Nonlinear Scale Interactions and Energy Pathways in the Ocean
|
|
- Oscar Hutchinson
- 5 years ago
- Views:
Transcription
1 Nonlinear Scale Interactions and Energy Pathways in the Ocean 1,2 Hussein Aluie, 1 Matthew Hecht & 3 Geoff Vallis 1 LANL, the 2 New Mexico Consortium and 3 U of Exeter with support from LANL s Institute for Geophysics, Planetary Physics and Signatures and Center for Nonlinear Studies
2 Ocean Circulation Multiscale Flow: O(10 4 ) km -- O(1) mm Source: NASA
3 Ocean Circulation Multiscale Flow: O(10 4 ) km -- O(1) mm Inhomogeneous and Anisotropic Source: NASA
4 Ocean Circulation Multiscale Flow: O(10 4 ) km -- O(1) mm Inhomogeneous and Anisotropic Mean Kinetic energy (KE) is concentrated in narrow intense currents. Source: NASA
5 Ocean Circulation Multiscale Flow: O(10 4 ) km -- O(1) mm Inhomogeneous and Anisotropic Mean Kinetic energy (KE) is concentrated in narrow intense currents. but much of the KE in the ocean resides in mesoscale eddies of size ~100 km Source: NASA
6 Ocean Circulation Multiscale Flow: O(10 4 ) km -- O(1) mm Inhomogeneous and Anisotropic Mean Kinetic energy (KE) is concentrated in narrow intense currents. but much of the KE in the ocean resides in mesoscale eddies of size ~100 km Source: NASA The Problem What is the flow of energy between different spatial scales, different forms?
7 Ocean Circulation Nonlinear Processes & Structures Baroclinic Instability Wind Barotropic Instability? Watts Mesoscale Eddies? Mean Flow Rossby Waves Bottom Drag Source: NASA Internal Waves?? Internal Waves The Problem What is the flow of energy between different spatial scales, different forms (how big are these arrows)?
8 Traditional Approach Source: NASA
9 Our Approach Coarse-graining (Filtering) Leonard (1974), Germano (1992), Eyink (1994), Piomelli et al. (1991), Liu et al (1994), Chen, Ecke, Eyink (2003),
10 Large-scale energy budget Cascade of Energy Energy flux
11 Large-scale energy budget Cascade of Energy Every point and every instant Energy flux Variable scale
12 Large-scale energy budget Measuring Energy Transfer
13 Measuring Energy Transfer Large-scale energy budget Subgrid scale (SGS) flux
14 Measuring Energy Transfer Large-scale energy budget Subgrid scale (SGS) flux Frisch (1995), used by Scott & Wang (2005), Tulloch, Marshall, Hill and Smith (2011) sweeping energy in space between structures
15 Measuring Energy Transfer Large-scale energy budget Subgrid scale (SGS) flux Frisch (1995), used by Scott & Wang (2005), Tulloch, Marshall, Hill and Smith (2011) Lindborg (2006), Mininni, et al. (2008) sweeping energy in space between structures
16 Measuring Energy Transfer Any measure of the energy exchange must satisfy: 1. Galilean Invariance 2. Florida Gulf Stream
17 Measuring Energy Transfer Any measure of the energy exchange must satisfy: 1. Galilean Invariance 2. Florida Gulf Stream
18 Measuring Energy Transfer Any measure of the energy exchange must satisfy: 1. Galilean Invariance 2. SGS definition Frisch (1995) definition
19 Measuring Energy Transfer Any measure of the energy exchange must satisfy: 1. Galilean Invariance 2. Frisch (1995) definition SGS definition V0 Simulation Domain
20 Measuring Energy Transfer Any measure of the energy exchange must satisfy: 1. Galilean Invariance 2. SGS definition After boosting Frisch (1995) definition After boosting
21 Measuring Energy Transfer Any measure of the energy exchange must satisfy: Vanish in the absence of subscale fluctuations
22 Measuring Energy Transfer Any measure of the energy exchange must satisfy: Vanish in the absence of subscale fluctuations SGS definition Lindborg (2006) definition
23 North Europe SGS definition Africa South North Europe Frisch definition Africa South
24 North Europe SGS definition = +0.9 W/km 2 /m Africa South North Europe Africa Frisch definition = W/km 2 /m South
25 North Europe SGS definition = +0.9 W/km 2 /m South North South Africa Europe Africa = -197 W/km 2 /m Frisch definition = W/km 2 /m = +319 W/km 2 /m
26 North Europe Africa South North Europe Africa South
27 In summary Traditional homogeneous/isotropic turbulence tools break down in the Ocean. Spectral Transfer and Flux can be qualitatively wrong. Guided by basic physical principles (Galilean invariance,.), the SGS approach to coarse-graining provides a robust means to measure energy transfer at different locations in the Ocean.
28 In summary Traditional homogeneous/isotropic turbulence tools break down in the Ocean. Spectral Transfer and Flux can be qualitatively wrong. Guided by basic physical principles (Galilean invariance,.), the SGS approach to coarse-graining provides a robust means to measure energy transfer at different locations in the Ocean. Were ready to publish last summer, before we realized we weren t
29 In summary Traditional homogeneous/isotropic turbulence tools break down in the Ocean. Spectral Transfer and Flux can be qualitatively wrong. Guided by basic physical principles (Galilean invariance,.), the SGS approach to coarse-graining provides a robust means to measure energy transfer at different locations in the Ocean. Were ready to publish last summer, before we realized we weren t Since then, have worked through issues of calculating energy transfer on the sphere (scale-dependent commutation of vector operations and filter).
Macroturbulent cascades of energy and enstrophy in models and observations of planetary atmospheres
Macroturbulent cascades of energy and enstrophy in models and observations of planetary atmospheres Peter Read + Roland Young + Fachreddin Tabataba-Vakili + Yixiong Wang [Dept. of Physics, University of
More informationSpectrally condensed turbulence in two dimensions
Spectrally condensed turbulence in two dimensions Hua Xia 1, Michael Shats 1, Gregory Falovich 1 The Australian National University, Canberra, Australia Weizmann Institute of Science, Rehovot, Israel Acnowledgements:
More informationModelling of turbulent flows: RANS and LES
Modelling of turbulent flows: RANS and LES Turbulenzmodelle in der Strömungsmechanik: RANS und LES Markus Uhlmann Institut für Hydromechanik Karlsruher Institut für Technologie www.ifh.kit.edu SS 2012
More informationNOTES AND CORRESPONDENCE. Comments on The k 3 and k 5/3 Energy Spectrum of Atmospheric Turbulence: Quasigeostrophic Two-Level Model Simulation
15 APRIL 2004 NOTES AND CORRESPONDENCE 937 NOTES AND CORRESPONDENCE Comments on The k 3 and k 5/3 Energy Spectrum of Atmospheric Turbulence: Quasigeostrophic Two-Level Model Simulation K. SHAFER SMITH
More informationOn the Wind Power Input and Eddy Residence Time
Hamburg Workshop 215 On the Wind Power Input and Eddy Residence Time Xiaoming Zhai Centre for Ocean and Atmospheric Sciences School of Environmental Sciences, University of East Anglia With David Marshall,
More informationOCEANIC SUBMESOSCALE SAMPLING WITH WIDE-SWATH ALTIMETRY. James C. McWilliams
. OCEANIC SUBMESOSCALE SAMPLING WITH WIDE-SWATH ALTIMETRY James C. McWilliams Department of Atmospheric & Oceanic Sciences Institute of Geophysics & Planetary Physics U.C.L.A. Recall the long-standing
More informationReynolds Averaging. Let u and v be two flow variables (which might or might not be velocity components), and suppose that. u t + x uv ( ) = S u,
! Revised January 23, 208 7:7 PM! Reynolds Averaging David Randall Introduction It is neither feasible nor desirable to consider in detail all of the small-scale fluctuations that occur in the atmosphere.
More informationParameterizations with and without Climate Process Teams
Parameterizations with and without Climate Process Teams Baylor Fox-Kemper Brown University, DEEP Sciences Mixed Layer Eddy Sponsors: NSF OCE-0612143, OCE-0612059, OCE-0825376, DMS-0855010, and OCE-0934737
More informationThe Atmospheric Boundary Layer. The Surface Energy Balance (9.2)
The Atmospheric Boundary Layer Turbulence (9.1) The Surface Energy Balance (9.2) Vertical Structure (9.3) Evolution (9.4) Special Effects (9.5) The Boundary Layer in Context (9.6) Fair Weather over Land
More informationRelation Between Structure Functions and Cascade Rates in Anisotropic Two-Dimensional Turbulence
Page 1 of 9 This draft was prepared using the LaTeX style file belonging to the Journal of Fluid Mechanics 1 Relation Between Structure Functions and Cascade Rates in Anisotropic Two-Dimensional Turbulence
More informationStatistical studies of turbulent flows: self-similarity, intermittency, and structure visualization
Statistical studies of turbulent flows: self-similarity, intermittency, and structure visualization P.D. Mininni Departamento de Física, FCEyN, UBA and CONICET, Argentina and National Center for Atmospheric
More informationLocality of Energy Transfer
(E) Locality of Energy Transfer See T & L, Section 8.2; U. Frisch, Section 7.3 The Essence of the Matter We have seen that energy is transferred from scales >`to scales
More informationFully-Coupled and Forced Ocean Sea-Ice Simulations Towards CESM2 (since mini-breck) Defining the Ocean Component of CESM2
Fully-Coupled and Forced Ocean Sea-Ice Simulations Towards CESM2 (since mini-breck) Defining the Ocean Component of CESM2 OMWG PLAN FOR DEFINING THE CESM2 OCEAN COMPONENT Timeline 01 March 2016 22 April
More informationLagrangian Statistics in Nonhydrostatic and QG turbulence Baylor Fox-Kemper (Brown)
Lagrangian Statistics in Nonhydrostatic and QG turbulence Baylor Fox-Kemper (Brown) LAPCOD, Schoodic Pt., ME 7/28/15 Sponsor: GoMRI/CARTHE P. E. Hamlington, L. P. Van Roekel, BFK, K. Julien, and G. P.
More informationTurbulence and Energy Transfer in Strongly-Stratified Flows
Turbulence and Energy Transfer in Strongly-Stratified Flows James J. Riley University of Washington Collaborators: Steve debruynkops (UMass) Kraig Winters (Scripps IO) Erik Lindborg (KTH) First IMS Turbulence
More informationTurbulence in the Atmosphere and Oceans
Turbulence in the Atmosphere and Oceans Instructors: Raffaele Ferrari and Glenn Flierl Course description The course will present the phenomena, theory, and modeling of turbulence in the Earth s oceans
More informationRelated Improvements. A DFS Application. Mark A. Bourassa
Related Improvements in Surface Turbulent Heat Fluxes A DFS Application Center for Ocean-Atmospheric Prediction Studies & Department of Earth, Ocean and Atmospheric Sciences, The Florida State University,
More informationContents. Parti Fundamentals. 1. Introduction. 2. The Coriolis Force. Preface Preface of the First Edition
Foreword Preface Preface of the First Edition xiii xv xvii Parti Fundamentals 1. Introduction 1.1 Objective 3 1.2 Importance of Geophysical Fluid Dynamics 4 1.3 Distinguishing Attributes of Geophysical
More informationResolution-dependent Eddy Parameterizations for Large-scale Ocean Models
Resolution-dependent Eddy Parameterizations for Large-scale Ocean Models Robert Hallberg with contributions from Alistair Adcroft NOAA / GFDL and Princeton University Mercator/Tripolar Resolution Required
More informationReduction of the usable wind work on the general circulation by forced symmetric instability
GEOPHYSICAL RESEARCH LETTERS, VOL. 37,, doi:10.1029/2010gl044680, 2010 Reduction of the usable wind work on the general circulation by forced symmetric instability L. N. Thomas 1 and J. R. Taylor 2 Received
More informationThe Lagrangian-Averaged Navier-Stokes alpha (LANS-α) Turbulence Model in Primitive Equation Ocean Modeling
The Lagrangian-Averaged Navier-Stokes alpha (LANS-α) Turbulence Model in Primitive Equation Ocean Modeling Mark R. Petersen with Matthew W. Hecht, Darryl D. Holm, and Beth A. Wingate Los Alamos National
More informationAn evaluation of a conservative fourth order DNS code in turbulent channel flow
Center for Turbulence Research Annual Research Briefs 2 2 An evaluation of a conservative fourth order DNS code in turbulent channel flow By Jessica Gullbrand. Motivation and objectives Direct numerical
More informationprimitive equation simulation results from a 1/48th degree resolution tell us about geostrophic currents? What would high-resolution altimetry
Scott 2008: Scripps 1 What would high-resolution altimetry tell us about geostrophic currents? results from a 1/48th degree resolution primitive equation simulation Robert B. Scott and Brian K. Arbic The
More informationTransformed Eulerian Mean
Chapter 15 Transformed Eulerian Mean In the last few lectures we introduced some fundamental ideas on 1) the properties of turbulent flows in rotating stratified environments, like the ocean and the atmosphere,
More informationEddies, Waves, and Friction: Understanding the Mean Circulation in a Barotropic Ocean Model
Eddies, Waves, and Friction: Understanding the Mean Circulation in a Barotropic Ocean Model Baylor Fox-Kemper Atmospheric and Oceanic Sciences Program, Princeton University and NOAA Climate and Global
More informationInfluence of forced near-inertial motion on the kinetic energy of a nearly-geostrophic flow
Abstract Influence of forced near-inertial motion on the kinetic energy of a nearly-geostrophic flow Stephanne Taylor and David Straub McGill University stephanne.taylor@mail.mcgill.ca The effect of forced
More informationRecovery of atmospheric flow statistics in a general circulation model without nonlinear eddy-eddy interactions
Click Here for Full Article GEOPHYSICAL RESEARCH LETTERS, VOL. 34, L22801, doi:10.1029/2007gl031779, 2007 Recovery of atmospheric flow statistics in a general circulation model without nonlinear eddy-eddy
More informationPotential Enstrophy in Stratified Turbulence
Potential Enstrophy in Stratified Turbulence Michael Waite University of Waterloo mwaite@uwaterloo.ca 11 June 2013 M. L. Waite (UWaterloo) Fields Sub-Meso 2013 11 June 2013 1 / 25 Introduction Introduction
More informationAER1310: TURBULENCE MODELLING 1. Introduction to Turbulent Flows C. P. T. Groth c Oxford Dictionary: disturbance, commotion, varying irregularly
1. Introduction to Turbulent Flows Coverage of this section: Definition of Turbulence Features of Turbulent Flows Numerical Modelling Challenges History of Turbulence Modelling 1 1.1 Definition of Turbulence
More informationConcurrent simulation of the eddying general circulation and tides in a global ocean model
Concurrent simulation of the eddying general circulation and tides in a global ocean model Brian K. Arbic 1 E. Joseph Metzger 2 Alan J. Wallcraft 2 1 Department of Oceanography and Center for Ocean-Atmospheric
More informationOliver Bühler Waves and Vortices
Oliver Bühler Waves and Vortices Four combined lectures Introduction, wave theory, simple mean flows Wave-driven vortex dynamics on beaches Three-dimensional gravity waves, recoil & capture Waves, vortices,
More informationLARGE EDDY SIMULATION OF MASS TRANSFER ACROSS AN AIR-WATER INTERFACE AT HIGH SCHMIDT NUMBERS
The 6th ASME-JSME Thermal Engineering Joint Conference March 6-, 3 TED-AJ3-3 LARGE EDDY SIMULATION OF MASS TRANSFER ACROSS AN AIR-WATER INTERFACE AT HIGH SCHMIDT NUMBERS Akihiko Mitsuishi, Yosuke Hasegawa,
More informationAtmosphere, Ocean, Climate Dynamics: the Ocean Circulation EESS 146B/246B
Atmosphere, Ocean, Climate Dynamics: the Ocean Circulation EESS 146B/246B Instructor: Leif Thomas TA: Gonçalo Zo Zo Gil http://pangea.stanford.edu/courses/eess146bweb/ Course Objectives Identify and characterize
More informationNon-orographic gravity waves in general circulation models
Non-orographic gravity waves in general circulation models Erich Becker Leibniz-Institute of Atmospheric Physics (IAP) Kühlungsborn, Germany (1) General problem and issues Assumed equilibirium state for
More informationAtmospheric turbulence spectrum: competing theories
Atmospheric turbulence spectrum: competing theories Explanations for Nastrom & Gage, JAS, 42, 1985 by Tung & Orlando, JAS, 60, 2003 Tulloch & Smith, PNAS, 103, 2006 (k p where p = 3, 5/3,...) as told by
More informationHydrodynamic conservation laws and turbulent friction in atmospheric circulation models
Hydrodynamic conservation laws and turbulent friction in atmospheric circulation models Erich Becker Leibniz-Institute of Atmospheric Physics, Kühlungsborn, Germany Including contributions from Ulrike
More informationA note on the numerical representation of surface dynamics in quasigeopstrophic turbulence: Application to the nonlinear Eady model
Submitted to JAS A note on the numerical representation of surface dynamics in quasigeopstrophic turbulence: Application to the nonlinear Eady model Ross Tulloch and K. Shafer Smith Center for Atmosphere
More informationSubgrid-scale modeling of helicity and energy dissipation in helical turbulence
Subgrid-scale modeling of helicity and energy dissipation in helical turbulence Yi Li, 1 Charles Meneveau, 1 Shiyi Chen, 1,2 and Gregory L. Eyink 3 1 Department of Mechanical Engineering and Center for
More informationmodel and its application to channel ow By K. B. Shah AND J. H. Ferziger
Center for Turbulence Research Annual Research Briefs 1995 73 A new non-eddy viscosity subgrid-scale model and its application to channel ow 1. Motivation and objectives By K. B. Shah AND J. H. Ferziger
More informationAtmosphere, Ocean and Climate Dynamics Fall 2008
MIT OpenCourseWare http://ocw.mit.edu 12.003 Atmosphere, Ocean and Climate Dynamics Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. Contents
More informationLES of turbulent shear flow and pressure driven flow on shallow continental shelves.
LES of turbulent shear flow and pressure driven flow on shallow continental shelves. Guillaume Martinat,CCPO - Old Dominion University Chester Grosch, CCPO - Old Dominion University Ying Xu, Michigan State
More informationA note on the numerical representation of surface dynamics in quasigeostrophic turbulence: Application to the nonlinear Eady model
A note on the numerical representation of surface dynamics in quasigeostrophic turbulence: Application to the nonlinear Eady model Ross Tulloch and K. Shafer Smith Center for Atmosphere Ocean Science Courant
More informationDo altimeter wavenumber spectra agree with interior or surface. quasi-geostrophic theory?
Do altimeter wavenumber spectra agree with interior or surface quasi-geostrophic theory? P.Y. Le Traon*, P. Klein*, Bach Lien Hua* and G. Dibarboure** *Ifremer, Centre de Brest, 29280 Plouzané, France
More informationThe impacts of stochastic noise on climate models
The impacts of stochastic noise on climate models Paul Williams Department of Meteorology, University of Reading, UK The impacts of στοχαστικός noise on climate models Paul Williams Department of Meteorology,
More informationATMOSPHERIC SCIENCE-ATS (ATS)
Atmospheric Science-ATS (ATS) 1 ATMOSPHERIC SCIENCE-ATS (ATS) Courses ATS 150 Science of Global Climate Change Credits: 3 (3-0-0) Physical basis of climate change. Energy budget of the earth, the greenhouse
More informationATMOSPHERIC AND OCEANIC FLUID DYNAMICS
ATMOSPHERIC AND OCEANIC FLUID DYNAMICS Fundamentals and Large-scale Circulation G E O F F R E Y K. V A L L I S Princeton University, New Jersey CAMBRIDGE UNIVERSITY PRESS An asterisk indicates more advanced
More informationWhat Vertical Mode Does the Altimeter Reflect? On the Decomposition in Baroclinic Modes and on a Surface-Trapped Mode
NOVEMBER 2009 L A P E Y R E 2857 What Vertical Mode Does the Altimeter Reflect? On the Decomposition in Baroclinic Modes and on a Surface-Trapped Mode GUILLAUME LAPEYRE Laboratoire de Météorologie Dynamique/IPSL,
More informationThe role of the midlatitude ocean in sub-seasonal prediction
The role of the midlatitude ocean in sub-seasonal prediction R. Saravanan Xiaohui Ma, Xue Liu, J. Steinweg-Woods J. Kurian, R. Montuoro, P. Chang, I. Szunyogh Yinglai Jia, Ocean University of China J.
More informationHigh-resolution Global Climate Modeling of Saturn s and Jupiter s tropospheric and stratospheric circulations
High-resolution Global Climate Modeling of Saturn s and Jupiter s tropospheric and stratospheric circulations Aymeric SPIGA, S. Guerlet, E. Millour, Y. Meurdesoif (LSCE/CEA), M. Indurain, S. Cabanes, M.
More informationA simple subgrid-scale model for astrophysical turbulence
CfCA User Meeting NAOJ, 29-30 November 2016 A simple subgrid-scale model for astrophysical turbulence Nobumitsu Yokoi Institute of Industrial Science (IIS), Univ. of Tokyo Collaborators Axel Brandenburg
More informationVortices in the ocean. Lecture 4 : Baroclinic vortex processes
Vortices in the ocean Lecture 4 : Baroclinic vortex processes Vortex generation by unstable currents (jets, coastal currents) Vortex generation by baroclinically unstable jets (e.g. Gulf Stream) Two-layer
More informationEngineering. Spring Department of Fluid Mechanics, Budapest University of Technology and Economics. Large-Eddy Simulation in Mechanical
Outline Geurts Book Department of Fluid Mechanics, Budapest University of Technology and Economics Spring 2013 Outline Outline Geurts Book 1 Geurts Book Origin This lecture is strongly based on the book:
More informationIsland Wakes in Shallow Water
Island Wakes in Shallow Water Changming Dong, James C. McWilliams, et al Institute of Geophysics and Planetary Physics, University of California, Los Angeles 1 ABSTRACT As a follow-up work of Dong et al
More informationLatest thoughts on stochastic kinetic energy backscatter - good and bad
Latest thoughts on stochastic kinetic energy backscatter - good and bad by Glenn Shutts DARC Reading University May 15 2013 Acknowledgments ECMWF for supporting this work Martin Leutbecher Martin Steinheimer
More informationPassive Scalars in Stratified Turbulence
GEOPHYSICAL RESEARCH LETTERS, VOL.???, XXXX, DOI:10.1029/, Passive Scalars in Stratified Turbulence G. Brethouwer Linné Flow Centre, KTH Mechanics, SE-100 44 Stockholm, Sweden E. Lindborg Linné Flow Centre,
More informationTurbulence. 2. Reynolds number is an indicator for turbulence in a fluid stream
Turbulence injection of a water jet into a water tank Reynolds number EF$ 1. There is no clear definition and range of turbulence (multi-scale phenomena) 2. Reynolds number is an indicator for turbulence
More informationGlobal Variability of the Wavenumber Spectrum of Oceanic Mesoscale Turbulence
802 J O U R N A L O F P H Y S I C A L O C E A N O G R A P H Y VOLUME 41 Global Variability of the Wavenumber Spectrum of Oceanic Mesoscale Turbulence YONGSHENG XU AND LEE-LUENG FU Jet Propulsion Laboratory,
More informationUpper Ocean Circulation
Upper Ocean Circulation C. Chen General Physical Oceanography MAR 555 School for Marine Sciences and Technology Umass-Dartmouth 1 MAR555 Lecture 4: The Upper Oceanic Circulation The Oceanic Circulation
More informationRegularization modeling of turbulent mixing; sweeping the scales
Regularization modeling of turbulent mixing; sweeping the scales Bernard J. Geurts Multiscale Modeling and Simulation (Twente) Anisotropic Turbulence (Eindhoven) D 2 HFest, July 22-28, 2007 Turbulence
More informationthat individual/local amplitudes of Ro can reach O(1).
Supplementary Figure. (a)-(b) As Figures c-d but for Rossby number Ro at the surface, defined as the relative vorticity ζ divided by the Coriolis frequency f. The equatorial band (os-on) is not shown due
More informationA dynamic global-coefficient subgrid-scale eddy-viscosity model for large-eddy simulation in complex geometries
Center for Turbulence Research Annual Research Briefs 2006 41 A dynamic global-coefficient subgrid-scale eddy-viscosity model for large-eddy simulation in complex geometries By D. You AND P. Moin 1. Motivation
More informationThe general circulation: midlatitude storms
The general circulation: midlatitude storms Motivation for this class Provide understanding basic motions of the atmosphere: Ability to diagnose individual weather systems, and predict how they will change
More information3-Fold Decomposition EFB Closure for Convective Turbulence and Organized Structures
3-Fold Decomposition EFB Closure for Convective Turbulence and Organized Structures Igor ROGACHEVSKII and Nathan KLEEORIN Ben-Gurion University of the Negev, Beer-Sheva, Israel N.I. Lobachevsky State University
More informationOn why dynamic subgrid-scale models work
/ / Center for Turbulence Research Annual Research Briefs 1995 25 On why dynamic subgrid-scale models work By J. Jim_nez 1 1. Motivation Dynamic subgrid models were introduced in (Germano et al. 1991)
More informationWind Gyres. curl[τ s τ b ]. (1) We choose the simple, linear bottom stress law derived by linear Ekman theory with constant κ v, viz.
Wind Gyres Here we derive the simplest (and oldest; Stommel, 1948) theory to explain western boundary currents like the Gulf Stream, and then discuss the relation of the theory to more realistic gyres.
More informationA Refined Life at High Resolution: Subgrid Modelling in the Eddy-Rich Regime
A Refined Life at High Resolution: Subgrid Modelling in the Eddy-Rich Regime Baylor Fox-Kemper (Brown University, USA) Major Contributions from Scott D. Bachman (CU-PhD, now Cambridge, UK), Thanks for
More informationThe Role of Water Droplets in Air-sea Interaction: Rain and Sea Spray
The Role of Water Droplets in Air-sea Interaction: Rain and Sea Spray Fabrice Veron Air-Sea Interaction Laboratory School of Marine Science and Policy College of Earth, Ocean, & Environment University
More informationwarmest (coldest) temperatures at summer heat dispersed upward by vertical motion Prof. Jin-Yi Yu ESS200A heated by solar radiation at the base
Pole Eq Lecture 3: ATMOSPHERE (Outline) JS JP Hadley Cell Ferrel Cell Polar Cell (driven by eddies) L H L H Basic Structures and Dynamics General Circulation in the Troposphere General Circulation in the
More informationThe geography of linear baroclinic instability in Earth s oceans
Journal of Marine Research, 65, 655 683, 2007 The geography of linear baroclinic instability in Earth s oceans by K. Shafer Smith 1 ABSTRACT Satellite observations reveal a mesoscale oceanic circulation
More information3. Midlatitude Storm Tracks and the North Atlantic Oscillation
3. Midlatitude Storm Tracks and the North Atlantic Oscillation Copyright 2006 Emily Shuckburgh, University of Cambridge. Not to be quoted or reproduced without permission. EFS 3/1 Review of key results
More informationEddy-induced meridional heat transport in the ocean
GEOPHYSICAL RESEARCH LETTERS, VOL. 35, L20601, doi:10.1029/2008gl035490, 2008 Eddy-induced meridional heat transport in the ocean Denis L. Volkov, 1 Tong Lee, 1 and Lee-Lueng Fu 1 Received 28 July 2008;
More informationSupercomputer Technologies for Modeling Climate Change
International Conference and Early Career Scientists School on Environmental Observations, Modeling and Information Systems ENVIROMIS-2010, 5-11 July 2010, Tomsk, Russia Supercomputer Technologies for
More information7 The General Circulation
7 The General Circulation 7.1 The axisymmetric state At the beginning of the class, we discussed the nonlinear, inviscid, axisymmetric theory of the meridional structure of the atmosphere. The important
More informationMagnetohydrodynamic Turbulence
Magnetohydrodynamic Turbulence Stanislav Boldyrev (UW-Madison) Jean Carlos Perez (U. New Hampshire), Fausto Cattaneo (U. Chicago), Joanne Mason (U. Exeter, UK) Vladimir Zhdankin (UW-Madison) Konstantinos
More informationTopographic Enhancement of Eddy Efficiency in Baroclinic Equilibration
Topographic Enhancement of Eddy Efficiency in Baroclinic Equilibration JPO, 44 (8), 2107-2126, 2014 by Ryan Abernathey Paola Cessi as told by Navid CASPO theory seminar, 28 May 2016 section 2 what s the
More informationUncertainty in Ocean General Circulation Model Mixing Tensors
Uncertainty in Ocean General Circulation Model Mixing Tensors Baylor Fox-Kemper, University of Colorado Boulder, Brown U. (>Jan. 2013) Cooperative Insititute for Research in Environmental Sciences and
More informationActive microwave systems (2) Satellite Altimetry * the movie * applications
Remote Sensing: John Wilkin wilkin@marine.rutgers.edu IMCS Building Room 211C 732-932-6555 ext 251 Active microwave systems (2) Satellite Altimetry * the movie * applications Altimeters (nadir pointing
More informationOn the feasibility of merging LES with RANS for the near-wall region of attached turbulent flows
Center for Turbulence Research Annual Research Briefs 1998 267 On the feasibility of merging LES with RANS for the near-wall region of attached turbulent flows By Jeffrey S. Baggett 1. Motivation and objectives
More informationA Reexamination of the Emergy Input to a System from the Wind
Emergy Synthesis 9, Proceedings of the 9 th Biennial Emergy Conference (2017) 7 A Reexamination of the Emergy Input to a System from the Wind Daniel E. Campbell, Laura E. Erban ABSTRACT The wind energy
More informationM.Sc. in Meteorology. Physical Meteorology Prof Peter Lynch. Mathematical Computation Laboratory Dept. of Maths. Physics, UCD, Belfield.
M.Sc. in Meteorology Physical Meteorology Prof Peter Lynch Mathematical Computation Laboratory Dept. of Maths. Physics, UCD, Belfield. Climate Change???????????????? Tourists run through a swarm of pink
More informationPhysical Oceanographic Context of Seamounts. Pierre Dutrieux Department of Oceanography, University of Hawai'i at Manoa, Honolulu, Hawai'i
Physical Oceanographic Context of Seamounts Pierre Dutrieux Department of Oceanography, University of Hawai'i at Manoa, Honolulu, Hawai'i PEW Workshop, October 2007 Seamounts: definitions submarine topographic
More informationEliassen-Palm Cross Sections Edmon et al. (1980)
Eliassen-Palm Cross Sections Edmon et al. (1980) Cecily Keppel November 14 2014 Eliassen-Palm Flux For β-plane Coordinates (y, p) in northward, vertical directions Zonal means F = v u f (y) v θ θ p F will
More informationAnalysis and modelling of subgrid-scale motions in near-wall turbulence
J. Fluid Mech. (1998), vol. 356, pp. 327 352. Printed in the United Kingdom c 1998 Cambridge University Press 327 Analysis and modelling of subgrid-scale motions in near-wall turbulence By CARLOS HÄRTEL
More informationFrom Climate to Kolmogorov - Simulations Spanning Upper Ocean Scales
From Climate to Kolmogorov - Simulations Spanning Upper Ocean Scales Baylor Fox-Kemper (CU-Boulder & CIRES) with Peter Hamlington (CU), Sean Haney (ATOC), Adrean Webb (APPM), Scott Bachman (ATOC), Katie
More informationSubmesoscale Routes to Lateral Mixing in the Ocean
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Submesoscale Routes to Lateral Mixing in the Ocean Amit Tandon Physics Department, UMass Dartmouth 285 Old Westport Rd
More informationIntroduction to Turbulence, its Numerical Modeling and Downscaling
560.700: Applications of Science-Based Coupling of Models October, 2008 Introduction to Turbulence, its Numerical Modeling and Downscaling Charles Meneveau Department of Mechanical Engineering Center for
More informationSchematic from Vallis: Rossby waves and the jet
Schematic from Vallis: Rossby waves and the jet Schematic from Vallis: Rossby waves and the jet A Barotropic Model Stochastic stirring + linear damping Force barotropic vort. eqn. with white noise in storm
More informationBaroclinic turbulence in the ocean: analysis with primitive equation and quasi-geostrophic simulations K. SHAFER SMITH
Generated using V3.0 of the official AMS LATX template journal page layout FOR AUTHOR US ONLY, NOT FOR SUBMISSION! Baroclinic turbulence in the ocean: analysis with primitive equation and quasi-geostrophic
More informationAFRICAN EASTERLY WAVES IN CURRENT AND FUTURE CLIMATES
AFRICAN EASTERLY WAVES IN CURRENT AND FUTURE CLIMATES Victoria Dollar RTG Seminar Research - Spring 2018 April 16, 2018 Victoria Dollar ASU April 16, 2018 1 / 26 Overview Introduction Rossby waves and
More informationHomogeneous Turbulence Dynamics
Homogeneous Turbulence Dynamics PIERRE SAGAUT Universite Pierre et Marie Curie CLAUDE CAMBON Ecole Centrale de Lyon «Hf CAMBRIDGE Щ0 UNIVERSITY PRESS Abbreviations Used in This Book page xvi 1 Introduction
More informationAnalysis of the Kolmogorov equation for filtered wall-turbulent flows
J. Fluid Mech. (211), vol. 676, pp. 376 395. c Cambridge University Press 211 doi:1.117/s2211211565 Analysis of the Kolmogorov equation for filtered wall-turbulent flows A. CIMARELLI AND E. DE ANGELIS
More informationApplying Basin-Scale HyCOM Hindcasts in Providing Open Boundary Conditions for Nested High-Resolution Coastal Circulation Modeling
Applying Basin-Scale HyCOM Hindcasts in Providing Open Boundary Conditions for Nested High-Resolution Coastal Circulation Modeling Ruoying He Woods Hole Oceanographic Institution December 7, 2005 Cape
More informationMagnetohydrodynamic Turbulence: solar wind and numerical simulations
Magnetohydrodynamic Turbulence: solar wind and numerical simulations Stanislav Boldyrev (UW-Madison) Jean Carlos Perez (U. New Hampshire) Fausto Cattaneo (U. Chicago) Joanne Mason (U. Exeter, UK) Vladimir
More informationFrictional Damping of Baroclinic Waves
Frictional Damping of Baroclinic Waves HHH, 26th May 2006 Bob Plant With thanks to Stephen Belcher, Brian Hoskins, Dan Adamson Motivation Control simulation, T+60 Simulation with no boundary layer turbulence,
More informationDownscaling Global Warming with a Regional Ocean- Atmosphere Model over the Tropical Atlantic
Downscaling Global Warming with a Regional Ocean- Atmosphere Model over the Tropical Atlantic Role of equatorial ocean dynamics: equatorial upwelling and ocean mesoscale variability Hyodae Seo and Shang-Ping
More informationClimate Change and Predictability of the Indian Summer Monsoon
Climate Change and Predictability of the Indian Summer Monsoon B. N. Goswami (goswami@tropmet.res.in) Indian Institute of Tropical Meteorology, Pune Annual mean Temp. over India 1875-2004 Kothawale, Roopakum
More informationReliability of LES in complex applications
Reliability of LES in complex applications Bernard J. Geurts Multiscale Modeling and Simulation (Twente) Anisotropic Turbulence (Eindhoven) DESIDER Symposium Corfu, June 7-8, 27 Sample of complex flow
More informationThe Turbulent Oscillator: A Mechanism of Low-Frequency Variability
The Turbulent Oscillator: A Mechanism of Low-Frequency Variability of the Wind-Driven Ocean Gyres People: Pavel Berloff 1,2 Andy Hogg 3 William Dewar 4 Institutions: 1 Woods Hole Oceanographic Institution,
More informationDynamical Evaluation of Gulf Stream Simulations in Models with High Vertical Resolution
Dynamical Evaluation of Gulf Stream Simulations in Models with High Vertical Resolution Harley E. Hurlburt 1, Eric P. Chassignet 2, E. Joseph Metzger 1, James G. Richman 1, William J. Schmitz, Jr. 3, Jay
More informationUsing Cloud-Resolving Models for Parameterization Development
Using Cloud-Resolving Models for Parameterization Development Steven K. Krueger University of Utah! 16th CMMAP Team Meeting January 7-9, 2014 What is are CRMs and why do we need them? Range of scales diagram
More information