Coastal Ocean Dynamics Baltic Sea Research Warnemünde

Slides:



Advertisements
Similar presentations
INTERNAL WAVE GENERATION, BREAKING, MIXING AND MODEL VALIDATION ALAN DAVIES (POL) JIUXING XING (POL) JARLE BERNTSEN (BERGEN)
Advertisements

Tides Tide producing forces Semi-diurnal; diurnal tides
Hans Burchard … … and many others from inside and outside IOW Leibniz Institute for Baltic Sea Research Warnemünde The.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde From the Navier-Stokes equations via the Reynolds decomposition.
Chapter 16 The Dynamic Ocean
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Trying to model Greenland’s fjords with GETM.
Direct numerical simulation study of a turbulent stably stratified air flow above the wavy water surface. O. A. Druzhinin, Y. I. Troitskaya Institute of.
Tides - The Last Wave Information by the University of California (Riverside) updated in 2014.
The Open Shelf Sea. 1. The primary source of buoyancy is surface heat flux. c p = specific heat capacity of seawater (= 3900 J kg -1 K -1 ) mean water.
Modeling the M 2 and O 1 Barotropic and Baroclinic Tides in the Gulf of Mexico Using the HYbrid Coordinate Ocean Model (HYCOM) Flavien Gouillon 1 ; B.
Examples of secondary flows and lateral variability.
Ocean Tides Introduction Definition and terms
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Periodic straining, a process which lakes (due to seiches)
9.2 Ocean Waves, Tides and Currents
About Estuarine Dynamics
Indirect Determination of Surface Heat Fluxes in the Northern Adriatic Sea via the Heat Budget R. P. Signell, A. Russo, J. W. Book, S. Carniel, J. Chiggiato,
1 Variability of sea surface temperature diurnal warming Carol Anne Clayson Florida State University Geophysical Fluid Dynamics Institute SSTST Meeting.
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.
Hans Burchard Baltic Sea Research Institute Warnemünde, Germany Collaboration: Thomas Badewien, Karsten Bolding, Götz Flöser,
A Circulation Model to Investigate the Movement of Wastes from an Open Ocean Aquaculture Site David W. Fredriksson U. S. Naval Academy NOAA Research -
Potential temperature ( o C, Levitus 1994) Surface Global zonal mean.
Growth and decay of the mixed layer and seasonal thermocline from November 1989 to September 1990 at the Bermuda Atlantic Time-series Station (BATS) at.
An Assimilating Tidal Model for the Bering Sea Mike Foreman, Josef Cherniawsky, Patrick Cummins Institute of Ocean Sciences, Sidney BC, Canada Outline:
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 1, Tom P. Rippeth 2 and Ulf Gräwe 1 1. Leibniz Institute for Baltic Sea Research Warnemünde, Germany 2. School of Ocean Sciences, University.
Define Current decreases exponentially with depth and. At the same time, its direction changes clockwise with depth (The Ekman spiral). we have,. and At.
Wind-Driven shelf dynamics and their influences on river plumes: implications for surface parcel transport Ed Dever, Oregon State University Image: Hickey.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde How to make a three-dimensional numerical model that.
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.
Sara Vieira Committee members: Dr. Peter Webster
Physical and Chemical Oceanography
Estimating Diffusivity from the Mixed Layer Heat and Salt Balances Meghan F Cronin 1, et al. 1 NOAA Pacific Marine Environmental Laboratory 4 April 2013.
High-resolution 3D modelling of oceanic fine structures using vertically adaptive coordinates Hans Burchard 1, Ulf Gräwe 1, Richard Hofmeister 2, Peter.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde, Germany Cooperation: Thomas Badewien 1, Johannes Becherer 2, Kaveh Purkiani 2 Götz.
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 ?
The Ocean General Circulation (satellite). Mean Circulation in the Ocean Gulf Stream.
POLLUTION OF COASTAL ZONES DUE TO DEFLECTIONS OF RIVERS UNDER THE INFLUENCE OF THE CORIOLIS FORCE Grigoriadou V., Konidaris A., Angelidis P., Kotsovinos.
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
Marine Physics Chapters 8, 9, 10 JUST COPY WHAT IS UNDERLINED!!!!!!
Mean 20 o C isotherm (unit: meter) The thermocline zone is sometimes characterized by the depth at which the temperature gradient is a maximum (the “thermocline.
General Description of coastal hydrodynamic model.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde, Germany Cooperation: Thomas Badewien 1, Johannes Becherer 2, Götz Flöser 3, Ulf Gräwe.
Investigation of Mixed Layer Depth in the Southern Ocean by using a 1-D mixed layer model Chin-Ying Chien & Kevin Speer Geophysical Fluid Dynamics Institute,
1D Long-term Modelling of Longshore Sediment Transport
Land-Ocean Interactions: Estuarine Circulation. Estuary: a semi-enclosed coastal body of water which has a free connection with the open sea and within.
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.
Do Now 4/28/14 1.Which of the following factors affects and/or helps create ocean currents? a) Wind b) Temperature c) Salinity (Salt) Levels d) Shorelines.
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,
Role of internal wave mixing in coastal seas with sloping bottoms
Reduction of numerical mixing by means of vertically adaptive coordinates in ocean models Hans Burchard 1, Ulf Gräwe 1, Richard Hofmeister 2, Knut Klingbeil.
Coastal Oceanography Outline Global coastal ocean Dynamics Western boundary current systems Eastern boundary current systems Polar ocean boundaries Semi-enclosed.
Center for Ocean-Atmospheric Prediction Studies
The effect of tides on the hydrophysical fields in the NEMO-shelf Arctic Ocean model. Maria Luneva National Oceanography Centre, Liverpool 2011 AOMIP meeting.
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
Leibniz Institute for Baltic Sea Research
Numerical Modelling of SImPSon
Hans Burchard, Elisabeth Schulz and Henk Schuttelaars
TALLEY Copyright © 2011 Elsevier Inc. All rights reserved
LCDR John Hendrickson 17SEP2008
하구및 연안생태Coastal management
Operational Oceanography OC/MR3570 William Swick
하구및 연안생태Coastal management
하구및 연안생태Coastal management
Physical and Chemical Oceanography
Presentation transcript:

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

North Sea bathymetry Source: Werner Alpers

Exclusive Economic Zones North Sea catchment areas and Exclusive Economic Zones Weser Elbe Rhine Source: OSPAR Commission

Annual cycle of sea surface temperature in North Sea

Generation of the semi-diurnal lunar (M2) tide http://www2.astro.psu.edu/users/cpalma/astro10/class21.html

Generation of the semi-diurnal solar (S2) tide http://www2.astro.psu.edu/users/cpalma/astro10/class21.html

Tidal chart for the M2 tide (phase lines) http://en.wikipedia.org/wiki/Amphidromic_point

Why do the tides in the North Sea look like this ? Tidal waves enter into North Sea through northern boundary and English Channel. Phase propagation is c = (g * depth)1/2, g = 9.81 m/s2 (depth = 40 m  c = 20 m/s = 72 km/h) Due to Earth rotation, tidal waves are Kelvin waves, leaning on a coast to the right. Energy loss due to bed friction: tidal waves loose power during their journey through the North Sea.

Tidal chart for the M2 tide full lines: amplitude dashed: phase (Source: POL)

Tidal chart for the M2 tide (phase lines)

M2 tidal chart of Southern North Sea Amphidromic point M2 tidal chart of Southern North Sea Prandle, 1981

Tidal propagation into the Baltic Sea is blocked !

Tides in the Wadden Sea (as seen in 200 m resolution model)

Wadden Sea model: M4 tidal elevations (phase and amplitude) as validation data. Gräwe et al., in prep.

Seasonality of tidal forcing How does this affect sediment transport due to tidal asymmetries (M4)? Gräwe et al. (in prep.) Müller et al. (in prep.)

Stratification in the North Sea Besides tides, seasonal stratification is characteristic for the North Sea dynamics. Annual cycle of temprature stratification in the Northern North Sea (as seen from a 1D model) Bolding and Burchard (2002)

Stratification is spatially not homogeneous Tidal front Doggerbank Doggerbank Model results by Burchard & Bolding, 2002

Tidal fronts Tidal fronts (stratified in deep, mixed in shallow water) are an environmentally very important phenomenon. Thus, in shallow water the bottom sediment is in direct contact with the surface waters, whereas in deeper waters, the bottom layers are clearly separated from the surface wates.

What determines the position of tidal fronts ? Stabilising: water depth H, surface buoyancy flux Q (heat flux, net precipitation). Destabilising: tides given as tidal velocity amplitude u. Important parameter by dimensional analysis: (Q * H) / u3 Large: stably stratified; Small: mixed Note: H / u3 is the famous Simpson-Hunter (1974) parameter.

Tidal mixing fronts in the Irish Sea stratified & deep mixed & shallow mixed & very shallow & warm or stratified due to river run-off Satellite images courtesy Alejandro Souza

Tidal Mixing fronts in the Irish Sea Stratification Simpson-Hunter parameter Numerical model result, Souza et al., in press.

Environmental effects of seasonal thermal stratification Surface heat flux (cumulated) during FLEX‘76 Burchard, 2002

FLEX 1976 Lateral effects are small, such that one-dimensional modelling may be successful Burchard, 2002

Summer stratification along 56°North Sea transect

Summer chlorophyll conc. along 56°North Sea transect

Northern North Sea: Annual cycle of stratification and primary production Burchard et al., 2005 Burchard, 2002

Rotating bulk shear in Monterey Bay Itsweire et al. (1989)

PROVESS-NNS study site (observations: Sep-Nov 1998) Wind ADCP, CTD, MST

Bulk property observations in NNS Wind Bulk shear squared Bulk shear direction vs. inertial rotation

Theory I 1D dynamic equations: Layer averaging:

Dynamic equation for bulk shear squared: Conclusion: Assuming bed stress being small, bulk shear is generated by the alignment of wind vector and shear vector.

Application of theory to observations

Impact of bulk shear on diapycnal mixing Conclusion: Increased interfacial mixing rates correlate with high shear. Can we resolve this in 3D models?

Transect in NNS Observations (Scanfish data from BSH) Model results (GETM with adaptive coordinates) Gräwe et al. (in prep.)