OCEAN MODELING. Joseph K. Ansong. (University of Ghana/Michigan)

Similar documents
5. General Circulation Models

Alexander Kurapov, in collaboration with R. Samelson, G. Egbert, J. S. Allen, R. Miller, S. Erofeeva, A. Koch, S. Springer, J.

WQMAP (Water Quality Mapping and Analysis Program) is a proprietary. modeling system developed by Applied Science Associates, Inc.

centrifugal acceleration, whose magnitude is r cos, is zero at the poles and maximum at the equator. This distribution of the centrifugal acceleration

Assimilation Impact of Physical Data on the California Coastal Ocean Circulation and Biogeochemistry

Lecture 3. Turbulent fluxes and TKE budgets (Garratt, Ch 2)

Torben Königk Rossby Centre/ SMHI

Comparison between vertical shear mixing and surface wave-induced mixing in the global ocean

OCEAN MODELING II. Parameterizations

Physical Oceanography, MSCI 3001 Oceanographic Processes, MSCI Dr. Katrin Meissner Week 5.

General Curvilinear Ocean Model (GCOM): Enabling Thermodynamics

Lecture 20 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY

Developing Coastal Ocean Forecasting Systems and Their Applications

Development of Ocean and Coastal Prediction Systems

OCEANIC SUBMESOSCALE SAMPLING WITH WIDE-SWATH ALTIMETRY. James C. McWilliams

John Kindle. Sergio derada Igor Shulman Ole Martin Smedstad Stephanie Anderson. Data Assimilation in Coastal Modeing April

Progress in embedding global tides into HYCOM simulations. Brian K. Arbic Institute for Geophysics The University of Texas at Austin

ESCI 485 Air/Sea Interaction Lesson 1 Stresses and Fluxes Dr. DeCaria

Introduction to Atmospheric Circulation

Assessment of the numerical efficiency of ocean circulation model : Hycom contribution to the COMODO project.

P1M.4 COUPLED ATMOSPHERE, LAND-SURFACE, HYDROLOGY, OCEAN-WAVE, AND OCEAN-CURRENT MODELS FOR MESOSCALE WATER AND ENERGY CIRCULATIONS

NCODA Implementation with re-layerization

OCEAN HYDRODYNAMIC MODEL

SIO 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes

Concurrent simulation of the eddying general circulation and tides in a global ocean model

Modeling the Columbia River Plume on the Oregon Shelf during Summer Upwelling. 2 Model

Lecture 1. Equations of motion - Newton s second law in three dimensions. Pressure gradient + force force

Moving Freshwater to the Ocean: Hydrology-Ocean Model Coupling

Overview of HYCOM activities at SHOM

New Salinity Product in the Tropical Indian Ocean Estimated from OLR

Introduction to Ocean Numerical Modeling #0 General Introduction. Global model SSH regional model SST

HYCOM Caspian Sea Modeling. Part I: An Overview of the Model and Coastal Upwelling. Naval Research Laboratory, Stennis Space Center, USA

Susan Bates Ocean Model Working Group Science Liaison

SUPPLEMENTARY INFORMATION

OCN/ATM/ESS 587. Ocean circulation, dynamics and thermodynamics.

2 Observing the Ocean Ships Navigation The Electronics Era 16

Ocean Modeling II. Parameterized Physics. Peter Gent. Oceanography Section NCAR

Ocean Mixing and Climate Change

Data Assimilation and Diagnostics of Inner Shelf Dynamics

ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Lecture 19. Learning objectives: develop a physical understanding of ocean thermodynamic processes

(chose the sign to ensure that it is evaporative)

Study of Forced and Free convection in Lid driven cavity problem

SMS 303: Integrative Marine

Modelling the Channel and the Bay of Biscay using the MARS model. Contributions: Dyneco Physed / Pelagos / Benthos EMH

Léo Siqueira Ph.D. Meteorology and Physical Oceanography

Ocean Modelling: An Introduction for Everybody

Oceanography Quiz 2. Multiple Choice Identify the choice that best completes the statement or answers the question.

Contents. Parti Fundamentals. 1. Introduction. 2. The Coriolis Force. Preface Preface of the First Edition

A numerical model of the circulation in the NW Mediterranean

Assessing Shelf Sea Tides in Global HYCOM

The Shallow Water Equations

Models of ocean circulation are all based on the equations of motion.

NWP Equations (Adapted from UCAR/COMET Online Modules)

Seasonal Simulaions of a coupled ice-ocean model in the Bohai Sea and North Yellow Sea

Chapter 7: Thermodynamics

Boundary Conditions, Data Assimilation and Predictability in Coastal Ocean Models

psio 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes Answer key

For example, for values of A x = 0 m /s, f 0 s, and L = 0 km, then E h = 0. and the motion may be influenced by horizontal friction if Corioli

Sea Level Variability in the Western North Pacific during the 20th Century

ATS 421/521. Climate Modeling. Spring 2015

Numerical Simulations of a Stratified Oceanic Bottom Boundary Layer. John R. Taylor - MIT Advisor: Sutanu Sarkar - UCSD

Storm surge forecasting and other Met Office ocean modelling

A Community Terrain-Following Ocean Modeling System (ROMS)

Donald Slinn, Murray D. Levine

Ocean Model Development for COAMPS

HWRF Ocean: MPIPOM-TC

TIDAL SIMULATION USING REGIONAL OCEAN MODELING SYSTEM (ROMS)

Lecture 17 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Learning objectives: understand the concepts & physics of

Winds and Global Circulation

An Overview of Nested Regions Using HYCOM

Modeling of the sea ice and the ocean in the Nares Strait

Northern Arabian Sea Circulation Autonomous Research (NASCar) DRI: A Study of Vertical Mixing Processes in the Northern Arabian Sea

Lecture #1 Tidal Models. Charles McLandress (Banff Summer School 7-13 May 2005)

Ocean Dynamics. The Great Wave off Kanagawa Hokusai

an accessible interface to marine environmental data Russell Moffitt

Components of the Climate System. Lecture 2: Earth s Climate System. Pop Quiz. Sub-components Global cycles What comes in What goes out

A Study on Residual Flow in the Gulf of Tongking

Developing a nonhydrostatic isopycnalcoordinate

Upper Ocean Circulation

Computer Models of the Earth s Climate

Lecture 2: Earth s Climate System

Lecture 2. Lecture 1. Forces on a rotating planet. We will describe the atmosphere and ocean in terms of their:

High-Resolution Satellite-Derived Ocean Surface Winds in the Nordic-Barents Seas Region in : Implications for Ocean Modeling

Dr Marc Lucas CLS Toulouse, France.

Actual bathymetry (with vertical exaggeration) Geometry of the ocean 1/17/2018. Patterns and observations? Patterns and observations?

BALANCED FLOW: EXAMPLES (PHH lecture 3) Potential Vorticity in the real atmosphere. Potential temperature θ. Rossby Ertel potential vorticity

wavelength (nm)

Rotating stratified turbulence in the Earth s atmosphere

Amita Mehta and Ana Prados

Lecture 9: Tidal Rectification, Stratification and Mixing

A Modeling Study on Flows in the Strait of Hormuz (SOH)

Internal Tides in the Bab el Mandab Strait. Ewa Jarosz and Cheryl Ann Blain Naval Research Laboratory, Stennis Space Center, MS

Internal Wave Modeling in Oceanic General Circulation Models

Eddy-resolving Simulation of the World Ocean Circulation by using MOM3-based OGCM Code (OFES) Optimized for the Earth Simulator

OCN/ATM/ESS 587. The wind-driven ocean circulation. Friction and stress. The Ekman layer, top and bottom. Ekman pumping, Ekman suction

Blended Sea Surface Winds Product

General Circulation. Nili Harnik DEES, Lamont-Doherty Earth Observatory

Properties of the Ocean NOAA Tech Refresh 20 Jan 2012 Kipp Shearman, OSU

Climate Change Research Centre

Size matters: another reason why the Atlantic is saltier than the Pacific C.S. Jones and Paola Cessi

Transcription:

OCEAN MODELING Joseph K. Ansong Email: jkansong@umich.edu (University of Ghana/Michigan)

OUTLINE INTRODUCTION MOTIVATION EQUATIONS OF MOTION INTRODUCTION TO ROMS (Regional Ocean Modeling System) EXAMPLES

Introduction: Approaches to oceanic studies Observational oceanography Emily & Drew - lectures

Introduction: Approaches to oceanic studies Satellite oceanography Ebenezer- lectures

Introduction: Approaches to oceanic studies Chemical oceanography Hydrography/Coastal morphology Liz- lectures Stephan - lectures

Introduction: Approaches to oceanic studies Laboratory tank Experiments Ocean modeling Brian/Dimitris/Joseph - lectures

What is an ocean model? It is a representation, in the form of equations/computer code, describing physical processes of our understanding of how the ocean works. -Dr. Stephenie Waterman

What is an ocean model? Physical processes: a) Ocean movement/dynamics, including horizontal and vertical advection b) Exchange of energy between the ocean and external sources (radiation, precipitation, evaporation, river-runoff, wind, etc) c) 3D mixing and dissipation processes

QUESTION Why do we need ocean modeling when we have alternative means?

Motivation: Why model the ocean?

Motivation: Why model the ocean? Comparatively less expensive Higher spatial/temporal resolution compared to other methods: Satellites provide only surface data, and In-situ measurement are limited in spatial coverage Ability to forecast (e.g. SSH, and positions of major fronts and eddies)

Motivation: Why model the ocean? helps in understanding the 3D dynamics of the ocean on a GLOBAL scale. Dynamics of the ocean include: the general circulation, waves, tides, turbulence, instabilities, convection, mixing, jets, etc.

Motivation: not a competition? Prof. Modeller

Motivation: global ocean currents

Motivation: internal waves Courtesy: Max-Planck institute of Ocean modeling

Where/how do I start learning ocean modeling?

Definition: ocean model It is a representation, in the form of equations/computer code, describing physical processes of our understanding of how the ocean works. -Dr. Stephenie Waterman

Equations of motion Start ocean modeling by understanding the equations of fluid flow (Navier-Stokes equations). Learn how to discretize the equations Understand some numerical analysis Others

Equations of motion r Du Dt 1 r r r + [?] =- Ñ p+ g+ F r o r o acceleration (local + advective) Presure gradient buoyancy Others (frictional, Tides, Winds, etc) where (u=[u,v,w]) are velocity components, p is the pressure, ρ the density, and g gravity.

Equations of motion r Du Dt 1 r r r + [?] =- Ñ p+ g+ F r o r o acceleration (local + advective) call DREW now! Presure gradient buoyancy Others (frictional, Tides, Winds, etc) where (u=[u,v,w]) are velocity components, p is the pressure, ρ the density, and g gravity.

Momentum equations: D u Dt + 2 Ω u = 1 ρ o p + ρ ρ o g + F acceleration (local + advective) Rotation Presure gradient buoyancy Others (frictional, Tides, Winds, etc) where (u=[u,v,w]) are velocity components, Ω is the earth s rotation rate, p is the pressure, ρ the density, and g gravity.

Continuity equation (Conservation of volume) u v w + + = x y z 0

Equation for tracers (Temperature, Salinity, and others), Advection-diffusion equation: T c r u T T T c + Ñ c = k Ñ 2 c T t = Tracers c

Equation of state (Linear) r = r [1-a(T- T ) + b(s-s )] 0 0 0 r 0 0 0 3 1028 kg / m coefficients of thermal, a, o T = 10 C = 283 K and salinecontraction, b S = = 35psu Where T is temperature and S is salinity.

Now that I understand the equations, what next?

Now that I understand the equations, what next?

A.Discretize equations Now that I understand the B. Consider the horizontal grid equations, what next? C. Consider the vertical grid D. Boundary conditions

Discretize equations Continuous equations algebraic equations (discrete set of operations) Discretization methods: Finite difference methods Finite element methods Finite volume methods Example early model grid by Lewis Fry Richardson (1928)

Model grid: horizontal Regular grids: regularly spaced lines On a spherical earth can t have both uniform grid spacing and straight lines

Model grid: horizontal Regular grids: regularly spaced lines On a spherical earth can t have both uniform grid spacing and straight lines Regular lat/lon grids have a problem at the poles where grid lines converge

Model grid: horizontal GHANA Regional grid Clever solution: tripolar grid -circular grid laid over Arctic region with poles on land

Model grid: vertical z-coordinate system based on a series of depth levels. Easy to setup. Difficult to locally increase resolution. terrain-following coordinate system. Mimics bathymetry and allows higher resolution near ocean floor.

Model grid: vertical density (isopycnal)- coordinate system based on density layers. Great in the deep ocean where there s less diapycnal mixing. Poor in regions with high vertical mixing.

Model grid: vertical hybrid-coordinate applies the best suited coordinate system in different regions. Gives improved results but at a high computational cost.

Boundary conditions Free surface Flux exchanges at surface: momentum and tracer (winds, solar radiation, rainfall, precipitation, etc). Ocean bottom Topography/bathymetry Velocity normal to bottom is zero Lateral boundaries (open/closed) Flow normal to solid boundary is zero

Modeling: summary Complex differential equations Set of algebraic equations SURFACE FORCING Step-by-step method of solution (model time stepping) at selected points in space (model spatial grid) Boundary conditions EQUATIONS Boundary conditions It takes years to develop a good ocean model! Bottom boundary

Ocean models MOM (The Modular Ocean Model: http://momocean.org/web ) POM (The Princeton Ocean Model: http://www.ccpo.odu.edu/pomweb/ ) POP (The Parallel Ocean Program: http://www.cesm.ucar.edu/models/cesm1.0/pop2 / )

Ocean models MITgcm (MIT general circulation model: http://mitgcm.org/ ) HYCOM (The Hybrid Coordinate Ocean Model : https://hycom.org/ ) ROMS (Regional Ocean Modeling System: www.myroms.org )

Introduction to ROMS What is ROMS? simple answer: a regional ocean model but there is a lot more to ROMS: active and continuous development of source code Lead by Hernan G. Arango (Rutgers University) and Alexander F. Shchepetkin (UCLA)

Where do I begin?

Learning about ROMS The ROMS website contains: Access to Source Code Documentation (WikiROMS) Access to Online Help Pre-processing Packages Grid generation, Input file creation, etc

Learning about ROMS Become a ROMS user: Register, download, install, compile and run the source code yourself Become a Collaborator: Collaborate with a ROMS user and use your combined expertise to investigate problems Example: A biologist may understand ecosystems but may not wish to do the numerical modeling themselves but would rather interpret the results from a model simulation.

Examples

Test Case 1: Upwelling East-West periodic channel Spatially-uniform winds blowing from east to west Wind stress = 0.1 Pascals Contributed by Anthony Macks and Jason Middleton (Macks, 1993)

Initial temperature distribution Upwelling

Upwelling

Case 2: Regional Modeling

Case 2: Regional Modeling Operational Guidelines: 1. Choose a domain and resolution. 2. Build a bathymetry. 3. Interpolate atmospheric forcing to the domain. 4. Choose vertical structure 5. Interpolate T/S climatology to the model domain and the chosen vertical structure. 6. Run the simulation. 7. Plot and analyze results.

Case 2: Regional Modeling 1/4th degree, ~ 28 km 32 vertical layers Etopo5: http://www.ngdc.noaa.gov/mgg/global/etopo5.html

Surface forcing data COADS05: Surface fluxes of global monthly climatology at 0.5 degrees resolution (Da Silva et al., 1994). http://iridl.ldeo.columbia.edu/sources/.d ASILVA/.SMD94/.climatology/index.html?S et-language=en

Climatological data WOA: World Ocean Atlas 2001 global dataset (monthly climatology at 1 degree resolution) -> 3D fields of temperature, salinity,etc. https://www.nodc.noaa.gov/oc5/woa01/p r_woa01.html

Tidal forcing data Tidal data are derived from the Oregon State University global models of ocean tides TPXO6 and TPXO7 (Egbert and Erofeeva, 2002): http://www.oce.orst.edu/research/po/resea rch/tide/global.html

Results: currents

Results: Tides

Results: tidal time series Challenge: compare to tide-gauge data (Takoradi/Tema)

Challenges to ocean modeling What are some challenges?

Challenges to ocean modeling 1. Variable spatial/temporal scales

Challenges to ocean modeling 2. Complex topography and lateral boundaries 3. Few observational measurements for validation -most available data are confined to upper ocean 4. Availability of computational power