Ventilation of Tropical Cyclones Brian Tang ATM 741 3/21/16.

Slides:



Advertisements
Similar presentations
Squall Lines Loosely defined: A line of either ordinary cells or supercells of finite length (10- hundreds of km) that may contain a stratiform rain region.
Advertisements

Topic 1: Tropical Cyclone Structure and Structure Change Topic 1.1: Environmental Interactions Rapporteur: Liz Ritchie (U.S.A.) Working Group:Jason Dunion.
mesovortex apex of bow echo Bow Echo: radar-observed features mid-level overhang weak echo notch bookend vortex.
Hurricane Dynamics 101 Roger K. Smith University of Munich.
Tropical Cyclone Intrinsic Variability & Predictability Gregory J. Hakim University of Washington 67th IHC/Tropical Cyclone Research Forum 6 March 2013.
5.6.1 Hurricane : introduction
Rappin et al. (2011) Paper Discussion Patrick Duran 1 of 22 Introduction Asymmetric Env.ConclusionsQuestionsSymmetric Env. The Impact of Outflow Environment.
Hurricane Frances. MODIS view of Hurricane Frances (Note that eye is present but clouds at base of eye make it look cloudy throughout)
Hurricanes and climate ATOC 4720 class22. Hurricanes Hurricanes intense rotational storm that develop in regions of very warm SST (typhoons in western.
Weismann (1992) Weisman, M. L., 1992: The role of convectively generated rear- inflow jets in the evolution of long-lived mesoconvective systems. J. Atmos.
Severe Convection and Mesoscale Convective Systems R. A. Houze Lecture, Summer School on Severe and Convective Weather, Nanjing, 11 July 2011.
Tropical storms and the First Law of Thermodynamics ATMO 435.
Thermodynamic Structure of Tropical Cyclones From Aircraft Reconnaissance Kay Shelton University at Albany/SUNY, Albany, New York.
Mesoscale Convective Systems Robert Houze Department of Atmospheric Sciences University of Washington Nebraska Kansas Oklahoma Arkansas.
USE OF HS3 DATA TO UNDERSTAND THE TROPICAL CYCLONE OUTFLOW LAYER John Molinari, Kristen Corbosiero, Stephanie Stevenson, and Patrick Duran University at.
Section 5: Tropical Cyclones 5.4 Theories for Genesis CISK WISHE Discussion Resources:
Convective-scale diagnostics Rob Rogers NOAA/AOML Hurricane Research Division.
Tropical cyclone intensification Roger Smith Ludwig-Maximilians University of Munich Collaborators: Michael Montgomery, Naval Postgraduate School, Monterey,
+ Effects of Climate Change on Ocean Storms Chloe Mawer.
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.
On the Multi-Intensity Changes of Hurricane Earl (2010) Daniel Nelson, Jung Hoon Shin, and Da-Lin Zhang Department of Atmospheric and Oceanic Science University.
Vertical Structure of the Tropical Troposphere (including the TTL) Ian Folkins Department of Physics and Atmospheric Science Dalhousie University.
Tropical cyclone intensification Roger Smith Ludwig-Maximilians University of Munich Collaborators: Michael Montgomery, Naval Postgraduate School, Monterey,
Sensitivity of Tropical Cyclone Inner-Core Size and Intensity to the Radial Distribution of Surface Entropy Flux Wang, Y., and Xu, 2010: Sensitivity of.
Hurricane structure and intensity change : Effects of wind shear and Air-Sea Interaction M é licie Desflots Rosenstiel School of Marine & Atmospheric Science.
Sensitivity of Simulated Tropical Cyclone Structure and Intensity to Horizontal Resolution Speaker: Wang, Jian-Cyuan Advisor: Prof. Yang, Ming-Jen Megan.
Hurricane Superintensity John Persing and Michael Montgomery JAS, 1 October 2003 Kristen Corbosiero AT April 2007.
Jian-Wen Bao Christopher W. Fairall Sara A. Michelson Laura Bianco NOAA/ESRL/Physical Sciences Division in collaboration with N. Surgi, Y. Kwon and V.
Work summarized in collaboration with: Roger Smith, Jun Zhang, S. Braun, Jason Dunion On the dynamics of secondary eyewall formation in Hurricane Edouard.
Energy Production, Frictional Dissipation, and Maximum Intensity of a Numerically Simulated Tropical Cyclone 4/ 蘇炯瑞 Wang, Y., and J. Xu, 2010: Energy.
Richard Rotunno NCAR *Based on:
Severe Convection and Mesoscale Convective Systems R. A. Houze Lecture, Indian Institute of Tropical Meteorology, Pune, 5 August 2010.
How Small-Scale Turbulence Sets the Amplitude and Structure of Tropical Cyclones Kerry Emanuel PAOC.
High-Resolution Simulation of Hurricane Bonnie (1998). Part II: Water Budget Braun, S. A., 2006: High-Resolution Simulation of Hurricane Bonnie (1998).
Tropical Cyclone Structure
Three Lectures on Tropical Cyclones Kerry Emanuel Massachusetts Institute of Technology Spring School on Fluid Mechanics of Environmental Hazards.
TC Lifecycle and Intensity Changes Part III: Dissipation / Transition
The Centre for Australian Weather and Climate Research A partnership between CSIRO and the Bureau of Meteorology The Tropical Cyclone Boundary Layer 4:
How Do Outer Spiral Rainband Affect Tropical Cyclone Structure and Intensity? The working hypothesis is based on the fact that the outer rainbands are.
Tropical Cyclones: Steady State Physics. Energy Production.
Overview of Tropical Cyclones AOS 453 April 2004 J. P. Kossin CIMSS/UW-Madison.
TropicalM. D. Eastin TC Lifecycle and Intensity Changes Part I: Genesis Hurricane Katrina (2005) August
Hurricane Physics Kerry Emanuel Massachusetts Institute of Technology.
High-Resolution Simulation of Hurricane Bonnie (1998). Part II: Water Budget SCOTT A. BRAUN J. Atmos. Sci., 63,
Sensitivity of Tropical Cyclone Intensity to Ventilation in an Axisymmetric Model Brian Tang, and Kerry Emanuel J. Atmos. Sci., 69, 2394–2413.
Idealized Tropical Cyclone Structure. Tropical Cyclone Extension of the Warm Core middle –level vortex to the surface. Inducement of Ekman pumping Non-linear.
Convective Oscillations in a Strongly Sheared Tropical Storm Jaclyn Frank and John Molinari The University at Albany, SUNY.
Microphysical-dynamical interactions in an idealized tropical cyclone simulation Stephen R. Herbener and William R. Cotton Colorado State University, Fort.
Shuyi S. Chen, Robert A. Houze Bradley Smull, David Nolan, Wen-Chau Lee Frank Marks, and Robert Rogers Observational and Modeling Study of Hurricane Rainbands.
The Centre for Australian Weather and Climate Research A partnership between CSIRO and the Bureau of Meteorology The Tropical Cyclone Boundary Layer 2:
A Lagrangian Trajectory View on Transport and Mixing Processes between the Eye, Eyewall, and Environment Using a High-Resolution Simulation of Hurricane.
Evolution of Hurricane Isabel’s (2003) Vortex Structure and Intensity
Mesoscale Applications for Microscale Model?
Rosenstial School of Marine and Atmospheric Science
Yumin Moon & David S. Nolan (2014)
NOAA Intensity Forecasting Experiment (IFEX)
Conceptual Models of Tropical Cyclone Structures
Tropical Cyclone Intensity Change
Spiral Rainbands in a Numerical Simulation of Hurricane Bill (2009)
Tropical Cyclone Structure
Bell, M. M. , M. T. Montgomery, and W. -C
台风的暖心结构与强度变化(1) 储可宽 组会.
Comparison of secondary eyewall and principal rainband in Hurricane Rita (2005) Not a modeling study Several theories out there for secondary eyewall formation.
Tong Zhu and Da-Lin Zhang
Impacts of Air-Sea Interaction on Tropical Cyclone Track and Intensity
A Multiscale Numerical Study of Hurricane Andrew (1992)
Scott A. Braun, 2002: Mon. Wea. Rev.,130,
GEORGE H. BRYAN and RICHARD ROTUNNO 2009, J. Atmos. Sci., 66,
Presentation transcript:

Ventilation of Tropical Cyclones Brian Tang ATM 741 3/21/16

Zeng et al. (2008) Tropical cyclone intensity distribution tends to smaller values as vertical wind shear (VWS) increases.

One possible mechanism by which VWS weakens TCs is ventilation. Ventilation is the inward flux of low-entropy (θ e ) air into the inner core of a TC or the outward flux of high-entropy (θ e ) air out of the inner core of a TC. A B AB >360 K <340 K θeθe Houze (2010)

Weakening the radial gradient of entropy causes the TC intensity to decrease. Thermal wind equation for an axisymmetric, balanced vortex (Emanuel 1986, Montgomery et al. 2006, Bryan and Rotunno 2009) V g,max = maximum gradient wind M = angular momentum (using gradient wind) T b -T o = temperature difference b/t top of boundary layer and outflow layer ds/dM = entropy gradient

θ ʹ + Gray (1968) Frank and Ritchie (2001) Wong and Chan (2004) Kwon and Frank (2005) Environmental flow Upper-level warm core mixed outward. TC weakens from the top down.

time (h) Frank and Ritchie (2001) K m s −1 “The level of maximum outward eddy flux descends with time, and the storm weakens throughout this period.”

Simpson and Riehl (1958) Cram et al. (2007) Tang and Emanuel (2010, 2012) low entropy Environmental flow Low-entropy parcels mixed directly into mid-level eyewall.

Storm-relative flow acts as a “constraint on the hurricane heat engine” (Simpson and Riehl 1958). Back trajectories in a simulation of a sheared TC indicate entrainment of environmental parcels, causing a ~1K decrease in eyewall θ e (Cram et al. 2007).

Powell (1990) Riemer et al. (2010, 2013) Zhang et al. (2013) low entropy Environmental flow Downdrafts flush low entropy air down into boundary layer.

z=1.5 km K m s −1 Riemer et al. (2013)

Tang and Emanuel (2012)

ASPECH experiments with parameterized ventilation Entropy and Ventilation J kg -1 K -1 Tang and Emanuel (2012)

H03H06H09H12H15 3 km6 km9 km12 km15 km Low-level and mid-level ventilation most harmful to TC

Ventilation is a hypothesized thermodynamic constraint on TCs. Some open questions… How does ventilation occur, i.e. what aspects of the TC structure interacting the with environmental VWS cause the ventilation (VRWs, quasi-mode, rainbands)? Does ventilation affect TC convection through entrainment or through the production of downdrafts and cold pools? Does the ventilation “flavor” change depending on the shape of the vertical wind shear profile or the TC structure/size/intensity?