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E. Schrama TU Delft, DEOS e-mail: schrama@geo.tudelft.nl
Error characteristics estimated from CHAMP, GRACE and GOCE derived geoids and from altimetry derived mean dynamic topography E. Schrama TU Delft, DEOS
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Contents Static Gravity Mean circulation inversion problem
Satellite altimetry Temporal Gravity Conclusions
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Static gravity Existing gravity field solutions New gravity missions
Gravity mission performance Cumulative geoid errors Characteristics of errors
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Existing gravity solutions
Satellite geodesy Range/Doppler observations Model/observe non-conservative accerations large linear equations solvers Sensitivity in lower degrees, resonances Physical geodesy Terrestrial gravity data, altimetric g Relative local geoid improvement wrt global models Surface integral relations Sensitivity at short wavelengths Quality determined by: data noise, coverage, combination
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New gravity missions Measuring (rather than modeling) non-conservative forces (CHAMP concept) Low-low satellite to satellite tracking (GRACE concept) Observation of differential accelerations in orbit: (GOCE concept) New gravity surveys (airborne gravity projects)
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Gravity mission performance
Bouman & Visser
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Cumulative geoid errors
SID 2000 report T = 1 year
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Characteristics of errors
All calculations so far considered geoid errors to by isotropic and homogeneous. We only considered commission errors, and did not average spatially (beta operator) In reality there is only one static gravity field Data subset solution Tailored cases. Optimal data combination is a non-trivial problem. The temporal gravity field is an error source for GOCE.
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EGM96 geoid error map Lemoine et al
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Mean Circulation Hydrographic inversion Dynamic topography examples
density gradients and tracer properties geostrophic balance Dynamic topography examples Hydrography Satellite Altimetry
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Hydrographic inversion
thermal wind equations conservation tracers geostrophic balance
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Dynamic Topography from hydrographic inversion
Le Grand,1998
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Dynamic topography from altimetry
JPL web site
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Satellite Altimetry System accuracy Averaging the mean sea level
Mesoscale variability Gulf stream wall detection Sampling characteristics Correlated Noise Correlated Signals
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System accuracy definition of the reference frame (?)
orbits (Laser+Doris, GPS, Altimeter) ( cm) accuracy/stability of the instrument (5 mm) accuracy of environmental corrections (troposphere, ionosphere, EM-bias) ( 1.5 cm ) accuracy of geophysical corrections ( 3 cm ) tides (ocean, earth, load, pole), inverse barometer Net system accuracy: 4-5 cm for T/P
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Averaging the mean sea level
GOCE: 12 months, GRACE: 60 months. White noise fades out as a sqrt(N) process If you had 300 T/P cycles then 5 cm r.m.s. goes down to 0.3 cm 30 cm r.m.s. goes down to 1.7 cm Spatial averaging helps to reduce this error. Yet we can’t average further than the required resolution of the geoid.
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Mesoscale variability map
JPL web site
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Gulf stream wall detection
Lillibridge et al
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Gulfstream T/P in COFS model
Lillibridge et al
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Gulfstream T/P + ERS2 in COFS
Lillibridge et al
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Infrared Gulfstream Lillibridge et al
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Gulf stream velocity (ERS-2)
DEOS (Vossepoel?)
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Sampling the sea level Gravity mapping orbits Repeat track orbits
Sun synchronous Frozen orbits Repeat length vs intertrack spacing
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T/P sampling 119 121 120 122
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Topex/Poseidon groundtrack
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Examples systematic errors
Errors that are definitely not white are: reference frame stability definition issues instrument biases geographical correlated orbit errors tides aliasing inverse barometer
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Examples of time correlated SLA
Equatorial Rossby and Kelvin waves ENSO Annual behavior Tides Internal tides
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Equatorial Kelvin and Rossby waves
Equator: 2.8 m/s 20 N: 8.5 cm/s
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El Niño
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Four seasons (Annual cycle)
JPL web site
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M2 tide
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Internal tides Hawaiian Island chain is formed on a sub-surface ridge
wave hits ridge (perpendicular) energy radiates away from ridge
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Temporal gravity Current situation Overview processes Challenges
Separation Signals/Noise
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Current situation Currently observed in the lower degree and orders
Signal approximately at the 1e-10 level Traditional observations by SLR: Lageos I + II, Stella, Starlette, GFZ, Champ Various geodynamic processes are responsible for changes in the gravity field. Increased spatial resolution by the new proposed missions
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Source: NRC 1997
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Temporal gravity and geodynamic processes (Chao,1994)
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Challenges Extreme sensitivity of low-low satellite to satellite tracking in the lower degree and orders (till L=70) The entire gravity field can be solved for after 30 days of data, temporal variations can be observed It opens the possibility to study e.g.: the continental water balance ocean bottom pressure observations. Open questions: How do you separate between signals. How do you suppress nuisance signals
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Surface mass layer to geoid
Model Purpose: convert equivalent water heights (h) to geoid undulations (dN)
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Properties Kernel function
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Geophysical contamination
Approximately mbar error (now-cast) is typical ECMWF and NCEP (Velicogna et al, 2001) averaging over space and time helps to drive down this error, better than 0.3 mbar is unlikely. Some regions are poorly mapped (South Pole) and the errors will be larger The low degree and orders are more affected and probably the gravity performance curves are too optimistic (see kernel function)
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Other Temporal gravity issues
Unclear how to separate different signals ( criteria: location, spatial patterns? EOF? Other?) Accuracy tidal models (3 cm rms currently)? Aliasing of S1/S2 radiational tides in sun-synchronous orbits used for gravity missions Edge effects near coastal boundaries Data gaps
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Round up Gravity missions: new missions discussed and their error characteristics, isotropy, homogeneity. Mean circulation: thermal wind, tracers, assimilation of observations, results from exiting approaches Satellite altimetry: typical results averaging and sampling in oceanic areas with high mesoscale signal, a sample of the scientific progress since 1992. Temporal gravity: current research and processes that are visible, contamination with geophysical signals, separation of individual signals and noise
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