part i. mike mcphaden--what we know and what is unresolved: an observational perspective part ii....
TRANSCRIPT
Part I. Mike McPhaden--What We Know and What
is Unresolved: An Observational Perspective
Part II. David Battisti--What We Know and What is Unresolved: A Theoretical and Modeling Perspective
Sleeping Lady Mountain Retreat
Leavenworth, WA
19 September 2005
ENSO Dynamics and Global Impacts(“A Benign Problem”)
Sleeping Lady Mountain Retreat
Leavenworth, WA
19 September 2005
Part I. What We Know and What is Unresolved:
An Observational Perspective
El Niño is often followed by or preceded by La Niña: an unusual cooling of the tropical Pacific
Upwelling zones
Western Pacific “warm pool”
El Niño happens roughly every 2-7 years, lasts 12-18 months, and peaks at the end of the calendar year
Ocean-Atmosphere Feedback Loops During El Niño
Winds SST
Fast Positive Feedback Warms
Thermocline Depth
Slow Negative Feedback Cools
Ocean-Atmosphere Feedback Loops During La Niña
Winds SST
Fast Positive Feedback Cools
Thermocline Depth
Slow Negative Feedback Warms
NINO3.4 and SOI, 1980-2005
Darwin Tahiti
NINO-3.4
SOI and NINO3.4 Correlation=-0.9 (maximum @zero lag)
NINO3.4 and SOI, 1980-2005
Darwin Tahiti
NINO-3.4
El Niño/Southern Oscillation (ENSO):Warm phase (El Niño) // Cold Phase (La Niña)
Build up of excess heat content along equator is a necessary precondition for El Niño to occur.
The time between El Niños is determined by the time to recharge.
El Niño purges excess heat to higher latitudes, which terminates the event.
Upper Ocean Heat Content and El Niño(Recharge Oscillator Theory*)
*Wyrtki, 1985; Cane et al, 1986; Jin, 1997
Janowiak et al (2003) rainfall & ERS wind
velocity
Reynolds et al (2003) SST & ERS wind
stress
Peak Phase, 1997
Peak Phase, 2004
Janowiak et al (2003) rainfall & Quikscat
wind velocity relative to ERS climatology
Reynolds et al (2003) SST & Quikscat wind stress relative to ERS
climatology
DRY
Processes Affecting Equatorial SST
Enhanced Surface
Heat Fluxes
Zonal Advection
Suppressed Upwelling
Atmospheric Circulation Changes During El Niño
Changes in tropical rainfall patterns affect the global atmospheric circulation via “teleconnections”
Heavy rain
Pacific-North American (PNA) Pressure Pattern
Subtropical Jet Stream in NH Splits, Southern Branch Shifts
South and Intensifies
Impacts on Global Weather PatternsEl Niño shifts the probability of droughts, floods, heat waves, and
extreme weather events in large regions of the globe.
El Niño tends to suppress formation of Atlantic hurricanes.
El Niño tends to increase intensity and geographic range of Pacific hurricanes.
Opposite tendencies occur during La Niña.
Impacts on Tropical Storms
El Niño shifts the probability of droughts, floods, heat waves, and extreme weather events in large regions of the globe.
Magnitude of impacts scales with magnitude of Pacific SST anomalies
La Niña impacts roughly opposite to those of El Niño
Impacts on Global Weather Patterns
El Niño shifts the probability of droughts, floods, heat waves, and extreme weather events in large regions of the globe.
Washington State:
For 9 El Niños between 1941-1995 Expected by Chance
6 warm winters (~2°F increase) 3
2 neutral winters 3
1 cold winter 3
Impacts on Global Weather Patterns
Social and Economic Consequences
El Niño can affect life, property, and economic vitality due to weather related hazards.
1997-98 El Niño: U.S. Impacts
• Negative– 189 Fatalities– $4-5 billion in economic losses
• Positive– 850 lives saved– $20 billion in economic gains
Weather Noise and ENSO Stability If ENSO is a freely oscillating instability of the ocean-atmosphere
system governed by basin scale dynamics (Schopf & Suarez, 1988: Battisti & Hirst, 1989), weather “noise” is not essential but introduces irregularity.
If ENSO is a stable or weakly damped oscillator, external forcing in the form of weather noise is essential for initiation and development of warm events (Penland & Sardeshmukh, 1995; Moore & Kleeman, 1999; Kessler, 2002).
Mean thermocline depth
Stability characteristics determined by strength of ocean-atmosphere coupling and may vary decadally with changing background conditions (Kirtman and Schopf, 1998; Fedorov and Philander, 2000)
Fedorov & Philander, 2000
A=1980-90s; B=1960-70s
Current Conditions
Thermocline slopes down to west because of trade wind forcing.
Cold subsurface (100-200 m) temperature anomalies may indicate trend towards La Niña cooling.
Weather Noise and Stochastic ForcingEpisodic westerly wind
forcing and downwelling Kelvin
wave responses
Weather Noise and Stochastic Forcing
June-July 2004 Westerly Wind Burst
BEFORE:
“It is…likely that ENSO-neutral conditions will continue for the next 3 months (through August 2004).”
NOAA/NCEP10 June 2004
AFTER:
“El Niño conditions are expected to develop during the next 3 months.”
NOAA/NCEP5 August 2004
Westerly Wind Bursts Amplitude and Phase of ENSO
Westerly Wind Bursts (2°N-2°S)
0
2
4
6
8
10
12
1 2 3 4 5 6 7 8
Number of Westerly Events (Anomalies > 2 m/s)Maximum Zonal Wind (m/s)Maximum Zonal Fetch (x1000 km)
1997 200019991998 2001 20032002 2004
Westerly Wind Bursts Amplitude and Phase of ENSO
Westerly Wind Bursts (2°N-2°S)
0
2
4
6
8
10
12
1 2 3 4 5 6 7 8
Number of Westerly Events (Anomalies > 2 m/s)Maximum Zonal Wind (m/s)Maximum Zonal Fetch (x1000 km)
1997 200019991998 2001 20032002 2004
29°C
Stochastic forcing not entirely random
Effects of Westerly Wind Bursts on Equatorial SST
Westerly wind bursts cool the western Pacific, and warm the central and eastern Pacific Ocean via processes similar to those that operate on longer time scales (Shinoda & Hendon, 1998; Zhang, 2001; McPhaden, 2002).
Nonlinear processes can rectify short time scale variations into lower frequency changes (Lukas and Lindstrom, 1991; Kessler et al, 1995; Kessler and Kleeman, 2000; Waliser et al, 2003)
Spatial structure resembles “optimal perturbations” in some coupled models of ENSO (Moore and Kleeman, 1999).
Enhanced Surface
Heat FluxesZonal
Advection
Suppressed Upwelling
Sleeping Lady Mountain Retreat
Leavenworth, WA
19 September 2005
Part II. What We Know and What is Unresolved: A Theoretical and
Modeling Perspective
ENSO and Models/Theory: Resolved Issues• ENSO is the result of coupled atmosphere-ocean physics
in the tropical Pacific.– Ocean models must be forced by Southern Oscillation to produce ‘El Ninos’;– Atmosphere models must be forced by ‘El Nino’ SST to produce the Southern
Oscillation.
• ENSO is a true mode of the coupled system. • ENSO is a strong function of the climatological mean
state.– The annual cycle acts to coordinate the ENSO mode to peak at the end of the
calendar year.
• ENSO is predictable 12 months in advance.• ENSO affects are teleconnected from the tropical Pacific
by well-understood atmosphere and ocean dynamics:– Atmospheric impact is nearly global in extent.
www.atmos.washington.edu/~david/enso_pcc.pdf
Examples from an intermediate atmosphere/ocean model
Some models of the tropical Pacific Atmosphere and Ocean system have realistic
ENSO cycles
The processes that affect SST during an ENSO cycle are time and space dependant
Horizontal advection, vertical mixing, entrainment and surface heat fluxes are all important for ENSO
Nino3
Nino1
SST
Ten
denc
y
Time ( model years)
Basic elements of ENSO in observations and models
The “delayed oscillator physics” and “recharge oscillator” are complimentary toy-model descriptions of the ENSO mode.
Oce
an A
djus
tmen
t
&
Bje
rkne
s
ENSO is a true eigenmode of the coupled atmosphere/ocean system in the Pacific
The Bjerknes Mechanism and the Ocean Dynamics are features of the ENSO mode
Few Global Climate models have realistic ENSOs
First EOF of tropical Pacific SST (all IPCC ‘04 models)
Models w/ realistic ENSO space/time variability
•Global Climate models can produce realistic ENSO variability:
- Eg, the high resolution GFDL tropical Pacific-global atmosphere model (Philander et al 1992); the paleo-CSM.
•Unfortunately, none of the current generation global climate models have realistic ENSO variability. Why?
- lousy mean states in the tropical Pacific (why?); too low resolution in equatorial ocean; etc.
Only one model used in the last IPCC assessment simulated ENSO variability that did not violate the robust observational constraints.
The ENSO mode (cont).
ENSO exists because of the structure in the annual average state of the atmosphere/ocean system in the tropical Pacific, and …
ENSO tends to peak at the end of the calendar year because of theannual cycle in the in the basic state.
Spectrum of the pure ENSO mode
Thompson and Battisti 2001
ENSO as a linear, stochastic system
Results from a linear coupled atmosphere-ocean model forced by white noise
ObservedModel
ENSO peaks at the end of the calendar year because the of the annual cycle in the mean state
Observation
Model
ENSO is Predictable
• Skill depends on knowing where you are on the ENSO mode
• The long-lead time for skillful forecast is due to long period of the ENSO mode
• Presently, empirically based forecast models are at least as skillful as coupled GCMS
ENSO is predictable
Empirical models skillfully predict the state of ENSO 12 months in advance.
Skill 1965-1993Persistence
Empirical Models
•Skill depends on the start month.
Empirical Model
Persistence
These plots are from an empirical model using tropical Pacific SST (1981-present). For this month’s forecast, see www.atmos.washington.edu/~wroberts/ENSO/LIM.html
ENSO is predictable
March Starts September Starts
Why is ENSO irregular?The Seasonal Footprinting Mechanism
•ENSO is variable, in part, because the mode interacts with the annual cycle.
•The Seasonal Footprinting Mechanism accounts for about 1/4 to 1/3 of ENSO variance.
•Other factors responsible for irregularity? - Westerly wind bursts?
Vimont et al. 2001, 02, 03
ENSO: Unresolved Issues
• Is the ENSO mode stable or unstable in the present climate? (consensus - stable)
– If stable, what are the sources of energy for ENSO?– Does stability matter for predictability?
• What is the limit of predictability?– 24 months? 12 months?
• How does ENSO affect the mean state?• Will ENSO change due to Global Warming?• What is the cause of the decadal ENSO-like
variability in the present (1900-2005) climate?
ENSO: Unresolved Issues• The leading pattern of variability in the tropical Pacific has an ENSO
like pattern in SST and atmosphere circulation.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Something new, or the debris that results from averaging over past ENSO events? (see Vimont 2005 if you aren’t already convinced)
ENSO and Models: Resolved Issues• ENSO is the result of coupled atmosphere-ocean physics
in the tropical Pacific.– Ocean models must be forced by Southern Oscillation to produce ‘El Ninos’;– Atmosphere models must be force by ‘El Nino’ SST to produce the Southern
Oscillation.
• ENSO is a true mode of the coupled system. • ENSO is a strong function of the climatological mean
state.– The annual cycle acts to coordinate the ENSO mode to peak at the end of the
calendar year.
• ENSO is predictable 12 months in advance.• ENSO affects are teleconnected from the tropical Pacific
by well-understood atmosphere and ocean dynamics:– Atmospheric impact is nearly global in extent.
www.atmos.washington.edu/~david/enso_pcc.pdf
ENSO: Unresolved Issues
• Is the ENSO mode stable or unstable in the present climate? (consensus - stable)
– If stable, what are the sources of energy for ENSO?– Does stability matter for predictability?
• What is the limit of predictability?– 24 months? 12 months?
• How does ENSO affect the mean state?• Will ENSO change due to Global Warming?• What is the cause of the decadal ENSO-like
variability in the present (1900-2005) climate?
•Skill depends on the start month.
Empirical Model
PersistenceMar
ch S
tart
sS
epte
mbe
r S
tart
s
These plots are from an empirical model using tropical Pacific SST (1981-present).
For this month’s forecast, see www.atmos.washington.edu/~wroberts/ENSO/LIM.html
ENSO is predictable