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The Hydrometeor Structure of The Hydrometeor Structure of

The Hydrometeor Structure of - PowerPoint Presentation

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The Hydrometeor Structure of - PPT Presentation

Mesoscale Convective Systems During DYNAMO Hannah C Barnes Robert A Houze Jr University of Washington 2013 Atmospheric System Research ASR Fall Working Group Meeting Hilton Washington DC Rockville Hotel amp Executive Meeting Center ID: 383937

vlr rain aggregates convective rain vlr convective aggregates reflectivity mixing ratio ice graupel hydrometeor houze utc light 2013 param

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Slide1

The Hydrometeor Structure of

Mesoscale Convective Systems During DYNAMOHannah C. BarnesRobert A. Houze, Jr.University of Washington2013 Atmospheric System Research (ASR) Fall Working Group MeetingHilton Washington DC / Rockville Hotel & Executive Meeting Center 5 November 2013

Funded by NSF –Grant AGS 1059611Slide2

Conceptual Model of Mesoscale Convective Systems (MCSs)

ConvectiveStratiformTOGA COARE: 3D, layer airflowKingsmill and Houze (1999a)Slide3

Indian

Ocean

Addu Atoll, Maldives

Dual wavelength

Only using S-Band

Doppler

Dual-polarimetric

Particle Identification Algorithm (

Vivekanandan

et al., 1999)

RHI sectors

SPolKa

DYNAMO-AMIE

-

CINDYSlide4

Objective

Characterize hydrometeor structure of MCSsComposite with respect to kinematic structureSlide5

Methodology

11 rain maximums during DYNAMO (Zuluaga and Houze, 2013)Subjectively identify cases SPolKa radial velocityLayer liftingRHI sector and within 100 kmOne per stormManually map hydrometeor location using PIDComposite around layer liftingZuluaga and Houze (2013)

Hourly Timeseries of Accumulated Rain

1

4

5

6

7

8

9

10

11

2

3Slide6

Convective Updraft

dBZVrad24 Oct 0250 UTCSlide7

Wet Aggregates

Dry Aggregates

Small Ice Crystals

Horz. Oriented Ice

Graupel / Rimed Aggregates

Graupel - Rain

Heavy Rain

Moderate Rain

Light Rain

Very Light Rain

Convective UpdraftSlide8

Conceptual Diagram of Convective UpdraftsSlide9

Distribution of Convective Polarimetric Variables

ReflectivityCorrelation CoefficientTemperature G GR HR MR LR VLR WA DA SI HI G GR HR MR LR VLR WA DA SI HI

G GR HR MR LR VLR WA DA SI HI

G GR HR MR LR VLR WA DA SI HI

Differential Reflectivity

Slide10

Mid-Level Inflow

dBZVrad23 Dec 1850 UTCSlide11

Wet Aggregates

Dry Aggregates Small Ice CrystalsHorz. Oriented IceGraupel / Rimed AggregatesGraupel - RainHeavy RainModerate RainLight RainVery Light Rain

Leading Line –

T

railing StratiformSlide12

Distribution of Squall Polarimetric Variables

ReflectivityDifferential ReflectivityCorrelation CoefficientTemperature G GR HR MR LR VLR WA DA SI HI

G GR HR MR LR VLR WA DA SI HI

G GR HR MR LR VLR WA DA SI HI

G GR HR MR LR VLR WA DA SI HI

Slide13

Conceptual Diagram of Mid-Level InflowSlide14

Conclusions

Comparison of model output and radar observationsSlide15

Mesoscale Modeling of Squall Line

WRF 3.4.1Resolution: Outer – 9km, Inner – 3kmCu Param: Outer – KF, Inner – NoneMP Param: Both - GoddardPBL Param: Both – UWForcing: ERAi00 UTC 23 Dec – 00 UTC 25 Dec

Reflectivity

Zonal WindSlide16

Distribution of Hydrometeor Mixing Ratio

Zonal Wind and ReflectivityRain Mixing RatioSnow Mixing RatioCloud Mixing Ratio Graupel Mixing Ratio Ice Mixing RatioSlide17

Model Representation of Anvils over Afirca

Powell et al., 2012 Slide18

Questions ?