Ice-Ice Collisions: An Ice Multiplication Process in Atmospheric Clouds by Vaughan Phillips (Uni. of Hawaii) Jun-Ichi Yano(Meteo France)

Slides:



Advertisements
Similar presentations
Precipitation Chapter 7
Advertisements

AOSC 200 Lesson 8.
URBAN GROWTH AND AEROSOL EFECTS ON CONVECTION OVER HOUSTON Gustavo G. Carrió, William R. Cotton, William Y. Cheng, and Steve M. Saleeby Colorado State.
Detailed vertical structure of orographic precipitation development in cold clouds An illustration of high-resolution airborne mm-wave radar observations.
Warm cloud microstructures
Hallet-Mossop Process as a Mechanism for Ice Multiplication Steven Brown Atmospheric Sciences 5/16/2011.
Part 2. Water in the Atmosphere Chapter 7 Precipitation Processes.
Lecture 13: Precipitation W & H: Sections 6.4 and 6.5.
Q. Why are cloud droplets larger over the ocean?
Impact of surface interaction and cloud seeding on orographic snowfall A downlooking airborne cloud radar view Bart Geerts University of Wyoming Gabor.
Most collide on forward edge Some collide on backside About a million average sized droplets would be required to produce a raindrop! Terminal velocity:
Numerical Simulations of Snowpack Augmentation for Drought Mitigation Studies in the Colorado Rocky Mountains William R. Cotton, Ray McAnelly, and Gustavo.
Chapter 5 Atmospheric Moisture.
Formation of snow and hails. Review of last lecture Forces acting on a cloud/rain droplet. Terminal velocity. How does it change with cloud drop radius?
5. Formation and Growth of Ice Crystals
Chapter 7 – Precipitation Processes
Acknowledgments This research was supported by the DOE Atmospheric Radiation Measurements Program (ARM) and by the PNNL Directed Research and Development.
Precipitation.
Topic #6: Moisture, Clouds and Precipitation Section #3: Cloud Types and Precipitation.
Hurricane Cloud Physics
The effect of the size of CCN on drizzle and rain formation in convective clouds Roelof T. Bruintjes Research Applications Program, National Center for.
In this work we present results of cloud electrification obtained with the RAMS model that includes the process of charge separation between ice particles.
GEF2200 Stordal - based on Durkee 10/11/2015 Relative sizes of cloud droplets and raindrops; r is the radius in micrometers, n the number per liter of.
Why does it rain on us???.  3 cloud properties, 9 ISCCP cloud types  Why do clouds constitute a wildcard for climate change? Competition between greenhouse.
Lightning: Charge Separation Mechanisms, Detection and Applications Kaitlyn Suski May 29, 2009 SIO 209
1. Clouds are made up of: A.Liquid water droplets B.Ice Crystals C.Water Vapor D.A combination of liquid water, ice, and water vapor.
Determining Precipitation Type. Rain (R, RA)- Rain is liquid precipitation that reaches the surface in the form of drops that are greater than 0.5 millimeters.
Why does it rain on us???.
Ice in the Atmosphere W+H 6.5; S+P Ch. 17 Start with some terminology –Warm clouds = T > 0 ºC (= K) –Cold clouds = T < 0 ºC Cold clouds may or may.
Precipitation, Air Masses, and Fronts
Cloud Microphysics Liz Page NWS/COMET Hydromet February 2000.
A study of ice formation by primary nucleation and ice multiplication in shallow precipitating embedded convection T. Choularton 1, I. Crawford 1, C. Dearden.
New proposal as part of the Research Unit: Experimental studies at the Mainz vertical wind tunnel Stephan Borrmann, Subir K. Mitra, Karoline Diehl, Miklós.
How Precipitation Forms: The Bergeron Process pp
NATS 101 Section 13: Lecture 13 Precipitation. Precipitation: Any form of water particles—liquid or solid—that falls from the atmosphere and reaches the.
Chien Wang Massachusetts Institute of Technology A Close Look at the Aerosol-Cloud Interaction in Tropical Deep Convection.
Jason Milbrandt Recherche en Prévision Numérique [RPN] Meteorological Research Division, Environment Canada GEM Workshop, June 12, 2007 Multi-Moment Cloud.
Describing Weather (cont.) Ms. Cervera. Bellringer # 2 Dew Point 1. When does dew form? Why? 2. What do you think dew point indicates?
UT/LS H 2 O validation issues Important issues that remain unresolved:  Establishing the frequency and also temperature dependence of supersaturation.
AOSC 200 Lesson 4. MOISTURE WATER VAPOR CONSTITUTES ONLY A SMALL FRACTION OF THE ATMOSPHERE. VARIES FROM 0 TO 4 PER CENT HOWEVER WATER IS PROBABLY THE.
Earth Science Chapter 18.1 – Water in the Atmosphere
Initiation of precipitation via the ice phase Part I: Microphysical processes Karoline Diehl University of Mainz, Germany Institute of Atmospheric Physics.
COPE PRESENTATION Process Modeling and Ice Nuclei.
1 Detailed Microphysical Model Simulations of Freezing Drizzle Formation Istvan Geresdi Roy Rasmussen University of Pecs, Hungary NCAR Research funded.
Part II: Implementation of a New Snow Parameterization EXPLICIT FORECASTS OF WINTER PRECIPITATION USING AN IMPROVED BULK MICROPHYSICS SCHEME Thompson G.,
Clouds (Condensed PPT)
Types of Precipitation
Production of secondary ice particles and splintering of freezing droplets as a potential mechanism of ice multiplication Annika Lauber, Mona Schätzle,
Review for Exam 2 Fall 2011 Topics on exam: Class Lectures:
Class #25: Friday, March 6 Clouds, fronts, precipitation processes, upper-level waves, and the extratropical cyclone Class #25: Friday, March 6, 2009.
1. Background for Cloud Physics
5. Formation and Growth of Ice Crystals
ATOC 4720 class19 Thunderstorms 1. Growth of clouds droplets in
Article Review Jennie Bukowski ATS Mar-2017
Review of Roesenfeld et al
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Presentation transcript:

Ice-Ice Collisions: An Ice Multiplication Process in Atmospheric Clouds by Vaughan Phillips (Uni. of Hawaii) Jun-Ichi Yano(Meteo France)

Main Message: ice-ice collision can lead to “explosive” ice multiplication zero-dimensional model >1 single parameter:

background: ice nuclei (IN) is Rare: Mixed Phase However: IN # << ice particle # ice multiplication?

ice multiplication (observational evidence): (Hobbs 1969) Ice particle# IN # Ice particle#

background: ice nuclei (IN) is Rare: Mixed Phase However: IN # << ice particle # ice multiplication? Main Message: ice-ice collision can lead to “explosive” ice multiplication along with Hallet- Mossop process

Ice-ice collison breakup : Experiment by Takahashi et al., (1995):

Ice-ice collision-breakup multiplication (nonlinear): r0r0 vTtvTt

Zero-Dimensinoal Model: primary ice generation rate = constant igG c0c0  f = 10min  g = 30min  i = 15min ice+ice collision ~  ice crystal (i), small graupel (g), large graupel (G) ~

lag model : numerical analysis relaxation model : analytical study

relaxation model analysis :

lag model analysis : c-dependence: Ice Enhancement Ratio: IE = n i /n i *

lag model analysis :  g -dependence: Ice Enhancement Ratio: IE = n i /n i *

lag model analysis : with Supercooled Rain Aloft: Ice Enhancement Ratio: IE = n i /n i *

lag model analysis : Hallet-Mossop process: Ice Enhancement Ratio: IE = n i /n i *

saturation -1% supersaturation lag model analysis : water-vapor depletetion (Korolev and Mazin 2007): Ice Enhancement Ratio: IE = n i /n i *

Conclusion The Ice-Ice Collision Ice-Breakup leads to “Nonlinear” Explosive Ice- Multiplication Porcess. Potentially more powerful than Hallete- Mossop process >1 single parameter:

ice multiplication processes: Hallet-Mossop (1974): (-3C)-(-8C): well established (Phillips et al., 2001, 2003, 2005, 2007, 2009) Ice-ice collison breakup (Hobbs&Farber 1972, Vardiman 1978, Takahashi et al., 1995): graupel + (large) graupel (small) graupel + (large) graupel + (small) graupel + supercooled cloud droplets (>24  m) rimed + graupel splinter ice splinter Ice (Ice Crystals) not well studied: established by this Talk

relaxation model analysis :

lag model analysis (numerical): example nini ngng nGnG n i *: without ice multiplication ii gg ff Ice Enhancement Ratio: IE = n i /n i *

?

summary a high IE ratio of 10 4 is attained about an hour af in standard run without supercooled rain the time for an IE ratio to exceed 10 4 is shortened to only 20 min with supercooled raindrops the HM process starts much sooner than mechanical break-up if active inclusion of the response of humidity to explosive ice multiplication yields a maximum IE ratio of the order of about 10 5