Coastal Ocean Dynamics Baltic Sea Research Warnemünde

Slides:



Advertisements
Similar presentations
Hans Burchard … … and many others from inside and outside IOW Leibniz Institute for Baltic Sea Research Warnemünde The.
Advertisements

Cape Fear River Estuary: Temporal Influences on Salinity and Circulation presented by May Ling Becker July 27, 2006 Wilmington Navassa Cape Fear R. DRAFT.
LANDSAT Aug 31, 2011 Sediment transport and deposition: salinity fronts and storm events David Ralston, Rocky Geyer, John Warner, Gary Wall Hudson River.
Temporal Variability  Tidal  Subtidal Wind and Atmospheric Pressure  Fortnightly M 2 and S 2  Monthly M 2 and N 2  Seasonal (River Discharge)
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Trying to model Greenland’s fjords with GETM.
Useful texts: Mann & Lazier, The Dynamics of Marine Ecosystems, Blackwell Science. Simpson, In: The Sea, vol 10, chapter 5. Simpson, In: The Sea, vol 11,
Estuarine Turbidity Maximum in Delaware Estuary
Hans Burchard Baltic Sea Research Institute Warnemünde, Germany Collaboration: Lars Arneborg, Thomas Badewien, Karsten.
1 University of Utrecht Modelling lateral entrapment of sediments in well-mixed estuaries Photo: mudbanks in the Ems Huib de Swart Karin Huijts, Henk Schuttelaars,
Examples of secondary flows and lateral variability.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Periodic straining, a process which lakes (due to seiches)
Estuaries: Background and Definitions Professor Mike Elliott, Institute of Estuarine & Coastal Studies, University of Hull, University of Hull, HU6 7RX,
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
About Estuarine Dynamics
Introduction to surface ocean modelling SOPRAN GOTM School Warnemünde: Hans Burchard Baltic Sea Research Institute Warnemünde, Germany.
Bangor, 10-12/04/06Simpson Retirement Conference1 Numerical Modelling of SImPSon Hans Burchard Baltic Sea Research Institute Warnemünde Bolding & Burchard.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Coastal Ocean Dynamics First course: Hydrodynamics.
Estuarine Variability  Tidal  Subtidal Wind and Atmospheric Pressure  Fortnightly M 2 and S 2  Monthly M 2 and N 2  Seasonal (River Discharge)
Hans Burchard Baltic Sea Research Institute Warnemünde, Germany Collaboration: Thomas Badewien, Karsten Bolding, Götz Flöser,
About the advantages of vertically adaptive coordinates in numerical models of stratified shelf seas Hans Burchard 1, Ulf Gräwe 1, Richard Hofmeister 2,
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde How to make a three-dimensional numerical model that.
Physical and numerical issues in river plume modeling Rob Hetland Rocky Geyer Rich Signell.
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.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Numerical model applications to lakes and estuaries.
Modelling 1: Basic Introduction. What constitutes a “model”? Why do we use models? Calibration and validation. The basic concept of numerical integration.
Physical Features of Estuaries. Basic Information Estuaries vary in origin, size and type Estuaries vary in origin, size and type Also called: lagoons,
High-resolution 3D modelling of oceanic fine structures using vertically adaptive coordinates Hans Burchard 1, Ulf Gräwe 1, Richard Hofmeister 2, Peter.
Formation of Estuarine Turbidity Maxima in partially mixed estuaries H.M. Schuttelaars 1,2, C.T. Friedrichs 3 and H.E. de Swart 1 1: Institute for Marine.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde, Germany Cooperation: Thomas Badewien 1, Johannes Becherer 2, Kaveh Purkiani 2 Götz.
Hans Burchard and Hannes Rennau Baltic Sea Research Institute Warnemünde Comparative quantification of physically and numerically.
CLOSED ENERGY BUDGETS FOR REGIONAL NUMERICAL SIMULATIONS Parker MacCready University of Washington.
Mixing From Stresses Wind stresses Bottom stresses Internal stresses Non-stress Instabilities Cooling Double Diffusion Tidal Straining Shear ProductionBuoyancy.
Hans Burchard Baltic Sea Research Institute Warnemünde, Germany The invisible extremes: The dynamics of Baltic Sea inflow.
What makes an ocean model coastal ?
S.A. Talke, H.E. de Swart, H.M. Schuttelaars Feedback between residual circulations and sediment distribution in highly turbid estuaries: an analytical.
Typical Mean Dynamic Balances in Estuaries Along-Estuary Component 1. Barotropic pressure gradient vs. friction Steady state, linear motion, no rotation,
FIGURE 2.1 The variation of mean sea level for the past 35,000 years based on data from the Atlantic continental shelf of the United States: the solid.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde, Germany Cooperation: Thomas Badewien 1, Johannes Becherer 2, Götz Flöser 3, Ulf Gräwe.
Land-Ocean Interactions: Estuarine Circulation. Estuary: a semi-enclosed coastal body of water which has a free connection with the open sea and within.
Outline of Presentation: Tidal sediment transport due to spatial vs. flood/ebb asymmetries (1) Minimizing spatial asymmetry → predicts channel convergence.
Hans Burchard 1, Henk M. Schuttelaars 2, and Rockwell W. Geyer 3 1. Leibniz Institute for Baltic Sea Research Warnemünde, Germany 2. TU Delft, The Netherlands.
Some GOTM Physics SOPRAN GOTM School Warnemünde: Hans Burchard Baltic Sea Research Institute Warnemünde, Germany.
Rivers By Emma Harridge.
Hans Burchard 1,2, Joanna Staneva 3, Götz Flöser 4, Rolf Riethmüller 4, Thomas Badewien 5, and Richard Hofmeister 1 1. Baltic Sea Research Institute Warnemünde,
Deep-water Intrusions in the Puget Sound Sally Warner Coastal & Estuarine Fluid Dynamics class Friday Harbor Labs Summer 2006.
Reduction of numerical mixing by means of vertically adaptive coordinates in ocean models Hans Burchard 1, Ulf Gräwe 1, Richard Hofmeister 2, Knut Klingbeil.
Estuaries Chapter 8 – Talley et al. Outline: What is an estuary?
ETM: The Estuarine Turbidity Maximum
Overview of Estuarine (and Puget Sound) Oceanography PSO 2009.
Typical Mean Dynamic Balances in Estuaries Along-Estuary Component 1. Barotropic pressure gradient vs. friction Steady state, linear motion, no rotation,
An introduction to cohesive sediment transport processes
Estuarine Hydrodynamics
Estuarine Circulation and the Knudsen Relation Puget Sound Oceanography 2011.
Salty water inflow (near the bottom) Freshwater input Along the Estuary: Pressure Gradient balanced by Friction (Pritchard, 1956) 0.
Estuarine Variability
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
Leibniz Institute for Baltic Sea Research
Land-Ocean Interactions: Estuarine Circulation
Numerical Modelling of SImPSon
Quantification of spurious dissipation and mixing in ocean models:
하구및 연안생태Coastal management
Hans Burchard, Elisabeth Schulz and Henk Schuttelaars
하구및 연안생태Coastal management
하구및 연안생태Coastal management
하구및 연안생태Coastal management
Deep Circulation Changes in density cause ocean currents Cold Warm
하구및 연안생태Coastal management
Freshwater input Salty water inflow (near the bottom)
하구및 연안생태Coastal management
하구및 연안생태Coastal management
Presentation transcript:

Coastal Ocean Dynamics Baltic Sea Research Warnemünde Seventh course: Estuarine Dynamics Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde hans.burchard@io-warnemuende.de

The principle of estuarine circulation MacCready and Geyer (2010)

Knudsen formula of 1900 Volume conservation: s=0 Salt conservation:

Analytical solution for estuarine circulation Balance between pressure gradient and friction: . With we obtain the analytical solution:

Example solution

Tidal straining after flood after ebb MacCready and Geyer (2010) after Simpson et al. (1990)

Estuarine circulation due to tidal straining 75% level 75% level MacCready & Geyer (2010) after Jay & Musiak (1994)

Simple model simulations of estuarine circulation under tidally energetic conditions With full-scale 1D model (GOTM, www.gotm.net): Gravitational circulation and tidal straining profiles can be decomposed. Estuarine circ. Straining Gravitational Result: Tidal straining makes about 2/3 of estuarine circulation. Burchard and Hetland (JPO 2010)

Lateral circulation in tidal estuaries Flood currents are faster in the deep channel such that salinity becomes higher in the channel centre than at the sides. This lateral density gradient then causes lateral circulation. Ebb is vice versa. MacCready & Geyer (2010)

Floating material collected at tidal front during flood (Conwy River, Wales, UK) Nunes & Simpson (1985)

Estuarine circulation due to lateral circulation During flood high (positive) surface momentum is vertically transported to the near bed region. During ebb, relatively high (negative, but less negative than in channel centre) is transported from the sides to the central near-bed region. This both supports estuarine circulation. MacCready & Geyer (2010)

Enhancement of estuarine circulation in channelised tidal flow (2D slice modelling with GETM) www.getm.eu Burchard et al. (JPO 2011)

Circulation in transverse estuary

of estuarine circulation Transverse structure of estuarine circulation Gravitational circulation Tidal straining circulation Advective circulation Barotropic circulation Burchard et al. (JPO 2011)

Estuarine circulation drives SPM fluxes

Estuarine circulation drives SPM fluxes Observations in the Elbe estuary: Kappenberg et al. (1995)

Generation of estuarine turbidity maxima (ETMs) Sediment accumulation

estuarine circulation on sediment transport Consequences of estuarine circulation on sediment transport ETM ETM = estuarine turbidity maximum Jay and Musiak (1994)

Modelling (2DV) ETM formation Burchard and Baumert (1998)

The lower Elbe River

Observations of ETM in lower Elbe River Run-off Neu-Darchau = 707 m3/s Salinity (g/kg) Courtesy Jens Kappenberg

Modelling (3D) ETM formation ebb tide low water flood tide high water Burchard et al. (2004)

Ems as hyperturbid estuary Talke et al. (2009)

Is there a positive feedback loop in estuarie? Winterwerp, 2013

What happened to the Ems estuary? Pers. Comm. Henk Schuttelaars, 2013 Elbe Winterwerp, 2013