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Satellite Winds Superobbing

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Satellite Winds Superobbing. Hurricane Opal October 1995. Image Courtesy of UW - CIMSS. Howard Berger Mary Forsythe John Eyre Sean Healy. Outline. Background/Problem Superob Methodology Method Observation Error Results Conclusions/Future Work. Problem:. - PowerPoint PPT Presentation
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1 Satellite Winds Superobbing Howard Berger Mary Forsythe John Eyre Sean Healy Image Courtesy of UW - CIMSS Hurricane Opal October 1995
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Page 1: Satellite Winds Superobbing

1

Satellite Winds Superobbing

Howard BergerMary Forsythe

John EyreSean Healy

ImageCourtesyof UW - CIMSS

Hurricane OpalOctober 1995

Page 2: Satellite Winds Superobbing

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Outline

•Background/Problem

•Superob Methodology•Method•Observation Error

•Results

•Conclusions/Future Work

Page 3: Satellite Winds Superobbing

Problem:• High - Resolution satellite wind data sets showed negative impact (Butterworth and Ingleby, 2000) Why?

•Suspected that observations errors were spatially correlated

•To account for this negative impact, wind data were/are thinned to 2º x 2º x 100 hPa boxes

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•Bormann et al. (2002) compared wind data to co-located radiosondes showing statistically significant spatial error correlations up to 800 km.

Cor

rela

tion

Met-7 W V NH Correlations

Graphic fromBormann et al.2002

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Question:

Can we lower the data volume to reduce the effect of correlated error while making some use of the high-resolution data?

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Proposed Solution:

Average the observation - background

(innovations) within a prescribed 3-d box to create

a superobservation.

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Advantages:

•Data volume is reduced to same resolution that resulted from thinning.

•Averaging removes some of the random, uncorrelated error within the data.

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SuperobbingMethod:

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1) Sort observations into 2º x 2º x 100 hPa boxes.

28 N

16 W

26 N

18 W

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2) Within each box: Average u and v component innovations, latitude, longitude and pressures.

28 N

26 N

16 W18 W

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3) Find observation that is closest to average position and add averaged innovation to thebackground value at that observation location.

26 N

28 N

16 W18 W

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Superob Observation Error

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•Superobbing removes some of the random observation error.

•This new error can be approximated by making a few assumptions about the errors within the background and the observation.

Superob Observation Error

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Superob Observation Error

Assume that within a box:

•Observation and background errors not correlated with each other.

•Background errors fully correlated.

•Background errors have the same magnitude.

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Assumptions (cont):

•All of the innovations weighted equally.

•Constant observation error correlation.

Superob Observation Error

Page 16: Satellite Winds Superobbing

Token Evil Math Slide

2 ( )Tse W DED W=

2se = Superob Observation Error

W =Vector of Weights (1xN)

D =Diagonal matrix of component observation errors (N x N)

E =Observation Error Correlation Matrix (NxN)

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1

1

a a

aE

a

a a

=

L

O O M

M O O

L

Observation Correlation Matrix

a =Correlation within box. Value calculated from correlation function in Bormann et al., 2002

1 1 1 2 1

2 1

1

n

n n n

c c c c c c

c cE

c c c c

=

L

O O M

M O O M

L L

i jc c =Correlation of ith observation with jth observation

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00z 10 June, 2003.(20 N - 40 N) (0E 30 E)

Old Observation Error Superob Error

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Experimental Design

•Control Run:•Operational Set up plus GOES BUFR VIS/IR/WV winds•GOES-9 is still Satob format

•Thinning to 2˚ x 2˚ x 100 hPa boxes

•Superob Experiment•Same as control run, except winds are superobbed to 2˚ x 2˚ x 100 hPa boxes

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• Trial Period: 24 Jan -17 Feb 2004

• 4 Analyses and 6-hr forecasts• 00z,06z,12z,18z

• 1 analysis and 5-day forecast (12z)

Experimental Design (cont)

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Token Model Info Slide

• Grid – point model (288 E-W x 217 N-S)

• Staggered Arakawa C-Grid

• Approx 100 km horizontal resolution (one-half operational resolution)

• 38 levels hybrid-eta configuration

• 3D-Var Data Assimilation

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Results

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• % normalized root mean square (rms) error against control rms differences calculated for:

•Mean sea-level pressure (PMSL) •500 hPa height (H500) •850 hPa wind (W850) •250 hPa wind (W250)

• In regions:•Northern Hemisphere (NH) •Tropics (TR) •Southern Hemisphere (SH)

•For forecast periods of:•T+24, T+48, T+72 ,T+96 , T+120

Trial Statistics

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-2

-1

0

1

2

3

4

PM

SL T

+2

4

PM

SL T

+4

8

PM

SL T

+7

2

PM

SL T

+9

6

PM

SL T

+1

20

H500 T

+24

H500 T

+48

H500 T

+72

W250 T

+24

W850 T

+24

W850 T

+48

W850 T

+72

W250 T

+24

PM

SL T

+2

4

PM

SL T

+4

8

PM

SL T

+7

2

PM

SL T

+9

6

PM

SL T

+1

20

H500 T

+24

H500 T

+48

H500 T

+72

W250 T

+24

Exp

erim

ent –

Con

trol

RM

S E

rror

(%

)

TP – ObservationsTP – Analysis

NH – ObservationsNH – Analysis

SH – ObservationsSH – Analysis

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Anomaly Correlations

Vs. Forecast RangeCompared to

Analysis500 hPa Height

NH

SH

TR

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T+24 Forecast – Sonde

RMS Vector Error 250 hPa Wind

NH

TR

SH

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250 hPa u-componentAnalysis Increments

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250 hPa u-componentAnalysis Increments

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Results Summary

•Superobbing experiment results are small and mixed

•Generally more positive in the northern hemisphere than in the southern hemisphere or tropics

•Time series results are mixed: Some forecasts better than control, some worse

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Implications

•Mixed results suggest either:•Random Error not most significant error component of AMVs

•Superobbing set up not ideal to treat random error

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Future Work

•Back to basics approach•Re-calculate observation errors from innovation statistics

•Experiment with “model independent” quality indicators and “model independent” components in Bufr file

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• Stripped down impact experiment (i.e no ATOVS radiances)

• Experiment using simulated AMV’s in Met Office System

• Ideas from IWW!!!!!

Future Work (cont)


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