Title: Robin Hogan, Julien Delanoe and Nicola Pounder
1Towards unified retrievals of clouds,
precipitation and aerosols
- Robin Hogan, Julien Delanoe and Nicola Pounder
- University of Reading
2Introduction
- Most exciting aspect to EarthCARE is synergy by
design - A well formulated synergistic algorithm ought to
always outperform a single-instrument algorithm - If different species present in the same profile
then need to retrieve them simultaneously in
order to interpret measurements that are
simultaneously sensitive to both (e.g.
path-integrated attenuation and radiances
sensitive to whole column) - In the RATEC project we will begin development of
a unified retrieval algorithm for clouds,
precipitation and aerosols - A variational formulation will weight information
from all sources (radar, lidar, radiances and
prior information) according to its error - This could also serve as 1- and 2-instrument
algorithms (to insure against instrument
degradation or failure) by simply removing
certain observations - This talk will present the ingredients that have
been gathered so far...
3Motivation and classification
Global-mean cloud fraction
Cloudsat radar
CALIPSO lidar
- Radar and lidar
- Radar only
- Lidar only
Insects Aerosol Rain Supercooled liquid
cloud Warm liquid cloud Ice and supercooled
liquid Ice Clear No ice/rain but possibly
liquid Ground
Preliminary target classification
4Retrieval framework
- Ingredients developed
- Not yet developed
5State variables ice clouds
- Ice clouds already done by Delanoe and Hogan
(2008), extended in CASPER to use HSRL lidar - Variational version of Donovan and Tinel
radar-lidar algorithms - Blends seamlessly between regions of cloud
detected by radar and lidar - State vector contains these elements to describe
ice clouds - Visible extinction coefficient at each gate, a
- Normalized number concentration parameter, N0
- Lidar extinction-to-backscatter ratio, S
- Prior information and other constraints
- Temperature dependence of N0(T) from aircraft
in-situ data - Smoothness constraint on the state variables so
that noisy observations (particularly lidar Mie
and Rayleigh channels) dont result in noisy
retrievals - Prior estimate of S (e.g. 20 sr)
- Microphysical model assumptions, e.g. mass-size
relationship, infrared scattering properties
6State variables liquid clouds
- Largely new, but will build on
- Smith Illingworth estimate of LWP from
path-integrated attenuation - CloudSat radar MODIS solar channels
- Information from HSRL using multiple-scattering
forward model - Possible state variables for liquid clouds
- Liquid water content, LWC (or possibly a) at each
gate - Droplet number concentration, constant in each
contiguous layer (via size information from MSI
channels, and combination of LWP from
path-integrated attenuation and optical depth
from MSI) - Prior information and other constraints
- Smoothness constraint on profile of LWC
- Prior estimate of number concentration (e.g. from
sea versus land) - Assume lidar extinction-to-backscatter ratio is
constant at 18.5 sr - LWC gradient at cloud base tends to the known
adiabatic profile given the temperature and
pressure
7State variables precipitation
- New would need to build on results of other
ESA/JAXA studies - Key ingredients would be radar multiple-scattering
model, surface return from ocean, profile of
attenuated reflectivity (e.g. CloudSat), and
Doppler velocity in stratiform conditions - Possible state variables for precipitation
- Rain rate profile, R
- Normalized number concentration, Nw (one value
per profile) - Riming factor for snow and for ice above rain
(one value per profile) invoked in convective
conditions to account for higher density ice, and
also in snow (treated as an extension to the
ice-cloud retrieval) - Melting-layer thickness scaling factor...
- Prior information and other constraints
- Strong smoothness constraint on profile of rain
rate - Estimate of Nw dependent on warm rain (e.g. Sc
drizzle) or cold rain - Warning this will be difficult!
8State variables aerosols
- New would need to build on results of other
ESA/JAXA studies - Key ingredients would be HSRL, MSI solar channels
in the day and optical depth constraint from
lidar ocean surface return - Relatively straightforward compared to
precipitation! - Possible state variables for aerosols
- Extinction coefficient at 355 nm
- Exinction-to-backscatter ratio (one value per
layer) - Mean particle size (one value per layer)?
- Prior information and other constraints
- Extinction-to-backscatter ratio estimate
dependent on geographical region
9Forward models active instruments
- Radar
- Microphysics scattering library for cloud
liquid, ice and precipitation particles, ideally
based on DDA and T-matrix rather than Mie - Propagation fast multiple-scattering model is
available (Hogan and Battaglia 2008) but needs an
analytic Jacobian model - Doppler terminal fallspeeds straightforward
main challenge is to characterize error due to
vertical wind and non-uniform beam filling - Surface return requires first pass to
interpolate between clear skies? - Lidar
- Microphysics backscatter problem overcome by
retrieving extinction-to-backscatter ratio, but
some uncertainty between phase functions - Propagation fast multiple-scattering forward
model exists for ice clouds, where we are in the
small-angle limit, but wide-angle model for
liquid clouds currently lacks an analytic
Jacobian model or the ability to represent the
individual HSRL channels - Depolarization currently no forward model for
either single-scatter depolarization, or
depolarization due to multiple scattering
10Forward models passive instruments
- Infrared radiances
- Microphysics scattering library for cloud
liquid, ice and aerosols required - Propagation two models suitable for use RTTOV
(used by ECMWF and Met Office data assimilation
systems) and the Delanoe and Hogan (2008) scheme - Model inputs note that the error in this model
is significantly determined by the error in the
temperature profile - Solar radiances
- Microphysics scattering library required for
liquid, ice and aerosols, with uncertainty in the
asymmetry factor and single-scatter albedo - Propagation fast Radiant code from Colorado
State University could be implemented - Model inputs Need to assume a surface albedo
- Other uncertainties three-dimensional scattering
effects could be important but very difficult to
incorporate in a 1D retrieval
11 Examples of wide-angle multiple scattering
- LITE lidar (lltr, footprint1 km)
- CloudSat radar (lgtr)
12Fast multiple scattering forward model
Hogan and Battaglia (J. Atmos. Sci. 2008)
- New method uses the time-dependent two-stream
approximation - Agrees with Monte Carlo but 107 times faster (3
ms) - Added to CloudSat simulator
CloudSat-like example
CALIPSO-like example
13Exploiting multiple scattering
14Results
- 1D-Var retrievals using Hogan and Battaglia
forward model (Nicola Pounder)
First 3 optical depths would be seen by HSRL
15Test dataset ER-2 radars and lidar
10-GHz radar
94-GHz radar
- Can perform 94-GHz radar precipitation retrievals
(using surface return from the oceans), then
evaluate them by forward modelling the less
attenuated 10-GHz radar
16Next steps
- Within RATEC
- Code up flexible retrieval framework and error
reporting - Add various forward models
- Implement ice and liquid cloud capability
- Test on A-train and aircraft datasets
- Provide product description for 3D scene
construction - Post RATEC
- Test in ECSIM
- Via collaboration, implement precipitation and
aerosol components - Test when in 1- and 2-instrument configurations
in case of instrument degradation or failure