Maine Core Service Zoom on HF correctionsgodae-data/OceanView/Events/COSS... · 2019-03-01 ·...
Transcript of Maine Core Service Zoom on HF correctionsgodae-data/OceanView/Events/COSS... · 2019-03-01 ·...
Maine Core Service
Zoom on HF corrections
Maine Core Service
•Ocean tide (water column deformation due to lunar/solar attraction) •Earth tide (Earth layer deformation due to lunar/solar attraction) •Polar tide (water column deformation due to the movement of the pole of rotation) + Load effect They are deduced from numerical models (GOT4.10, FES2014)
Ex: 1 year of the Jason 1 mission (2004 : cycles 73 to 109).
GOT00.2 correction mean GOT00.2 correction variance
-5cm 5 cm 0.26 m²
Tide Corrections
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Sampling of a temporal signal of period T
With a sampling period of T0, we cannot reconstruct a periodic signal of period lower than 2T0 (Nyquist period)
If T0 > T/2 → Ta is the aliased period
T
T 0
T a
Time
Amplitude
Aliasing phenomena
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T/P-Jason altimeter : 10 days sampling (9,9156 days exactly)
Nyquist period = 20 days for TP/Jason
Signal theory aliasing of all signals T < 20 days
High frequency spectrum (T < 20 days) is aliased in the low frequency band (T > 20 days)
Tidal aliasing in altimeter measurement
T/P; Jason GFO ENVISAT; ERS-
2
9,9156 17,0505 35Nom de
Darwin
Période (jours) Aliasing (jours) Aliasing (jours) Aliasing (jours)
On
de
s
lon
gu
es
pé
rio
de
s Ssa 182,62109 182,621095 182,621095 182,621095Mm 27,554551 27,5545507 44,727399 129,530031Mf 13,660791 36,1676995 68,7148383 79,9227517
On
de
s d
iru
ne
s Q1 1,1195149 69,364499 74,0495979 132,806118O1 1,0758059 45,7141825 112,953531 75,0669737P1 1,0027454 88,8908701 4466,66574 365,24219K1
L0,9972696 173,192245 175,447852 365,24219
K1S
0,9972696 173,192245 175,447852 365,24219
On
de
s se
mi
diu
rne
s
N2 0,5274312 49,5281768 52,0720468 97,3929566M2 0,5175251 62,1074853 317,108085 94,4864493S2 0,5 58,7417062 168,816832 #DIV/0!K2
S0,4986348 86,5961223 87,7239259 182,621095
pollution of climatic/mesoscale
signals estimations
need to remove tides from
altimeter measurements = need
accurate global tide models !
Maine Core Service
T/P-Jason altimeter : 10 days sampling (9,9156 days exactly)
Nyquist period = 20 days for TP/Jason
Signal theory aliasing of all signals T < 20 days
High frequency spectrum (T < 20 days) is aliased in the low frequency band (T > 20 days)
Tidal aliasing in altimeter measurement
► pollution of climatic/mesoscale signals estimations ► remove tides from altimeter measurements ► need accurate tide models
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2 types of Global models Empirical models
exclusively based on observations
Estimation of altimeter residuals preliminary corrected with FES model
Examples= GOT (R. Ray), EOT (Bosch et al.), DTU (Andersen et al.) …
Hydrodynamic models with/without data assimilation
Hydrodynamic equations = shallow water equations
2D models at present time
3D models just start to be developed mostly for SWOT issues (small scales, internal tides …)
Examples= FES , TPXO
Tidal models
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Regular grid /finite difference discretization: GOT, DTU, TPXO
Finite elements discretization : FES, TUGO models
Resolution of Tidal models
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Centimetric in deep ocean
Thanks to the use of altimeter measurements
Thanks to the modeling of the barotropic tide dissipation via internal tides generation (FES)
Stronger errors in coastal regions
> 10 cm rms
Complex bathymetry (modelisation errors)
Strong non linear interaction areas = many non linear tides arise
These non linear waves are not/a few modeled (omission and modeling error)
Accuracy of Tidal models
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9
Performances vs tide gauge databases
– Coastal = BODC + WOCE + R. Ray database (shallow_fes09) + SONEL
– Shelf = GLOUP (shelf) + ROSAME
– Deep = ACCLAIM + DART + GLOUP (open ocean)
Coastal Shelf Deep
Complex
differences
(cm)
K1 M2
Accuracy of tidal models
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To get more accurate tidal solutions locally, one can develop regional tidal models
Improved bathymetry from regional databases (hydrographic services …)
Improved coastlines
Higher resolution mesh more adapted to shallow water/coastal scales
OBC from global ocean models
Regional tidal models
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Example on NEA region
Grid cells from 1 km to 20 km
Pairaud et al. 2008
Regional tidal models
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Example of Amazone estuary
(Le Bars et al. 2010)
Regional tidal models
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The ocean static response to atmospheric pressure forcing (inverse barometer 1 mbar ↔1 cm) [ Low frequency (> 20 days) signal only]
Pressure anomalies P’ are calculated using pressure estimates from the ECMWF model P’=Pressure-<P> where <P> is the spatial average (over the ocean) of the instantaneous pressure map (every 6 hours).
Motivation: known, static response + necessity to remove this signal before mapping
Barotropic response to pressure and wind from the MOG2D model [High frequency (<20 days) signal only]
Motivation : avoid high frequency oceanic signal to be aliased in the final products.
Dynamic Atmospheric Correction (DAC)
DAC = IB_LF + MOG2D_HF
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Limits: The high frequency baroclinic signals are not removed. The 20 days cut-off length corresponds to the JASON/TOPEX aliasing period. For ERS/ENVISAT, the cut-off length should be 70 days.
Ex: 1 year of the Jason 1 mission (2004 : cycles 73 to 109).
MOG2D-HR correction mean MOG2D-HRcorrection variance
-0.12 m 0.15 m 0.012 m²
DAC = IB_LF + MOG2D_HF
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MOG2D model
• Barotropic model, « time-stepping », non linear (Lynch and Gray,
1979; Greenberg and Lyard; Carrère and Lyard 2003)
• Shallow water equations
Movement:
Continuity:
temporal
derivation
Coriolis
Advectio
n Bottom
friction
horizontal
viscosity Forcing Pressur
e effect
Dissipatio
n
DhEhFhuhghuhfuuhtuh
.
21
0
uh
t
h
The MOG2D model
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Finite elements discretization • Allows increasing resolution in all regions of interest: shallow waters, ocean ridges, slope of continental shelves, small straits …
• at a reasonable computation cost
Finite elements grid used for operational correction: • ~240 000 nodes
• cell size from 150 km to 10 km
MOG2D model The MOG2D model
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MOG2D model
• Meteorological forcing
• ECMWF operational analysis
• Spatial resolution from 1° until 1/8° today
• Atmospheric pressure and 10 m wind speed
• 6-hours temporal resolution → aliasing problem for S2 atmospheric tide …
• At present time S1 and S2 atmospheric signals are removed with a
climatology and then the corrected atmospheric fields are injected in the
model
→ DAC and tide corrections are consistent at S1S2 freq.
The MOG2D model
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Impact of the Dynamic Atmospheric correction • Comparison with tidal gauges database (GLOSS):
• DAC correction is better than IB on most regions. •Weak improvement in the equatorial regions (ocean response is mostly barolinic) • DAC in shallow water regions -> strong reduction of the TG residual variance • not so good in some regions, mostly around Indonesia.
Discussion Which dynamics would/do you want to validate with altimetry or assimilate in your models?
Equivalent modeled SLA: how to compute it to be consistent with altimetry in regional/coastal seas?
For assimilation, is it possible to manage the low-frequency altimetry time sampling of the HF phenomena?
Locally replace the global DAC by a regional DAC, extracted from your 3D system ?