Variability of Stochastically Forced Zonal Jets Laura Cope , Peter - - PowerPoint PPT Presentation

variability of stochastically forced zonal jets
SMART_READER_LITE
LIVE PREVIEW

Variability of Stochastically Forced Zonal Jets Laura Cope , Peter - - PowerPoint PPT Presentation

Variability of Stochastically Forced Zonal Jets Laura Cope , Peter Haynes Department of Applied Mathematics and Theoretical Physics, University of Cambridge MOTIVATION Gaseous Giant Planets Earths Atmosphere & Oceans What insights can


slide-1
SLIDE 1

Variability of Stochastically Forced Zonal Jets

Laura Cope, Peter Haynes

Department of Applied Mathematics and Theoretical Physics, University of Cambridge

slide-2
SLIDE 2

MOTIVATION

Gaseous Giant Planets Earth’s Atmosphere & Oceans

Credit: NASA/JPL-Caltech/Space Science Institute Credit: https://www.nasa.gov Credit: NASA / Science Photo Library Credit: NASA, ESA

What insights can we learn about the variability of jet streams using idealized models?

slide-3
SLIDE 3

OBSERVATIONS

Earth’s Atmosphere Earth’s Oceans

Increasing time variability

(earth.nullschool.net) (Sokolov, Rintoul 1996) 40°S 50°S 60°S 1995 1996 Year

Jupiter

Voyager 1979-1980

slide-4
SLIDE 4

OBSERVATIONS

Earth’s Atmosphere Earth’s Oceans

Increasing time variability

(earth.nullschool.net) (Sokolov, Rintoul 1996) 40°S 50°S 60°S 1995 1996 Year

Jupiter

Voyager 1979-1980 Cassini 2000

slide-5
SLIDE 5

40°S 50°S 60°S 40°S 50°S 60°S 1995 1996 Year

slide-6
SLIDE 6

OVERVIEW OF IDEALIZED MODELS

Planetary rotation Turbulence Jets Friction

slide-7
SLIDE 7

IDEALIZED MODELS: MATHEMATICAL FORMULATION

Stochastic Force

Fourier space: Physical space:

Equation of Motion: Vorticity Equation

Stochastic forcing Linear friction Hyper- viscosity Planetary Rotation Beta, Energy input rate,. Damping rate, .

µ

<latexit sha1_base64="lHfLRKj6qzQlWtG4bt8R2dg4o4s=">AB6nicdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHiOYByRJmJ5NkyMzsMjMrhCWf4MWDIl79Im/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlo5TRWiTxDxWnQhrypmkTcMp51EUSwiTtvR5Grut+p0iyWd2a0FDgkWRDRrCx0m1PpP1C0XP9UhBUfOS5tVotqJSXxCtXke96CxRhUa/8N4bxCQVBrCsdZd30tMmGFlGOF0lu+lmiaYTPCIdi2VWFAdZotTZ+jcKgM0jJUtadBC/T6RYaH1VES2U2Az1r+9ufiX103NsBpmTCapoZIsFw1TjkyM5n+jAVOUGD61BPF7K2IjLHCxNh08jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQGAED/AEzw53Hp0X53XZuasZk7gB5y3T+06ji0=</latexit><latexit sha1_base64="lHfLRKj6qzQlWtG4bt8R2dg4o4s=">AB6nicdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHiOYByRJmJ5NkyMzsMjMrhCWf4MWDIl79Im/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlo5TRWiTxDxWnQhrypmkTcMp51EUSwiTtvR5Grut+p0iyWd2a0FDgkWRDRrCx0m1PpP1C0XP9UhBUfOS5tVotqJSXxCtXke96CxRhUa/8N4bxCQVBrCsdZd30tMmGFlGOF0lu+lmiaYTPCIdi2VWFAdZotTZ+jcKgM0jJUtadBC/T6RYaH1VES2U2Az1r+9ufiX103NsBpmTCapoZIsFw1TjkyM5n+jAVOUGD61BPF7K2IjLHCxNh08jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQGAED/AEzw53Hp0X53XZuasZk7gB5y3T+06ji0=</latexit><latexit sha1_base64="lHfLRKj6qzQlWtG4bt8R2dg4o4s=">AB6nicdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHiOYByRJmJ5NkyMzsMjMrhCWf4MWDIl79Im/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlo5TRWiTxDxWnQhrypmkTcMp51EUSwiTtvR5Grut+p0iyWd2a0FDgkWRDRrCx0m1PpP1C0XP9UhBUfOS5tVotqJSXxCtXke96CxRhUa/8N4bxCQVBrCsdZd30tMmGFlGOF0lu+lmiaYTPCIdi2VWFAdZotTZ+jcKgM0jJUtadBC/T6RYaH1VES2U2Az1r+9ufiX103NsBpmTCapoZIsFw1TjkyM5n+jAVOUGD61BPF7K2IjLHCxNh08jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQGAED/AEzw53Hp0X53XZuasZk7gB5y3T+06ji0=</latexit><latexit sha1_base64="lHfLRKj6qzQlWtG4bt8R2dg4o4s=">AB6nicdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHiOYByRJmJ5NkyMzsMjMrhCWf4MWDIl79Im/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlo5TRWiTxDxWnQhrypmkTcMp51EUSwiTtvR5Grut+p0iyWd2a0FDgkWRDRrCx0m1PpP1C0XP9UhBUfOS5tVotqJSXxCtXke96CxRhUa/8N4bxCQVBrCsdZd30tMmGFlGOF0lu+lmiaYTPCIdi2VWFAdZotTZ+jcKgM0jJUtadBC/T6RYaH1VES2U2Az1r+9ufiX103NsBpmTCapoZIsFw1TjkyM5n+jAVOUGD61BPF7K2IjLHCxNh08jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQGAED/AEzw53Hp0X53XZuasZk7gB5y3T+06ji0=</latexit>

β

<latexit sha1_base64="2pJr3QmNpmuNZ2f/k9v5P74Yqu4=">AB7HicdVBNS8NAEN3Ur1q/qh69LBbBU0haS9pbwYvHCqYtKFstpt26WYTdidCf0NXjwo4tUf5M1/4/ZDUNEHA4/3ZpiZF6aCa3CcD6uwsbm1vVPcLe3tHxwelY9POjrJFGU+TUSieiHRTHDJfOAgWC9VjMShYN1wer3wu/dMaZ7IO5ilLIjJWPKIUwJG8gchAzIsVxzbrXpe3cWO3Ww2vXptRZxaA7u2s0QFrdEelt8Ho4RmMZNABdG67zopBDlRwKlg89Ig0ywldErGrG+oJDHTQb48do4vjDLCUaJMScBL9ftETmKtZ3FoOmMCE/3bW4h/ef0MokaQc5lmwCRdLYoygSHBi8/xiCtGQcwMIVRxcyumE6IBZNPyYTw9Sn+n3Sqtmuyur2qtKrOIroDJ2jS+QiD7XQDWojH1HE0QN6Qs+WtB6tF+t1Vqw1jOn6Aest09TwY7</latexit><latexit sha1_base64="2pJr3QmNpmuNZ2f/k9v5P74Yqu4=">AB7HicdVBNS8NAEN3Ur1q/qh69LBbBU0haS9pbwYvHCqYtKFstpt26WYTdidCf0NXjwo4tUf5M1/4/ZDUNEHA4/3ZpiZF6aCa3CcD6uwsbm1vVPcLe3tHxwelY9POjrJFGU+TUSieiHRTHDJfOAgWC9VjMShYN1wer3wu/dMaZ7IO5ilLIjJWPKIUwJG8gchAzIsVxzbrXpe3cWO3Ww2vXptRZxaA7u2s0QFrdEelt8Ho4RmMZNABdG67zopBDlRwKlg89Ig0ywldErGrG+oJDHTQb48do4vjDLCUaJMScBL9ftETmKtZ3FoOmMCE/3bW4h/ef0MokaQc5lmwCRdLYoygSHBi8/xiCtGQcwMIVRxcyumE6IBZNPyYTw9Sn+n3Sqtmuyur2qtKrOIroDJ2jS+QiD7XQDWojH1HE0QN6Qs+WtB6tF+t1Vqw1jOn6Aest09TwY7</latexit><latexit sha1_base64="2pJr3QmNpmuNZ2f/k9v5P74Yqu4=">AB7HicdVBNS8NAEN3Ur1q/qh69LBbBU0haS9pbwYvHCqYtKFstpt26WYTdidCf0NXjwo4tUf5M1/4/ZDUNEHA4/3ZpiZF6aCa3CcD6uwsbm1vVPcLe3tHxwelY9POjrJFGU+TUSieiHRTHDJfOAgWC9VjMShYN1wer3wu/dMaZ7IO5ilLIjJWPKIUwJG8gchAzIsVxzbrXpe3cWO3Ww2vXptRZxaA7u2s0QFrdEelt8Ho4RmMZNABdG67zopBDlRwKlg89Ig0ywldErGrG+oJDHTQb48do4vjDLCUaJMScBL9ftETmKtZ3FoOmMCE/3bW4h/ef0MokaQc5lmwCRdLYoygSHBi8/xiCtGQcwMIVRxcyumE6IBZNPyYTw9Sn+n3Sqtmuyur2qtKrOIroDJ2jS+QiD7XQDWojH1HE0QN6Qs+WtB6tF+t1Vqw1jOn6Aest09TwY7</latexit><latexit sha1_base64="2pJr3QmNpmuNZ2f/k9v5P74Yqu4=">AB7HicdVBNS8NAEN3Ur1q/qh69LBbBU0haS9pbwYvHCqYtKFstpt26WYTdidCf0NXjwo4tUf5M1/4/ZDUNEHA4/3ZpiZF6aCa3CcD6uwsbm1vVPcLe3tHxwelY9POjrJFGU+TUSieiHRTHDJfOAgWC9VjMShYN1wer3wu/dMaZ7IO5ilLIjJWPKIUwJG8gchAzIsVxzbrXpe3cWO3Ww2vXptRZxaA7u2s0QFrdEelt8Ho4RmMZNABdG67zopBDlRwKlg89Ig0ywldErGrG+oJDHTQb48do4vjDLCUaJMScBL9ftETmKtZ3FoOmMCE/3bW4h/ef0MokaQc5lmwCRdLYoygSHBi8/xiCtGQcwMIVRxcyumE6IBZNPyYTw9Sn+n3Sqtmuyur2qtKrOIroDJ2jS+QiD7XQDWojH1HE0QN6Qs+WtB6tF+t1Vqw1jOn6Aest09TwY7</latexit>

<latexit sha1_base64="rJNyLzTlYpLFsmnVy72JKa9NeZ4=">AB73icdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHCOYByRJmJ5NkyOzMOjMrhCU/4cWDIl79HW/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlpapIrRJeqE2FNORO0aZjhtJMoiuOI03Y0uZr7XuqNJPi1kwTGsZ4JNiQEWys1OnRDMuRb9Q9Fy/FAQVH3lurVYLKuUl8cpV5LveAkVYodEvPcGkqQxFYZwrHX9xITZlgZRjid5XupgkmEzyiXUsFjqkOs8W9M3RulQEaSmVLGLRQv09kONZ6Gke2M8ZmrH97c/Evr5uaYTXMmEhSQwVZLhqmHBmJ5s+jAVOUGD61BPF7K2IjLHCxNiI8jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQIDAzBs3PnPDovzuydc1ZzZzADzhvn9ytkHc=</latexit><latexit sha1_base64="rJNyLzTlYpLFsmnVy72JKa9NeZ4=">AB73icdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHCOYByRJmJ5NkyOzMOjMrhCU/4cWDIl79HW/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlpapIrRJeqE2FNORO0aZjhtJMoiuOI03Y0uZr7XuqNJPi1kwTGsZ4JNiQEWys1OnRDMuRb9Q9Fy/FAQVH3lurVYLKuUl8cpV5LveAkVYodEvPcGkqQxFYZwrHX9xITZlgZRjid5XupgkmEzyiXUsFjqkOs8W9M3RulQEaSmVLGLRQv09kONZ6Gke2M8ZmrH97c/Evr5uaYTXMmEhSQwVZLhqmHBmJ5s+jAVOUGD61BPF7K2IjLHCxNiI8jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQIDAzBs3PnPDovzuydc1ZzZzADzhvn9ytkHc=</latexit><latexit sha1_base64="rJNyLzTlYpLFsmnVy72JKa9NeZ4=">AB73icdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHCOYByRJmJ5NkyOzMOjMrhCU/4cWDIl79HW/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlpapIrRJeqE2FNORO0aZjhtJMoiuOI03Y0uZr7XuqNJPi1kwTGsZ4JNiQEWys1OnRDMuRb9Q9Fy/FAQVH3lurVYLKuUl8cpV5LveAkVYodEvPcGkqQxFYZwrHX9xITZlgZRjid5XupgkmEzyiXUsFjqkOs8W9M3RulQEaSmVLGLRQv09kONZ6Gke2M8ZmrH97c/Evr5uaYTXMmEhSQwVZLhqmHBmJ5s+jAVOUGD61BPF7K2IjLHCxNiI8jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQIDAzBs3PnPDovzuydc1ZzZzADzhvn9ytkHc=</latexit><latexit sha1_base64="rJNyLzTlYpLFsmnVy72JKa9NeZ4=">AB73icdVDLSgNBEOz1GeMr6tHLYBA8LbuJYZNbwIvHCOYByRJmJ5NkyOzMOjMrhCU/4cWDIl79HW/+jZOHoKIFDUVN91dUcKZNp734aytb2xubed28rt7+weHhaPjlpapIrRJeqE2FNORO0aZjhtJMoiuOI03Y0uZr7XuqNJPi1kwTGsZ4JNiQEWys1OnRDMuRb9Q9Fy/FAQVH3lurVYLKuUl8cpV5LveAkVYodEvPcGkqQxFYZwrHX9xITZlgZRjid5XupgkmEzyiXUsFjqkOs8W9M3RulQEaSmVLGLRQv09kONZ6Gke2M8ZmrH97c/Evr5uaYTXMmEhSQwVZLhqmHBmJ5s+jAVOUGD61BPF7K2IjLHCxNiI8jaEr0/R/6RVcn2b1c1lsV5axZGDUziDC/AhgDpcQwOaQIDAzBs3PnPDovzuydc1ZzZzADzhvn9ytkHc=</latexit>

2D (barotropic) Doubly periodic Beta plane Stochastic force

Features

𝜖𝜂 𝜖𝑢 + 𝒗 & ∇𝜂 + 𝛾𝑤 = 𝜊 − 𝜈𝜂 + 𝜉/∇0/𝜂

slide-8
SLIDE 8

Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Increasing zonal wavenumber

IDEALIZED MODELS: MATHEMATICAL FORMULATION

slide-9
SLIDE 9

Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Low modes ≤ 𝚳 High modes > 𝚳 Increasing zonal wavenumber Separation = 𝚳

IDEALIZED MODELS: MATHEMATICAL FORMULATION

slide-10
SLIDE 10

Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Low modes ≤ 𝚳 Increasing zonal wavenumber High modes > 𝚳 Separation = 𝚳

IDEALIZED MODELS: MATHEMATICAL FORMULATION

slide-11
SLIDE 11

Overview

Low modes ≤ 𝚳 High modes > 𝚳 Generalized Quasilinear Approximation

Low-high mode decomposition: Basic vorticity equation: Low modes: High modes: Vorticity equation:

𝜔 = 5

|7|89

𝑓;7< = 𝜔7 + 5

|7|>9

𝑓;7< = 𝜔7 = ? 𝜔 + 𝜔′

AB AC = ℒ 𝜂 + 𝒪[𝜂, 𝜂] A? B AC = ℒ

̅ 𝜂 + H 𝒪[ ̅ 𝜂, ̅ 𝜂] + H 𝒪[𝜂J, 𝜂J]

ABL AC = ℒ 𝜂J + 𝒪J[ ̅

𝜂, 𝜂J] +[HHNL]

𝜖𝜂 𝜖𝑢 + 𝒗 & ∇𝜂 + 𝛾𝑤 − HHNL = 𝜊 − 𝜈𝜂 + 𝜉/∇0/𝜂

IDEALIZED MODELS: MATHEMATICAL FORMULATION

slide-12
SLIDE 12

SUMMARY OF IDEALIZED MODELS

Reduction in nonlinearity

Nonlinear (Λ = 𝑂) Generalized Quasilinear (Λ = 1) Quasilinear (Λ = 0)

slide-13
SLIDE 13

NUMERICAL SIMULATIONS – NONLINEAR (NL) MODEL

Zonal velocity field Zonal mean zonal velocity Zonal mean zonal velocity evolution in time

slide-14
SLIDE 14

NONLINEAR (NL) MODEL - TYPES OF VARIABILITY

Randomly wandering Merging & nucleating Migrating

New type of variability found: jets migrate north and south

Result 1

slide-15
SLIDE 15

ALL MODELS - TYPES OF VARIABILITY

Randomly wandering Merging & nucleating Migrating QL Model (Λ = 0) No clear migration GQL Model (Λ = 1) NL Model (Λ = 𝑂)

slide-16
SLIDE 16

A CLOSER LOOK AT ZONAL JET MIGRATION

Question 1 Question 3 Question 2

Why do jets migrate only when Λ ≥ 1?

Low modes ≤ 𝚳 High modes > 𝚳

Do jets migrate in more complex systems? Can we predict the speed

  • f migration?
slide-17
SLIDE 17

A CLOSER LOOK AT ZONAL JET MIGRATION

Question 1

Why do jets migrate only when Λ ≥ 1?

Low modes ≤ 𝚳 High modes > 𝚳

Do jets migrate in more complex systems? Can we predict the speed

  • f migration?
slide-18
SLIDE 18

AN INTRODUCTION TO ZONONS

Reference: Sukoriansky, Dikovskaya, Galperin (2008), PRL

NL Model (Λ = 𝑂) Zonons (Nonlinear waves)

Coherent structures excited by Rossby waves with same 𝑙< and same phase speed Nonlinear zonons Linear Rossby wave

slide-19
SLIDE 19

AN INTRODUCTION TO ZONONS

Reference: Sukoriansky, Dikovskaya, Galperin (2008), PRL

Zonons (Nonlinear waves)

Coherent structures excited by Rossby waves with same 𝑙< and same phase speed Nonlinear zonons Linear Rossby wave

GQL Model (Λ = 1)

slide-20
SLIDE 20

AN INTRODUCTION TO ZONONS

Reference: Sukoriansky, Dikovskaya, Galperin (2008), PRL

Zonons (Nonlinear waves)

Coherent structures excited by Rossby waves with same 𝑙< and same phase speed Nonlinear zonons Linear Rossby wave

QL Model (Λ = 0)

slide-21
SLIDE 21

NL Model QL Model Not Migrating Migrating North No clear migration

Migration requires Λ ≥ 1 when jets and zonons coexist

Result 2

jet zonons

Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?

slide-22
SLIDE 22

NL Model QL Model Not Migrating Migrating North No clear migration

Migration requires Λ ≥ 1 when jets and zonons coexist

Result 2

jet zonons

Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?

slide-23
SLIDE 23

Migrating north Migrating south Not migrating 𝜂(𝑦, 𝑧, 𝑢) Schematic

Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?

slide-24
SLIDE 24

Migrating north Migrating south Not migrating 𝜂(𝑦, 𝑧, 𝑢) Schematic

Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?

slide-25
SLIDE 25

Result 3

Migration requires an asymmetric eddy forcing and mean flow

Reynolds stress force Zonal mean flow

Zonal mean forcing

AH [ AC = 𝑤′𝜂′ −𝜈?

𝑣

Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?

slide-26
SLIDE 26

A CLOSER LOOK AT ZONAL JET MIGRATION

Question 2

Why do jets migrate only when Λ ≥ 1? Do jets migrate in more complex systems? Can we predict the speed

  • f migration?
slide-27
SLIDE 27

Q2: CAN WE PREDICT THE SPEED OF MIGRATION?

ZMF index Jet migration speed

0.3 0.9

Result 4

Migration speed is given approximately by: speed ∝ (ZMF)ef

Zonal mean flow index (ZMF)

ZMF = Fraction of energy in mean flow 1

No jets No eddies Eddies & jets

𝜀𝑦 𝜀𝑢 speed = 𝜀𝑦 𝜀𝑢

slide-28
SLIDE 28

Result 4

Zonal mean flow index (ZMF)

ZMF = Fraction of energy in mean flow 1

No jets No eddies Eddies & jets

speed = 𝜀𝑦 𝜀𝑢

log (Jet migration speed) slope = -3 log (ZMF index)

Migration speed is given approximately by: speed ∝ (ZMF)ef

𝜀𝑦 𝜀𝑢

Q2: CAN WE PREDICT THE SPEED OF MIGRATION?

slide-29
SLIDE 29

A CLOSER LOOK AT ZONAL JET MIGRATION

Question 3

Why do jets migrate only when Λ ≥ 1? Can we predict the speed

  • f migration?

Do jets migrate in more complex systems?

slide-30
SLIDE 30

Q3: DO JETS MIGRATE IN MORE COMPLEX SYSTEMS?

General circulation model: Poleward drift Atmosphere observations: Poleward drift General circulation model: Equatorward drift

30°S 60°S 90°S EQ 150 days Kemke & Kaspi (2015), JAMES Feldstein (1998), JAS Young, Read & Wang (2019), Icarus

slide-31
SLIDE 31

CONCLUSIONS

OBJECTIVE METHOD MODELS

Study of jet stream variability Rotation + turbulence + friction = zonal jet Generalized quasilinear approximation

slide-32
SLIDE 32

CONCLUSIONS

Migration requires an asymmetric eddy forcing

4 2 1 3

Migration speed is approximately: speed ∝ (ZMF)ef New type of jet variability found: migrating jets Migration requires Λ ≥ 1 when jets and zonons coexist