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Preface xi
Select bibliography xv
The authors xix
1 Observed flow in the Earth's midlatitudes 1
1.1 Vertical structure 1
1.2 Horizontal structure 4
1.3 Transient activity 11
1.4 Scales of motion 14
1.5 The Norwegian frontal model of cyclones 15
Theme 1 Fluid dynamics of the midlatitude atmosphere 25
2 Fluid dynamics in an inertial frame of reference 27
2.1 Definition of fluid 27
2.2 Flow variables and the continuum hypothesis 29
2.3 Kinematics: characterizing fluid flow 30
2.4 Governing physical principles 35
2.5 Lagrangian and Eulerian perspectives 36
2.6 Mass conservation equation 38
2.7 First Law of Thermodynamics 40
2.8 Newton's Second Law of Motion 41
2.9 Bernoulli's Theorem 45
2.10 Heating and water vapour 47
3 Rotating frames of reference 53
3.1 Vectors in a rotating frame of reference 53
3.2 Velocity and Acceleration 55
3.3 The momentum equation in a rotating frame 56
3.4 The centrifugal pseudo-force 57
3.5 The Coriolis pseudo-force 59
3.6 The Taylor-Proudman theorem 61
4 The spherical Earth 65
4.1 Spherical polar coordinates 65
4.2 Scalar equations 67
4.3 The momentum equations 68
4.4 Energy and angular momentum 70
4.5 The shallow atmosphere approximation 73
4.6 The beta effect and the spherical Earth 74
5 Scale analysis and its applications 77
5.1 Principles of scaling methods 77
5.2 The use of a reference atmosphere 79
5.3 The horizontal momentum equations 81
5.4 Natural coordinates, geostrophic and gradient wind balance 83
5.5 Vertical motion 87
5.6 The vertical momentum equation 89
5.7 The mass continuity equation 91
5.8 The thermodynamic energy equation 92
5.9 Scalings for Rossby numbers that are not small 95
6 Alternative vertical coordinates 97
6.1 A general vertical coordinate 97
6.2 Isobaric coordinates 100
6.3 Other pressure-based vertical coordinates 103
6.4 Isentropic coordinates 106
7 Variations of density and the basic equations 109
7.1 Boussinesq approximation 109
7.2 Anelastic approximation 111
7.3 Stratification and gravity waves 113
7.4 Balance, gravity waves and Richardson number 115
7.5 Summary of the basic equation sets 121
7.6 The energy of atmospheric motions 122
Theme 2 Rotation in the atmosphere 125
8 Rotation in the atmosphere 127
8.1 The concept of vorticity 127
8.2 The vorticity equation 129
8.3 The vorticity equation for approximate sets of equations 131
8.4 The solenoidal term 132
8.5 The expansion/contraction term 134
8.6 The stretching and tilting terms 135
8.7 Friction and vorticity 138
8.8 The vorticity equation in alternative vertical coordinates 144
8.9 Circulation 145
9 Vorticity and the barotropic vorticity equation 149
9.1 The barotropic vorticity equation 149
9.2 Poisson's equation and vortex interactions 151
9.3 Flow over a shallow hill 155
9.4 Ekman pumping 159
9.5 Rossby waves and the beta plane 160
9.6 Rossby group velocity 166
9.7 Rossby ray tracing 170
9.8 Inflexion point instability 172
10 Potential vorticity 177
10.1 Potential vorticity 177
10.2 Alternative derivations of Ertel's theorem 180
10.3 The principle of invertibility 182
10.4 Shallow water equation potential vorticity 186
11 Turbulence and atmospheric flow 189
11.1 The Reynolds number 189
11.2 Three-dimensional flow at large Reynolds number 194
11.3 Two-dimensional flow at large Reynolds number 196
11.4 Vertical mixing in a stratified fluid 201
11.5 Reynolds stresses 203
Theme 3 Balance in atmospheric flow 209
12 Quasi-geostrophic flows 211
12.1 Wind and temperature in balanced flows 211
12.2 The quasi-geostrophic approximation 215
12.3 Quasi-geostrophic potential vorticity 219
12.4 Ertel and quasi-geostrophic potential vorticities 221
13 The omega equation 225
13.1 Vorticity and thermal advection form 225
13.2 Sutcliffe Form 231
13.3 Q-vector form 233
13.4 Ageostrophic flow and the maintenance of balance 238
13.5 Balance and initialization 240
14 Linear theories of baroclinic instability 245
14.1 Qualitative discussion 245
14.2 Stability analysis of a zonal flow 247
14.3 Rossby wave interpretation of the stability conditions 256
14.4 The Eady model 264
14.5 The Charney and other quasi-geostrophic models 271
14.6 More realistic basic states 275
14.7 Initial value problem 281
15 Frontogenesis 291
15.1 Frontal scales 291
15.2 Ageostrophic circulation 294
15.3 Description of frontal collapse 299
15.4 The semi-geostrophic Eady model 305
15.5 The confluence model 307
15.6 Upper-level frontogenesis 309
16 The nonlinear development of baroclinic waves 311
16.1 The nonlinear domain 311
16.2 Semi-geostrophic baroclinic waves 312
16.3 Nonlinear baroclinic waves on realistic jets on the sphere 320
16.4 Eddy transports and zonal mean flow changes 323
16.5 Energetics of baroclinic waves 332
17 The potential vorticity perspective 337
17.1 Setting the scene 337
17.2 Potential vorticity and vertical velocity 340
17.3 Life cycles of some baroclinic waves 342
17.4 Alternative perspectives 346
17.5 Midlatitude blocking 350
17.6 Frictional and heating effects 352
18 Rossby wave propagation and potential vorticity mixing 361
18.1 Rossby wave propagation 361
18.2 Propagation of Rossby waves into the stratosphere 363
18.3 Propagation through a slowly varying medium 365
18.4 The Eliassen-Palm flux and group velocity 370
18.5 Baroclinic life cycles and Rossby waves 372
18.6 Variations of amplitude 373
18.7 Rossby waves and potential vorticity steps 375
18.8 Potential vorticity steps and the Rhines scale 381
Appendices 389
Appendix A: Notation 389
Appendix B: Revision of vectors and vector calculus 393
B.1 Vectors and their algebra 393
B.2 Products of vectors 394
B.3 Scalar fields and the grad operator 396
B.4 The divergence and curl operators 397
B.5 Gauss' and Stokes' theorems 398
B.6 Some useful vector identities 401
Index 403
We have developed this book from lectures given by us and others in the Department of Meteorology at the University of Reading. Since 1965, this department has been an important centre for the study of meteorology and atmospheric science. Indeed, for many years, it was the only independent department of meteorology in the United Kingdom able to offer a full range of undergraduate and postgraduate teaching in meteorology. Many scientists and meteorologists have spent time at Reading either as students or researchers. So our book is a record of one facet of the teaching they met at Reading, and it aspires to encapsulate something of the spirit of the Reading department.
During the early part of the twentieth century, meteorology made the transition from a largely descriptive, qualitative science to a firmly quantitative science. At the heart of that transition was the recognition that the structure and development of weather systems were essentially problems in fluid dynamics. In the 1920s, the scientists of the Bergen School recognized this but lacked the mathematical tools to link their descriptive models of cyclone development in terms of air masses and fronts to the basic equations of fluid dynamics. In the 1940s, modern dynamical meteorology was born out of the recognition by Eady, Charney and others that cyclone development could be viewed as a problem in fluid dynamical instability.
Even so, great simplifications proved necessary to render the problem tractable. Amongst these simplifications was the linearization of the governing equations. The highly nonlinear equations governing fluid dynamics were reduced to relatively simple linear forms whose solutions can be written in terms of traditional analytic functions. Even so, these simplified equations could only be solved for very simple idealized circumstances. For example, the work of both Charney and Eady was confined to flows which varied linearly in the vertical but had no variation in other directions. There was still a big gap between theory and observation. The development of the digital computer in the 1950s opened up the possibility of bridging this gap. While their nonlinearity and complexity rendered the governing equations resistant to analytical solution, the digital computer could generate numerous particular solutions to discretized analogues to the governing equations. So two separate branches of dynamical meteorology developed. On one hand, the drive for weather forecasts and, increasingly, for climate modelling led to the development of elaborate numerical models of atmospheric flow. As computer power increased, these models became more realistic, with higher resolution and fewer approximations or simplifications to the governing equations, and with more elaborate representation of the processes driving atmospheric motion such as radiative transfer, cloud processes and friction. On the other hand, more sophisticated mathematical techniques drove the development of analytical theory either to better approximations to the governing equations or to explore more complex physical scenarios. As a result, there was a growing gulf between numerical modelling, theoretical meteorology and observation.
Our approach at Reading, both in terms of teaching and research, started with the intention of bridging this gulf. The word ‘model' had become somewhat limited in its use in meteorology: it tended to refer to the large and elaborate numerical weather prediction and global circulation models that were primary tools in many applications of meteorology. But the word has far wider meaning than that. A model is any abstraction of the real world, any representation in which certain complexities are eradicated or idealized. All of meteorology, indeed, all of science, deals in models. They may be very basic, starting with conceptual verbal or picture models such as the Norwegian frontal model of cyclone development. They may be exceedingly complex and include a plethora of different processes. The coupled atmosphere–ocean global circulation models now used to study climate change exemplify this sort of model. But between these extremes lie a hierarchy of models of differing degrees of complexity. These range from highly idealized analytic models, models with only very few degrees of freedom, through models of intermediate complexity, right up to fully elaborated numerical models. Good science involves the interaction between these different levels of model and with observations, finding out which elements of the observed world are captured or lost by the different levels of model complexity.
A very complex model may give a faithful representation of the observed atmosphere, but of itself it can lead to rather limited understanding. A very simple model is transparent in its working but generally gives but a crude imitation of a complex reality. Intermediate models, grounded in constant reference to observations and to other models in the hierarchy, can illuminate the transition from transparent simplicity to elaborate complexity.
Our book focuses on the simpler and intermediate complexity models in this hierarchy. Although we shall refer to the results of calculations using elaborate numerical models, we have not set out to describe such models. That is a major topic, bringing together dynamical meteorology and numerical analysis, and deserves a textbook of its own. However, we shall make use of results from numerical models in a number of places.
Our textbook is based upon various lecture courses that we have given to students, both postgraduate and advanced undergraduate, in the Department of Meteorology, University of Reading, over many years. Many of our postgraduate students came to Reading with a first degree in other quantitative disciplines, so our teaching assumed no prior acquaintance with fluid dynamics and the mathematical techniques used in that discipline. Neither did we assume any prior knowledge of meteorology or atmospheric science. We did assume basic knowledge of vector calculus and differential equations. However, in order to make this book self-contained, we have included an appendix which gives a brief introduction to the essential elements of vector calculus assumed in the main body of the text. So our intended readership is primarily postgraduate and advanced undergraduate students of meteorology. We hope others, particularly quantitative scientists who wish to become better acquainted with dynamical meteorology, will also find our book interesting.
Our text begins with an opening chapter which gives a broad brush survey of the structure of the atmosphere and the character of atmospheric flow, particularly in the midlatitude troposphere. This opening chapter introduces in a qualitative way a number of concepts which will be elaborated in subsequent chapters.
Then follows our first major theme: a basic introduction to classic fluid dynamics as applied to the Earth's atmosphere. After deriving the fundamental equations in Chapter 2, we introduce the various modifications that are needed for this application. Foremost among these are the roles that the rotation of the Earth and its spherical geometry, and the stable stratification of the atmosphere play. Perhaps the most important chapter in our first theme is Chapter 5, which develops the technique of scale analysis and applies it systematically to flows in the atmosphere. Our focus of interest is upon the synoptic scale weather systems of the midlatitudes, but the discussion points to how other situations might be approached.
Our second theme recognizes that atmospheric flow on the larger scales is dominated by rotation. The Earth rotates on its axis and individual fluid elements spin as they move around. Such spin is a primary property of the atmosphere or ocean, and our insight into atmospheric behaviour is developed by rewriting the equations in terms of spin or ‘vorticity'. Equations describing the processes which generate and modify vorticity result, and we spend some time exploring these equations in simple contexts. These simple examples help to develop a language and a set of conceptual principles to explore more elaborate and more realistic examples. A powerful unifying concept is a quantity called ‘potential vorticity', which is introduced in Chapter 10.
Our third theme makes up the remainder of our book. That theme is the dynamical understanding of middle latitude weather systems exploiting the near balance between certain terms in the governing equations. Such a balance links together dynamical, pressure and temperature fields and constrains their evolution. Maintaining a near-balanced state determines the response of the atmosphere to thermal and other forcing. With these concepts, we are able to discuss the evolution of weather systems as problems in fluid dynamical instability, and we are able to extend our discussion to more elaborate, nonlinear regimes. Frontal formation is revealed as an integral part of cyclone development, and at the same time, developing weather systems play a central part in determining the larger scale flow in which they are embedded. Through the concept of balance, potential vorticity is revealed as a primary concept in modern dynamical meteorology.
This book is intended as a readable textbook rather than a research monograph. We hope that the material is largely self-contained. Consequently, we have made no attempt to provide a comprehensive and exhaustive bibliography. Rather we have included some suggestions for further reading which will give the interested reader a starting point from which to explore the literature. Modern electronic databases and citation indices make such exploration much easier...
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