WMO International Cloud Modeling Workshop

Slides:



Advertisements
Similar presentations
Simulating cloud-microphysical processes in CRCM5 Ping Du, Éric Girard, Jean-Pierre Blanchet.
Advertisements

WMO International Cloud Modeling Workshop, July 2004 A two-moment microphysical scheme for mesoscale and microscale cloud resolving models Axel Seifert.
Parametric representation of the hydrometeor spectra for LES warm bulk microphysical schemes. Olivier Geoffroy, Pier Siebesma (KNMI), Jean-Louis Brenguier,
Toward Improving Representation of Model Microphysics Errors in a Convection-Allowing Ensemble: Evaluation and Diagnosis of mixed- Microphysics and Perturbed.
URBAN GROWTH AND AEROSOL EFECTS ON CONVECTION OVER HOUSTON Gustavo G. Carrió, William R. Cotton, William Y. Cheng, and Steve M. Saleeby Colorado State.
Clear air echoes (few small insects) -12 dBZ. Echoes in clear air from insects Common is summer. Watch for echoes to expand area as sun sets and insects.
To perform statistical analyses of observations from dropsondes, microphysical imaging probes, and coordinated NOAA P-3 and NASA ER-2 Doppler radars To.
Ju-Hye Kim and Dong-Bin Shin* Department of Atmospheric Sciences
Size Sorting in Bulk & Bin Models Onset of precip – development of particles large enough to sediment relative to cloud droplets & ice crystals. Larger.
Clouds and Climate: Forced Changes to Clouds SOEE3410 Ken Carslaw Lecture 4 of a series of 5 on clouds and climate Properties and distribution of clouds.
Predicting lightning density in Mediterranean storms based on the WRF model dynamic and microphysical fields Yoav Yair 1, Barry Lynn 1, Colin Price 2,
What we have learned about Orographic Precipitation Mechanisms from MAP and IMPROVE-2: MODELING Socorro Medina, Robert Houze, Brad Smull University of.
1 Radar Displays PPI - Plan position Indicator Maps the received signals on polar coordinates in plan view. The antenna scans 360° at fixed elevation angle.
A new approach to parameterize ice-phase cloud microphysics The Predicted Particle Properties (P3) Scheme WWOSC 2014 Montreal, Canada August 17, 2014 Hugh.
1 st UNSTABLE Science Workshop April 2007 Science Question 3: Science Question 3: Numerical Weather Prediction Aspects of Forecasting Alberta Thunderstorms.
Aerosol effects on rain and hail formation and their representation using polarimetric radar signatures Eyal Ilotovich, Nir Benmoshe and Alexander Khain.
ON THE RESPONSE OF HAILSTORMS TO ENHANCED CCN CONCENTRATIONS William R. Cotton Department of Atmospheric Science, Colorado State University.
Impact of Graupel Parameterization Schemes on Idealized Bow Echo Simulations Rebecca D. Adams-Selin Adams-Selin, R. D., S. C. van den Heever, and R. D.
Microphysics Parameterizations 1 Nov 2010 (“Sub” for next 2 lectures) Wendi Kaufeld.
Ensemble Numerical Prediction of the 4 May 2007 Greensburg, Kansas Tornadic Supercell using EnKF Radar Data Assimilation Dr. Daniel T. Dawson II NRC Postdoc,
Microphysics complexity in squall line simulations. As high-resolution climate models increasingly turn towards an explicit representation of convection,
In this work we present results of cloud electrification obtained with the RAMS model that includes the process of charge separation between ice particles.
Thompson Runs Precipitation Comparison John D. McMillen.
Cloud Resolving Model Studies of Tropical Deep Convection Observed During HIBISCUS By Daniel Grosvenor, Thomas W. Choularton, & Hugh Coe - The University.
Bin resolved modeling of ice microphysics Wolfram Wobrock, Andrea Flossmann Workshop on Measurement Problems in Ice Clouds Zurich, Switzerland July 5-6,
DYMECS: Dynamical and Microphysical Evolution of Convective Storms (NERC Standard Grant) University of Reading: Robin Hogan, Bob Plant, Thorwald Stein,
The three-dimensional structure of convective storms Robin Hogan John Nicol Robert Plant Peter Clark Kirsty Hanley Carol Halliwell Humphrey Lean Thorwald.
Comparison of Evaporation and Cold Pool Development between Single- Moment (SM) and Multi-moment (MM) Bulk Microphysics Schemes In Idealized Simulations.
High-Resolution Simulation of Hurricane Bonnie (1998). Part II: Water Budget Braun, S. A., 2006: High-Resolution Simulation of Hurricane Bonnie (1998).
Dual-Polarization and Dual-Wavelength Radar Measurements Vivek National Center for Atmospheric Research Boulder, Colorado I.Polarization and dual- wavelength.
Evaluating Cloud Microphysics Schemes in the WRF Model Fifth Meeting of the Science Advisory Committee November, 2009 Andrew Molthan transitioning.
LIDAR OBSERVATIONS CONSTRAINT FOR CIRRUS MODELISATION IN Large Eddy Simulations O. Thouron, V. Giraud (LOA - Lille) H. Chepfer, V. Noël(LMD - Palaiseau)
Edward Mansell National Severe Storms Laboratory Donald MacGorman and Conrad Ziegler National Severe Storms Laboratory, Norman, OK Funding sources in the.
WRF Version 2: Physics Update Jimy Dudhia NCAR/MMM.
What does radar measure? Hydrometeors: rain drops, ice particles Other objects: e.g. birds, insects.
Norman Weather Forecast Office Gabe Garfield 2/23/11.
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.
Numerical Simulation and Prediction of Supercell Tornadoes Ming Xue School of Meteorology and Center for Analysis and Prediction of Storms University of.
Modeling. How Do we Address Aerosol-Cloud Interactions? The Scale Problem Process Models ~ 10s km Mesoscale Models Cloud resolving Models Regional Models.
Update on the 2-moment stratiform cloud microphysics scheme in CAM Hugh Morrison and Andrew Gettelman National Center for Atmospheric Research CCSM Atmospheric.
Vincent N. Sakwa RSMC, Nairobi
Analysis of High-Resolution WRF Simulations During A Severe Weather Event Jason A. Otkin* Cooperative Institute for Meteorological Satellite Studies, University.
Update on progress with the implementation of a new two-moment microphysics scheme: Model description and single-column tests Hugh Morrison, Andrew Gettelman,
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.
Development of cloud resolving model with microphysical bin model and parameterizations to predict the initial cloud droplet size distribution KUBA, Naomi.
Jason Milbrandt Recherche en Prévision Numérique [RPN] Meteorological Research Division, Environment Canada GEM Workshop, June 12, 2007 Multi-Moment Cloud.
Control Run Precipitation Comparison John D. McMillen.
ARPS( Advanced Regional Prediction System ) Version Center for Analysis and Prediction of Storms (CAPS), Oklahoma University tridimensional compressible.
Impact of Cloud Microphysics on the Development of Trailing Stratiform Precipitation in a Simulated Squall Line: Comparison of One- and Two-Moment Schemes.
Part II: Implementation of a New Snow Parameterization EXPLICIT FORECASTS OF WINTER PRECIPITATION USING AN IMPROVED BULK MICROPHYSICS SCHEME Thompson G.,
QUEST-Meeting, 14. Dez. 2007, Offenbach Das neue COSMO-EU Mikrophysikschema: Validierung von Eisgehalten Axel Seifert Deutscher Wetterdienst, Offenbach.
Diagnosing latent heating rates from model and in-situ microphysics data: Some (very) early results Chris Dearden University of Manchester DIAMET Project.
Reflections on Radar Observations of Mesoscale Precipitation
Chap. V Precipitation measurements
Using microphysical observations during
An accurate, efficient method for calculating hydrometeor advection in multi-moment bulk and bin microphysics schemes Hugh Morrison (NCAR*) Thanks to:
Influences of Particle Bulk Density of Snow and Graupel in Microphysics-Consistent Microwave Brightness Temperature Simulations Research Group Meeting.
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
By SANDRA E. YUTER and ROBERT A. HOUZE JR
GEORGE H. BRYAN AND HUGH MORRISON
A new approach to parameterize ice-phase microphysics
The DYMECS project A statistical approach for the evaluation of convective storms in high-resolution models Thorwald Stein, Robin Hogan, John Nicol, Robert.
Sensitivity of WRF microphysics to aerosol concentration
Development of a New Parameterization for Below-Cloud Scavenging of Size-Resolved Particles by Rain and Snow Xihong Wang1, Leiming Zhang2, and Michael.
Dual-Aircraft Investigation of the Inner Core of Hurricane Nobert
Sensitivity of idealized squall-line simulations to the level of complexity used in two-moment bulk microphysics schemes. Speaker: Huan Chen Professor:
Scott A. Braun, 2002: Mon. Wea. Rev.,130,
Pan, Y., M. Xue, and G. Ge, 2016 Mon. Wea. Rev., 144, 371–392.
Presentation transcript:

WMO International Cloud Modeling Workshop Simulation of Hail using a Triple-moment Microphysics Scheme Jason Milbrandt and M. K. Yau WMO International Cloud Modeling Workshop July 12, 2004

OBJECTIVES OF PRESENTATION: 1. Discuss the role of the shape parameter in bulk microphysics schemes 2. Demonstrate that hail sizes can be simulated using a bulk scheme 3. Compare sensitivity experiments using various bulk methods

Representation of a hydrometeor size distribution: BULK METHOD Representation of a hydrometeor size distribution: N(D) D [ m] 100 [m-3  m-1] 20 40 60 80 101 10-1 10-2 ANALYTIC FUNCTION 1 m3 (unit volume) [e.g. Cloud droplets]

Representation of a hydrometeor size distribution: BULK METHOD Representation of a hydrometeor size distribution: GAMMA DISTRIBUTION FUNCTION or, etc.

Representation of a hydrometeor size distribution: BULK METHOD Representation of a hydrometeor size distribution: GAMMA DISTRIBUTION FUNCTION Size Distribution Parameters: Various quantities: N0x : “intercept” lx : “slope” ax : shape parameter Qx : Mass content (Qx = r qx) NTx: Total number concentration Zx : Radar reflectivity Dmx: Mean-mass diameter

Typical double-moment method: BULK METHOD Typical double-moment method: Predict changes to Qx and NTx Implies changes to values of the N0x and lx (ax is held constant)

Alternative bulk methods: 1. Diagnostic-ax (double-moment) - ax = f (Qx, NTx) 2. Prognostic-ax (triple-moment) - a third moment must be predicted e.g. add dZx/dt equation

How important is the shape parameter (x ) ROLE OF ALPHA How important is the shape parameter (x ) in a bulk scheme? Continuity equation for x: Only SEDIMENTATION and SOURCE terms are affected by the microphysics scheme (and hence by ax) x: Predictive variable for hydrometeor category x

Analytic bin model calculation: (1D column) ROLE OF ALPHA: 1. SEDIMENTATION Analytic bin model calculation: (1D column) 10 5 z (km) Mass [g m-3] 1 1. Prescribe Q(z): D log N(D) N0 Di 2. Compute N(Di, z): [from a prescribed distribution] For every size bin i: zi(t) = zi(0) - Vi(Di)  t 3. Compute locations of each particle after sedimentation for time t:

Analytic bin model calculation: (1D column) ROLE OF ALPHA: 1. SEDIMENTATION Analytic bin model calculation: (1D column) Mass Content Total Number Concentration Equivalent Reflectivity Mean-mass Diameter INITIAL 5 min z [km] 10 min 15 min 20 min Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] Contours every 5 min

ROLE OF ALPHA: 1. SEDIMENTATION BULK SCHEMES = number-weighted fall velocity DM = reflectivity-weighted fall velocity TM SM = mass-weighted fall velocity

Mass Content ROLE OF ALPHA: 1. SEDIMENTATION BULK vs. ANALYTIC z [km] Q [g m-3] 5 min 10 min 15 min 20 min INITIAL Analytic model: Mass Content Bulk schemes: Q [g m-3] z [km] DOUBLE- MOMENT Fixed a = 0 SINGLE- Diagnosed a TRIPLE-

ROLE OF ALPHA: 1. SEDIMENTATION BULK vs. ANALYTIC For the prediction of NT, Z, and Dm, the various bulk methods exhibit similar relative abilities for pure sedimentation (as for Q). NOTE: No size-sorting mechanism exists for single-moment schemes For the double-moment scheme with a = 0, excessive size-sorting results in very large Dm and Z

CONTINUOUS COLLECTION ROLE OF ALPHA: 2. GROWTH RATES 2. MICROPHYSICS SOURCES/SINKS CONTINUOUS COLLECTION OF CLOUD WATER (CLcx): ( ) ( )

ROLE OF ALPHA: 2. GROWTH RATES A scheme’s ability to predict the growth rates depends on its ability to compute the value of certain moments [ranging from Mx(bx) to Mx(2+bx)] e.g. The accretion rate for hail (CLch) is proportional to Mh(2.6) HAIL bx  0.6

Analytic bin model calculation for sedimentation: ROLE OF ALPHA: 2. GROWTH RATES RECALL: Analytic bin model calculation for sedimentation: Mass Content Total Number Concentration Reflectivity z [km] Q [g m-3] NT [m-3] Ze [dBZ] Q NT Z } N0 l a {  At each level: M (2.6)_BULK

ROLE OF ALPHA: 2. GROWTH RATES (e.g. CLch) Ratio of Growth Rates: CLch_BULK CLch_ ANAL Mh(2.6)_BULK Mh(2.6)_ANAL = 2 min 10 5 0.8 1.0 1.2 8 min 10 5 0.8 1.0 1.2 z (km) z (km) Mh(2.6)_BULK Mh(2.6)_ANAL ANALYTIC SM DM_FIX_0 DM_FIX_3 DM_DIAG TM Mh(2.6)_BULK Mh(2.6)_ANAL

* Milbrandt and Yau, 2004 [J. Atmos. Sci., accepted] TESTING IN 3D: The New* Microphysics Scheme Six hydrometeor categories: 2 liquid: cloud and rain 4 frozen: ice, snow, graupel and hail ~50 distinct microphysical processes warm-rain scheme based on Cohard and Pinty (2000a) ice-phase based on Murakami (1990), Ferrier (1994), Meyers et al. (1997), Reisner et al. (1998), etc. diagnosed-a relations added for double-moment version* predictive equations for Zx added for triple-moment version* * Milbrandt and Yau, 2004 [J. Atmos. Sci., accepted]

Canadian MC2 mesoscale model - non-hydrostatic, fully compressible CONTROL SIMULATION MODEL: Canadian MC2 mesoscale model - non-hydrostatic, fully compressible - interfaced with new microphysics scheme (triple-moment version for CONTROL run) CASE: 14 July 2000 “Pine Lake storm”, Alberta, Canada - long-lasting supercell - F3 tornado - golf ball-sized hail

CONTROL SIMULATION: Nesting Strategy 12-km DOMAIN NOTE: No CPS, perturbation, nudging (or anything else) was used to initiate the convection ALBERTA 3-km DOMAIN 1-km DOMAIN 12 18 00 06 UTC 3 km 12 km 14 JULY 15 JULY Model Nesting Times 1 km

CONTROL SIMULATION: Accumulated Total Precipitation mm 40 30 25 20 16 13 10 8 6 4 RADAR: Accumulated Precipitation N 8:00 pm 50 km RADAR 33 mm 1-km CNTR 8:00 pm 1-km SIMULATION: Accumulated TOTAL Precipitation 50 km N 30 25 20 15 10 5 mm

CONTROL SIMULATION: Hail Swath 27 26 25 24 23 22 21 20 19 18 17 16 kg m-2 VIL  27 kg m-2  LARGE HAIL RADAR: Composite of Maximum VIL N 8:00 pm 50 km RADAR 1-km SIMULATION: Accumulated SOLID Precipitation 10 mm 8:00 pm 1-km CNTR 50 km N 10 8 6 4 2 mm

CONTROL SIMULATION: Storm Structure: REFLECTIVITY RADAR: 0030 UTC [6:30 pm] 1-km SIMULATION: 4:30 h [6:30 pm] 40 km 16 km 40 km 16 km dBZ dBZ 65 60 57 54 51 48 45 42 39 36 33 30 Maximum: 60 – 65 dBZ COMPOSITE Maximum: 63.6 dBZ 750 hPa N N

CONTROL SIMULATION: Storm Structure: HOOK ECHO RADAR: 0030 UTC [6:30 pm] 1-km SIMULATION: 4:15 h [6:15 pm] Reflectivity CAPPI (2 km) 10 km Equivalent Reflectivity (750 hPa) 10 km

CONTROL SIMULATION: Hail Sizes How can the maximum hail sizes at the ground be inferred? D * LARGE HAIL log Nh(D) These distributions have identical mean diameters (Dm) D Flux of large of hail (D > D*):

D* = 2 cm OBSERVABLE D* = 3 cm NEGLIGIBLE CONTROL SIMULATION: Simulated Hail Sizes At 5:45 pm (simulation time: 4:45 h): D* = 2 cm Rh*(2 cm) = 5.010-2 m-2 s-1 or, 1 hailstone D  2 cm per 20 m2 every 20 seconds OBSERVABLE D* = 3 cm Rh*(3 cm) = 2.310-4 m-2 s-1 or, 1.4 hailstones D  3 cm per 100 m2 every 1 minute NEGLIGIBLE Walnut-sized (2 – 3 cm) hail was simulated Golf ball-sized (3 – 4 cm) hail was observed MAXIMUM:

ALL RUNS USE DIFFERENT VERSIONS OF THE SAME SCHEME SENSITIVITY EXPERIMENTS List of Runs: 1. TRIPLE-MOMENT (control run) 2. DOUBLE-MOMENT with DIAGNOSED-a 3. DOUBLE-MOMENT with FIXED-a (2 for r ; 0 for c, i, s, g, h) 4. SINGLE-MOMENT (similar parameters as Lin et al. 1983) ALL RUNS USE DIFFERENT VERSIONS OF THE SAME SCHEME

6-h ACCUMLATED TOTAL PRECIPITATION [mm] SENSITIVITY EXPERIMENTS: TOTAL Precipitation 6-h ACCUMLATED TOTAL PRECIPITATION [mm] TRIPLE-MOMENT DOUBLE-MOMENT Diagnosed a 33 34 SINGLE-MOMENT DOUBLE-MOMENT Fixed a 43 28 42 CONTOURS: 5, 10, 20, 30, 40 mm

6-h ACCUMLATED SOLID PRECIPITATION [mm] SENSITIVITY EXPERIMENTS: SOLID Precipitation (HAIL) 6-h ACCUMLATED SOLID PRECIPITATION [mm] TRIPLE-MOMENT DOUBLE-MOMENT Diagnosed a 10 9 9 SINGLE-MOMENT DOUBLE-MOMENT Fixed a 35 25 14 23 34 13 CONTOUR INTERVAL: 2 mm

700 hPa: SENSITIVITY EXPERIMENTS: Equivalent Hail Reflectivity Zeh [dBZ] 700 hPa: Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT DOUBLE-MOMENT Diagnosed a 100 km SINGLE-MOMENT DOUBLE-MOMENT Fixed a

SENSITIVITY EXPERIMENTS: Equivalent Hail Reflectivity, Zeh [dBZ] Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT 63.6 dBZ DOUBLE-MOMENT Diagnosed a 63.6 dBZ SINGLE-MOMENT 68.3 dBZ DOUBLE-MOMENT Fixed a 83.9 dBZ 10 km 0 km 25 km 50 km 75 km 100 km MAXIMUM VALUE

SENSITIVITY EXPERIMENTS: Hail Mass Content, Qh [g m-3] Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT 5.51 g m-3 DOUBLE-MOMENT Diagnosed a 5.58 g m-3 SINGLE-MOMENT 3.71 g m-3 DOUBLE-MOMENT Fixed a 4.91 g m-3 Dashed contour: 0.1 g m-3 MAXIMUM VALUE

SENSITIVITY EXPERIMENTS: Hail Number Concentration log NTh [m-3] Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT 5.18 DOUBLE-MOMENT Diagnosed a 4.07 SINGLE-MOMENT 1.53 DOUBLE-MOMENT Fixed a 5.22 Dashed contour: 1.0 m-3 MAXIMUM VALUE

SENSITIVITY EXPERIMENTS: Mean Hail Diameters, Dmh [mm] Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT 14.9 mm DOUBLE-MOMENT Diagnosed a 11.2 mm SINGLE-MOMENT 6.15 mm DOUBLE-MOMENT Fixed a 67.2 mm MAXIMUM VALUE

SENSITIVITY EXPERIMENTS: Large Hail Concentration, Nh*{1 cm} [m-3] (grape-sized or larger) Local time: 6:30 pm (Simulation time: 4:30 h) TRIPLE-MOMENT 1.03 m-3 DOUBLE-MOMENT Diagnosed a 0.79 m-3 SINGLE-MOMENT 1.76 m-3 DOUBLE-MOMENT Fixed a 0.68 m-3 Dashed contour: 0.01 m-3 MAXIMUM VALUE

SENSITIVITY EXPERIMENTS: Maximum hail sizes (at surface) 3 – 4 cm (Golf ball-sized ) hail was observed [at 5:45 pm, time of maximum hail rate in CONTROL RUN] TRIPLE-MOMENT DOUBLE-MOMENT Diagnosed a 2 – 3 cm (Walnut-sized) 1 – 2 cm (Grape-sized) SINGLE-MOMENT DOUBLE-MOMENT Fixed a 4 – 5 cm (Baseball-sized) 8 – 9 cm (Grapefruit-sized)

CONCLUSIONS    THANK YOU 1. The value of the shape parameter is important in bulk microphysics schemes TRIPLE- MOMENT DOUBLE- Diagnosed a SINGLE- Fixed a    2. For the overall QPF, storm structure, hydrometeor values, and the simulation of hail sizes: THANK YOU

SINGLE-moment bulk scheme (SM): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] ANALYTIC BIN model (ANA): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm]

DOUBLE-moment bulk scheme (FIX0): a = 0 z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] ANALYTIC BIN model (ANA): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm]

DOUBLE-moment bulk scheme (FIX3): a = 3 z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] ANALYTIC BIN model (ANA): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm]

TRIPLE-moment bulk scheme (TM): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] ANALYTIC BIN model (ANA): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm]

DOUBLE-moment bulk scheme (DIAG): a = f(Dm) z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm] ANALYTIC BIN model (ANA): z [km] Q [g m-3] NT [m-3] Ze [dBZ] Dm [mm]