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The classical picture of turbulence | |
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The ubiquitous nature of turbulence | |
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The experiments of Taylor and Benard | |
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Flow over a cylinder | |
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Reynolds' experiment | |
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Common themes | |
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The ubiquitous nature of turbulence | |
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Different scales in a turbulent flow: a glimpse at the energy cascade of Kolmogorov and Richardson | |
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The closure problem of turbulence | |
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Is there a 'theory of turbulence'? | |
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The interaction of theory, computation, and experiment | |
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The equations of fluid mechanics | |
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The Navier-Stokes equation | |
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Newton's second law applied to a fluid | |
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The convective derivative | |
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Integral versions of the momentum equation | |
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The rate of dissipation of energy in a viscous fluid | |
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Relating pressure to velocity | |
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Vorticity dynamics | |
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Vorticity and angular momentum | |
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The vorticity equation | |
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Kelvin's theorem | |
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Tracking vorticity distributions | |
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A definition of turbulence | |
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The origins and nature of turbulence | |
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The nature of chaos | |
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From non-linearity to chaos | |
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More on bifurcations | |
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The arrow of time | |
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Some elementary properties of freely evolving turbulence | |
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Various stages of development | |
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The rate of destruction of energy in fully developed turbulence | |
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How much does the turbulence remember? | |
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The need for a statistical approach and different methods of taking averages | |
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Velocity correlations, structure functions and the energy spectrum | |
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Is the asymptotic state universal? Kolmogorov's theory | |
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The probability distribution of the velocity field | |
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Turbulent shear flows and simple closure models | |
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The exchange of energy between the mean flow and the turbulence | |
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Reynolds stresses and the closure problem of turbulence | |
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The eddy-viscosity theories of Boussinesq and Prandtl | |
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The transfer of energy from the mean flow to the turbulence | |
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A glimpse at the k-[epsilon] model | |
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Wall-bounded shear flows and the log-law of the wall | |
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Turbulent flow in a channel and the log-law of the wall | |
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Inactive motion--a problem for the log-law? | |
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Turbulence profiles in channel flow | |
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The log-law for a rough wall | |
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The structure of a turbulent boundary layer | |
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Coherent structures | |
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Spectra and structure functions near the wall | |
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Free shear flows | |
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Planar jets and wakes | |
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The round jet | |
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Homogeneous shear flow | |
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The governing equations | |
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The asymptotic state | |
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Heat transfer in wall-bounded shear flows--the log-law revisited | |
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Turbulent heat transfer near a surface and the log-law for temperature | |
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The effect of stratification on the log-law--the atmospheric boundary layer | |
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More on one-point closure models | |
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A second look at the k-[epsilon] model | |
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The Reynolds stress model | |
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Large eddy simulation: a rival for one-point closures? | |
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The phenomenology of Taylor, Richardson, and Kolmogorov | |
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Richardson revisited | |
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Time and length-scales in turbulence | |
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The energy cascade pictured as the stretching of turbulent eddies | |
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The dynamic properties of turbulent eddies | |
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Kolmogorov revisited | |
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Dynamics of the small scales | |
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Turbulence induced fluctuations of a passive scalar | |
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The intensification of vorticity and the stretching of material lines | |
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Enstrophy production, the skewness factor, and scale invariance | |
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Sheets or tubes? | |
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Examples of concentrated vortex sheets and tubes | |
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Are there singularities in the vorticity field? | |
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The stretching of material line elements | |
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The interplay of the strain and vorticity fields | |
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Turbulent diffusion by continuous movements | |
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Taylor diffusion of a single particle | |
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Richardson's law for the relative diffusion of two particles | |
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The influence of mean shear on turbulent dispersion | |
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Why turbulence is never Gaussian | |
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The experimental evidence and its interpretation | |
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A glimpse at closure schemes which assume near-Gaussian statistics | |
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Closure | |
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The statistical equations for a passive scalar in isotropic turbulence: Yaglom's four-thirds Law and Corrsin's integral | |
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Freely decaying, homogeneous turbulence | |
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Isotropic turbulence (In real space) | |
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Introduction: exploring isotropic turbulence in real space | |
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Deterministic cartoons versus statistical phenomenology | |
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The strengths and weaknesses of Fourier space | |
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An overview of this chapter | |
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The governing equations of isotropic turbulence | |
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Kinematics | |
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Dynamics | |
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Overcoming the closure problem | |
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The dynamics of the large scales | |
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Loitsyansky's integral | |
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Kolmogorov's decay laws | |
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Landau's angular momentum | |
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Batchelor's pressure forces | |
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The Saffman-Birkhoff spectrum | |
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A reappraisal of the long-range pressure forces in E-k[superscript 4] turbulence | |
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The characteristic signature of eddies of different shape | |
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Townsend's model eddy | |
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Other model eddies | |
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Intermittency in the inertial-range eddies | |
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A problem for Kolmogorov's theory? | |
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The [beta]-model of intermittency | |
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The log-normal model of intermittency | |
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The distribution of energy and vorticity across the different eddy sizes | |
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A 'real-space' function which represents, approximately, the distribution of energy | |
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Cascade dynamics in real space | |
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A 'real-space' function which represents, approximately, the distribution of enstrophy | |
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A footnote: can we capture Richardson's vision with our mathematical analysis? | |
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Turbulence composed of Townsend's model eddy | |
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The role of numerical simulations | |
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What is DNS or LES? | |
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Direct numerical simulation | |
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Large eddy simulations | |
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On the dangers of periodicity | |
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Structure in chaos | |
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Tubes, sheets, and cascades | |
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On the taxonomy of worms | |
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Structure and intermittency | |
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Shear flows | |
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Postscript | |
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Isotropic turbulence (in spectral space) | |
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Kinematics in spectral space | |
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The Fourier transform and its properties | |
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The Fourier transform as a filter | |
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The autocorrelation function | |
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The transform of the correlation tensor and the three-dimensional energy spectrum | |
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One-dimensional energy spectra | |
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Relating the energy spectrum to the second-order structure function | |
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A footnote: singularities in the spectrum arising from anisotropy | |
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Another footnote: the transform of the velocity field | |
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Definitely the last footnote: what do E(k) and E[subscript 1](k) really represent? | |
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Dynamics in spectral space | |
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An evolution equation for E(k) | |
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Closure in spectral space | |
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Quasi-Normal type closure schemes (Part 2) | |
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Special topics | |
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The influence of rotation, stratification, and magnetic fields on turbulence | |
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The importance of body forces in geophysics and astrophysics | |
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The influence of rapid rotation and stable stratification | |
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The Coriolis force | |
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The Taylor-Proudman theorem | |
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Properties of inertial waves | |
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Turbulence in rapidly rotating systems | |
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Turbulence with moderate rotation | |
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From rotation to stratification (or from cigars to pancakes) | |
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The influence of magnetic fields I--the MHD equations | |
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The interaction of moving conductors and magnetic fields: a qualitative overview | |
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From Maxwell's equations to the governing equations of MHD | |
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Simplifying features of low magnetic Reynolds number MHD | |
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Simple properties of high magnetic Reynolds number MHD | |
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The influence of magnetic fields II--MHD turbulence | |
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The growth of anisotropy in MHD turbulence | |
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The evolution of eddies at low magnetic Reynolds number | |
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The Landau invariant for homogeneous MHD turbulence | |
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Decay laws at low magnetic Reynolds number | |
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Turbulence at high magnetic Reynolds number | |
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The combined effects of Coriolis and Lorentz forces | |
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The shaping of eddies by Coriolis and magnetic forces | |
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Turbulence in the core of the earth | |
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Turbulence near the surface of the sun | |
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Two-dimensional turbulence | |
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The classical picture of two-dimensional turbulence: Batchelor's self-similar spectrum | |
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What is two-dimensional turbulence? | |
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What does the turbulence remember? | |
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Batchelor's self-similar spectrum | |
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The inverse energy cascade of Batchelor and Kraichnan | |
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Different scales in two-dimensional turbulence | |
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The shape of the energy spectrum: the k[superscript -3] law | |
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Problems with the k[superscript -3] law | |
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A Richardson-type law for the inertial range | |
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Coherent vortices: a problem for the classical theory | |
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The evidence | |
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The significance | |
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The governing equations in statistical form | |
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Correlation functions, structure functions, and the energy spectrum | |
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The two-dimensional Karman-Howarth equation and its consequences | |
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Loitsyansky's integral in two dimensions | |
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Variational principles for predicting the final state in confined domains | |
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Minimum enstrophy | |
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Maximum entropy | |
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Quasi-two-dimensional turbulence: bridging the gap with reality | |
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The governing equations for shallow-water, rapidly rotating flow | |
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Karman-Howarth equation for shallow-water, rapidly rotating turbulence | |
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Epilogue | |
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Appendices | |
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Vector identities and an introduction to tensor notation | |
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Vector identities and theorems | |
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An introduction to tensor notation | |
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The properties of isolated vortices: invariants, far-field properties, and long-range interactions | |
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The far-field velocity induced by an isolated eddy | |
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The pressure distribution in the far field | |
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Integral invariants of an isolated eddy | |
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Long-range interactions between eddies | |
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Long-range pressure forces in isotropic turbulence | |
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A dynamic equation for the pressure-induced, long-range correlations | |
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Experimental evidence for the strength of long-range pressure forces | |