Title: Impacts of AirSea Interaction on Tropical Cyclone Track and Intensity
1Impacts of Air-Sea Interaction on Tropical
Cyclone Track and Intensity
- Liguang Wu, Bin Wang, and Scott A. Braun
- Submitted to Mon. Wea. Rev.
- June 2004
2Introduction
- A tropical cyclone (TC) develops and maintains
itself by drawing its primary energy from the
underlying ocean surface. - The surface wind stress associated with a TC can
generate strong turbulent mixing, deepening of
the ocean mixed layer (ML) and entrainment of
cooler water to the surface that can lead to
significant SST decreace.
3Introduction
- Khain and Ginis (1991) found that westward-moving
(eastward-moving) TCs in coupled experiments were
displayed farther to the south (north) than in
the corresponding experiments without air-sea
interaction. - They attributed these track differences to
asymmetric precipitation patterns which were
shifted azimuthally because of air-sea
interaction.
4Model and experimental design
- Hurricane model is designed by Wang (1998).
- Grid size 25km.
- 16 vertical layers.
- Two and one half layer ocean model is developed
by Wang et al. (1995). - The SST and wind stress are passed between the
hurricane and ocean models every 3 minutes.
5Modified ocean model for TC simulation
- The Kraus-Turner scheme to parameterize the
vertical turbulent mixing (entrainment) is
replaced by the Deardorffs scheme to include the
important shear instability. - The downward heat flux decreases exponentially in
the mixed layer and the turbulent momentum and
heat fluxes are not allowed to penetrate below
the ML base in the modified ocean model.
6Modified ocean model for TC simulation
- The vertical temperature gradient in the
entrainment layer is proportional to the mean
vertical temperature gradient in the thermocline
layer.
7Model and experimental design
The maximum wind (Vm) is 25 ms-1 at rm100 km. b
is set to 0.5
8Ocean response in the coupled model (E2C)
Quasi-steady state
1.2ms-1
1.1ms-1
Maximum current speeds
3.5oC
Minimum ML temperature
4
996h ocean responses in the coupled experiment of
E2 (E2C)
rightward bias
- SST anomaly
- ML depth anomaly
- entrainment rate
- thermocline depth anomaly
- currents in the ML
- currents in the thermocline layer
Function of
1.Wind stress
2.Velocity shear at the base of ML 3.Convective
overturning due to the surface buoyancy fluxes
4
10Time series of the maximum wind speed and minimum
central pressure in experiments E2, E1 and E3.
? fixed SST ? asymmetric SST ? coupled
symmetric SST
12ms-1
14ms-1
10ms-1
24mb
18mb
32mb
11Decomposition of the SST anomalies at 96 h
resulting from hurricane-ocean interaction in the
coupled experiment of E2 (E2C)
(a) symmetric component
(b) asymmetric component
12(a) The lowest-level asymmetric wind field in the
fixed SST experiment of E2 (E2F).
(b) The wind difference between the asymmetric
forcing (E2A) and fixed SST (E2F) experiments of
E2 at 96 h.
13TC tracks in the fixed SST (dashed) and coupled
(solid) experiments for (a) E1, (b) E2, (c) E3,
(d) B2, (e) B1, and (f) B3.
ß-effect
14- Rainfall rate in
- the fixed SST
- asymmetric forcing
- symmetric forcing
- experiments of E1
15TC tracks in the fixed (solid circles), symmetric
(open squares) and asymmetric (open circles) SST
experiments.
16Rainfall rate of E2.
17Rainfall rate of E3.
18Conclusions
- The coupled model can reasonably produce the
major features of the ocean responses to moving
TC forcing.
ML deepening, SST cooling, ML
and thermocline layer currents - The influence of the asymmetric anomalies is
insignificant while the resulting symmetric
cooling plays a decisive role in the weakening of
TC intensity.
19Conclusions
- The symmetric and asymmetric SST anomalies modify
the asymmetry of the diabatic heating with
respect to the TC center, thus affecting TC
motion. - When the vortex strength is relatively weak
(strong), a TC in the coupled model moves to the
north (south) of the TC in the corresponding
fixed SST experiments.
20THANK YOU
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