Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe...

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Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe Storms Laboratory, Norman, OK Funding sources in the Office of Naval Research, NSF, NSSL, the National Research Council, and the Oklahoma State Regents Lightning at NSSL: Numerical Modeling and Data Assimilation

Transcript of Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe...

Page 1: Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe Storms Laboratory, Norman, OK Funding sources in the.

Edward MansellNational Severe Storms Laboratory

Donald MacGorman and Conrad ZieglerNational Severe Storms Laboratory, Norman, OK

Funding sources in the Office of Naval Research, NSF, NSSL, the National

Research Council, and the Oklahoma State Regents

Lightning at NSSL: Numerical Modeling and Data Assimilation

Page 2: Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe Storms Laboratory, Norman, OK Funding sources in the.

• Storm electrification modeling:

• Basic understanding of electrification processes

• Lightning-storm relationships

• Lightning data assimilation (COAMPS)

• On mesoscale (>10km), control convection parameterization scheme.

• Storm-scale EnKF radar data assimilation

Modeling Activities/Capabilities

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Storm Model (COMMAS)• Full dynamic, microphysical, and

electrical simulation model

• Collisional charge separation, explicit small ion processes, branched lightning.

• Two-moment bulk microphysics: Predict particle concentrations (and mass) for all hydrometeors (droplets, rain, ice crystals, snow, graupel, hail) and simple bulk CCN.

• MPI capable

[Mansell et al. 2002, 2005, (2009 in review), also Fierro et al, Kuhlman et al.]

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Supercell Simluation

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Small Storm Simluation

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Lightning and Charge Structure

Inferred charge structure from lightning sources

+

+–

Model-simulated charge structure and lightning

West -30km -25km East

Alti

tude

(km

)

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Sensitivity to CCN concentration

Volume

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Simulated Lightning Rate Correlations

Isolated cells: 0.7

multiple cells: 0.5

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Total Flash Rate Correlation Coefficient with

Parameter Isolated Storms Storm Systems

Maximum Elec. Field 0.08 0.10

Graupel Volume 0.69 0.50

Updraft Mass Flux (-10°C) 0.82 0.39

Updraft Volume (>10 m s-1) 0.73 0.29

Cloud Ice Mass Flux (-30°C)

0.79 0.65

Cloud Ice Mass 0.25 0.36

Rain Mass 0.64 0.63

Maximum Updraft 0.30 0.06

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Assimilating Lightning Data

[Mansell, Ziegler, and MacGorman, 2007]

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Method is similar to Rogers et al. (2000) for radar assimilation.

Force/suppress Kain-Fritsch based on presence/absence of lightning. Add up to 1.0 g/kg of moisture to get deep convection (10m/s updraft, 7km cloud depth).

Allow KF scheme to generate precipitation rates and latent heating and evaporative cooling. (Other methods can be used to adjust or impose latent heating rates based on rainfall relations)

LMA sources

KSCO

NE

Case study with COAMPS on 20-21 July 2000

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Test caseSpin-up period: Obs. Precip vs. Control

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Spin-up period: Obs. Precip vs. Assimilation

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Spin-up period: Control vs. Assimilation

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Surface Temperature (C)

Warm-start Model Conditions:Control Assimilation

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01 UTC 21 July

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02 UTC 21 July

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0-6 hr Precip: Obs and forecastsControl

Fcst from ltg. assim.

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Summary

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Issues

• Must consider lightning location accuracy in terms of model resolution.

• What does a “flash” represent in the observing system? (large variations in flash extent) Method tied to data source.

• For resolved convection or convection-permitting EnKF, need to relate lightning to model variables or derived quantities. And/Or use lightning mainly to initiate deep convection.

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