör

Wischh. Süderelbe

Schwinge

Krückau

Pinnau

Este

Lühe

Med

em

Brunsbüttel

Glückstadt

Stade

Hamburg 630

640 650

660

670

680

690

700

710 720

730

740

Strom-km 700

Trischen

Watt

WGE Be 10.96

Mühlen- berger Loch

Pagensand

Medemgrund

Neufelder Sand

Großer Vogelsand

Medemsand

Gelbsand

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 3/23

PhenomenologySPM observations in the tidal Elbe

Pers. comm. Jens Kappenberg

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 4/23

PhenomenologySPM observations in the tidal Elbe

Pers. comm. Jens Kappenberg

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 5/23

PhenomenologySPM observations in Columbia River

Salinity

SPM

Pers. comm. David Jay, Phillip Orton

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 6/23

Classical conceptual models• Flocculation of riverine colloids due to the ion

content of the saline sea water (Lucht [1953]).• "The peculiar process of mixing between riverine

and marine water in the tidal zone works as aSPM trap." (Postma und Kalle [1955]).

Schoellhamer & Burau, 1998

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 7/23

Classical conceptual modelsDensity currents from numerical lock exchange

t = 5 h

-15

-10

-5

10 20 30 40 50 600

1

2

3

4

5

x / km

z / m

PSfrag replacements

σt / kg m−3

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 8/23

Conceptual model

Jay & Musiak, 1994

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 9/23

Computer simulations

Burchard & Baumert, 1998

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 10/23

Computer simulations

Burchard & Baumert, 1998

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 11/23

Computer simulations

Burchard & Baumert, 1998

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 12/23

Turbulenzmodellierung

http

://w

ww

.got

m.n

et

Challenge

Aim

The Idea

Key features

Software

Fortran code

Test cases

Forcing

How to run?

Information

What's

Publications

E-mail list

FAQ

User Group

Hot Links

Who's Who?

Guestbook

PPM:

10/26/00 20:48:54

New

GOTM is a one-dimensional numerical modeldeveloped and supported by a core team ofocean modellers. GOTM aims at simulatingaccurately vertical exchange processes in themarine environment where mixing is known toplay a key role. GOTM is freely available underthe GPL (Gnu Public License).

The interested user can download the sourcecode, a set of test cases (Papa, November, Flex,...) and a comprehensive report.

You are warmly invited to join the GOTM mailinglist and send any comments/questions to theGOTM team or become a GOTM contributor. TheGOTM developers are grateful to their sponsors.

Page "www.gotm.net" maintained by webmaster. Last update: 10/28/00 18:10:02

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 13/23

Liverpool Bay

SST (Degrees C.)

Land/Cloud

11.0-11.9

12.0-12.9

13.0-13.9

14.0-14.9

15.0-15.9

16.0-16.9

17.0-17.9

18.0-18.9

19.0-19.9

20.0-20.9

21.0-21.9

22.0-22.9

AVHRR Sea Surface Temperature image (11 July 1999, 17:00)

� �� �� �� � � � �

Courtesy Caren E. Binding, BangorFWG-Kolloquium, Kiel, 12. Februar 2003 – p. 14/23

Liverpool Bay

SST (Degrees C.)

Land/Cloud

11.0-11.9

12.0-12.9

13.0-13.9

14.0-14.9

15.0-15.9

16.0-16.9

17.0-17.9

18.0-18.9

19.0-19.9

20.0-20.9

21.0-21.9

22.0-22.9

AVHRR Sea Surface Temperature image (11 July 1999, 17:00)

� �� �� �� � � � �

Courtesy Caren E. Binding, BangorFWG-Kolloquium, Kiel, 12. Februar 2003 – p. 14/23

Liverpool BaySection of Temperature and Salinity

1 1

1 1 .5

1 2

1 2 .5

1 3

1 3 .5

1 4

1 4 .5

1 5

1 5 .5

1 6

3 2 .2

3 2 .4

3 2 .6

3 2 .8

3 3

3 3 .2

3 3 .4

3 3 .6

3 3 .8

3 4

3 4 .2

3 4 .4

2 3 .6

2 3 .8

2 4

2 4 .2

2 4 .4

2 4 .6

2 4 .8

2 5

2 5 .2

2 5 .4

2 5 .6

2 5 .8

2 6

2 6 .2

2 6 .4

2 6 .6

0

-20

-40

-60

0

-20

-40

-60

0

-20

-40

-60

0

-20

-40

-60

100 90 80 70 60 50 40 30 20 10 0

100 90 80 70 60 50 40 30 20 10 0

100 90 80 70 60 50 40 30 20 10 0

Fig 2.a Temperature (Degrees C)

Fig 2.b Salinity (PSU)

Fig 2.c Sigma T (kg/m3)

Distance Along Transect (km)

De

pth

(m

)D

ep

th (

m)

De

pth

(m

)

LB2

Rippeth, Fisher, Simpson [2001]

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 15/23

Liverpool BayObserved and simulated temperature and salinity

Simpson, Burchard, Fisher, Rippeth [2002]

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 16/23

Liverpool BayObserved and simulated current velocity

Simpson, Burchard, Fisher, Rippeth [2002]

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 17/23

Liverpool BayObserved and simulated dissipation rates

Simpson, Burchard, Fisher, Rippeth [2002]

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 18/23

Liverpool BayObserved and simulated dissipation rates

Simpson, Burchard, Fisher, Rippeth [2002]

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 18/23

Three-dimensional modelling

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%$ � & '"( � )$( * $ � *+ $( & � � � ' , * �� -

33.8

33.9

34

34.1

34.2

34.2

34.3

34.3

34.4

34.4

34.5

34.5

34.6

34.6

34.7

34.7

34.8

34.833.8

33.9

34

34.1

34.2 34.3

34.4

34.5

34.5

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34.6

34.7

34.7

34.8

34.8

33.8

33.9

34

34.1 34.2

34.3

34.4

34.4

34.5

34.5

34.6

34.6

34.7

34.7

34.8

34.8

34.8

33.8

33.9

34

34.1

34.2

34.3

34.3

34.4

34.4

34.5

34.5

34.6

34.6

34.7

34.7

34.8

34.8

34.8

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 19/23

Suspended matter moduleTransport equation:

∂tC +∂x(uC)+∂y(vC)+∂z((w−ws)C)−∂z(ν′

t∂zC) = 0 (1)

Bottom boundary condition:

−wsC − ν ′

t∂zC = Fe − Fs (2)

Erosion & sedimentation flux:

Fe =ce

ρ0

(|τb| − τce)+; Fs =

wsCb

τcs

(|τb| − τcs)− (3)

Bottom SPM pool:∂t(B) = Fs − Fe (4)

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 20/23

Two-dimensional experiments

• Salinity and SPM (click for animation), noadvection of turbulence

Salinity and eddy diffusivity (click for animation),no advection of turbulence

Zusammenarbeit mit Manuel Ruiz Villarreal, Spanish Institute of Oceanography, A Coruña

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 21/23

Tide-Elbe in 3D: GETM

9°00' 10' 20' 30' 40' 50' 50' 40' 30' 10°00'

54°00'

53°30' 0 10km

53°40'

53°50'

20' 8°10'

54°10'

Scharhörn

Gr. Knechtsand

Neuwerk

Cuxhaven

Friedrichskoog

Oste

Nord-

Ost

see-

Kana

l

Stör

Wischh. Süderelbe

Schwinge

Krückau

Pinnau

Este

Lühe

Med

em

Brunsbüttel

Glückstadt

Stade

Hamburg 630

640 650

660

670

680

690

700

710 720

730

740

Strom-km 700

Trischen

Watt

WGE Be 10.96

Mühlen- berger Loch

Pagensand

Medemgrund

Neufelder Sand

Großer Vogelsand

Medemsand

Gelbsand

Animation

Zusammenarbeit mit Manuel Ruiz Villarreal, Spanish Institute of Oceanography, A Coruña

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 22/23

Conclusions• In many estuaries, turbidity maxima (ETMs) are

observed at the tip of the salt intrusion.• These types of ETMs have been numerically

simulated with different 2D- and 3D-models.• Two major ETM generation mechanisms have

been pinpointed, residual gravitational circulationand tidal velocity asymmetry.

• The simulation of ETM generation in a realisticestuary has been sucessfully carried out with athree-dimensional model coupling mean flow,salinity, turbulence and suspended matter.

FWG-Kolloquium, Kiel, 12. Februar 2003 – p. 23/23