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Estimation of wave spectra with SWIM on CFOSAT – illustration on a real case
C. Tison (1), C. Manent(2), T. Amiot(1), V. Enjolras(3), D. Hauser(2), L. Rey(3), P. Castillan(1)
(1) CNES, « Altimetry and Radar » department, France(2) UVSQ, CNRS, LATMOS-IPSL, France(3) Thalès Alenia Space, France
IGARSS’11 – July, 2011 2
Overview of the presentation
■SWIM instrument and measures
■Performance budget SimuSWIM – an end-to-end simulator A real sea state condition Results
IGARSS’11 – July, 2011 3
The CFOSAT mission
■ Status of the program: Conception and Development phase Launch planned end of 2014
■ SWIM Measurement of the oceanic wave properties Real-aperture radar with 6 beams (Ku band)
■ SCAT Measurement of wind sea surface Real-aperture radar (bi polar, Ku band)
■ KuROS Airborne sensor developed by LATMOS Validation of SWIM and SCAT
More on the CFOSAT mission tomorrow – session WE4.T10 Altimetry I
China France Oceanography SATellite
IGARSS’11 – July, 2011 4
SWIM instrument (1/2)
SWIM: Surface Wave Investigation and Monitoring
Ku-band radar (scatterometer)6 beams
IGARSS’11 – July, 2011 5
SWIM instrument (2/2)
Wind sea
Swell Nadir signal SWH and wind speed- Accuracy SWH: max(10% of SWH, 50 cm)-Accuracy wind speed: 2 m/s
10°, 8° and 6° beams wave spectrum- spatial sampling of 70 x 70 Km²- Detectable wave wavelength : λ ~ [70 - 500] m- Azimuth accuracy: 15°- Energy accuracy: 15%
All beams backscattering coefficient profiles:- Absolute accuracy < +/- 1 dB- Relative accuracy (between beams) < +/- 0.1 dB
IGARSS’11 – July, 2011 6
Estimation of wave spectra
Wave topography: ξ(x,y)2),((),( yxTFkkF yx ξ=
Directional wave spectrum F(kx,ky)
Modulation of the backscattering coefficient
),()(2
)),((),( 222 ϕθαπφφ kFkL
XmTFkPy
m ==
Signal modulation
Modulation spectrum Pm
Received power
X∂∂∝ ξ
σδσ
Wave slopesX∂
∂ξ
)(),(σδσφ fXm =
Link slope/signal modulation
IGARSS’11 – July, 2011
Simulations
■Simulations from the sea surface to the estimated signal Input = sea state conditions Output = wave spectrum
computation of backscattered intensity and processing similar to the future ground segment
use SWIM parameters
End-to-end simulation tool: SimuSWIM
320320320320320320Bc (MHz)
2.34.86.88.711.924.3SNR (dB)
2371921446060110Nimp (fixed)
6340-6667 variable
6378-6707 variable
6407-6739variable
2125fixed
2125fixed
2125fixed
PRF (Hz)
37.430.122.531.531.551.8Max integration time (ms)
10°8°6°4°2°0°
IGARSS’11 – July, 2011 8
SimulationsEnd-to-end simulation tool: SimuSWIM
Input spectrum(models, measurements)
Surface computation
Backscattered signal(knowing SWIM
geometry and properties)
At a given azimuth direction:- Computation of the Nimp backscattered
pulses2 options:1. Computation of the Nimp pulses (with
geometrical migrations and noises for each)
2. Computation of one pulse and additions of noise (thermal+speckle) to create the Nimp pulses with central migrations
- Addition of the Nimp signals
Nimp pulses per cycles
IGARSS’11 – July, 2011 9
SimulationsEnd-to-end simulation tool: SimuSWIM
Input spectrum(models, measurements)
Surface computation
Backscattered signal(knowing SWIM
geometry and properties)
Estimated modulation spectrum
Quality criteria
IGARSS’11 – July, 2011 10
Impact of migrations (1/2)
Nimp
Nimp/2
NRER
MR
FR
ΔxMR
Due to satellite advection and antenna rotation: MIGRATIONS range (of each target) different at each impulse
-3 kinds of migration:-Centre migration-Migration along elevation-Migration along wave front
-NB: at the cycle scale, no impact of antenna rotation
Corrected by chirp scalingNon correctable
Two ways of simulation (for computation time constraints):2. With only central migrations and elevation migrations3. With all migrations
IGARSS’11 – July, 2011 11
Impact of migrations (2/2)
(a) Reference 2D modulation spectrum
(b) Estimated 2D modulation spectrum WITHOUT complete migration
(c) Estimated 2D modulation spectrum WITH complete migrationsDirection Wave-
length
Energy
Swell 0°
0°
0%
3%
13% 10%
Wind sea 11°
14°
27% 16%
19% 12%
IGARSS’11 – July, 2011
A real sea state condition: “Prestige case”
■Case of November, 2002 storm in Atlantic ocean Lead to the sinking of the Prestige (oil
tanker)
■Very different conditions during the day00:00: low wind sea + dominant swell06:00: very young wind sea (high
wind) + dominant swell 08:00: mature wind sea + dominant
swell15:00: crossed wind seas (old +
young) Wind sea rotated by about 120°
SpainGalician coast
© B
SA
M/D
ou
an
es f
ran
çai
ses
IGARSS’11 – July, 2011
A real sea state condition: “Prestige case”
IGARSS’11 – July, 2011
A real sea state condition: “Prestige case”
■Available data MFWAM output with ALADIN winds (Météo France models of wind and waves)
2D polar azimuth/frequency height spectrum converted into 2D cartesian wavenumber by bilinear interpolation
Subset of results: 00, 06, 08, 10, 15 UTC (different wind and waves cases)
■Simulation conditions Incidence angle: 10°
Nimp = 237 pulses per cycle ( averaging for noise reduction)
Rotation speed = 5.7 rpm ( 49 cycles / 360°)
IGARSS’11 – July, 2011
Simulation results06:00 UTC
Reference: 2D spectrum from WAM model CFOSAT/SWIM estimation
(simulations from SimuSWIM)
Same detection of swell and wind sea partitionsSmall underestimation
IGARSS’11 – July, 2011
1D modulation spectra
6h UTC
Swell Φ=135° (SE-NW look direction)
Sea wind Φ = 235° (NE-SW look direction)
Φ = angle between satellite track (assumed S-N) and radar look direction
IGARSS’11 – July, 2011
00:00 UTC 06:00 UTC 08:00 UTC 15:00 UTC10:00 UTC
Reference: 2D spectrum from WAM model
CFOSAT/SWIM estimation (simulations from SimuSWIM)
Hs: 6.5 mU: 17.3 m/s
Hs: 6.1 mU: 8.8 m/s
Hs: 5.8 mU: 22.2 m/s
Hs: 5.1 mU: 11.7 m/s
Hs: 6.5 mU: 21.0 m/s
Prestige SOS 14:00 UTC
IGARSS’11 – July, 2011
Performance quality
5%19%7°6%12%3°15h
7%6%11°8%8%0°10h
6%18%11°7%1%0°08h
19%27%11°13%0%0°06h
---4%0%3°00h
EλΦEλΦ
WIND SEASWELL
Estimation errors on wave direction (Φ), wave wavelength (λ) and energy (E):
<15° <10-20% <15%Requirements:
IGARSS’11 – July, 2011
Conclusions
■Simulations of SWIM wave products End-to-end simulations Software with realistic sensor conditions
Accurate results with a large variety of sea state conditions
■Next steps Keep-on the definition of the inversion algorithms
Optimize inversion up to wave spectrum estimation of the transfer function (α)
),()(2
)),((),( 222 ϕθαπφφ kFkL
XmTFkPy
m ==