modeling of large-scale edge waves generated by the hurricane landfall
DESCRIPTION
Modeling of Large-Scale Edge Waves Generated by the Hurricane Landfall. Alexander Yankovsky Marine Science Program and Department of Geological Sciences University of South Carolina, USA. 2008 ROMS/TOMS European Workshop. Acknowledgements: National Science Foundation - PowerPoint PPT PresentationTRANSCRIPT
Modeling of Large-Scale Edge Waves Generated by the Hurricane Landfall
Modeling of Large-Scale Edge Waves Generated by the Hurricane Landfall
Alexander Yankovsky
Marine Science Program and Department of Geological Sciences
University of South Carolina, USA
Alexander Yankovsky
Marine Science Program and Department of Geological Sciences
University of South Carolina, USA
2008 ROMS/TOMS European Workshop2008 ROMS/TOMS European Workshop
Acknowledgements:
-National Science Foundation
-US Geological Survey, Florida Integrated Science Center
-Drs. Eduardo Patino, Burl Goree (USGS)
Acknowledgements:
-National Science Foundation
-US Geological Survey, Florida Integrated Science Center
-Drs. Eduardo Patino, Burl Goree (USGS)
15
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25
30
35
40
45
-85 -80 -75 -70 -65 -60 -55 -50 -45
Hurricane Wilma15-25 October 2005
Hurricane
Tropical Storm
Tropical Dep.
Extratropical
Subtr. Storm
Subtr. Dep.
00 UTC Pos/Date
12 UTC Position
Low / Wave
PPP Min. press (mb)
25
24
23
22
21
20
1918
26
1617
882 mb
from: Pasch et al. (2005)
Wilma’s track
Time series of storm surge
Wilma’s landfall
Long waves trapped in the coastal ocean:
- Subinertial coastal trapped waves (σ≤f); propagate with the coast on their right in NH, the effects of Earth’s rotation are crucial.
- Edge waves (σ>f); refraction of long gravity waves, propagate in both directions
ROMS, 2D configurationbc: radiation
bc:
Cha
pman
bc: radiationbc
: w
all
Atmospheric vortex in gradient wind balance
Standard Case:
- Pressure anomaly in the cyclone’s center is 3 hPa (wind is ~ 12 m/s)
- Translation speed of the storm system is 10 m/s eastward
- Quadratic bottom stress, C =10-3;
- f =6.3×10-5 s-1 (26 °N);
- Spatial resolution: Δx = Δy = 2.5 km
Standard case: phase diagram
Temporal and alongshore evolution of free surface at the coast
0)( 222
kgh
f
h
hkf
h
h yyyyy
Linear shallow water equations on f-plane
Boundary conditions:
kfy
0 )( y
)0)0(,0( hy
0yv )( Ly Assume: Q =kf/ω
22
22
2
)]([ kgh
f
h
hQ
h
h
fghQ
ghQ yyyyy
(y=0) (y=L) Qy yyy Q AX=μX
MATLAB EIG routine
Standard case, dispersion diagram of the edge wave modes propagating downstream (solid line) and upstream (dashed line)
Across-shelf structure of edge wave modes
From ROMS
Case B
Us = 5 m/s
Case C
Us = 3 m/s
Us=10 m/s Us=5 m/s Us=3 m/s
Case D
Us = 8.66 m/s
Vs = -5 m/s
Case E
Us = 8.66 m/s
Vs = 5 m/s
Case F: strong wind
ΔP = -20 hPa (max wind ≈ 34 m/s); C = 3×10-3
· Hurricane Wilma’s landfall generated a long-wave pulse traveling downstream (northwestward) along the coast. This wave pulse lasted ~6 hrs and its height was ~1.5 m in the detided sea level.
· Zero-mode edge waves dominate the response. Their structure in the model is very close to the theoretical estimates.
· The wave pulse is identified as an edge wave of large spatial and temporal scales. Numerical calculations show that such waves can be generated by a fast-moving storm crossing the continental shelf at the close-to-normal angle.
Conclusions