introduction to dynamical models and theory behind seasonal forecasting david g. dewitt

50
Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Upload: godwin-francis

Post on 16-Jan-2016

241 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Introduction to Dynamical Models and Theory Behind Seasonal Forecasting

David G. DeWitt

Page 2: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Thanks to Amit Apte, Ravi Nanjundaiah , and Sulochana Gadgil for inviting me to come speak and sponsoring my trip.

Thanks to L. Goddard,R. Koster, A. Weigel, for letting me borrow slides.

Page 3: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Outline

1. Relationship of this talk to data assimilation.

2. Dominant mechanisms of seasonal variability

a. ENSO

i. Delayed Oscillator

ii. Global teleconnections

b. Soil moisture

c. Stratosphere-troposphere connections

3. Two-tiered (uncoupled) versus one-tiered (coupled) forecast systems

4. Dynamical cores:

a. Current (spectral) versus future (finite volume)

b . Equations for spectral method

5.

Page 4: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Relationship between these talks and data assimilation:

Seasonal forecasts of the climate state need data assimilation in at least 2 ways:

1. Dynamical seasonal forecasting with general circulation models requires specification of the initial state of the ocean and atmosphere (ice, land, etc). This is frequently done using data assimilation products.

2. Given the sparseness of observed data in the ocean (atmosphere), data assimilation products also act as an estimate of the observed state for verification procedures. This is not without problems especially the fact that different assimilation products can produce different estimates of the observed state.

Hypothesis:

In order to construct assimilation systems it is desirable to know about the physical system and the models that represent it. These talks will try to give some insight on these aspects for the seasonal climate forecasting problem.

Page 5: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Physical Phenomena Associated with Seasonal Climate Variations

1. El-Nino Southern Oscillation (ENSO)

a.SST variability in central and eastern equatorial Pacific

b. Global teleconnections forced by changes in convective heating (rainfall) associated with SST variability in central and eastern Pacific

2. Soil moisture anomalies

3. Straosphere-troposphere interactions

4. SST variability in other parts of the ocean (Indian Ocean Dipole)

5. Sea-ice variability

ENSO is the dominant factor in seasonal climate variations. It has an

irregular period of 3 to 5 years.

Fortunately, it is also the phenomena we can model “most” skillfully but

there is still room for improving these forecasts.

Page 6: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

How does ENSO work?First order model for ENSO is known as the Delayed Oscillator.

This model relies on the properties of equatorial ocean waves and

fast response of the tropical atmosphere to SST anomalies.

Variants of this theory such as the Recharge Oscillator which differs

in how mass gets transported back to Equator from Rossby Waves

Main aspect of theory is how to get period plus why oscillation in SST exists.

Key oceanic equatorial wave properties:

1. First vertical mode Eq. Kelvin waves travel eastward at about 2.8m/s.

2. First vertical model Eq. Rossby waves travel westward at 1/3 Eq. Kelvin wave speed.

3. Eq. Rossby waves reflect at western boundaries as Eq. Kelvin waves.

4. Eq. Kelvin waves reflect at eastern boundaries as Eq. Rossby waves and coastal Kelvin waves.

5. A westward wind stress anomaly will produce downwelling Kelvin waves and upwelling Rossby waves.

Page 7: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 8: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 9: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 10: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 11: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 12: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 13: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 14: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 15: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 16: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Rectifying the ENSO Period

Simple wave dynamics gives a 2 year oscillation for ENSO but the observed period is slower: Why?

-The equatorial atmosphere quickly responds to SST anomalies.

the wind stress response to SST anomalies forces the ocean in a way

that reinforces the SST anomalies.

-Warm SST anomalies lead to westerly wind anomalies which lead to

downwelling Kelvin waves which leads to maintaining or intensifying

the warm SST anomalies.

-In order to change phase of SST need for opposite signed Kelvin

waves to be generated in the central and western Pacific and cancel

original anomaly plus whatever growth occurred due to coupling.

-Oscillation is irregular with warm events usually followed closely by

cold events but not vice versa.

-Lower order mode Rossby waves with wider meridional structure are important. These have much slower phase velocities

Page 17: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Response to Anomalous Convection Associated with El Nino

Anomalous convective heating along the equator drives global atmospheric circulation anomalies:

1. Warm zonal anomaly near the equator associated with Kelvin waves propagating eastward. Leads to positive height anomalies near the equator.

2. Quasi-stationary Rossby waves that propagate meridionally away from the equator and eastward. This leads to some well known patterns of variability in the NH, in particular the PNA.

3. These dynamic and thermodynamic anomalies interact with the local flow to alter precipitation patterns including Indian monsoon.

4. Modifications to the Hadley circulation.5. Response to El-Nino and La-Nina although generally of opposite

sign has important asymmetries.6. Effects of El-Nino are felt globally: Summary studies byRopelewski and Halpert, Goddard and Mason.

Page 18: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 19: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 20: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

A. Weigel

Page 21: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Probabilisticcomposites ofabove normalprecipitation keyed to …

El Nino

La Nina

Seasonal climate forecasting works because ENSO has a strong influence globally and ENSO variability is predictable

Page 22: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Soil Moisture Anomalies Effect on Seasonal Climate

After (Tropical) SST anomalies, soil moisture anomalies are considered to be important for driving seasonal climate anomalies.

Realizing the predictive skill associated with soil moisture anomalies is

problematic because there are very few observations of soil moisture

On large spatial and long temporal (decades) scale. Most soil moisture

Older systems drive land surface models offline with observed precipitation and radiation to get soil moisture anomalies.

More formal data assimilation approach to assimilating the sparse observations into land surface models is now an area of active research.

Comparison experiment on impacts of “correctly” initializing soil moisture on seasonal forecast skill: GLACE(2)

Page 23: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

R. Koster

Page 24: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

R. Koster

Page 25: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

R. Koster

Page 26: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

R. Koster

Page 27: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 28: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 29: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Different Approaches to Dynamical Seasonal Forecasts

In order to do dynamical seasonal climate forecasting a minimum system needs an AGCM and a method for forecasting SST. There are 2 common approaches:

1. One-tier (coupled) models: Include an oceanic model such as an OGCM.

2. Two-tiered (uncoupled) models: Use an offline model (statistical or dynamical) to predict SST and prescribe for AGCM.

Large part of the community believes that one-tier models are needed because of air-sea interaction in places like Indian ocean. Smaller part of the community (DeWitt, Gadgil and collaborators, Kumar) believes that two-tier approach still has value. Ultimately, with a marginal skill problem you should take skill where you can get it (multi-model ensemble). Finally, the real argument here isn’t whether coupling is important but when, i.e. timescale. Weather services generally don’t use coupled models.

Page 30: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Positive Attributes of Different Approaches to Seasonal Forecasting

2-Tiered Forecast Systems:-Relatively inexpensive computationally-Potentially more accurate SST data due to input from multiple sources-No drift of SST annual cycle on which anomalies are superimposed

1-Tiered Forecast Systems:-Potentially more accurate representation of physical interaction between ocean and atmosphere: Transient (waves) and time mean

Page 31: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Effect of Coupling on Simulated Indian Summer Monsoon

correlations (%) with CPC GSOD 1980–2003

coupled uncoupled

obs daily rainfall frequency

Page 32: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Simple Test for Importance of Coupling

1. Run set of coupled model forecasts.

2. Take SST from coupled model forecasts and prescribe in AGCM component model with less frequency than every time step.

3. Compare uncoupled and coupled model fields such as

Precipitation, near-surface air temperature, oceanic surface fluxes.

For long free-running coupled runs differences are large and important.

For seasonal forecasting results are very similar. One place they are different is southeastern Asia. But is one solution better than another?

Page 33: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Precipitation-SST (SST Tend) JJA Forecast (May IC)

Page 34: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Precipitation Forecast Skill JJA Forecast (May IC)

Page 35: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

T2m Forecast Skill JJA Forecast (May IC)

Page 36: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Organizing modelsDynamics / Physics

Con

vect

ion

Adv

ectio

n

Mix

ing

PB

L

Rad

iatio

n

Clo

uds

∂A/∂t = – UA + M + P – LA{

∂A/∂t = Dynamical Core Physics

}}+

Page 37: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Spectral Core Essential Elements

Spherical harmonic representation of dynamicsExact calculation of horizontal derivativesPhysical parameterizations and non-linear dynamical

products calculated on an associated Gaussian gridGibbs phenomena associated with sharp gradientsNeed to include artificial horizontal diffusion to keep model stable, i.e. spectral blockingTime step constraint due to CFL instabilityStill used by many forecast centers for seasonal

forecasting (ECMWF, JMA, NCEP,CMA)

Page 38: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Finite Volume Dynamical Core Elements

Employs finite volume as opposed to finite difference

No Gibbs phenomena

Diffusion occurs due to choice of curve fit

No stability constraint for time step

Has become dominant dynamical core in US large scale modeling that cares about tracer transport (upper level moisture, chemical species, aerosols): GSFC, GFDL, NCAR (CAM)

Page 39: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

How do Simulations with FV and Spectral Compare?

Finite volume much more accurate for tracer transport (flux conservative)

Finite volume tends to produce smaller scale precipitation features

Finite volume has less wavy artificial features

Finite volume schemes generally use fully implicit time integration schemes allowing timestep to be set by accuracy not stability (CFL) constraints. Spectral methods generally employ semi-implicit methods and so are still CFL constrained.

Page 40: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Compare FV versus Finite Difference

Conventional finite difference

Lin-Rood built with Piecewise Parabolic Method

Page 41: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Consider the measurements of atmospheric constituents

N2O

NOy

OBSERVATIONS

Enormous amount of information• Mixing physics• Mixing time scales• Chemical production and loss

Page 42: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Spectral method and correlations

N2O

NOy

Spectral Method(widens over time)

Sources of pathology• Inability to fit local features• Inconsistency between tracer and fluid continuity equation• Dispersion errors• Filtering

Page 43: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

Van Leer method and correlations

N2O

NOy

Van Leer Method

Why does this work?• Consideration of volumes and mixing these volumes consistently.

Page 44: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

What does Spectral Filtering Due to Orography?

Smooth out maxim

Create negative values even for positive definite fields such as orography

More recent techniques of smoothing orography help to minimize these effects but it still exists.

Page 45: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt
Page 46: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

DKRZ, ECHAM3

Page 47: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

DKRZ, ECHAM3

Page 48: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

DKRZ, ECHAM3

Page 49: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

DKRZ, ECHAM3

Page 50: Introduction to Dynamical Models and Theory Behind Seasonal Forecasting David G. DeWitt

DKRZ, ECHAM3