Title: Mathematics in the Ocean
1Mathematics in the Ocean
- Andrew Poje
Mathematics Department College
of Staten Island
- M. Toner
- A. D. Kirwan, Jr.
- G. Haller
- C. K. R. T. Jones
- L. Kuznetsov
- and many more!
U. Delaware
Brown U.
April is Math Awareness Month
2Why Study the Ocean?
- Fascinating!
- 70 of the planet is ocean
- Ocean currents control climate
- Dumping ground - Where does waste go?
3Ocean Currents The Big Picture
- HUGE Flow Rates (Football
Fields/second!) - Narrow and North in West
- Broad and South in East
- Gulf Stream warms Europe
- Kuroshio warms Seattle
image from Unisys Inc. (weather.unisys.com)
4Drifters and FloatsMeasuring Ocean Currents
5Particle (Sneaker) Motion in the Ocean
6Particle Motion in the OceanMathematically
- Particle locations (x,y)
- Change in location is given by velocity of water
(u,v) - Velocity depends on position (x,y)
- Particles start at some initial spot
7Ocean Currents Time Dependence
- Global Ocean Models
- Math Modeling
- Numerical Analysis
- Scientific Programing
- Results
- Highly Variable Currents
- Complex Flow Structures
- How do these effect transport properties?
image from Southhampton Ocean Centre. http//www.
soc.soton.ac.uk/JRD/OCCAM
8Coherent Structures Eddies, Meddies, Rings
Jets
- Flow Structures responsible for Transport
- Exchange
- Water
- Heat
- Pollution
- Nutrients
- Sea Life
- How Much?
- Which Parcels?
image from Southhampton Ocean Centre. http//www.
soc.soton.ac.uk/JRD/OCCAM
9Coherent Structures Eddies, Meddies, Rings
Jets
10Mathematics in the OceanOverview
- Mathematical Modeling
- Simple, Kinematic Models
(Functions or Math 130) - Simple, Dynamic Models
(Partial Differential Equations or Math
331) - Full Blown, Global Circulation Models
- Numerical Analysis (a.k.a. Math 335)
- Dynamical Systems (a.k.a. Math 330/340/435)
- Ordinary Differential Equations
- Where do particles (Nikes?) go in the ocean
11Modeling Ocean CurrentsSimplest Models
- Abstract reality
- Look at real ocean currents
- Extract important features
- Dream up functions to mimic ocean
- Kinematic Model
- No dynamics, no forces
- No why, just what
12Modeling Ocean CurrentsSimplest Models
- Jets Narrow, fast currents
- Meandering Jets Oscillate in time
- Eddies Strong circular currents
13Modeling Ocean CurrentsSimplest Models
Dutkiewicz Paldor JPO 94 Haller Poje
NLPG 97
14Particle Dynamics in a Simple Model
15Modeling Ocean CurrentsDynamic Models
- Add Physics
- Wind blows on surface
- F ma
- Earth is spinning
- Ocean is Thin Sheet (Shallow Water Equations)
- Partial Differential Equations for
- (u,v) Velocity in x and y directions
- (h) Depth of the water layer
16Modeling Ocean CurrentsShallow Water Equations
ma F
Mass Conserved
Non-Linear
17Modeling Ocean CurrentsShallow Water Equations
- Channel with Bump
- Nonlinear PDEs
- Solve Numerically
- Discretize
- Linear Algebra
- (Math 335/338)
- Input Velocity Jet
- More Realistic (?)
18Modeling Ocean CurrentsShallow Water Equations
19Modeling Ocean CurrentsComplex/Global Models
- Add More Physics
- Depth Dependence (many shallow layers)
- Account for Salinity and Temperature
- Ice formation/melting Evaporation
- Add More Realism
- Realistic Geometry
- Outflow from Rivers
- Real Wind Forcing
- 100s of coupled Partial Differential Equations
- 1,000s of Hours of Super Computer Time
20Complex ModelsNorth Atlantic in a Box
- Shallow Water Model
- b-plane (approx. Sphere)
- Forced by Trade Winds and Westerlies
21Particle Motion in the OceanMathematically
- Particle locations (x,y)
- Change in location is given by velocity of water
(u,v) - Velocity depends on position (x,y)
- Particles start at some initial spot
22Particle Motion in the OceanSome Blobs S t r
e t c h
23Dynamical Systems TheoryGeometry of Particle
Paths
- Currents Characteristic Structures
- Particles Squeezed in one
direction Stretched in another - Answer in Math 330 text!
24Dynamical Systems TheoryHyperbolic Saddle Points
Simplest Example
25Dynamical Systems TheoryHyperbolic Saddle Points
26North Atlantic in a BoxSaddles Move!
- Saddle points appear
- Saddle points disappear
- Saddle points move
- but they still affect particle behavior
27Dynamical Systems TheoryThe Theorem
- As long as saddles
- dont move too fast
- dont change shape too much
- are STRONG enough
- Then there are MANIFOLDS in the flow
- Manifolds dictate which particles go where
28Main Theorem
29Dynamical Systems TheoryMaking Manifolds
UNSTABLE MANIFOLD A LINE SEGMENT IS INITIALIZED
ON DAY 15 ALONG THE EIGENVECTOR ASSOCIATED WITH
THE POSITIVE EIGENVALUE AND INTEGRATED FORWARD
IN TIME
STABLE MANIFOLD A LINE SEGMENT IS INITIALIZED
ON DAY 60 ALONG THE EIGENVECTOR ASSOCIATED WITH
THE NEGATIVE EIGENVALUE AND INTEGRATED BACKWARD
IN TIME
30Dynamical Systems TheoryMixing via Manifolds
31Dynamical Systems TheoryMixing via Manifolds
32North Atlantic in a BoxManifold Geometry
- Each saddle has pair of Manifolds
- Particle flow IN on Stable
Out on Unstable - All one needs to know about particle paths (?)
33BLOB HOP-SCOTCH
BLOB TRAVELS FROM HIGH MIXING REGION IN THE EAST
TO HIGH MIXING REGION IN THE WEST
34BLOB HOP-SCOTCHManifold Explanation
35RING FORMATION
A saddle region appears around day 159.5
Eddy is formed mostly from the meander water No
direct interaction with outside the jet structures
36SummaryMathematics in the Ocean?
- ABSOLUTELY!
- Modeling Numerical Analysis Ocean on
Anyones Desktop - Modeling Analysis Predictive Capability
(Just when is that Ice Age coming?) - Simple Analysis Implications for Understanding
Transport of Ocean Stuff - . and thats not the half of it .
April is Math Awareness Month!