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Hurricanes and Climate

Change









Kerry Emanuel

Massachusetts Institute of Technology

Program





• Effect of climate change on hurricane activity



• Hurricanes in the climate system

Effect of Climate Change on

Hurricanes

No Obvious Trend in Global TC Frequency, 1970-2006









Data Sources: NOAA/TPC and NAVY/JTWC

Better Intensity Metric:



The Power Dissipation Index





PDI   V dt 3

max

0



A measure of the total frictional dissipation of kinetic

energy in the hurricane boundary layer over the

lifetime of the storm

Power Dissipation Based on 3 Data Sets for

the Western North Pacific

(smoothed with a 1-3-4-3-1 filter)





Years

included:

1949-2004









aircraft recon







Data Sources: NAVY/JTWC, Japan Meteorological Agency, UKMO/HADSST1, Jim Kossin, U. Wisconsin

Atlantic Storm Maximum Power Dissipation

(Smoothed with a 1-3-4-3-1 filter)









Years

Power Dissipation Index (PDI)









included:

1870-2006









Data Source: NOAA/TPC

Atlantic Sea Surface Temperatures and

Storm Max Power Dissiaption

(Smoothed with a 1-3-4-3-1 filter)



Years

included:

Power Dissipation Index (PDI)









1870-2006









Scaled Temperature

Data Sources: NOAA/TPC, UKMO/HADSST1

Energy Production

Distribution of Entropy in Hurricane Inez, 1966









Source: Hawkins and Imbembo, 1976

Theoretical Upper Bound on

Hurricane Maximum Wind Speed:

Surface

temperature





C T T  

|V pot |2 k s o  k *k 

C T  0 

D o  

Ratio of Outflow Air-sea enthalpy

exchange temperature disequilibrium

coefficients of

enthalpy and

momentum

Heat Engine Theory Predicts

Maximum Hurricane Winds









MPH

Combine with Ocean Surface Energy

Balance

Net outgoing radiation

Sea Surface

Temperature Incoming solar Ocean mixed layer

radiation entrainment





Ts  To F  F  Fentrain

V 2



CD  | Vs |

pot

To

Temperature at top of storm Surface Trade Wind speed







Derived by combining potential intensity expression with ocean

surface energy balance

Observed Tropical Atlantic Potential Intensity









Data Sources: NCAR/NCEP re-analysis with pre-1979 bias correction, UKMO/HADSST1

What is Causing Changes in

Tropical Atlantic Sea Surface

Temperature?

10-year Running Average of Aug-Oct NH Surface T and

MDR SST

Tropical Atlantic SST(blue), Global Mean Surface

Temperature (red),

Aerosol Forcing (aqua)





Global mean surface temperature









Tropical Atlantic sea surface temperature





Sulfate aersol radiative forcing







Mann, M. E., and K. A. Emanuel, 2006. Atlantic hurricane trends linked to climate change. EOS, 87, 233-244.

Best Fit Linear Combination of Global Warming

and Aerosol Forcing (red) versus Tropical Atlantic

SST (blue)



Tropical Atlantic sea surface temperature









Global Surface T + Aerosol Forcing









Mann, M. E., and K. A. Emanuel, 2006. Atlantic hurricane trends linked to climate change. EOS, 87, 233-244.

Pushing Back the Record of

Tropical Cyclone Activity:



Paleotempestology

Paleotempestology

barrier beach

upland

overwash fan

backbarrier marsh

a) lagoon









barrier beach

upland

overwash fan

backbarrier marsh

b) lagoon







terminal lobes

flood tidal delta







Source: Jeff Donnelly, WHOI

Source: Jeff Donnelly, Jon Woodruff,

Phil Lane; WHOI

Source: Jeff Donnelly, Jon Woodruff, Phil Lane; WHOI

Source: Jeff Donnelly, Jon Woodruff, Phil Lane; WHOI

Projecting into the Future:

Downscaling from Global

Climate Models

Today’s global climate

models are far too coarse to

simulate tropical cyclones

Our Approach

• Step 1: Randomly seed ocean basins with weak

(25 kt) warm-core vortices



• Step 2: Determine tracks of candidate storms

using a beta-and-advection model



• Step 3: Run a deterministic coupled tropical

cyclone intensity model along each synthetic

track, discarding all storms that fail to achieve

winds of at least 35 kts



• Step 4: Assess risk using statistics of surviving

events

Synthetic Track Generation,

Using Synthetic Wind Time Series



• Postulate that TCs move with vertically averaged

environmental flow plus a “beta drift” correction

(Beta and Advection Model, or “BAMS”)



• Approximate “vertically averaged” by weighted

mean of 850 and 250 hPa flow

Synthetic wind time series



• Monthly mean, variances and co-

variances from NCEP re-analysis data



• Synthetic time series constrained to have

the correct mean, variance, co-variances

and an  power series

3

Track:



Vtrack   V850  1    V250  V ,

Empirically determined constants:



  0.8,

1

u  0 ms ,

1

v  2.5 ms

Tropical Cyclone Intensity

• Run coupled deterministic model (CHIPS,

Emanuel et al., 2004) along each track

• Use monthly mean potential intensity,

ocean mixed layer depth, and sub-mixed

layer thermal stratification

• Use shear from synthetic wind time series

• Initial intensity specified as 12 ms 1

• Tracks terminated when v < 17 ms 1

Example: 200 Synthetic Tracks

6-hour zonal displacements in region bounded by

10o and 30o N latitude, and 80o and 30o W

longitude, using only post-1970 hurricane data

Present Climate: Spatial

Distribution of Genesis Points



Observed









Synthetic

Calibration





• Absolute genesis frequency calibrated

to North Atlantic during the period

1980-2005

Genesis rates

Seasonal Cycles









Atlantic

Seasonal Cycles









Western North Pacific

Cumulative Distribution of Storm Lifetime

Peak Wind Speed, with Sample of 2946

Synthetic Tracks

Atlantic ENSO Influence

Year by Year Comparison with Best Track

and with Knutson et al., 2007

Simulated vs. Observed Power Dissipation Trends, 1980-2006

Now Use Daily Output from IPCC

Models to Derive Wind

Statistics, Thermodynamic State

Needed by Synthetic Track

Technique

Compare two simulations each

from 7 IPCC models:



1. Last 20 years of 20th century

simulations



2. Years 2180-2200 of IPCC

Scenario A1b (CO2 stabilized at

720 ppm)

Model Institution Atmospheric Designation in this Potential

Resolution paper Intensity

Multiplicative

Factor

Community National Center for T85, 26 levels CCSM3 1.2

Climate System Atmospheric Research

Model, 3.0

CNRM-CM3 Centre National de T63, 45 levels CNRM 1.15

Recherches

Météorologiques, Météo-

France

CSIRO-Mk3.0 Scientific and Research T63, 18 levels CSIRO 1.2

Organization

ECHAM5 Max Planck Institution T63, 31 levels ECHAM 0.92

GFDL-CM2.0 NOAA Geophysical Fluid 2.5o X 2.5 o , 24 GFDL 1.04

Dynamics Laboratory levels





MIROC3.2 CCSR/NIES/FRCGC, Japan T42, 20 levels MIRO 1.07



mri_cgcm2.3.2a Meteorological Research T42, 30 levels MRI 0.97

Institute,

Genesis Distributions

Basin-Wide Percentage Change

in Power Dissipation

Basin-Wide Percentage Change

in Storm Frequency

7 Model Consensus Change in

Storm Frequency

Why does frequency decrease?



sm  sb

Critical control parameter in m  * ,

CHIPS: s0  sb

Lv q *

sm  sb  sm  s*  (H  1)  Rv Hq *ln H,

T



Entropy difference between boundary layer

and middle troposphere increases with

temperature at constant relative humidity

Change in Frequency when T held constant in m

Feedback of Global Tropical

Cyclone Activity on the

Climate System

The wake of Hurricane Emily (July 2005).









Hurricane Dennis

(one week earlier)









Source: Rob Korty, CalTech

Direct mixing by tropical cyclones









Emanuel (2001) estimated global rate of heat input as



1.4 X 1015 Watts



Source: Rob Korty, CalTech

Response of Ocean to Point Mixing:





Scott, J. R. and J.

Marotzke, 2002: The

location of diapycnal

mixing and the

meridional

overturning

circulation. J. Phys.

Ocean., 32, 3578–

3595

TC Mixing May Induce Much or Most of the

Observed Poleward Heat Flux by the Oceans









Trenberth and Caron, 2001

Results from EPIC 2001

50

Raymond et al. (2004) report that

background mixing is essentially zero

in the tropical eastern Pacific.

100





“…motions below the thermocline

were very weak, but they

200 intensified…as energy from a strong

storm worked its way downward. The

accompanying mixing accounted for

most of what little mixing there was

between depths of 100-200 m. Mixing

in the thermocline…appears to

respond mostly to wind stress.

September 2001, 10oN, 95oW Slide courtesy of Rob Korty, CalTech

“…the strongest atmospheric

Diffusivity Estimated from Analysis of ERA-40

Wake Recoveries









Figure courtesy of Ron Sriver and Matt Huber, Purdue University

Linear trend (1955–2003)

of the zonally integrated

heat content of the world

ocean by one-degree

latitude belts for 100-m

thick layers. Source:

Levitus et al., 2005

TC-Mixing may explain

difference between

observed and modeled

ocean warming







Zonally averaged

temperature trend due

to global warming in a

coupled climate model.

TC-Mixing may be Crucial for High-Latitude Warmth

and Low-Latitude Moderation During Warm Climates,

such as that of the Eocene

Interactive TC-Mixing Moderates Tropical Warming and

Amplifies High-Latitude Warming in Coupled Climate Models

DSST: elevated mixing to 360 meters – uniform









10 x CO2 in both experiments

Source: Rob Korty, CalTech

Multiple Equilibria and Hysteresis in a Two-Column

Coupled Model (Emanuel, JGR, 2002)









SS

T









Climate Forcing

Summary:



• Tropical cyclones are sensitive to the

climate state



• Observations together with detailed

modeling suggest that TC power

dissipation increases by ~65% for a

10% increase in potential intensity

• Storm-induced mixing of the upper tropical

ocean may be the principal driver of the

ocean’s thermohaline circulation



• Increased TC power dissipation in a warming

climate will drive a larger poleward heat flux

by the oceans, tempering tropical warming

but amplifying the warming of middle and

high latitudes

• This feedback between TCs and ocean heat

flux is not included in any current climate

model; its inclusion may change our

understanding of climate dynamics and our

predictions of the earth’s response to

increased greenhouse gases

Transects of SSH

anomalies from passage

of Hurricane Edouard,

which passed through

transect on Day 239.

Scale of anomlies is 10

cm. (Analysis and figure

courtesy of Peter

Huybers.) Height rise

implies net heat input of

2 X 1021 J.

Variations in Solar Output (IPCC, 2007)

Variation with Time of Natural Climate Forcings:

Comparing 1980-1990 (quiet) to

1995-2005 (active)



104-156 HURDAT tracks 1000 Synthetic tracks









Cumulative distributions of storm lifetime maximum wind

Sensitivity to Shear and Potential

Intensity

Examples of Annual Cycles of Storm

Counts by Month

ATLANTIC









NCAR CCSM3 GFDL CM2.0

Examples of Annual Cycles of Storm

Counts by Month

Western North Pacific









NCAR CCSM3 GFDL CM2.0

Examples of Shifts in Hurricane Track

Density (GFDL CM2.0)









1980-1999 2180-2199

Examples of Shifts in Hurricane Track

Density (GFDL CM2.0)









1980-1999 2180-2199


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