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Nonlinearity of atmospheric response
to ENSO and MJO Hai Lin Recherche en Prévision Numérique, Environment and Climate Change Canada BIRS Workshop 17w5061, November 19-24, 2017 Banff, Alberta
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Outlines Extratropical response to El Nino and La Nina Observations
Numerical experiments Extratropical response to MJO
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ENSO Leading source of seasonal forecasting skill in the extratropics → El Niño & La Niña Is the extratropical response to El Niño a mirror image of that to La Niña? Why?
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Composite of T2m anomaly for 5 El Nino winters and 5 La Nina winters
Hoerling et al. 1997, JCLIM
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Composite of Z500 anomaly for 5 El Nino winters and 5 La Nina winters
Hoerling et al. 1997, JCLIM
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Composite of SST anomaly for 5 El Nino winters and 5 La Nina winters
Hoerling et al. 1997, JCLIM
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Composite of precip anomaly for 5 El Nino winters and 5 La Nina winters
Hoerling et al. 1997, JCLIM
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Explanation for extratropical nonlinearity
One possible explanation is the nonlinear relationship between SST and precipitation in the tropics: Positive SST anomalies can initiate deep convection within the core of the east Pacific cold tongue, whereas negative SST anomalies will have their largest effect in the west Pacific warm pool region. Any other dynamical reason?
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Numerical experiments
Primitive equation model (Hall 2000) Specified tropical diabatic heating anomaly similar to ENSO, Fixed location 61 experiments with different heating amplitudes from negative to positive 30 members of 120 day integrations for each amplitude
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Ensemble mean Z550 anomaly response
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Dominant response patterns
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Transient response Three sets of experiments:
Each set has 50 integrations from different initial conditions Each integration lasts 30 days Daily ensemble difference → response Control run ─ climatological forcing; El Niño run ─ climatological forcing + tropical heating anomaly La Niña run ─ climatological forcing + tropical cooling anomaly The same 50 initial conditions for all three sets of experiments, so that the only difference is the thermal perturbation.
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Forcing anomaly Only in temperature equation Maximum at 350 mb
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Day 1
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Day 2
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Day 3
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Day 4
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Day 5
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Day 6
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Day 7
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Day 8
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Day 9
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Day 10
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Day 11
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Day 12
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Day 13
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Day 14
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Days 16-30
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W vector Days 16-30
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ω’ = - h’ / [α – cp(∂T/ ∂p + ∂T’/ ∂p)]
Tropical circulation Why La Niña has a stronger response? →Stronger vertical motion due to changes in static stability _ ω’ = - h’ / [α – cp(∂T/ ∂p + ∂T’/ ∂p)] In the center of response, adiabatic process tends to balance the diabatic heating anomaly El Nino: ∂T’/ ∂p < 0 La Nina: ∂T’/ ∂p > 0
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Asymmetric development of tropical waves
To the west of thermal forcing: El Nino, upper troposphere easterly suppress Rossby wave development La Nina, upper troposphere westerly favors Rossby wave development In the center of response, adiabatic process tends to balance the diabatic heating anomaly
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Feedback from transients
Modified storm track Vorticity flux convergence by transients
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Days 16-30 Anomaly of Z550 rms for transients El Niño La Niña
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Days 16-30 Z550 tendency by transients El Niño La Niña
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MJO Leading source of skill for subseasonal predictions
Is there difference between extratropical response pattern to +MJO and that to -MJO?
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Composites of tropical
Precipitation rate for 8 MJO phases, according to Wheeler and Hendon index. Xie and Arkin pentad data,
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Lagged probability of the NAO index Positive: upper tercile; Negative: low tercile
Phase 1 2 3 4 5 6 7 8 Lag 0 +45% −42% Lag +1 +47% −46% Lag +2 +50% +42% −41% Lag +3 +48% −48% Lag +4 −39% Lag +5 (Lin et al. JCLIM, 2009)
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Z500 anomaly composites following MJO phase 3 and 7
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Wintertime North Atlantic weather regimes
From Cassou (2008)
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Observed nonlinearity
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Dominant tropical subseasonal OLR patterns
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MJO forcing structure
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Experiments with MJO forcing
Three sets of experiments: Each set has 360 integrations from different initial conditions Each integration lasts 20 days Daily ensemble difference → response Control run ─ climatological forcing; +MJO run ─ climatological forcing + MJO -MJO run ─ climatological forcing - MJO The same 50 initial conditions for all three sets of experiments, so that the only difference is the thermal perturbation.
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Z500 ensemble mean response
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Spread Z500 response
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Z500 response to +MJO
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Z500 response to -MJO
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STRM200 response to +MJO STRM200 response to -MJO
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Summary Asymmetric response to El Nino and La Nina
In addition to the nonlinear relationship between SST and precipitation, there are dynamical mechanisms. Mechanisms include: 1) changes in static stability; 2) aymmetric development of tropical waves; and 3) feedback from synoptic-scale transients. The extratropical response to MJO is also nonlinear A better representation of such nonlinearity in numerical models would be helpful for subseasonal to seasonal predictions.
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