downscaling ability of the ncep regional spectral model v.97: the big brother experiment

1
Tropical Domain Results Downscaling Ability of the NCEP Regional Spectral Model v.97: The Big Brother Experiment Conclusions: Motivation: The Big Brother Experiment methodology allows us to assess the errors in regional climate simulations which are solely due to the nesting strategy. Deborah Herceg * Adam Sobel *†‡ Liqiang Sun Stephen Zebiak *Department of Applied Physics and Applied Mathematics Columbia University New York, NY †Department of Earth and Environmental Sciences Columbia University New York, NY ‡International Research Institute For Climate Prediction Columbia University Palisades, NY [email protected] Setup of the Big Brother Experiment: Our Experiment : Domains STEPS : 1.We first perform a large-domain high resolution regional model simulation, the “Big Brother”. 2.This reference simulation is then degraded by filtering out short-scales which would be unresolved in the GCM 3.This filtered reference is then used to drive the same regional climate model, integrated at the same resolution as the Big Brother, but over a smaller domain embedded in the large domain, called the Little Brother 4.We then compare the climate statistics of the Little Brother with those of the Big Brother on the Little Brother Domain 5.Since the same model is used for both the Big Brother and Little Brother experiments, the climate of the two should in principle be identical. Any difference in the solutions can only be attributed to the nesting strategy, and not to model error. TROPICAL DOMAIN: MIDLATITUDE DOMAIN: Midlatitude Domain Results Experimental Details: NOAA 29 th Annual Climate Diagnostics and Prediction Workshop; October 18-22, 2004, Madison, Wisconsin Table Legend: The Big Brother Experiment (BBE) Large Limited Area High Resolution Model Regiona l Climate Validat ion Filter Small Scales Small Limited-area High Resolution model Small regional High Resolution Simulation Correspondi ng Data Set Model IC and LBC IC LBC IC = Initial Condition LBC = Lateral Boundary Condition LEGEND: Global Low- Resolution Data Set Large regional High Resolution Reference Simulation BIG BROTHER LITTLE BROTHER LITTLE BROTHER BIG BROTHER The Model: NCEP Regional Spectral Model, v. 97 – Juang et al., 1997. ECHAM4.5 data, archived every 6 hours was used to drive the Big Brother simulation. The Big Brother simulation data was archived every 6 hours for the nesting of the Little Brother simulation, as well. All experiments were executed for a month. All of the statistical computations were performed excluding the first day in order to reject any short time-scale spin-up phenomenon. A ten grid point lateral boundary zone was also excluded. To mimic the resolution of the operational GCM (ECHAM at T-42 resolution), a cutoff wavelength of ~900 km was used in the filtering of the Big Brother output before using it to drive the Little Brother. This experiment was first performed by Denis et al. (2001), using a grid point model for a midlatitude winter simulation. Our study extends theirs by using both a tropical and a midlatitude domain case, and using a different (in this case, spectral) model. One month simulation completed for April, 1994 Both domains centered at 37.5°W and 5°S Horizontal resolution of 60 km Big Brother domain at 181 x 182 grid points Little Brother domain at 91 x 92 grid points 18 vertical layers One month simulation completed for February, 2001 Both domains centered at 70°W and 47°N Horizontal resolution of 50 km Big Brother domain at 151 x 142 grid points Little Brother domain at 81 x 77 grid points 18 vertical layers BIG BROTHER LITTLE BROTHER BIG BROTHER LITTLE BROTHER PRECIPITATION SEA+LAND SEA LAND Stat . Corr . Tran s. Corr . Stat. Var. Ratio Trans. Var. Ratio Stat. Corr. Trans. Corr. Stat. Corr. Trans. Corr. Tota l 0.81 47 0.42 57 1.317 1.4374 0.7841 0.405 0.884 7 0.4834 LW 0.85 34 0.53 82 1.2967 1.3442 0.8227 0.5061 0.927 2 0.577 SW 0.22 47 0.12 93 1.7362 1.8379 0.2075 0.0921 0.261 8 0.1258 SPECIFIC HUMIDITY (850 MBAR) SEA+LAND SEA LAND Stat . Corr . Trans . Corr. Stat. Var. Ratio Trans. Var. Ratio Stat. Corr. Trans. Corr. Stat . Corr . Trans. Corr. Tota l 0.99 35 0.933 6 1.0061 1.0188 0.9938 0.9345 0.97 75 0.835 LW 0.99 36 0.939 1 1.0064 1.0182 0.994 0.9363 0.97 92 0.8448 SW 0.98 41 0.750 4 0.9834 1.072 0.9848 0.845 0.98 1 0.8305 PRECIPITATION SEA+LAND SEA LAND Stat . Corr . Tran s. Corr . Stat . Var. Rati o Tran s. Var. Rati o Stat. Corr. Trans. Corr. Stat . Corr . Trans. Corr. Tot al 0.94 52 0.73 82 1.06 39 1.05 02 0.966 3 0.7258 0.88 44 0.6980 LW 0.95 89 0.79 41 1.04 92 1.03 88 0.975 0 0.7944 0.91 53 0.7524 SW 0.82 11 0.41 40 1.18 63 1.18 89 0.823 2 0.4149 0.81 96 0.4750 SPECIFIC HUMIDITY (850 MBAR) SEA+LAND SEA LAND Stat . Corr . Tran s. Corr . Stat . Var. Rati o Tran s. Var. Rati o Stat. Corr. Trans . Corr. Stat . Corr . Trans. Corr. Tota l 0.99 72 0.96 41 1.06 82 1.04 82 0.998 1 0.962 1 0.99 61 0.9526 LW 0.99 73 0.96 45 1.06 76 1.04 71 0.998 2 0.962 7 0.99 61 0.9558 SW 0.99 72 0.95 88 1.07 95 1.08 99 0.997 6 0.964 5 0.99 65 0.9494 Total Field (TOTAL) is separated into a small-scale component (SW), and large-scale component (LW); defined as the wave numbers above and below the cutoff wave number. Stationary Correlation (Stat. Corr.) = spatial correlation of time-mean fields. Stationary Variance Ratio (Stat. Var. Ratio)=ratio of variances of time-mean fields. Transient Correlation (Trans. Corr.), Transient Variance Ratio (Trans. Var. Ratio) = spatial correlation, variance ratio of transient fields (total-stationary). Statistics provided for sea and land separately, as well as total. In most fields, good agreement between Big and Little Brothers was obtained, for both small and large scales, after a brief initial spin-up period. Precipitation was the exception. For our tropical domain experiment, the small-scale features of the precipitation field in the Big Brother were not reproduced by the Little Brother. The spatial and temporal variations of the large-scale component of the precipitation were well reproduced. The reason for the poor reproduction of the small-scale component of the precipitation is that this component is inherently unpredictable, at least in this model, rather than because of any inherent flaw in the nesting strategy. This was shown by an ensemble of identically forced Little Brother simulations which were initialized at different times differing by 6-24 hours, in which the correlations of the small-scale precipitation between these different simulations was nearly as low as that between the Big and Little Brothers. Related to this, the agreement between Big and Little Brothers is fairly insensitive to the choice of the cutoff wave number used for the filtering. Good reproduction of the small- scale precipitation was obtained for a wintertime midlatitude simulation. Thus, the relatively poor reproduction of this field for the tropical case appears to be due to specifically tropical (convective) precipitation processes. “Ensemble” Simulations Results ZONAL WIND (850 MBAR) SEA+LAND SEA LAND Stat . Corr . Tran s. Corr . Stat . Var. Rati o Tran s. Var. Rati o Stat. Corr. Trans . Corr. Stat . Corr . Trans. Corr. Tot al 0.99 36 0.93 36 1.14 07 1.11 16 0.995 1 0.934 3 0.99 2 0.924 LW 0.99 4 0.93 44 1.14 11 1.11 21 0.995 5 0.935 4 0.99 26 0.9263 SW 0.98 60 0.92 02 1.13 26 1.11 37 0.988 5 0.927 8 0.98 23 0.9113 ZONAL WIND (850 MBAR) SEA+LAND SEA LAND Stat . Corr . Tran s. Corr . Stat. Var. Ratio Trans. Var. Ratio Stat. Corr. Trans. Corr. Stat . Corr . Trans. Corr. Tota l 0.97 62 0.91 8 0.8878 0.9766 0.977 0.9168 0.98 36 0.8754 LW 0.97 68 0.92 27 0.8879 0.9748 0.9773 0.9194 0.98 47 0.8821 SW 0.96 00 0.78 6 0.8726 1.0451 0.9667 0.8440 0.94 89 0.8028 Stat. Corr. Stat. Var. Ratio Trans. Corr. Trans. Var. Ratio T=06 HR Tot al 0.902 5 0.9382 0.4744 1.0981 LW 0.940 0 0.9396 0.5905 1.1085 SW 0.356 1 0.9120 0.1484 1.0779 T=12 HR Tot al 0.874 2 0.8398 0.4346 1.0747 LW 0.914 1 0.8410 0.5406 1.0809 SW 0.315 8 0.8013 0.1231 1.0836 T=18 HR Tot al 0.774 7 0.9637 0.3590 1.2473 LW 0.817 6 0.9540 0.4544 1.2457 SW 0.226 6 0.9423 0.0783 1.3260 T=24 HR Tot al 0.884 5 1.0883 0.4398 1.0224 LW 0.927 4 1.0969 0.5601 1.0428 0.234 PRECIPITATION FIELD ENSEMBLES The table on the left shows the “ensemble” results comparing the identically forced Little Brother simulations, but initialized at different times differing by 6-24 hours; the correlations of the small-scale precipitation between these different simulations was almost as low as that between the Big and Little Brother “ensemble”

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Large Limited Area High Resolution Model. Small Limited-area High Resolution model. Deborah Herceg * Adam Sobel *†‡ Liqiang Sun ‡ Stephen Zebiak ‡ *Department of Applied Physics and Applied Mathematics Columbia University New York, NY †Department of Earth and Environmental Sciences - PowerPoint PPT Presentation

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Page 1: Downscaling Ability of the NCEP Regional Spectral Model v.97: The Big Brother Experiment

Tropical Domain Results

Downscaling Ability of the NCEP Regional Spectral Model v.97: The Big Brother Experiment

Conclusions:

Motivation: The Big Brother Experiment methodology allows us to assess the errors in regional climate simulations which are solely due to the nesting strategy.

Deborah Herceg*

Adam Sobel*†‡

Liqiang Sun‡

Stephen Zebiak‡

*Department of Applied Physics and Applied Mathematics

Columbia UniversityNew York, NY

†Department of Earth and Environmental Sciences

Columbia UniversityNew York, NY

‡International Research Institute For Climate

PredictionColumbia University

Palisades, NY

[email protected]

Setup of the Big Brother Experiment:

Our Experiment : Domains

STEPS:

1.We first perform a large-domain high resolution regional model simulation, the “Big Brother”.

2.This reference simulation is then degraded by filtering out short-scales which would be unresolved in the GCM

3.This filtered reference is then used to drive the same regional climate model, integrated at the same resolution as the Big Brother, but over a smaller domain embedded in the large domain, called the Little Brother

4.We then compare the climate statistics of the Little Brother with those of the Big Brother on the Little Brother Domain

5.Since the same model is used for both the Big Brother and Little Brother experiments, the climate of the two should in principle be identical. Any difference in the solutions can only be attributed to the nesting strategy, and not to model error.TROPICAL

DOMAIN:MIDLATITUDE DOMAIN:

Midlatitude Domain Results

Experimental Details:

NOAA 29th Annual Climate Diagnostics and Prediction Workshop; October 18-22, 2004, Madison, Wisconsin

Table Legend:

The Big Brother Experiment (BBE)

Large Limited Area High Resolution

Model

Regional Climate Validation

Filter Small Scales

Small Limited-area High Resolution

model

Small regional High Resolution

Simulation

Corresponding Data Set

Model

IC and LBC

IC LBC

IC = Initial Condition

LBC = Lateral Boundary Condition

LEGEND:

Global Low-Resolution Data

Set

Large regional High Resolution

Reference Simulation

BIG BROTHER

LITTLE BROTHER

LITTLE BROTHER

BIG BROTHER

The Model: NCEP Regional Spectral Model, v. 97 – Juang et al., 1997.

ECHAM4.5 data, archived every 6 hours was used to drive the Big Brother simulation. The Big Brother simulation data was archived every 6 hours for the nesting of the Little Brother simulation, as well.All experiments were executed for a month. All of the statistical computations were performed excluding the first day in order to reject any short time-scale spin-up phenomenon. A ten grid point lateral boundary zone was also excluded. To mimic the resolution of the operational GCM (ECHAM at T-42 resolution), a cutoff wavelength of ~900 km was used in the filtering of the Big Brother output before using it to drive the Little Brother.

This experiment was first performed by Denis et al. (2001), using a grid point model for a midlatitude winter simulation. Our study extends theirs by using both a tropical and a midlatitude domain case, and using a different (in this case, spectral) model.

One month simulation completed for April, 1994Both domains centered at 37.5°W and 5°SHorizontal resolution of 60 kmBig Brother domain at 181 x 182 grid pointsLittle Brother domain at 91 x 92 grid points18 vertical layers

One month simulation completed for February, 2001Both domains centered at 70°W and 47°NHorizontal resolution of 50 kmBig Brother domain at 151 x 142 grid pointsLittle Brother domain at 81 x 77 grid points18 vertical layers

BIG BROTHER LITTLE BROTHER

BIG BROTHER LITTLE BROTHER

PRECIPITATION

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var.

Ratio

Trans. Var.

RatioStat. Corr.

Trans. Corr.

Stat. Corr.

Trans. Corr.

Total

0.8147

0.4257 1.317 1.4374 0.7841 0.405

0.8847 0.4834

LW0.8534

0.5382 1.2967 1.3442 0.8227 0.5061

0.9272 0.577

SW0.2247

0.1293 1.7362 1.8379

0.2075

0.0921

0.2618

0.1258

SPECIFIC HUMIDITY (850 MBAR)

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var.

Ratio

Trans. Var.

RatioStat. Corr.

Trans. Corr.

Stat. Corr

.Trans. Corr.

Total

0.9935

0.9336 1.0061 1.0188 0.9938 0.9345

0.9775 0.835

LW0.9936

0.9391 1.0064 1.0182 0.994 0.9363

0.9792 0.8448

SW0.9841

0.7504 0.9834 1.072

0.9848 0.845

0.981

0.8305

PRECIPITATION

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var. Rati

o

Trans.

Var. Rati

oStat. Corr.

Trans. Corr.

Stat. Corr

.Trans. Corr.

Total

0.9452

0.7382

1.0639

1.0502

0.9663 0.7258

0.8844 0.6980

LW0.9589

0.7941

1.0492

1.0388

0.9750 0.7944

0.9153 0.7524

SW0.8211

0.4140

1.1863

1.1889

0.8232

0.4149

0.8196

0.4750

SPECIFIC HUMIDITY (850 MBAR)

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var. Rati

o

Trans.

Var. Rati

oStat. Corr.

Trans.

Corr.Stat. Corr.

Trans. Corr.

Total

0.9972

0.9641

1.0682

1.0482

0.9981

0.9621

0.9961 0.9526

LW0.9973

0.9645

1.0676

1.0471

0.9982

0.9627

0.9961 0.9558

SW0.9972

0.9588

1.0795

1.0899

0.9976

0.9645

0.9965

0.9494 Total Field (TOTAL) is separated into a small-scale

component (SW), and large-scale component (LW); defined as the wave numbers above and below the cutoff wave number.Stationary Correlation (Stat. Corr.) = spatial correlation of time-mean fields. Stationary Variance Ratio (Stat. Var. Ratio)=ratio of variances of time-mean fields.Transient Correlation (Trans. Corr.), Transient Variance Ratio (Trans. Var. Ratio) = spatial correlation, variance ratio of transient fields (total-stationary).Statistics provided for sea and land separately, as well as total.

In most fields, good agreement between Big and Little Brothers was obtained, for both small and large scales, after a brief initial spin-up period.

Precipitation was the exception. For our tropical domain experiment, the small-scale features of the precipitation field in the Big Brother were not reproduced by the Little Brother. The spatial and temporal variations of the large-scale component of the precipitation were well reproduced.

The reason for the poor reproduction of the small-scale component of the precipitation is that this component is inherently unpredictable, at least in this model, rather than because of any inherent flaw in the nesting strategy. This was shown by an ensemble of identically forced Little Brother simulations which were initialized at different times differing by 6-24 hours, in which the correlations of the small-scale precipitation between these different simulations was nearly as low as that between the Big and Little Brothers. Related to this, the agreement between Big and Little Brothers is fairly insensitive to the choice of the cutoff wave number used for the filtering.

Good reproduction of the small-scale precipitation was obtained for a wintertime midlatitude simulation. Thus, the relatively poor reproduction of this field for the tropical case appears to be due to specifically tropical (convective) precipitation processes.

“Ensemble” Simulations Results

ZONAL WIND (850 MBAR)

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var. Rati

o

Trans.

Var. Rati

oStat. Corr.

Trans.

Corr.Stat. Corr.

Trans. Corr.

Total

0.9936

0.9336

1.1407

1.1116

0.9951 0.9343 0.992 0.924

LW0.99

40.9344

1.1411

1.1121

0.9955 0.9354

0.9926 0.9263

SW0.9860

0.9202

1.1326

1.1137

0.9885

0.9278

0.9823

0.9113

ZONAL WIND (850 MBAR)

  SEA+LAND SEA LAND

 

Stat. Corr

.

Trans.

Corr.

Stat. Var.

Ratio

Trans. Var.

RatioStat. Corr.

Trans. Corr.

Stat. Corr.

Trans. Corr.

Total

0.9762 0.918 0.8878 0.9766 0.977 0.9168

0.9836 0.8754

LW0.9768

0.9227 0.8879 0.9748 0.9773 0.9194

0.9847 0.8821

SW0.9600

0.786 0.8726 1.0451

0.9667

0.8440

0.9489

0.8028

 

Stat. Corr.

Stat. Var.

RatioTrans. Corr.

Trans. Var. Ratio

T=06 HR

Total 0.9025 0.9382 0.4744 1.0981

LW 0.9400 0.9396 0.5905 1.1085

SW 0.3561 0.9120 0.1484 1.0779

T=12 HR

Total 0.8742 0.8398 0.4346 1.0747

LW 0.9141 0.8410 0.5406 1.0809

SW 0.3158 0.8013 0.1231 1.0836

T=18 HR

Total 0.7747 0.9637 0.3590 1.2473

LW 0.8176 0.9540 0.4544 1.2457

SW 0.2266 0.9423 0.0783 1.3260

T=24 HR

Total 0.8845 1.0883 0.4398 1.0224

LW 0.9274 1.0969 0.5601 1.0428

SW 0.2343 1.0506 0.0765 1.0228

PRECIPITATION FIELD ENSEMBLES

The table on the left shows the “ensemble” results comparing the identically forced Little Brother simulations, but initialized at different times differing by 6-24 hours; the correlations of the small-scale precipitation between these different simulations was almost as low as that between the Big and Little Brother “ensemble” simulations (not shown here).