Validation of the Simulated Microphysical Structure within the Midlevel Inflow Region of a Tropical, Oceanic Squall Line Hannah C. Barnes, Robert A. Houze.

Slides:



Advertisements
Similar presentations
An intraseasonal moisture nudging experiment in a tropical channel version of the WRF model: The model biases and the moisture nudging scale dependencies.
Advertisements

The Impact of Ice Microphysics on the Genesis of Hurricane Julia (2010) Stefan Cecelski 1 and Dr. Da-Lin Zhang Department of Atmospheric and Oceanic Science.
Dynamical Downscaling of CCSM Using WRF Yang Gao 1, Joshua S. Fu 1, Yun-Fat Lam 1, John Drake 1, Kate Evans 2 1 University of Tennessee, USA 2 Oak Ridge.
Structure of mid-latitude cyclones crossing the California Sierra Nevada as seen by vertically pointing radar Socorro Medina, Robert Houze, Christopher.
Radar signatures in complex terrain during the passage of mid-latitude cyclones Socorro Medina Department of Atmospheric Sciences University of Washington.
A WRF Simulation of the Genesis of Tropical Storm Eugene (2005) Associated With the ITCZ Breakdowns The UMD/NASA-GSFC Users' and Developers' Workshop,
Scientific Objectives and Required Facilities Socorro Medina, Robert Houze, and Stacy Brodzik TIMREX Planning Meeting, Tainan, Taiwan, 9 November 2007.
What we have learned about Orographic Precipitation Mechanisms from MAP and IMPROVE-2: MODELING Socorro Medina, Robert Houze, Brad Smull University of.
Strong Polar Anticyclone Activity over the Northern Hemisphere and an Examination of the Alaskan Anticyclone Justin E. Jones, Lance F. Bosart, and Daniel.
MAP and IMPROVE II Experimental Areas SHARE Workshop, Boulder, 5 May 2005.
The Effect of the Terrain on Monsoon Convection in the Himalayan Region Socorro Medina 1, Robert Houze 1, Anil Kumar 2,3 and Dev Niyogi 3 Conference on.
ASSIMILATION of RADAR DATA at CONVECTIVE SCALES with the EnKF: PERFECT-MODEL EXPERIMENTS USING WRF / DART Altuğ Aksoy National Center for Atmospheric Research.
The Effect of the Terrain on Monsoon Convection in the Himalayan Region Socorro Medina 1, Robert Houze 1, Anil Kumar 2,3 and Dev Niyogi 3 Cloud and Precipitation.
The effect of terrain and land surface on summer monsoon convection in the Himalayan region Socorro Medina, Robert Houze, Anil Kumar, and Dev Niyogi 13.
Lessons learned in field studies about weather radar observations in the western US and other mountainous regions Socorro Medina and Robert Houze Department.
A new approach to parameterize ice-phase cloud microphysics The Predicted Particle Properties (P3) Scheme WWOSC 2014 Montreal, Canada August 17, 2014 Hugh.
Principal Rainband of Hurricane Katrina as observed in RAINEX Anthony C. Didlake, Jr. 28 th Conference on Hurricanes and Tropical Meteorology April 29,
R. A. Houze, Jr., Socorro Medina, Ellen Sukovich, B. F. Smull University of Washington M. Steiner Princeton University Mechanisms of Orographic Precipitation.
Background In deriving basic understanding of atmospheric phenomena, the analysis often revolves around discovering and exploiting relationships between.
Orographic triggering and mesoscale organization of extreme storms in subtropical South America Kristen Lani Rasmussen Robert A. Houze, Jr. ICAM 2013,
Jamie Wolff Jeff Beck, Laurie Carson, Michelle Harrold, Tracy Hertneky 15 April 2015 Assessment of two microphysics schemes in the NOAA Environmental Modeling.
The MJO Precipitating Cloud Population over the Central Indian Ocean as seen by the TRMM PR Hannah C. Barnes Robert A. Houze, Jr. University of Washington.
The mesoscale organization and dynamics of extreme convection in subtropical South America Kristen Lani Rasmussen Robert A. Houze, Jr., Anil Kumar 2013.
Orographic Precipitation Enhancement in Midlatitude Baroclinic Storms: Results from MAP and IMPROVE II Robert A. Houze and Socorro Medina.
A Conceptual Model for the Hydrometeor Structure of Mesoscale Convective Systems during the MJO Active Stage Hannah C. Barnes Robert A. Houze, Jr. University.
A Conceptual Model for the Hydrometeor Structure of Mesoscale Convective Systems during the MJO Active Stage Hannah C. Barnes Robert A. Houze, Jr. University.
Real-Time Dissemination of Hurricane Wind Fields Determined from Airborne Doppler Radar John Gamache NOAA/AOML/Hurricane Research Division Collaborators:
Earth-Sun System Division National Aeronautics and Space Administration SPoRT SAC Nov 21-22, 2005 Regional Modeling using MODIS SST composites Prepared.
Accounting for Uncertainties in NWPs using the Ensemble Approach for Inputs to ATD Models Dave Stauffer The Pennsylvania State University Office of the.
Figure sec mean topography (m, shaded following scale at upper left) of the Intermountain West and adjoining regions,
Dual-Aircraft Investigation of the inner Core of Hurricane Norbert. Part Ⅲ : Water Budget Gamache, J. F., R. A. Houze, Jr., and F. D. Marks, Jr., 1993:
Aircraft, Satellite Measurements and Numerical Simulations of Gravity Waves in the Extra-tropical UTLS Region Meng Zhang, Fuqing Zhang and Gang Ko Penn.
Research on the HWRF Model: Intensification and Uncertainties in Model Physics Research on the HWRF Model: Intensification and Uncertainties in Model Physics.
S-Band Radar Dual-Polarization Observations of Winter Storms P. C. Kennedy and S. A. Rutledge CSU-CHILL Radar Facility.
Meng, Z., F. Zhang, P. Markoswki, D. Wu, and K. Zhao, 2012: A modeling study on the development of a bowing structure and associated rear inflow within.
Funded by NSF –Grant AGS Conceptual Model of Mesoscale Convective Systems (MCSs) ConvectiveStratiform TOGA COARE: 3D, layer airflow Kingsmill.
High-Resolution Simulation of Hurricane Bonnie (1998). Part II: Water Budget SCOTT A. BRAUN J. Atmos. Sci., 63,
DRAFT – Page 1 – January 14, 2016 Development of a Convective Scale Ensemble Kalman Filter at Environment Canada Luc Fillion 1, Kao-Shen Chung 1, Monique.
MJO Insights from the S-PolKa radar in DYNAMO Robert A. Houze, Jr. H. C. Barnes, S. W. Powell, A. K. Rowe, M. Zuluaga University of Washington Symposium.
Cloud structure and organization under suppressed conditions during DYNAMO/AMIE/CINDY2011 Angela Rowe and Robert Houze, Jr. University of Washington 31.
Orographic Precipitation in Potentially Unstable Alpine Storms: MAP IOPs 2b, 3, and 5 Socorro Medina and Robert A. Houze.
Numerical Simulation and Prediction of Supercell Tornadoes Ming Xue School of Meteorology and Center for Analysis and Prediction of Storms University of.
Understanding Convection in Relation to the Non-aerosol Environment ASR Science Team Meeting, Tyson’s Corner, VA, March 17, 2015 Robert Houze With help.
Active and passive microwave remote sensing of precipitation at high latitudes R. Bennartz - M. Kulie - C. O’Dell (1) S. Pinori – A. Mugnai (2) (1) University.
Cheng-Zhong Zhang and Hiroshi Uyeda Hydroshperic Atmospheric Research Center, Nagoya University 1 November 2006 in Boulder, Colorado Possible Mechanism.
Mesoscale Assimilation of Rain-Affected Observations Clark Amerault National Research Council Postdoctoral Associate - Naval Research Laboratory, Monterey,
Implementation of Terrain Resolving Capability for The Variational Doppler Radar Analysis System (VDRAS) Tai, Sheng-Lun 1, Yu-Chieng Liou 1,3, Juanzhen.
Franklin, C. N., G. J. Holland, and P. T. May, 2005: Sensitivity of tropical cyclone rainbands to ice-phase microphysics. Mon. Wea. Rev., 133,
Impact of Cloud Microphysics on the Development of Trailing Stratiform Precipitation in a Simulated Squall Line: Comparison of One- and Two-Moment Schemes.
Jennifer DeHart and Robert Houze
Tropical Convection and MJO
Parameterization of Cloud Microphysics Based on the Prediction of Bulk Ice Particle Properties. Part II: Case Study Comparisons with Observations and Other.
WRF model runs of 2 and 3 August
Yumin Moon & David S. Nolan (2014)
By SANDRA E. YUTER and ROBERT A. HOUZE JR
Simulation of the Arctic Mixed-Phase Clouds
  Robert Gibson1, Douglas Drob2 and David Norris1 1BBN Technologies
Water Budget of Typhoon Nari(2001)
The Microphysical Structure of Mesoscale Convective Systems
Group interests RICO data required
Sensitivity of WRF microphysics to aerosol concentration
Radiation fogs: WRF and LES numerical experiments
Bodine, D. J., and K. L. Rasmussen, 2017
Microphysics of 2-Day Rain Events During the Active Stage
Application of radar observations to the evaluation and improvement of cloud permitting regional model simulations of MJO Samson M. Hagos, Zhe Feng, Kiranmayi.
The use of multi-frequency radar measurements for investigating microphysical processes during DYNAMO/AMIE Angela Rowe and Robert Houze, Jr. University.
Dual-Aircraft Investigation of the Inner Core of Hurricane Nobert
Scott A. Braun, 2002: Mon. Wea. Rev.,130,
Group interests RICO data in support of studies
Precipitation hydrometeor type
Presentation transcript:

Validation of the Simulated Microphysical Structure within the Midlevel Inflow Region of a Tropical, Oceanic Squall Line Hannah C. Barnes, Robert A. Houze Jr. University of Washington 37 th Conference on Radar Meteorology 14 th September 2015 Embassy Suites Hotel and Conference Center, Norman, OK Funded by NSF Grant AGS-1355 and DOE Grant DE-SC

Microphysical Structure of Squall Lines Observation and validation difficult Observation / Validation Method Aircraft Observations Particle ID (PID) from dual- polarimetric radar Numerical Simulations Advantages In situ Large spatial coverage Increased temporal coverage Complete spatial coverage Complete temporal coverage All processes Disadvantages Spatially limited Temporally limited Difficult to validate Theory & observation based Limited by radar quality Dominant only Difficult to validate Theory based Parameterizations Different schemes Objective: Is microphysical structure from PID and WRF consistent with each other and dynamics?

Milbrandt - Yau Morrison WDM6 S-PolKa Microphysical Structure Intercomparison Microphysical structure linked to dynamical structure Intercomparison framed around midlevel inflow PID Analysis (Barnes and Houze, 2014) Midlevel inflow from radial velocity Composite around midlevel inflow Numerical Simulations Assimilate radial velocity Composite around “forced” midlevel inflow Distance from S-PolKa (km) Horizontal Wind Speed Height (km) Radial Velocity

PID Microphysical Analysis NCAR S-PolKa during DYNAMO / AMIE (Vivekanandan 1999) –Nov 2011 – Jan 2012 –Central Indian Ocean 9 hydrometeor types –Uses dual-polarimetric and sounding data –Thresholds based on previous studies, theory, field experience –Dominant type only Frozen hydrometeors represent microphysical processes Spatially composited around midlevel inflow –Layered structure Barnes and Houze, Normalized Height Normalized Range Small Ice Crystals = Deposition Dry Aggregates = Aggregation Graupel / Rimed Aggregates = Riming Wet Aggregates = Melting Midlevel Inflow Spatial Composites

WRF Data Assimilation Group production terms by process All processes Provides rate (kg kg -1 s -1 ) Composite members containing midlevel inflow Simulation Time23 Dec UTC Assimilation TimeEvery 15 mins starting at 1800 UTC InitializationERA-Interim Vertical Levels39, Top at 26 km Domains3 km, 1 km Members50 AssimilateS-PolKa radial velocity Planetary Boundary Layer Parameterization Bretherton and Park (UW) Longwave Radiation Parameterization RRTM Shortwave Radiation Parameterization Dudhia Surface Layer Parameterization Monin-Obikhov Microphysics Parameterization Milbrandt – Yau Morrison WDM6 Penn State University EnKF / WRF Longitude Latitude Domain 1 (3 km) Domain 2 (1 km) S-PolKa S-PolKa and WRF Domains

Squall Line 1930 UTC, 23 December 2011

Milbrandt - Yau Morrison WDM6 PPI Maximum Reflectivity S-PolKa Squall Line Structure RHI Wind Speed (along red line above) Height (km) Normalized Zonal Distance Distance from S-PolKa (km) Height (km) Distance from S-PolKa (km) Distance from S-PolKa

Microphysical Intercomparison Only compare location

Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mean Production Rate (kg kg -1 s -1 ) Adjusted Height Normalized Zonal Distance S-PolKa PID Normalized Height DepositionDeposition 3.1e-6 4.4e-8 3.7e-7 5.2e-9 Normalized Range Small Ice Crystals = Deposition -20°C 0°C -20°C 0°C -20°C 0°C

Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mean Production Rate (kg kg -1 s -1 ) Adjusted Height Normalized Zonal Distance 1.3e-5 1.3e e e-22 Aggregation Frozen Collecting Frozen S-PolKa PID Normalized Height Normalized Range Dry Aggregates = Aggregation -20°C 0°C -20°C 0°C -20°C 0°C

Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mean Production Rate (kg kg -1 s -1 ) Adjusted Height Normalized Zonal Distance S-PolKa PID Normalized Height 1e-4 3.4e e-7 6.3e-13 Riming Frozen Collecting LiquidRiming Normalized Range Graupel/Rimed Aggregates = Riming -20°C 0°C -20°C 0°C -20°C 0°C

Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mean Production Rate (kg kg -1 s -1 ) Adjusted Height Normalized Zonal Distance S-PolKa PID Normalized Height Melting Normalized Range Wet Aggregates = Melting 9.6e-5 2.8e-8 1.6e-6 4.9e °C 0°C -20°C 0°C -20°C 0°C

ConclusionsConclusions PID and WRF provide good spatial and temporal coverage of microphysical structure –Both difficult to validate –Do they provide complementary data? Is microphysical structure consistent with dynamical structure and other method? –Framed around midlevel inflow –General structure consistent Layered –Details differ Aggregation and riming - WRF deeper Melting – Consistent except Milbrandt-Yau Deposition – WRF extends lower

Back Up Slides

1900 UTC 23 Dec 2011 Z Scale Factor X Scale Factor 1.) Map kinematics and hydrometeors using radial velocity and PID 2.) Composite around layer lifting model Methodology: Compositing m/s Radial Velocity Distance from S-Polka (km ) Height (km ) Generic Midlevel Inflow Particle ID SIC HIC WA DA G/R G/RA LR MR HR H/R H

Wet Aggregates Normalized Height Normalized Range Methodology: Composite Results

Longitude Height (kn) Shading: Horz. Speed White Contours: Reflectivity m/s Midlevel Inflow Member Selection Shading: Horz. Speed White Contours: Reflectivity Black Contours: Horz. Speed > 18 m/s Shading: Horz. Speed White Contours: Reflectivity Black Contours: Horz. Speed > 18 m/s Dots: Max Speed at level Milbrandt - Yau: Member UTC 23 Dec 2011 Shading: Horz. Speed White Contours: Reflectivity Black Contours: Horz. Speed > 18 m/s Dots: Max Speed at level post tests

Midlevel Inflow Compositing Milbrandt - Yau: Member UTC 23 Dec 2011 Height (km) Shading: Reflectivity Black Contours: Horz. Speed > 18 m/s Dots: Max speed at level post test Red Lines: Analysis boundaries Longitude dBZ Shading: Reflectivity Black Contours: Horz. Speed > 18 m/s Scaled Height (km) Longitude dBZ Original

Microphysical Process Definitions

Radial Velocity Preparation 1. Radar Quality Control Locations were PID present only PID used to remove Biological 2 nd trip Saturation Remove pixels with: Low signal-to-noise ratio Clutter High spectral Width 2. Super-Observations Bins: 2° x 1 km Quality control: < |45 ms -1 | Rules: < 2 obs in each bin Remove all Obs std(bin) > std(all) Remove all obs (obs – bin mean) > 2*std(bin) Remove obs at fault Median value Distance from S-PolKa (km) Raw Radial Velocity QCed Radial Velocity SuperObs Radial Velocity UTC 24 Dec 2011: 5°

Large Scale Environmental Milbrandt - Yau Morrison WDM6 Mean Temperature Map at 1000 hPa Distance from S-PloKa (km) Normalized Zonal Distance Composite Relative Humidity Cross Section with Temperature Contours Height (km) Composite Vertical Velocity Cross Section with Temperature Contours Height (km) Normalized Zonal Distance 0°C0°C -5 ° C -20 ° C -40 ° C 0°C0°C -5 ° C -20 ° C -40 ° C 0°C0°C -5 ° C -20 ° C -40 ° C 0°C0°C -5 ° C -20 ° C -40 ° C 0°C0°C -5 ° C -20 ° C -40 ° C 0°C0°C -5 ° C -20 ° C -40 ° C °

GraupelGraupel Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mixing Ratio (kg kg -1 ) Height (km) Normalized Zonal Distance 5e-3 5.9e-6 1e-6 2e-7

IceIce Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mixing Ratio (kg kg -1 ) Height (km) Normalized Zonal Distance 9e-4 2.2e-6 4.6e-5 1e-7

SnowSnow Milbrandt - Yau Morrison WDM6 Occurrence Frequency Mixing Ratio (kg kg -1 ) Height (km) Normalized Zonal Distance 1e-3 3.2e-6 8e-5 1.3e-7