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Microphysics
Parameterizations
1 Nov 2010
(“Sub” for next 2 lectures)
Wendi Kaufeld
Sources for these lectures...
• Your Stensrud Parameterization Schemes book
• Rogers & Yau: A Short Course in Cloud Physics
• WRF User’s website: past WRF Workshop presentations
• Notes from ATMS 597P, Matt Gilmore’s Cloud Microphysics
Parameterization class
• Notes from ATMS 501, Greg McFarquhar’s Physical
Meteorology class
• Comet module: “How Models Produce Precipitation and
Clouds”
http://www.meted.ucar.edu/nwp/model_precipandclouds/
Basics...
• Parameterization:
• AMS Glossary = “The representation, in a
dynamic model, of physical effects in terms of
admittedly oversimplified parameters, rather
than realistically requiring such effects to be
consequences of the dynamics of the system.”
• Black Box syndrome:
• The meteorological cancer of researchers
• Ignorance of assumptions, processes,
implementations within the parameterization
 Blindly choosing a parameterization?
Inconceivable!
• So many schemes... Why does the microphysics
parameterization you choose matter?
• Why do microphysical parameterizations matter?
• Spatial distribution of precipitation
Gilmore et al. (2004b)
Kessler, Lin (no ice), and Lin (ice)
• Why do microphysical parameterizations matter?
• Domain-total precipitation
• Behavior can change through the course of development
Kaufeld – MS Thesis (2010)
WRFv3.0.1 WRFv3.2
WRF-Chem responses to total aerosol, v3.0.1 & 3.2
Gilmore et al. (2004a)
• Why do microphysical parameterizations matter?
• Vertical distribution of mass (hydrometeors)
 Vertical distribution of latent heating
Varying only intercept param. & graupel density, individually
Gilmore et al. (2004a)
• Why do microphysical parameterizations matter?
• Ultimately can dictate evolution of system
Varying only intercept param. & graupel density, individually
• Microphysics:
• An emulation of the processes by which moisture is removed
from the air, based on other thermodynamic and kinematic fields
represented within a model
• Attempting to accurately account for sub-grid scale updrafts,
clouds, and precipitation
Basics... Terminology
Trouble in looking at only one output variable:
illusion of getting it right for the wrong reasons!
Basics... Interaction
• Convective Parameterizations + Microphysics
Parameterizations?
• CP: redistribution of Temperature, Moisture (reduce instability)
• Resolve sub-grid updrafts due to convection
• MP: Limited by CP
• High resolution: convection (updrafts) can be explicity modeled,
and no sub-grid emulation of convection is required
• Convective Parameterization obsolete!
• 1-2 km resolution reasonable for this assumption, though others
suggest much higher resolution may be required (Bryan 2003)
• Results feed back into other schemes: radiation
Basics... Terminology
• Hydrometeors
• Species (types):
• Cloud Droplets (QCLOUD) – no terminal velocity
• Raindrops (QRAIN)
• Ice Crystals and Aggregates (QICE)
• Rimed Ice Particles, Graupel, Hail (QGRAUP)
• Habits?
• Scales represented?
• Shapes?
• Non-hydrometeors:
• Aerosol vs. CN vs. CCN vs IN
 Not in most WRF configurations
represent this!
Basics... Representation
• How to represent these hydrometeors (and
non-hydrometeors)?
• PARTICLE SIZE DISTRIBUTIONS
• BULK representation types:
• Inverse exponential (Marshall-Palmer)
• Lognormal
• Gamma function
• BIN representation:
• No specified distribution
• Particle distribution divided into a finite
number of categories
• “Moments”
• 1 = mass, 2 = number, 3 = reflectivity
Basics... Representation
• BULK representation types:
• Inverse exponential: Marshall and
Palmer (1948)
• As rainfall rate increases, so does
number of large particles
Diameter (mm)
N
D
(m
-3
mm
-1
)
n (D) = n0e−λD
0 ≤ D ≤ Dmax
λ= 41 R-0.21
, R [mm h-1
], λ [cm-1
]
N = 8x104
m-3
cm-1
D = particle diameter
N = # particles per unit volume
λ = Slope parameter
n0 = Intercept parameter (max # of particles per volume at D=0)
• Raindrops
• Snow
• Graupel
• Hail
In double-moment schemes, this becomes a variable
Basics... Representation
• BULK representation types:
• Gamma distribution
• Small particle size relies heavily
upon μ
Diameter (mm)
N
D
(m
-3
mm
-1
)
n(D) = n0Dμ
e−λD
0 ≤ D ≤ Dmax
μ can be positive or negative
• Raindrops
• Snow
• Graupel
• Hail
In double-moment schemes, this becomes a variable
D = particle diameter
N = # particles per unit volume
λ = Slope parameter
n0 = Intercept parameter (max # of particles per
volume at D=0)
„Recently the first three-moment scheme
has been published by Milbrandt and Yau (2005)“
 Stensrud cites one by Clark (1974)
• BULK representation types: increasing in complexity!
(courtesy Seifert 2006)
Basics... Representation
Bulk Advantages
• Fewer number of
prognostic variables =
Computationally cheap!
• Easy to integrate
• Tweakable parameters
Bulk Limitations
• Cannot represent more
than one distribution at
a time (different
distributions may exist in
different parts of the
cloud/domain)
• “Frozen” distributions
for single-moment
schemes
Basics... Representation
Bin Advantages
• More realistic
• Processes that depend
on size distribution
(Terminal Velocity 
aggregation) better
represented
• Represent specific
parameterizations &
particle interactions
• Allows for bimodal
(+)distributions – and for
them to vary
Bin Limitations
• Very computationally
expensive!!!
• Difficult to validate
• Knowledge of ice phase
physics is lacking
essentially, tests the limits of our
current scientific understanding
and resources
Basics... Representation
Single-Moment Advantages
• Computationally
efficient
Single-Moment Limitations
• Inherent uncertainty due
to fixed parameters
• Situational dependence
Double-Moment Advantages
• Mass and number are
independent: can
represent different
environments!
• Less “parameter-tuning”
Double-Moment Limitations
• Difficult to validate
• Mass and Number are
independent: very
sensible to use with bin
scheme
Basics... Representation
• What’s “better” for YOUR research –
• a BULK or BIN parameterization?
• SINGLE, or DOUBLE moment (mass, number, both)?
Small Group ACTIVITY
5 minutes: meet with small group
5 minutes: meet with larger group
Pick group spokesperson for larger group
Things to think about...
-- what are you interested in forecasting/representing?
-- what time & spatial scales are important to you?
-- computational resources
Ideal MP scheme:
• Includes all relevant processes and hydrometeor types
• Perfect parameterizations
• Infinitely small grid size
 explicitly resolving each particle
• Easy to see why this is not currently possible...
•Parameterizations appear to be situationally dependent
•Limitations on computational power
So what does WRF have to offer?
WRF: MP Schemes Available*
* PUBLICLY available! Many more in development
ALL BULK SCHEMES

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WRF model Cloud Microphysics paramterization

  • 1. Microphysics Parameterizations 1 Nov 2010 (“Sub” for next 2 lectures) Wendi Kaufeld
  • 2. Sources for these lectures... • Your Stensrud Parameterization Schemes book • Rogers & Yau: A Short Course in Cloud Physics • WRF User’s website: past WRF Workshop presentations • Notes from ATMS 597P, Matt Gilmore’s Cloud Microphysics Parameterization class • Notes from ATMS 501, Greg McFarquhar’s Physical Meteorology class • Comet module: “How Models Produce Precipitation and Clouds” http://www.meted.ucar.edu/nwp/model_precipandclouds/
  • 3. Basics... • Parameterization: • AMS Glossary = “The representation, in a dynamic model, of physical effects in terms of admittedly oversimplified parameters, rather than realistically requiring such effects to be consequences of the dynamics of the system.” • Black Box syndrome: • The meteorological cancer of researchers • Ignorance of assumptions, processes, implementations within the parameterization  Blindly choosing a parameterization? Inconceivable!
  • 4. • So many schemes... Why does the microphysics parameterization you choose matter?
  • 5. • Why do microphysical parameterizations matter? • Spatial distribution of precipitation Gilmore et al. (2004b) Kessler, Lin (no ice), and Lin (ice)
  • 6. • Why do microphysical parameterizations matter? • Domain-total precipitation • Behavior can change through the course of development Kaufeld – MS Thesis (2010) WRFv3.0.1 WRFv3.2 WRF-Chem responses to total aerosol, v3.0.1 & 3.2
  • 7. Gilmore et al. (2004a) • Why do microphysical parameterizations matter? • Vertical distribution of mass (hydrometeors)  Vertical distribution of latent heating Varying only intercept param. & graupel density, individually
  • 8. Gilmore et al. (2004a) • Why do microphysical parameterizations matter? • Ultimately can dictate evolution of system Varying only intercept param. & graupel density, individually
  • 9. • Microphysics: • An emulation of the processes by which moisture is removed from the air, based on other thermodynamic and kinematic fields represented within a model • Attempting to accurately account for sub-grid scale updrafts, clouds, and precipitation Basics... Terminology Trouble in looking at only one output variable: illusion of getting it right for the wrong reasons!
  • 10. Basics... Interaction • Convective Parameterizations + Microphysics Parameterizations? • CP: redistribution of Temperature, Moisture (reduce instability) • Resolve sub-grid updrafts due to convection • MP: Limited by CP • High resolution: convection (updrafts) can be explicity modeled, and no sub-grid emulation of convection is required • Convective Parameterization obsolete! • 1-2 km resolution reasonable for this assumption, though others suggest much higher resolution may be required (Bryan 2003) • Results feed back into other schemes: radiation
  • 11. Basics... Terminology • Hydrometeors • Species (types): • Cloud Droplets (QCLOUD) – no terminal velocity • Raindrops (QRAIN) • Ice Crystals and Aggregates (QICE) • Rimed Ice Particles, Graupel, Hail (QGRAUP) • Habits? • Scales represented? • Shapes? • Non-hydrometeors: • Aerosol vs. CN vs. CCN vs IN  Not in most WRF configurations represent this!
  • 12. Basics... Representation • How to represent these hydrometeors (and non-hydrometeors)? • PARTICLE SIZE DISTRIBUTIONS • BULK representation types: • Inverse exponential (Marshall-Palmer) • Lognormal • Gamma function • BIN representation: • No specified distribution • Particle distribution divided into a finite number of categories • “Moments” • 1 = mass, 2 = number, 3 = reflectivity
  • 13. Basics... Representation • BULK representation types: • Inverse exponential: Marshall and Palmer (1948) • As rainfall rate increases, so does number of large particles Diameter (mm) N D (m -3 mm -1 ) n (D) = n0e−λD 0 ≤ D ≤ Dmax λ= 41 R-0.21 , R [mm h-1 ], λ [cm-1 ] N = 8x104 m-3 cm-1 D = particle diameter N = # particles per unit volume λ = Slope parameter n0 = Intercept parameter (max # of particles per volume at D=0) • Raindrops • Snow • Graupel • Hail In double-moment schemes, this becomes a variable
  • 14. Basics... Representation • BULK representation types: • Gamma distribution • Small particle size relies heavily upon μ Diameter (mm) N D (m -3 mm -1 ) n(D) = n0Dμ e−λD 0 ≤ D ≤ Dmax μ can be positive or negative • Raindrops • Snow • Graupel • Hail In double-moment schemes, this becomes a variable D = particle diameter N = # particles per unit volume λ = Slope parameter n0 = Intercept parameter (max # of particles per volume at D=0)
  • 15. „Recently the first three-moment scheme has been published by Milbrandt and Yau (2005)“  Stensrud cites one by Clark (1974) • BULK representation types: increasing in complexity! (courtesy Seifert 2006)
  • 16. Basics... Representation Bulk Advantages • Fewer number of prognostic variables = Computationally cheap! • Easy to integrate • Tweakable parameters Bulk Limitations • Cannot represent more than one distribution at a time (different distributions may exist in different parts of the cloud/domain) • “Frozen” distributions for single-moment schemes
  • 17. Basics... Representation Bin Advantages • More realistic • Processes that depend on size distribution (Terminal Velocity  aggregation) better represented • Represent specific parameterizations & particle interactions • Allows for bimodal (+)distributions – and for them to vary Bin Limitations • Very computationally expensive!!! • Difficult to validate • Knowledge of ice phase physics is lacking essentially, tests the limits of our current scientific understanding and resources
  • 18. Basics... Representation Single-Moment Advantages • Computationally efficient Single-Moment Limitations • Inherent uncertainty due to fixed parameters • Situational dependence Double-Moment Advantages • Mass and number are independent: can represent different environments! • Less “parameter-tuning” Double-Moment Limitations • Difficult to validate • Mass and Number are independent: very sensible to use with bin scheme
  • 19. Basics... Representation • What’s “better” for YOUR research – • a BULK or BIN parameterization? • SINGLE, or DOUBLE moment (mass, number, both)? Small Group ACTIVITY 5 minutes: meet with small group 5 minutes: meet with larger group Pick group spokesperson for larger group Things to think about... -- what are you interested in forecasting/representing? -- what time & spatial scales are important to you? -- computational resources
  • 20. Ideal MP scheme: • Includes all relevant processes and hydrometeor types • Perfect parameterizations • Infinitely small grid size  explicitly resolving each particle • Easy to see why this is not currently possible... •Parameterizations appear to be situationally dependent •Limitations on computational power So what does WRF have to offer?
  • 21. WRF: MP Schemes Available* * PUBLICLY available! Many more in development ALL BULK SCHEMES

Editor's Notes

  • #4: Different hydrometeors represented Warm: Kessler // Cold also? Single-moment vs. double-moment Black Box syndrome... Too complicated to deal with? Lots added within last couple of years – more developments on the way.
  • #9: Hierarchy of model needs to produce “realistic” precipitation: actually other factors are “more” important than mp scheme!!! (Because it depends on the predicted quantities, u,v,T,q)
  • #11: Habits: where things get interesting.
  • #12: Bulk types... Differing degrees of complexity
  • #13: Represent most hydrometeors in this fashion. * ONLY MANIFESTS IN AVERAGES: not direct observations
  • #14: Represent most hydrometeors in this fashion. * ONLY MANIFESTS IN AVERAGES: not direct observations
  • #19: Habits: where things get interesting.
  • #21: # of hydrometeors Types of hydrometeors Consideration of different types of cloud droplets? HOW MANY OF THESE CAN INCLUDE DEPENDENCE ON AEROSOL?