Nonlinear Dynamics and Statistical Theories for Basic Geophysical Flows

Author: Andrew Majda; Xiaoming Wang  

Publisher: Cambridge University Press‎

Publication year: 2006

E-ISBN: 9780511166549

P-ISBN(Paperback): 9780521834414

Subject: P3 Geophysics

Keyword: 流体力学

Language: ENG

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Nonlinear Dynamics and Statistical Theories for Basic Geophysical Flows

Description

The general area of geophysical fluid mechanics is truly interdisciplinary. Now ideas from statistical physics are being applied in novel ways to inhomogeneous complex systems such as atmospheres and oceans. In this book, the basic ideas of geophysics, probability theory, information theory, nonlinear dynamics and equilibrium statistical mechanics are introduced and applied to large time-selective decay, the effect of large scale forcing, nonlinear stability, fluid flow on a sphere and Jupiter's Great Red Spot. The book is the first to adopt this approach and it contains many recent ideas and results. Its audience ranges from graduate students and researchers in both applied mathematics and the geophysical sciences. It illustrates the richness of the interplay of mathematical analysis, qualitative models and numerical simulations which combine in the emerging area of computational science.

Chapter

1.4 Barotropic geophysical flows in a channel domain – an important physical model

1.4.1 The impulse and conserved quantities

1.4.2 Conservation of circulation

1.4.3 Summary of conserved quantities: channel geometry

1.5 Variational derivatives and an optimization principle for elementary geophysical solutions

1.5.1 Some important variational derivatives

1.5.2 An optimization principle for elementary geophysical solutions

1.6 More equations for geophysical flows

1.6.1 The models

1.6.2 Relationships between various models

Derivation of the barotropic one-layer model from the continuously stratified model

Derivation of the two-layer model from the continuously stratified model

Derivation of the one- and one-half-layer model from the two-layer model

Derivation of the barotropic quasi-geostrophic model from the F-plane model

References

2 The response to large-scale forcing

2.1 Introduction

A remarkable identity

2.2 Non-linear stability with Kolmogorov forcing

2.2.1 Non-linear stability in restricted sense

2.2.2 Finite-dimensional dynamics on the ground modes and non-linear stability

Fourier representation for the dynamic equations

2.2.3 Counter-example of unstable ground state modes dynamics for truncated inviscid flows

2.3 Stability of flows with generalized Kolmogorov forcing

References

3 The selective decay principle for basic geophysical flows

3.1 Introduction

3.2 Selective decay states and their invariance

3.3 Mathematical formulation of the selective decay principle

The Rossby waves degenerate into generalized Taylor vortices in the absence of the geophysical beta-plane effect.

3.4 Energy–enstrophy decay

3.5 Bounds on the Dirichlet quotient, A (t)

3.6 Rigorous theory for selective decay

3.6.1 Convergence to an asymptotic state

3.6.2 Convergence to the selective decay state

3.6.3 Stability of the selective decay states

3.6.4 Underlying simplifying mechanisms

3.7 Numerical experiments demonstrating facets of selective decay

3.7.1 Measure of anisotropy

3.7.2 Explicit solutions of the sinh–Poisson equation

3.7.3 Numerical examples

References

Appendix 1 Stronger controls on A (t)

Appendix 2 The proof of the mathematical form of the selective decay principle in the presence of the beta-plane effect

4 Non-linear stability of steady geophysical flows

4.1 Introduction

4.2 Stability of simple steady states

4.2.1 Non-linear stability and the energy method

4.2.2 Simple states with topography, but no mean flow or beta-effect

4.2.3 Simple states with topography, mean flow, and beta-effect

4.3 Stability for more general steady states

4.4 Non-linear stability of zonal flows on the beta-plane

4.5 Variational characterization of the steady states

References

5 Topographic mean flow interaction, non-linear instability, and chaotic dynamics

5.1 Introduction

5.2 Systems with layered topography

5.2.1 Hamiltonian structure

5.3 Integrable behavior

5.3.1 The case h = 0

5.3.2 The case Beta = 0

5.3.3 Single mode topography

5.4 A limit regime with chaotic solutions

5.4.1 Single mode topography

5.4.2 Interaction of non-linear resonances

5.4.3 Two modes in the topography: a perturbative Melnikov analysis

5.5 Numerical experiments

5.5.1 Perturbation of single mode topography

5.5.2 Two-mode layered topography and topographic blocking events

5.5.3 Random perturbations with multi-mode topography

5.5.4 Symmetry breaking perturbations and topographic blocking events

References

Appendix 1

Appendix 2

6 Introduction to information theory and empirical statistical theory

6.1 Introduction

6.2 Information theory and Shannon’s entropy

6.3 Most probable states with prior distribution

6.4 Entropy for continuous measures on the line

6.4.1 Continuous measure on the line

6.4.2 Entropy and maximum entropy principle

6.4.3 Coarse graining and loss of information

6.4.4 Relative entropy as a “distance” function

6.4.5 Information theory and the finite-moment problem for probability measures

6.5 Maximum entropy principle for continuous fields

6.6.1 The Prior distribution

6.6.2 Constraints on the potential vorticity distribution

6.6.3 Statistical predictions of the maximum entropy principle

6.6.4 Determination of the multipliers and geophysical effect

6.7 Application of the maximum entropy principle to geophysical flows with topography and mean flow

6.7.1 One-point statistics for potential vorticity and large-scale mean velocity and Shannon entropy

6.7.2 The constraints on the one-point statistics

6.7.3 Maximum entropy principle and statistical prediction

6.7.4 Determination of the multipliers and geophysical effects

References

7 Equilibrium statistical mechanics for systems of ordinary differential equations

7.1 Introduction

7.2 Introduction to statistical mechanics for ODEs

7.2.1 The Liouville property

7.2.2 Evolution of probability measures and the Liouville equation

7.2.3 Conserved quantities and their ensemble averages

7.2.4 Shannon entropy and the maximum entropy principle

7.2.5 The most probable state and Gibbs measure

7.2.6 Ergodicity and time averaging

7.2.7 A simple example violating the Liouville property

7.3 Statistical mechanics for the truncated Burgers–Hopf equations

7.3.1 The truncated Burgers–Hopf systems and their conserved quantities

7.3.2 The Liouville property

7.3.3 The Gibbs measure and the prediction of equipartition of energy

7.3.4 Numerical evidence of the validity of the statistical theory

7.3.5 Truncated Burgers–Hopf equation as a model with statistical features in common with atmosphere

A scaling theory for temporal correlations

Numerical evidence for the correlation scaling theory

7.4 The Lorenz 96 model

7.4.1 Geophysical properties of the Lorenz 96 model

Rossby waves

7.4.2 Equilibrium statistical theory for the undamped unforced L-96 model

7.4.3 Statistical properties of the damped forced and undamped unforced L96 models

Rescaling the damped forced L96 model

Linear stability of the mean state

The bulk behavior of the rescaled problem

The climatology of different forcing regimes in rescaled coordinates

References

8 Statistical mechanics for the truncated quasi-geostrophic equations

8.1 Introduction

8.2 The finite-dimensional truncated quasi-geostrophic equations

8.2.1 The spectrally truncated quasi-geostrophic equations

8.2.2 Conserved quantities for the truncated system

8.2.3 Non-linear stability of some exact solutions the truncated system

8.2.4 The Liouville property

8.3 The statistical predictions for the truncated systems

8.4 Numerical evidence supporting the statistical prediction

8.5 The pseudo-energy and equilibrium statistical mechanics for fluctuations about the mean

8.6 The continuum limit

8.6.1 The case with a large-scale mean flow

8.6.2 The case without large-scale mean flow but with generic topography

8.6.3 The case with no geophysical effects

8.6.4 The case with no large-scale mean flow but with topography having degenerate spectrum

High energy subcase

8.7 The role of statistically relevant and irrelevant conserved quantities

References

Appendix 1

9 Empirical statistical theories for most probable states

9.1 Introduction

9.2 Empirical statistical theories with a few constraints

9.2.1 The energy–circulation empirical theory with a general prior distribution

9.2.2 The energy–circulation impulse theory with a general prior distribution

9.3 The mean field statistical theory for point vortices

9.3.1 Derivation of the mean field point-vortex theory from an empirical statistical theory

9.3.2 Complete statistical mechanics for point vortices

The dynamics of point vortices in the plane

Liouville property

The mean field limit equations as N …

9.4 Empirical statistical theories with infinitely many constraints

9.4.1 Maximum entropy principle incorporating all generalized enstrophies

9.4.2 The most probable state and the mean field equation

9.5 Non-linear stability for the most probable mean fields

References

10 Assessing the potential applicability of equilibrium statistical theories for geophysical flows: an overview

10.1 Introduction

10.2 Basic issues regarding equilibrium statistical theories for geophysical flows

Some basic applied issues

Some basic theoretical issues

10.3 The central role of equilibrium statistical theories with a judicious prior distribution and a few external constraints

10.4 The role of forcing and dissipation

10.5 Is there a complete statistical mechanics theory for ESTMC and ESTP?

References

11 Predictions and comparison of equilibrium statistical theories

11.1 Introduction

11.2 Predictions of the statistical theory with a judicious prior and a few external constraints for beta-plane channel flow

11.2.1 Statistical theory

Numerical techniques

Role of symmetries

11.2.2 Coherent geophysical vortices (monopoles and dipoles)

Basic solutions with no geophysical effects (V = Beta = 0)

Langevin theory

Dilute PV Limit

Geophysical solutions…

Langevin theory

Dilute PV theory

11.2.3 Statistical predictions of generalized Rhines’ scale

Vortex streets in the dilute PV limit

Langevin monopole

11.3 Statistical sharpness of statistical theories with few constraints

11.3.1 Statistical sharpness and generalized selective decay principle

11.3.2 The statistical sharpness of macrostates from ESTMC

11.3.3 Statistical sharpness of macrostates of ESTP

Energy–enstrophy statistical theories (EEST)

Point-vortex statistical theories (PVST)

11.4 The limit of many-constraint theory (ESTMC) with small amplitude potential vorticity

11.4.1 The asymptotic expansion

11.4.2 Interpretation of the asymptotic equation through renormalized topography

References

12 Equilibrium statistical theories and dynamical modeling of flows with forcing and dissipation

12.1 Introduction

12.2 Meta-stability of equilibrium statistical structures with dissipation and small-scale forcing

12.2.1 The numerical model

12.2.2 Approximate dynamics for Langevin and dilute PV theory

Algorithm for the approximate dynamics

12.2.3 Statistical consistency of freely decaying vortex states

Free decay of vortex monopoles

Free decay of vortex streets

12.2.4 Statistical consistency of damped and driven vortex states

Inverse cascade from small-scale forcing of single-signed vortices

Maintenance of vortex streets by small-scale, double-signed forcing

Vortex coalescence in strongly forced shear flow

12.3 Crude closure for two-dimensional flows

12.3.1 The equation and the problem

12.3.2 Description of the crude closure dynamics

12.3.3 Numerical results with Newtonian dissipation

Spin-up of large vortex

Forcing by alternating or opposite signed vortices

12.4 Remarks on the mathematical justifications of crude closure

References

13 Predicting the jets and spots on Jupiter by equilibrium statistical mechanics

13.1 Introduction

13.1.1 The observational record for Jupiter and the quasi-geostrophic model

13.1.2 Predictions of the ESTP with a suitable prior and the observational record

13.2 The quasi-geostrophic model for interpreting observations and predictions for the weather layer of Jupiter

13.2.1 Fitting the non-dimensional model with the dimensional parameters of Jupiter

13.2.2 Fitting the lower layer topography

13.3 The ESTP with physically motivated prior distribution

13.3.1 The ESTP with a family of prior distributions with anti-cyclonic skewness

13.3.2 The centered Gamma distribution as a family of skewed prior distributions for ESTP

13.4 Equilibrium statistical predictions for the jets and spots on Jupiter

13.4.1 The southern hemisphere domain

13.4.2 The northern hemisphere domain

References

14 The statistical relevance of additional conserved quantities for truncated geophysical flows

14.1 Introduction

14.1.1 The traditional spectral truncation and equilibrium statistical theory

14.2 A numerical laboratory for the role of higher-order invariants

14.2.1 The spectral truncation with many conserved quantities

14.2.2 Numerical experiments demonstrating the statistical relevance of C3(q) at large scales

14.2.3 Mixing and decay of temporal correlations

14.2.4 The large-scale mean flow

14.2.5 The energy spectrum

14.3 Comparison with equilibrium statistical predictions with a judicious prior

14.3.1 The probability distribution function of potential vorticity

14.3.2 Equilibrium statistical predictions of the non-linear mean state

14.4 Statistically relevant conserved quantities for the truncated Burgers–Hopf equation

References

Appendix 1 Spectral truncations of quasi-geostrophic flow with additional conserved quantities

A.1.1 Some basic facts about Hamiltonian systems

A.1.2 The equations for Barotropic flow in Fourier space

A.1.3 The sine-bracket truncation with many additional conserved quantities

15 A mathematical framework for quantifying predictability utilizing relative entropy

15.1 Ensemble prediction and relative entropy as a measure of predictability

15.1.1 Practical and mathematical issues for predictability

15.1.2 Gaussian prior distribution for predictability

15.1.3 Invariance of the predictability measure under a general change of coordinates

15.1.4 Canonical form for a Gaussian climate: EOF basis

15.2 Quantifying predictability for a Gaussian prior distribution

15.2.1 The signal and dispersion decomposition for a Gaussian prior

15.2.2 Rigorous lower bounds on predictive information content with a Gaussian prior

15.2.3 Choosing reduced variables to order the predictive information content

15.2.4 The relative entropy and the entropy difference for quantifying predictive information content

15.3 Non-Gaussian ensemble predictions in the Lorenz 96 model

15.4 Information content beyond the climatology in ensemble predictions for the truncated Burgers–Hopf model

15.4.1 Relaxation of ensemble predictions to the climate distribution

15.4.2 The signal, dispersion, and variations in predictive utility

15.5 Further developments in ensemble predictions and information theory

References

16 Barotropic quasi-geostrophic equations on the sphere

16.1 Introduction

16.1.1 Common differential operators and integration by parts formulas on the sphere

16.1.2 Eigenfunctions of the Laplace operator and the Legendre functions

16.2 Exact solutions, conserved quantities, and non-linear stability

16.2.1 Some special exact solutions

Independent linear dynamics on the ground energy shell

Exact interesting dynamics of the ground state modes and another energy shell

Exact solutions with generalized Kolmogorov forcing

Steady state solutions

16.2.2 Conserved quantities

Conserved quantities with general topography

Conserved quantities with topography living on the ground energy shell

Conserved quantities in the presence of odd symmetry in z

Conserved quantities in the presence of odd symmetry in z and topography living on the ground energy shell

Summary of conserved quantities

16.2.3 Non-linear stability of exact solutions

Non-linear stability of steady states

Restricted stability of motion on the first two energy shells

16.3 The response to large-scale forcing

16.4 Selective decay on the sphere

16.4.1 The equation

16.4.2 Physicist’s selective decay states

16.4.3 Formulation of the selective decay principle

16.4.4 Sketch of the proof

Overview of equilibrium statistical theories for the sphere

16.5 Energy enstrophy statistical theory on the unit sphere

16.5.1 Energy–enstrophy theory with topography – empirical statistical theory

Empirical energy–enstrophy theory with general topography

Empirical energy–enstrophy theory with ground state topography

16.5.2 Complete statistical mechanics.

Conservation of energy and potential enstrophy

The Liouville property

Most probable state for the truncated system

The continuum limit

Comment on the case with ground state topography

16.6 Statistical theories with a few constraints and statistical theories with many constraints on the unit sphere

A few constraint theory with prior distribution

Energy–circulation theory

The point vortex theory

16.6.1 Infinitely many constraint statistical theory

References

Appendix 1

Appendix 2

Index

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