diagnosis of model biases by using dart · emphasis on the large-scale divergent motions (tropics)....

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Diagnosis of model biases by using DART N. Žagar, J. Tribbia, J. Anderson and K. Raeder, National Center for Atmospheric Research, Boulder, CO Datasets Datasets Three analysis datasets for July 2007, global fields every 6 hours DART/CAM: ensemble mean of an 80-member ensemble produced by the DART system. For details see http://www.image.ucar.edu/DAReS/DART/ . The CAM version is 3.1, horizontal resolution T85, 26 vertical levels up to 3.5 hPa. ECMWF operational analyses: 12-hour 4D-Var system, Cycle 32r2, T799 interpolated to N64 grid, 91 vertical level up to 1 Pa. NCEP-NCAR reanalyses: 3D-Var system, T46 horizontal resolution, 28 vertical levels up to 2.7 hPa. An old system compared to the operational NCEP data. Tropical winds in 3 analysis datasets in July 2007 Tropical winds in 3 analysis datasets in July 2007 DART/CAM: u wind, 370 hPa, along 5N NCEP: u wind, 370 hPa, along 5N ECMWF: u wind, 370 hPa, along 5N Tropics as envisaged by A. Gill (1980): CAM/DART analyses Tropics as envisaged by A. Gill (1980): CAM/DART analyses On average, divergent flow in the lower and upper troposphere is reversed, i.e. easterlies fond over the Pacific in the lower troposphere and westerlies in the lower troposphere. Kelvin mode an important contributor to the zonal winds over the Pacific and the equatorial Africa. (Length of the wind vectors for ROT modes three times larger than for IG modes.) Summary Summary The normal mode expansion is applied to the ensembles of analyses and forecasts produced by using the CAM 3.1 T85 model and the ensemble adjustment Kalman filter (Data Assimilation Research Testbed system - DART). The selection of normal modes accounts for over 90% of the flow variance in the free atmosphere. Of particular interest are large-scale divergent motions. Result show that about 12% of the wave energy is associated with the inertio-gravity motions, and that the difference between the eastward and westward propagating waves is due to Kelvin waves. Large scale flow in CAM/DART analyses compares well with other existing analysis datasets, i.e. NCEP-NCAR and ECMWF analyses. Comparison of three datasets illustrates the uncertainties in the description of the large-scale tropical circulation. Tropics are also the area with largest biases in three studied datasets. It is proposed that the “perfect model” assimilation experiment be utilized as a diagnosis tool for understanding model biases in terms of various motions types and scales. Motivation Motivation Divergent tropical circulations crucial for understanding the climate but unreliable from present (re)analysis Unclear how large part of the global atmospheric energetics pertains to the divergent motion i.e. inertio-gravity waves. Large-scale equatorial waves in recent years diagnosed from different mass- field observations and models, but exact quantification of their variance and dynamical relevance not completely understood. Objectives Objectives Apply normal mode functions (NMFs) to the analysis and forecast fields to quantify percentage of energy contained in balanced (Rossby) and inertio- gravity (IG) motions. Estimate energy spectra for the Community Atmospheric Model (CAM), with emphasis on the large-scale divergent motions (tropics). Compare analyses produced using CAM 3.1 T85 and the Data Assimilation Research Testbad (DART) system with other analysis datasets Analyze model biases by carrying out the “perfect model” experiment Total biases in 3 analysis systems Total biases in 3 analysis systems y o x b x a y o x b x a background analysis x o x f x f “Perfect model observations” simulation forecast 6 hrs long free model run o b s e r v a ti o n s + σ o + σ o forecast Normal mode expansion Normal mode expansion Applied set of orthogonal modes was derived by A. Kasahara (Kasahara and Puri, MWR, 1981). Basic idea in the present application is to select the subset of modes which provides the best fit (best correlation and variance fit to the input grid-point fields) tuning of the truncation parameters N k , N n , N m N m – number of vertical modes, index m N n – number of meridional modes per wave type, index n N k – number of zonal waves, index k T g P v u ) , , ( = X ∑∑ = = = = Π = m n i k k N m N n N N k knm knm z t t z 1 1 0 3 , 2 , 1 ) , , ( ) ( ) , , , ( ϕ λ χ ϕ λ m S X common expansion coefficient normalization matrix 3D normal mode functions input data vector , ) ln( s o p RT gz P + = knm m knm z z Η Φ = Π ) ( ) , , ( ϕ λ vertical normal modes Hough functions ' ' ' ' ' ' , mm nn kk m n k knm δ δ δ = Π Π orthogonal 3D expansion basis ( ) ( ) = eq eq eq H gH gH 0 0 0 0 0 0 2 / 1 2 / 1 m S Vertical Vertical eigenstructures eigenstructures for CAM for CAM Input information: vertical discretization, vertical mean temperature (T o ) and stability profiles H eq - separation constant for vertical and horizontal structure (“equivalent depth”) H eq in range from 10 km to 0.3 m: 10 km, 6.2 km, 2.2 km, 985 m, 572 m, 379 m, 250 m, 162 m, 107 m. Modes 10-26 have H eq below 100 m m=1 m=2 m=3 m=4 m=5 m=6 m=7 m=8 m=9 Truncation parameters selected for CAM are: N k = 80, N n = 25,N m = 25. Verification of the expansion into NMFs performed by comparing input fields to those obtained after projection and its inverse. On average, expansion accounts for over 90% of the variance above 900 hPa which allows reliable quantification of the percentage of energy contained in various motions. Correlation coefficients are between 0.9 and 1. nzagar Contact information jla raeder tribbia @ucar.edu Energy distribution in CAM Energy distribution in CAM 25-day period average: 6-31 July 2007 2 k n m knm eq gH χ ROT EIG WIG ROT- non-divergent (Rossby) EIG - eastward inertio-gravity WIG – westward inertio-gravity ROT: 87.9% EIG: 7.4% WIG: 4.7% MRG: 1.0% KW: 2.7% %*10 %*10 % % % Zonally averaged state (k=0) is not included. m=25 m=26 m=22 m=23 m=24 m=19 m=20 m=21 Rotational modes + MRG 269 hPa 868 hPa Inertio-gravity modes Eastward inertio-gravity modes Kelvin modes Inter Inter - - comparison of divergent tropical comparison of divergent tropical motion in 3 analysis datasets motion in 3 analysis datasets Temporal evolution of the KW, k=1 signal CAM ECMWF NCEP-NCAR Conclusions Conclusions Large-scale flow in CAM/DART analyses compares well to other existing analysis datasets. Tropics are areas with largest uncertainties in existing analysis datasets. Tropics are also the area with largest biases in three studies data assimilation systems. Normal mode expansion allows to quantify energy in various motions and to modify traditional view of inertio- gravity motions as junk. With normal modes it is possible to quantify variance in various tropical divergent motions and its relevance for data assimilation. Application of normal modes offers a physically attractive approach to quantification of uncertainties in analyses and forecasts. Uncertainties vary in time and space, thus an argument for a flow-dependent estimates of the forecast errors, i.e. the ensemble data assimilation. The normal mode application may also help to address modeling aspects such as model-error covariances and initialization. Uncertainty of analysis solution as estimated from Uncertainty of analysis solution as estimated from the CAM/DART 80 the CAM/DART 80 - - member ensemble member ensemble CAM ECMWF NCEP-NCAR m m m m m m CAM ECMWF NCEP-NCAR Lower troposphere Upper troposphere Monthly-averaged analysis increments are used as a proxy for analysis bias (model biases + observation biases). Most of bias is in the tropical wind field, especially in cross-equatorial winds CAM ECMWF NCEP-NCAR Lower troposphere biases: ROT modes Biases projecting to IG modes Tropical wind biases are largely in the divergent component and especially in the meridional wind in the Indian ocean. This is consistent in all 3 analysis systems. Analysis Analysis - - forecast cycle forecast cycle ROT %*10 %*100 %*100 EIG WIG CAM 3.1 T85 perfect model experiment: biases CAM 3.1 T85 perfect model experiment: biases Biases due to all modes Biases due to IG modes 269 hPa 788 hPa Tropics Tropics : : Questions Questions How much of the large-scale tropical circulation is made up by the Kelvin wave, mixed Rossby-gravity wave, other inertio-gravity waves? How is this dependent on the model resolution, physics, biases? What are the spectra of forecast errors in the tropics like? How are the tropical forecast errors spread across the scales and motion types? What modes do the biases project onto? How important are Kelvin, mixed Rossby-gravity and other large-scale IG for tropical and global the data assimilation? Energy in each mode is normalized by total energy in all waves. In July 2007, ~12% of energy in IG motion. Percentage values pertain to the integrated energy across all scales (except k=0). Difference between EIG and WIG almost completely due to Kelvin waves (KW). Energy spread in each mode is normalized by total average wave energy in the ensemble mean. Areas of the modal space with largest uncertainties do not coincide with the scales containing most of the energetic flow. Most of divergent circulation is in the tropics, except for NCEP-NCAR reanalysis. Analyses agree to some extent about the divergent component of the zonal tropical circulation. But significant differences exist for example in the Indian ocean, related to the monsoon circulation. Antarctic circulation divergent in all analyses. In perfect model experiment, the impact of model errors is removed provided good observation coverage. Present experiment used conventional observation; thus, the southern hemisphere poorly observed here, model errors establish in time- averaged analysis increments. Most of these extra-tropical biases reside in balanced motions.

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Diagnosis of model biases by using DARTN. Žagar, J. Tribbia, J. Anderson and K. Raeder, National Center for Atmospheric Research, Boulder, CO

DatasetsDatasetsThree analysis datasets for July 2007, global fields every 6 hours

DART/CAM: ensemble mean of an 80-member ensemble produced by the DART system. For details see http://www.image.ucar.edu/DAReS/DART/. The CAM version is 3.1, horizontal resolution T85, 26 vertical levels up to 3.5 hPa.

ECMWF operational analyses: 12-hour 4D-Var system, Cycle 32r2, T799 interpolated to N64 grid, 91 vertical level up to 1 Pa.

NCEP-NCAR reanalyses: 3D-Var system, T46 horizontal resolution, 28 vertical levels up to 2.7 hPa. An old system compared to the operational NCEP data.

Tropical winds in 3 analysis datasets in July 2007Tropical winds in 3 analysis datasets in July 2007DART/CAM: u wind, 370 hPa, along 5N NCEP: u wind, 370 hPa, along 5N ECMWF: u wind, 370 hPa, along 5N

Tropics as envisaged by A. Gill (1980): CAM/DART analysesTropics as envisaged by A. Gill (1980): CAM/DART analyses

On average, divergent flow in the lower and upper troposphere is reversed, i.e. easterlies fond over the Pacific in the lower troposphere and westerlies in the lower troposphere.

Kelvin mode an important contributor to the zonal winds over the Pacific and the equatorial Africa. (Length of the wind vectors for ROT modes three times larger than for IG modes.)

SummarySummaryThe normal mode expansion is applied to the ensembles of analyses and forecasts produced by using the CAM 3.1 T85 model and the ensemble adjustment Kalman filter (Data Assimilation Research Testbed system - DART). The selection of normal modes accounts for over 90% of the flow variance in the free atmosphere. Of particular interest are large-scale divergent motions. Result show that about 12% of the wave energy is associated with the inertio-gravity motions, and that the difference between the eastward and westward propagating waves is due to Kelvin waves.

Large scale flow in CAM/DART analyses compares well with other existing analysis datasets, i.e. NCEP-NCAR and ECMWF analyses. Comparison of three datasets illustrates the uncertainties in the description of the large-scale tropical circulation. Tropics are also the area with largest biases in three studied datasets. It is proposed that the “perfect model” assimilation experiment be utilized as a diagnosis tool for understanding model biases in terms of various motions types and scales.

MotivationMotivationDivergent tropical circulations crucial for understanding the climate but

unreliable from present (re)analysis

Unclear how large part of the global atmospheric energetics pertains to the divergent motion i.e. inertio-gravity waves.

Large-scale equatorial waves in recent years diagnosed from different mass-field observations and models, but exact quantification of their variance and dynamical relevance not completely understood.

ObjectivesObjectivesApply normal mode functions (NMFs) to the analysis and forecast fields to

quantify percentage of energy contained in balanced (Rossby) and inertio-gravity (IG) motions.

Estimate energy spectra for the Community Atmospheric Model (CAM), with emphasis on the large-scale divergent motions (tropics).

Compare analyses produced using CAM 3.1 T85 and the Data Assimilation Research Testbad (DART) system with other analysis datasets

Analyze model biases by carrying out the “perfect model” experiment

Total biases in 3 analysis systemsTotal biases in 3 analysis systems

yo

xb

xa

yo

xb

xa

background

analysis

xo xf xf“Perfect model observations” simulation

forecast 6 hrs

long free model run

observations + σo + σo

forecast

Normal mode expansionNormal mode expansionApplied set of orthogonal modes was derived by A. Kasahara (Kasahara and Puri, MWR, 1981). Basic idea in the present application is to select the subset of modes which provides the best fit (best correlation and variance fit to the input grid-point fields) tuning of the truncation parameters Nk, Nn, Nm

Nm – number of vertical modes, index mNn – number of meridional modes per wave type, index n

Nk – number of zonal waves, index k

T

gPvu ),,(=X

∑ ∑ ∑=

= −==

Π=m n

i

k

k

N

m

N

n

N

Nkknmknm zttz

1

1

03,2,1

),,()(),,,( ϕλχϕλ mSX

common expansion coefficientnormalization matrix

3D normal mode functions

input data vector

, )ln( so pRTgzP +=

knmmknm zz Η⋅Φ=Π )(),,( ϕλvertical normal modes Hough functions

'''''', mmnnkkmnkknm δδδ=ΠΠ orthogonal 3D expansion basis

( )( )

⎜⎜⎜⎜

=

eq

eq

eq

HgH

gH

000000

2/1

2/1

mS

Vertical Vertical eigenstructureseigenstructures for CAMfor CAM

Input information: vertical discretization, vertical mean temperature (To) and stability profiles

Heq- separation constant for vertical and horizontal structure (“equivalent depth”)

Heq in range from 10 km to 0.3 m: 10 km, 6.2 km, 2.2 km, 985 m, 572 m, 379 m, 250 m, 162 m, 107 m. Modes 10-26 have Heqbelow 100 m

m=1

m=2

m=3

m=4

m=5

m=6

m=7

m=8

m=9

Truncation parameters selected for CAM are: Nk = 80, Nn = 25,Nm= 25.

Verification of the expansion into NMFs performed by comparing input fields to those obtained after projection and its inverse.

On average, expansion accounts for over 90% of the variance above 900 hPa which allows reliable quantification of the percentage of energy contained in various motions.

Correlation coefficients are between 0.9 and 1.

nzagar

Contact information

jla

raeder

tribbia

@ucar.edu

Energy distribution in CAMEnergy distribution in CAM

25-day period average: 6-31 July 2007

2∑∑∑k n m

knmeqgH χ

ROT

EIGWIG ROT- non-divergent (Rossby)

EIG - eastward inertio-gravity WIG – westward inertio-gravity

ROT: 87.9% EIG: 7.4% WIG: 4.7%

MRG: 1.0% KW: 2.7%%*10%*10

% % %

Zonally averaged state (k=0) is not included.

m=25

m=26

m=22

m=23

m=24

m=19

m=20

m=21

Rotational modes + MRG

269 h

Pa

868 h

Pa

Inertio-gravity modes Eastward inertio-gravity modes Kelvin modes

InterInter--comparison of divergent tropical comparison of divergent tropical motion in 3 analysis datasetsmotion in 3 analysis datasets

Temporal evolution of the KW, k=1 signalCAM ECMWF NCEP-NCAR

Conclusions Conclusions

Large-scale flow in CAM/DART analyses compares well to other existing analysis datasets.

Tropics are areas with largest uncertainties in existing analysis datasets. Tropics are also the area with largest biases in three studies data assimilation systems.

Normal mode expansion allows to quantify energy in various motions and to modify traditional view of inertio-gravity motions as junk. With normal modes it is possible to quantify variance in various tropical divergent motions and its relevance for data assimilation.

Application of normal modes offers a physically attractive approach to quantification of uncertainties in analyses and forecasts. Uncertainties vary in time and space, thus an argument for a flow-dependent estimates of the forecast errors, i.e. the ensemble data assimilation. The normal mode application may also help to address modeling aspects such as model-error covariances and initialization.

Uncertainty of analysis solution as estimated from Uncertainty of analysis solution as estimated from the CAM/DART 80the CAM/DART 80--member ensemblemember ensemble

CAM

ECM

WF

NCEP-

NCAR

m

m

m m

m

m

CAM

ECM

WF

NCEP-

NCAR

Lower troposphere Upper troposphere

Monthly-averaged analysis increments are used as a proxy for analysis bias (model biases + observation biases).

Most of bias is in the tropical wind field, especially in cross-equatorial winds

CAM

ECM

WF

NCEP-

NCAR

Lower troposphere biases: ROT modes Biases projecting to IG modes

Tropical wind biases are largely in the divergent component and especially in the meridional wind in the Indian ocean. This is consistent in all 3 analysis systems.

AnalysisAnalysis--forecast cycleforecast cycle

ROT

%*10 %*100 %*100

EIG WIG

CAM 3.1 T85 perfect model experiment: biases CAM 3.1 T85 perfect model experiment: biases

Biases due to all modes Biases due to IG modes

269 h

Pa

788 h

Pa

TropicsTropics:: Questions Questions How much of the large-scale tropical circulation is made

up by the Kelvin wave, mixed Rossby-gravity wave, other inertio-gravity waves?

How is this dependent on the model resolution, physics, biases?

What are the spectra of forecast errors in the tropics like? How are the tropical forecast errors spread across the scales and motion types?

What modes do the biases project onto?

How important are Kelvin, mixed Rossby-gravity and other large-scale IG for tropical and global the data assimilation?

Energy in each mode is normalized by total energy in all waves. In July 2007, ~12% of energy in IG motion. Percentage values pertain to the integrated energy across all scales (except k=0). Difference between EIG and WIG almost completely due to Kelvin waves (KW).

Energy spread in each mode is normalized by total average wave energy in the ensemble mean.

Areas of the modal space with largest uncertainties do not coincide with the scales containing most of the energetic flow.

Most of divergent circulation is in the tropics, except for NCEP-NCAR reanalysis.

Analyses agree to some extent about the divergent component of the zonal tropical circulation. But significant differences exist for example in the Indian ocean, related to the monsoon circulation.

Antarctic circulation divergent in all analyses.

In perfect model experiment, the impact of model errors is removed provided good observation coverage. Present experiment used conventional observation; thus, the southern hemisphere poorly observed ⇒ here, model errors establish in time-averaged analysis increments.

Most of these extra-tropical biases reside in balanced motions.