Variability of Stochastically Forced Zonal Jets Laura Cope , Peter - - PowerPoint PPT Presentation
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
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?
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
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
40°S 50°S 60°S 40°S 50°S 60°S 1995 1996 Year
OVERVIEW OF IDEALIZED MODELS
Planetary rotation Turbulence Jets Friction
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
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Features
𝜖𝜂 𝜖𝑢 + 𝒗 & ∇𝜂 + 𝛾𝑤 = 𝜊 − 𝜈𝜂 + 𝜉/∇0/𝜂
Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Increasing zonal wavenumber
IDEALIZED MODELS: MATHEMATICAL FORMULATION
Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Low modes ≤ 𝚳 High modes > 𝚳 Increasing zonal wavenumber Separation = 𝚳
IDEALIZED MODELS: MATHEMATICAL FORMULATION
Generalized Quasilinear Approximation Marston, Chini, Tobias (2016) Reference: Low modes ≤ 𝚳 Increasing zonal wavenumber High modes > 𝚳 Separation = 𝚳
IDEALIZED MODELS: MATHEMATICAL FORMULATION
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
SUMMARY OF IDEALIZED MODELS
Reduction in nonlinearity
Nonlinear (Λ = 𝑂) Generalized Quasilinear (Λ = 1) Quasilinear (Λ = 0)
NUMERICAL SIMULATIONS – NONLINEAR (NL) MODEL
Zonal velocity field Zonal mean zonal velocity Zonal mean zonal velocity evolution in time
NONLINEAR (NL) MODEL - TYPES OF VARIABILITY
Randomly wandering Merging & nucleating Migrating
New type of variability found: jets migrate north and south
Result 1
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)
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?
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?
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
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)
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)
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?
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?
Migrating north Migrating south Not migrating 𝜂(𝑦, 𝑧, 𝑢) Schematic
Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?
Migrating north Migrating south Not migrating 𝜂(𝑦, 𝑧, 𝑢) Schematic
Q1: WHY DO JETS MIGRATE ONLY WHEN 𝚳 ≥ 𝟐?
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?
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?
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
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?
A CLOSER LOOK AT ZONAL JET MIGRATION
Question 3
Why do jets migrate only when Λ ≥ 1? Can we predict the speed
- f migration?