Cloud Formation and Explicit Precipitation
Physical Processes
Cloud Formation
Clouds are formed as air parcels are forced to rise, cool and condense.
This forcing can be accomplished in several ways including surface heating,
frontal lifting, or mixing of the air (fog). In warm clouds, droplets can
grow by condensation in a supersaturated environment and by colliding and
coalescing with other cloud droplets. Cloud droplets can also form
with the aid of cloud condensation nuclei in an unsaturated environment
(RH > 90%). If a cloud extends above the 0°C line, it is called
a cold cloud. Even though the temperature may be below 0°C, water droplets
can still exist in clouds as super-cooled droplets. As a matter of
fact, cloud temperatures frequently need to get below -10°C for any
significant number of ice particles to form. If a cold cloud contains
both ice particles and super-cooled droplets, it is a mixed cloud.
If a cold cloud consists entirely of ice, it is said to be glaciated. Since
cloud droplets are small, they are hardest to freeze. Condensation
nuclei help the cloud droplets to freeze.
Precipitation Formation
In warm clouds, growth by condensation slows as the droplet radius increases.
There must be another means for warm clouds to produce precipitation.
Warm cloud droplets grow and form precipitation by the collision-coalescence
process. In cold clouds, precipitation forms by deposition, riming,
and aggregation. The growth of ice crystals, first by deposition
from the vapor phase in mixed clouds, and then by riming and/or aggregation
can produce precipitation-sized particles in reasonable periods of time
(see figure below). Precipitation sized particles actually start
falling once gravity overcomes the upward vertical movements of the drops
in the cloud sustaining them.

Model Implementations
Grid box Clouds
ETA Model
-
Temperature > 0°C cloud is liquid.
-
Temperature < -15°C cloud is ice.
-
Temperature between 0°C and 15°C cloud is ice if ice cloud existed
in box or box above during previous time step.
-
There is only one phase of cloud water computed per grid box.
-
Ice clouds form snow and liquid clouds form rain.
-
Clouds condense when relative humidity is > 75% for land and > 80% for
ocean.
Rapid Update Cycle (RUC)
-
The RUC uses the NCAR/Penn State mesoscale model MM5 parameterization for
cloud formation. Cloud hydrometeor species represented:
- cloud is water when temperature is greater than or equal to zero
degrees Celsius
- cloud is ice when temperatures is less than zero degrees Celsius
- the Marshall-Palmer size distribution is assumed for rain and snow
hydrometeors
Weather Research and Forecast (WRF)
To be determined
Nested Grid Model (NGM)
-
Cloud cover is not computed.
NOGAPS
-
Clouds are not explicitly predicted.
Spectral Clouds
Global Spectral Model (GSM) and Regional Spectral Model (RSM)
-
Clouds can exist in most model layers except near the surface and above
the tropopause.
-
Stratiform clouds are computed from mean cloud and relative humidity relationships.
AVN/MRF
-
Cloud parameterization scheme predicts cloud liquid and ice based on RH
and temperatures in each model layer.
-
Clouds can be advected and partial cloudiness is allowed.
Grid box Precipitation
ETA Model
-
A 3-D array indicates if precipitation is solid or liquid.
-
Precipitation within a box can be liquid and solid.
-
A snow water equivalent of 10" snow = 1" water is used because snow depths
not reported.
-
Two sources of condensation are large scale and convective processes.
-
According to Mike Staudenmaier, Jr. in "The Explicit Cloud Prediction Schemein
the Meso-Eta Model," these are the 6 microphysical processes are represented
the ETA model:
- autoconversion of cloud water to rain
- collection of cloud droplets by falling rain drops
- autoconversion of ice particles to snow
- collection of ice particles by falling snow
- melting of snow below freezing level
- evaporation of precipitation below cloud bases
-
Sublimation, deposition, evaporation, condensation, melting, and freezing
of raindrops is considered.
RUC
-
Included in the model is a freezing level for precipitation type determination.
-
Model removes supersaturation as precipitation.
-
Recognizes orographically induced precipitation.
-
Evaporation of precipitation occurs with convective precipitation but not
with stable precipitation.
-
Convective precipitation is formed on a sub-grid scale.
-
Stable precipitation is formed on a grid scale.
-
The RUC uses the NCAR/Penn State mesoscale model MM5 parameterization for
precipitation formation. Precipitation species represented:
- cloud water
- cloud ice
- snow
- graupel
- rain
NGM
-
Grid scale precipitation occurs when relative humidity > 95%.
-
Relative humidity < 95% causes evaporation of precipitation.
-
All precipitation falls as rain.
-
Snow depth analysis is not available.
Weather Research and Forecast (WRF)
To be determined
NOGAPS
-
Precipitation is not explicitly predicted.
Spectral Precipitation
GSM and RSM
-
Rain evaporates in unsaturated layers in the model below the condensation
level.
-
Precipitation falls as snow if temperatures in the lowest model layer and
at the ground are less than 0°C.
-
The grid scale condensation scheme: excess moisture is precipitated into
lower layers resulting in ground precipitation.
-
Arakawa-Schubert cumulus parameterization scheme gives smaller resolution
in the precipitation scheme.
AVN/MRF
-
Diagnoses rain and/or snow rates based on the amount of cloud liquid or
ice predicted.
Advantages and Disadvantages
Advantages
-
GSM and RSM can have precipitation that falls as snow.
-
ETA considers sublimation, deposition, evaporation, condensation, melting,
and freezing of raindrops.
-
ETA is simple enough to be used in operational meteorology, in terms of
computational speed and storage.
-
ETA and RUC both show cloud droplets that are super-cooled. This is important
for aviation but does not matter for weather forecasting.
-
ETA and RUC recognize orographically induced precipitation.
-
RUC recognizes land/ocean differences in precipitation formation.
-
AVN/MRF does a good job of predicting precipitation generated by large
cyclonic storms, due to well predicted large scale motions.
Disadvantages
-
The NGM does not compute cloud cover.
-
There is no stratiform rain in the NGM.
-
All precipitation from the NGM falls as rain. This would not be good in
regions of the world where frozen precipitation is common.
-
NGM and ETA do not report snow depth. This would again not be good in regions
of the world where frozen precipitation is common.
-
ETA does not consider precipitation advection.
-
ETA is not initialized with cloud information.
-
AVN/MRF does a poor job at predicting lake effect or orographic snow events.
-
AVN/MRF cannot predict isolated convective storms because the model does
not forecast for convective motion
Conclusions
-
The RSM is a local version of the GSM.
-
The RUC parameterizations are very similar to those used in the ETA model.
The RUC can be used as a short range ETA model.
-
The RUC seems to be the 'best' model to use for cloud cover and explicit
precipitation as it uses cloud data when initialized and uses an almost
identical scheme for explicit precip formation .
-
AVN is a good product for synoptic scale predictions in the field due to
its updating of initial conditions four times a day.
-
MRF initially is good for the beginning of its forecast period of synoptic
events, but lacks credibility compared to AVN as initial conditions are
updated.
References
Benjamin, Stan, NOAA, 3 January 1998: "Information on RUC/MAPS."
http://maps.fsl.noaa.gov/MAPS.40km.html.
-
Benjamin, Stan, NOAA/ERL Forecast Systems Lab, 16 June 1994: "Implementation
of the RUC."
-
http://maps.fsl.noaa.gov/tpbruc.cgi.
-
Black, Thomas L., June 1994: "The New NMC Mesoscale Eta Model: Description
and Forecast Examples."
-
Weather and Forecasting. pp. 265-278.
-
-
"Does the Cloud Scheme Interact with the Convective Scheme?"
-
http://www.emc.ncep.noaa.gov/mmb/research/FAQ-eta.html#ETA5.
-
-
Hoke, James E., September 1989: "The Regional Analysis and Forecast System
of the National Meteorological Center."
-
Weather and Forecasting. pp. 323-334. http://sgi62.wwb.noaa.gov:8080/rsm/
document.html.
-
-
Juang, 21 March 1997: "The NCEP Regional Spectral Model: An Update."
-
Bulletin of the American Meteorological Society. pp. 2125-2143.
-
-
Junker, Norman W., September 1989: "Performance of NMC's Regional Models."
-
Weather and Forecasting. pp. 368-390.
-
-
Mittelstadt, Jon, WRH-SSD, 27 January 1997: "The Eta-32 Model."
-
http://nimbo.wrh.noaa.gov/wrhq/98TAs/9803/index.html.
-
-
National Weather Service: "National Weather Service Medium Range Forecast(MRF)
Model Performance."
-
http://www.airfield-ops.hill.af.mil/osw/tips/mrf-perf.htm
-
-
"Parameterization Schemes."
-
http://www.wrh.noaa.gov/wrhq/96TAs/TA9606/ta96-06.html.
-
Robson, Alan, 5 November 1997: "Model Biases."
-
http://www.hpc.ncep.noaa.gov.
-
-
Staudenmaier, Jr., Mike, WRH-SSD, 19 November 1996: "The Explicit Cloud
Prediction Scheme in the Meso Eta Model."
-
http://nimbo.wrh.noaa.gov/wrhq/96TAs/TA9629/ta96-29.html.
-
-
Wallace and Hobbs: Atmospheric Science. pp. 143-214.
-
-
"What's the Deal with the Snow Cover in the NGM/ETA/AVN?"
http://www.emc.ncep.noaa.gov/mmb/research/FAQ-eta.html#GEN1.
-
"Why are the RH's So Low?"
http://www.emc.ncep.noaa.gov/mmb/research/FAQ-eta.html#ETA7.
-
Wu, Wan-shu, NCEP, 5 November 1997: "Changes to the 1997 NCEP Operational
MRF Model Analysis/ Forecast System."
-
http://sgi62.wwb.noaa.gov:8080/tpb97/tpb975_wp.html.
-
-
Zhao, Qingyun, August 1997: "A Prognostic Cloud Scheme for Operational
NWP Models."
-
Monthly Weather Review. pp. 1931-1953.
"Operational Models Matrix"
http://meted.comet.ucar.edu/nwp/pcu2/index.htm
"Generating
Clouds and Precipitation" (illustration)
http://meted.ucar.edu/nwp/pcu1/ic3/frameset.htm
Webpage Constructors
Lori Grimm
Todd Kostelecky
April 28, 1998
Webpage Editors
Jesse Peterson
Lionel Peyraud
Craig Porter
February 1, 1999
Webpage Editors
Todd Shoemake
Jon Wilson
Andrew Geyer
February 20, 2001
Webpage Editors
Trent Cloer
David Huston
February 21, 2002
URL: http://www.met.tamu.edu/class/metr452/models/precip.html
Return to the top of page.
Click here
to return to the main modeling page.