Modelling 2: Introduction to modelling assignment. A basic physical-biological model. Model equations. Model operation. The assignment.

Slides:



Advertisements
Similar presentations
Parametrization of surface fluxes: Outline
Advertisements

Introduction Irina Surface layer and surface fluxes Anton
Section 2: The Planetary Boundary Layer
0 The vertical structure of the open ocean surface mixed layer 11:628:320 Dynamics of Marine Ecosystems.
Introduction to Biological Oceanography Biological Oceanography -Productivity-
Nutrient Cycles Eutrophication Nitrogen –Chemical Forms in the Aquatic Environment –Chemical Transformations –Cycle f-ratio Carbon.
Oceans.
Reading: Text, (p40-42, p49-60) Foken 2006 Key questions:
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,
The material in this slide show is provided free for educational use only. All other forms of storage or reproduction are subject to copyright- please.
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.
Ken T.M. Wong Department of Civil Engineering, The University of Hong Kong Red Tide Field Monitoring and Forecasting at Kat O and Lamma Island, HK.
About Estuarine Dynamics
Surface Exchange Processes SOEE3410 : Lecture 3 Ian Brooks.
Atmospheric Analysis Lecture 3.
Linear Wave Theory fundamental description: L - wave length H - wave height T - period d - water depth Shore Protection Manual, 1984 Overview of Waves.
Trait-based models for functional groups Jorn Bruggeman Theoretische biologie Vrije Universiteit Amsterdam.
Institute of Oceanogphy Gdańsk University Jan Jędrasik The Hydrodynamic Model of the Southern Baltic Sea.
Prof. Heidi Fuchs
The Ocean’s primary Productivity
Phytoplankton Dynamics Primary Productivity (g C/m 2 /yr) Gross (total) production = total C fixed Net production = C remaining after respiration Standing.
Wind Driven Circulation I: Planetary boundary Layer near the sea surface.
Chapter 20 Section 1 Review Page 500
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.
Monin-Obukhoff Similarity Theory
Surface wind stress Approaching sea surface, the geostrophic balance is broken, even for large scales. The major reason is the influences of the winds.
Open Oceans: Pelagic Ecosystems II
MAMA Malta meeting, January 2004 Expert Meeting Towards Operational ecological models in coastal areas
Evaporation What is evaporation? How is evaporation measured? How is evaporation estimated? Reading: Applied Hydrology Sections 3.5 and 3.6 With assistance.
Simple coupled physical-biogeochemical models of marine ecosystems
Courtney K. Harris Virginia Institute of Marine Sciences In collaboration with Katja Fennel and Robin Wilson (Dalhousie), Rob Hetland (TAMU), Kevin Xu.
Mind maps (from interviews) Atmosphere.mm Ocean.mm Mind maps (from interviews) Atmosphere.mm Ocean.mm Query tools CIM software.png CIM software.png CIM.
Regional Advanced School on Physical and Mathematical Tools for the study of Marine Processes of Coastal Areas Physical and Biogeochemical Coupled Modelling.
VERTICAL STRUCTURE OF THE OCEAN – from Knauss Chapters 1 and 2 Oceanographers divide the ocean into zones.
Modelling 1: Basic Introduction. What constitutes a “model”? Why do we use models? Calibration and validation. The basic concept of numerical integration.
OCEAN CURRENTS.
Plankton and Their Importance in the Marine Ecosystem Video.
Prof. Heidi Fuchs Suggestions for getting an A How to deal with equations? –Don’t panic! –If you understand an equation, you.
Equations that allow a quantitative look at the OCEAN
Momentum Equations in a Fluid (PD) Pressure difference (Co) Coriolis Force (Fr) Friction Total Force acting on a body = mass times its acceleration (W)
USE THESE VALUES. e(T) = e s (T Dew ) PRACTICE WITH STABILITY.
Transport in Aquatic Ecosystems Horizontal Inflows - Advection Turbulence – critical for vertical fluxes.
The Aquatic Environment. Introduction Aquatic systems are those in which the primary medium inhabited by organisms is water. Aquatic systems are those.
Open Oceans: Pelagic Ecosystems III. Comparing the makeup of water and plankton Mean Elemental Ratios of N, and P Organisms: 16.0N / 1P Sea Water: 14.7N.
UNIT THREE: Matter, Energy, and Earth  Chapter 8 Matter and Temperature  Chapter 9 Heat  Chapter 10 Properties of Matter  Chapter 11 Earth’s Atmosphere.
Class #14 Wednesday, September 30 Class #14: Wednesday, September 30 Chapters 6 and 7 Thermal Circulation, Scales of Motion, Global Winds 1.
General Description of coastal hydrodynamic model.
Nutrient Cycles in Marine Ecosystems Part II
PATTREN OF PRIMARY PRODUCTION
WLRD Science Seminar Sammamish River Water Quality Model Status Report November 19, 2002.
Conservation of Salt: Conservation of Heat: Equation of State: Conservation of Mass or Continuity: Equations that allow a quantitative look at the OCEAN.
Marine Ecosystem Simulations in the Community Climate System Model
Observed Structure of the Atmospheric Boundary Layer
Ch Life in the Oceans. Ocean Chemistry and Marine Life Ocean plants and animals remove and return many types of nutrients and gases to the water.
Oceans. Why is the Ocean Salty? 1. The ocean is salty because of dissolved chemicals eroded from the Earth's crust and washed into the sea. 2. Ejections.
CHANGSHENG CHEN, HEDONG LIU, And ROBERT C. BEARDSLEY
Lab 5 Physical and Chemical Properties of Sea Water
Regional Advanced School on Physical and Mathematical Tools for the study of Marine Processes of Coastal Areas Physical and Biogeochemical Coupled Modelling.
Sedimentology Flow and Sediment Transport (1) Reading Assignment: Boggs, Chapter 2.
0 The vertical structure of the open ocean surface mixed layer 11:628:320 Dynamics of Marine Ecosystems.
LOCAL WINDS Land and Sea Breezes At night the reverse takes place.
Nutrient Cycles in Marine Ecosystems – Part 3
Simple coupled physical-biogeochemical models of marine ecosystems
Nutrient Cycles in Marine Ecosystems Part II
Earth’s Atmosphere.
Oceans.
Ocean circulation: key questions
Lecture 1: Introduction
Impacts of Air-Sea Interaction on Tropical Cyclone Track and Intensity
Presentation transcript:

Modelling 2: Introduction to modelling assignment. A basic physical-biological model. Model equations. Model operation. The assignment.

A basic physical-biological model. The IMPRESS model - a recent modification of the Phyto1D model described in: Sharples, J Investigating the seasonal vertical structure of phytoplankton in shelf seas. Marine Models Online, 1, A 1-D (vertical) coupled physical- biological model. Applicable to shelf seas. Uses supplied meteorological and tidal data. Uses a turbulence closure scheme. Cell-quota threshold limitation model of primary production n-2 n-1 n velocities and scalars vertical turbulent mixing coefficients Wind stress Cooling Heating Tidally-oscillating slope z zz Seabed friction and nutrient source z=0 z=h

Model equations. (The Basics) Changes in velocity Oscillating pressure gradient (m tidal constituents) Coriolis force Frictional coupling through water (including wind stress and bottom friction boundary conditions. The structure of the water currents is controlled by the equation of motion: The boundary conditions (friction at the sea surface and the sea bed)  shear in the current profile  turbulence  mixing

Meteorological forcing. The model water column is heated by: Solar irradiance at the surface. Exponential decay of heat down through the water column. Heat losses from the surface caused by infra-red back radiation, conduction, and evaporation. Surface wind stress. Turbulent mixing of the heat through the water.

S N1 N1 X1X1 N2 N2 X2X2 PAR grazing and respiration recycled nutrient uptake sink / swim S = dissolved inorganic nitrogen N = algal internal nutrient X = algal chlorophyll biomass Subscripts 1 and 2 refer to the two possible phytoplankton taxa/ species Schematic diagram of the biological scalars and processes at each grid cell. Vertical turbulent mixing between neighbouring grid cells The biological model. At each grid cell: 1 or 2 species of phytoplankton (we will only use one species). Phytoplankton consist of chlorophyll (or carbon) and an internal nutrient store. Phytoplankton receive light (PAR; solar irradiance from the meteorological data, with an exponential depth profile). Phytoplankton take up nutrients from the surrounding dissolved inorganic nitrogen (S). Phytoplankton and nitrogen are affected by turbulent mixing.

Modelling phytoplankton - chlorophyll biomass X. At each grid cell in the model phytoplankton changes are caused by…... Turbulent mixing through the water column between grid cells Growth within the grid cell (can be positive or negative) Losses to grazers (always negative) Sinking or swimming of the phytoplankton Growth requires sufficient light and a store of nutrients. Sufficient light  phytoplankton need to remain above their critical depth.

Modelling turbulent mixing. A key component of the model is the ability to link the ability of turbulence to mix properties vertically through the water to the strength of the stability of the water. At each grid cell in the model, the turbulent diffusivity and turbulent viscosity are related to the gradient Richardson number. K z, N z Ri Ri critical

The Assignment. The aims of this exercise are: Develop an appreciation of how coupled physical-biological models can be used to investigate processes in the ocean. Appreciate the need to make sure a model is applicable to the question you are addressing. Develop an appreciation of how sensitive model results are to the driving parameters. Use the model to develop your understanding of the physics and biology of shelf seas. Use the model as an experimental tool, developing your ability to plan, record, and report on a methodical investigation. You need the documents: model.doc assignment.doc