CRTM_Overview_2011_HIWWG_Chen

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Overview of Community Radiative Transfer

Model (CRTM)

Fuzhong Weng, Yong Chen and Min-Jeong Kim

NOAA/NESDIS/Center for Satellite Applications and Research and

Joint Center for Satellite Data Assimilation

High Impact Weather Working Group Workshop,

February 24, 2011, Norman, OK

CRTM Application Areas

CRTM was initially proposed to support primarily the JCSDA partners to assimilate satellite radiance data into global/regional forecast systems

It is now also supporting the US satellite program developments through generating a high quality proxy data for algorithm tests, developments and integrations

It has been used in the NOAA/NESDIS microwave sounding product system

It can be used to generate the synthetic satellite radiances from NWP nature runs for observation system simulation experiments

(OSSE)

It is linked to other key projects such as climate reanalysis and satellite cal/val

Joint Center for Satellite Data

Assimilation (JCSDA)

Partner Organizations

2

Requirements on CRTM

Perform fast and accurate forward, tangent linear/adjoint calculations

Support all the satellite instruments

(US and foreign) that are used in

NWP models

Work under all atmospheric and surface conditions

Have a flexible interface with different NWP models such as

GFS, NOGAPS, and WRF

Allow future expansion for broader applications

CRTM supports more than 100 Sensors

GOES-R ABI

Metop IASI/HIRS/AVHRR/AMSU/MHS

TIROS-N to NOAA-19 AVHRR

TIROS-N to NOAA-19 HIRS

GOES-8 to 14 Imager

GOES-8 to 14 sounder IR channel 08-13

Terra/Aqua MODIS Channel 1-10

MSG SEVIRI

Aqua AIRS, AMSR-E, AMSU-A,HSB

NOAA-15 to 19 AMSU-A

NOAA-15 to 17 AMSU-B

NOAA-18/19 MHS

TIROS-N to NOAA-14 MSU

DMSP F13 to15 SSM/I

DMSP F13,15 SSM/T1

DMSP F14,15 SSM/T2

DMSP F16-20 SSMIS

Coriolis Windsat

TiROS-NOAA-14 SSU

FY-3 IRAS, MWTS,MWHS,MWRI

NPP/JPSS CrIS/ATMS

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Highlights on CRTM Software Architecture, Sciences and Physical Processes

Atmospheric gaseous absorption

Band absorption coeff trained by LBL spectroscopy data with sensor response

 functions

Variable gases ( H

2

O, CO

2

, O

3 etc) .

Zeeman splitting effects near 60 GHz

Cloud/precipitation scattering and emission

Fast LUT optical models at all phases including non-spherical ice particles

Gamma size distributions

Aerosol scattering and emission

GOCART 5 species (dust, sea salt, organic/black carbon, )

Lognormal distributions with 35 bins

Surface emissivity/reflectivity

Two-scale microwave ocean emissivity

Large scale wave IR ocean emissivity

Land mw emissivity including vegetation and snow

Land IR emissivity data base

Radiative transfer scheme

Tangent linear and adjoints

Inputs and outputs at pressure level coordinate

Advanced double and adding scheme

Other transfer schemes such as SOI, Delta

Eddington

“Technology transfer made possible by CRTM is a shining example for collaboration among the JCSDA Partners and other organizations, and has been instrumental in the JCSDA success in accelerating uses of new satellite data in operations” – Dr. Louis Uccellini, Director of

National Centers for Environmental Prediction

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CRTM Infrared Spectroscopy

Corresponding to AIRS, IASI and CrIS

CRTM simulated brightness temperature (BT) spectrum for hyper-spectral infrared sensors IASI (black line), AIRS (red line), and CrIS (blue line).

5

CRTM Validation

using CloudSat data (non-precipitating weather)

CloudSat Data Set NCEP, ECMWF Data Set

Cloud profiles

( IWC, LWC)

Atmospheric profiles, surface conditions

Radiances and Brightness

Temperatures

CRTM Forward Model

Satellite zenith angles,

Solar zenith angles

Coincidental/Collocated Satellite

Data Set

Bias calculations and analysis, find the causes for the biases in the context of radiative physics and improve the CRTM performance.

6

Simulations Using Cloudsat Data and GDAS Profiles

Cloudsat data are averaged along the track of NOAA-18 satellite within each AMSU,

MHS and AVHRR IFOVs and then used as inputs to

CRTM

GDAS temperatures and water vapor profiles matched with Cloudsat profiles

Simulations are compared with NOAA-18 AMSU-A,

MHS, AVHRR observations

It is shown that both bias and

RMS errors are reduced with

Cloudsat data used in CRTM

AMSUA FOV (~50km diameter)

MHS

FOV

CloudSat FOV

~50 CloudSat FOVs

AVHRR FOV (GAC)

~4km diameter

(Chen et al., 2008, JGR) 7

Histograms of the Observed and Simulated for

AMSUA, MHS BTs over Ocean

Observation

Simulation

Reasonable agreements of observed and simulated BT distributions at all frequencies.

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Histograms of the BT Difference (Observation – Simulation) over

Ocean under Clear and Cloudy Conditions

Cloudy

Clear

The distributions are in

Gaussian shapes with maximum observation at or near zero, which confirm that the agreement between observed and simulated BTs are very good under clear and cloudy conditions.

There are clear-sky biases in certain surface sensitive microwave channels of the order of 1–2 K which is due to the sea-surface emission model used in CRTM.

9

CRTM Jacobian Calculations Compared with RTTOV

RTTOV is another fast radiative transfer model used by NWP community for satellite data assimilation

Radiance Jacobians at 6.2 and 7.2 micron water vapor channels

(GOES-R ABI and MSG

SEVIRI) are derived from CRTM

& RTTOV

Both models produce Jacobian profiles peaked at the same altitude

But the magnitudes are slightly different between two fast models

Assumption: surface emissivity =

0.98, local zenith angle = 0 deg., and skin temperature = 300 K

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Inter-comparison of CRTM with RTTOV at MSG SEVIRI Water Vapor Channels

Simulated vs observed brightness temperatures using 457 radiosonde profiles

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CRTM Simulated GOES-R ABI Visible Channel

Using WRF-Chem Model Outputs

GOESR ABI 0.64 µm

1.

Hourly GOES-R ABI proxy data simulated for the period of 10:00 UTC 24 to 03 UTC 25 August 2006 is produced with WRF-Chem air quality simulations and visible-enabled version of the CRTM.

2.

The dataset covers CONUS domain with all 16 ABI bands. The high resolution

(4km) aerosol and ozone data sets have been created over the continental US.

3.

Compared with MODIS observations, simulated reflectance over land appears lower than observed and cloud reflectance is somewhat brighter

MODIS 0.645 µm

Brad Pierce, 2009, GOES-R AWG workshop

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Microwave Surface Emissivity Models in CRTM

Oceans

– two-scale roughness theory

Sea ice

– Coherent reflection

Canopy

– Four layer clustering scattering

Bare soil

– Coherent reflection and surface roughness

• Snow/desert – Random media

Weng et al (2001, JGR)

Surface Emissivity Spectra (

=53

0

)

1.0

0.9

0.8

0.7

0.6

0.5

0.4

0.3

0.2

0 20 40 60 80 100 120 140 160 180 200

Frequency (GHz)

Snow

Canopy

Bare Soil

Wet Land

Desert

Ocean

Surface Emissivity Spectra (

=53

0

)

1.0

0.9

0.8

0.7

0.6

0.5

0.4

0.3

0.2

0 20 40 60 80 100 120 140 160 180 200

Frequency (GHz)

13

Snow

Canopy

Bare Soil

Wet Land

Desert

Ocean

Infrared Land Emissivity Data Base in CRTM

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CRTM Applications in GOES-R Retrieval Algorithms

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Progress in Cloudy Radiance Assimilation

 CRTM was implemented in NCEP GSI for clear sky satellite data assimilation and will be used for cloudy radiance assimilation

 Need to ensure a best trade-off between accuracy and computational efficiency

T o achieve improved forecast scores through cloudy radiance assimilation, we need:

Linearity of models

Appropriate background and observation errors

Error statistics (non-Gausian vs. Gausian pdf)

Quality control

Representativeness of observations and model

Bias correction

The fundamental works such as bias characterization, observation error covariance in cloudy conditions just started.

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AMSU Observation – Background (O-B) from GFS

Clear and cloudy sky over the ocean Clear sky over the ocean

O-B pdfs for all sky conditions appear very similar to those for clear-only conditions

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First Guess Departure as a Function of Cloud Liquid Water

Using average CLW, it seems that the bias is less dependent on cloud liquid water which will simplify the bias correction algorithm in GFS

18

Observation Error Covariance as a Function of Cloud Liquid Water

13 K 7K

9 K

10 K

1.3 K

0.55 K

However, observation error covariances remain highly dependent on CLW

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Summary and Conclusions

A new generation of radiative transfer model (Community

Radiative Transfer Model (CRTM)) has been developed for the

JCSDA partner’s NWP satellite data assimilation

CRTM Version 2 upgrades include radiance calculations in pressure coordinate, new microwave snow and sea ice emissivity, trace gas absorption, aerosol scattering and absorption

Independent assessments indicate an excellent performance of

CRTM in both forward and Jacobian computations

O-B bias and error covariance from CRTM in GFS under cloudy conditions are characterized for AMSU with which the AMSU cloudy radiances will be first tested for impact studies

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