Title: Time Variations of the European Gravity Field, 1997-2001
1Time Variations of the European Gravity Field,
1997-2001
- David Crossley, Saint Louis University, Missouri,
USA - Jacques Hinderer, EOST / IPG, Strasbourg, France
- Jean-Paul Boy, NASA Goddard Space Flight Center,
Maryland, USA
2Global Geodynamics Project Phase 1 1997-2003
IUGG SEDI initiative Workshops Brussels 1997,
Munsbach 1999, Jena 2002
3GGP Stations 1997 - 2003
4GGP Satellite Project
- CHAMP and GRACE satellite calibration and
validation - Provides surface gravity measurements that are
independent of satellite observations, compared
to other methods that rely on modeling - Goal is to find and interpret coherent seasonal
gravity effects using European GGP ground stations
5GGP and Satellite Missions
6Ground and SatelliteGravity Contributions
7Objectives
- Use Superconducting Gravimeter (SG) data from the
European sub-network of GGP - Compute residual gravity series for each station,
July 1997 to December 2001 - Combine series spatially into a surface that
approximates the length scale of GRACE data over
Europe (200 -1000 km) - Estimate the error in this surface and compare to
GRACE accuracy predictions (0.4 mgal at 300 km) - Compare with existing CHAMP satellite data
- Set up a semi-automatic procedure for producing
European surface gravity for the duration of the
CHAMP and GRACE missions
8Simulation of Hydrology Recovery 5 year model
for Manaus, Amazon Basin (Wahr et al., 1998)
9GGP Stations Europe 1997 - 2003
BE Belgium BR Brasimone PO Potsdam MB Membach MC
Medicina ME Metsahovi MO Moxa ST Strasbourg VI
Vienna WE Wettzell BH Bad Homberg WA Walferdange
10Processing GGP Data
- Start with uncorrected ICET 1 minute files
- Fix pressure - linear interpolation for gaps
- Remove local tide (solid and oceanic components)
and local barometric pressure - Fix gaps and remove spikes replace with linear
interpolation - Decimate to 1 hour, remove IERS polar motion
11Tides, Local Pressure and Polar Motion Removed
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16Processing Drift and Offsets
- Simultaneous Drift and Offset Estimation VERY
IMPORTANT TO DO THIS RIGHT - Offsets need to be checked against station log
files - Drift and offsets can differ even between two
spheres of a single instrument - Drift and offsets should be consistent between SG
residuals and AG measurements
17Wettzell - Initial Drift and Offsets CD029
Uncorrected GGP 1 minute data from ICET
18Strasbourg Residuals - SG, AG and Polar Motion
19Medicina Residuals, SG AG
Corrected for tides, air pressure, polar motion
(Romagnoli et al. 2003)
20SG Drift Estimation (mgal / yr)
21Station Residuals BE to MO
22Station Residuals PO to WE2
23Atmospheric Loading Models
- Local pressure, admittance 0.3 mgal / hPa
includes direct attraction loading - Global pressure using only surface data, e.g.
ECMWF. Includes treatment of oceans as static,
IB, or non-IB. Thin atmosphere no vertical
structure (e.g. Boy et al., 1998) -
- Global (p,T) - as above, but model r(h) as a
function of surface (P,T) perfect gas to 20
km (e.g. Boy et al., 2002) - Full 3-D vertical structure from actual 3-D
meteorological data. Computationally intensive,
but important at seasonal periods (Boy et al.,
2002).
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27Atmospheric loading, station ME
28Combined Daily Residuals
29Minimum Curvature Surface
- For each day fit a minimum curvature surface to
all the stations - This surface goes through every station and
therefore does no spatial averaging
30Minimum Curvature Surface, All Stations
316-month Samples, all Stations
32Spatial Smoothing
- Insufficient data to reconstruct a smoothed
field from spherical harmonic analysis - Insufficient station data to fit a surface
directly - Instead, fit an nth degree polynomial 2-D
surface to the minimum curvature surface
33Comparison of Surfaces
Minimum Curvature
3rd Degree Polynomial
343rd Degree Surface All Stations
35Reconstruct Gravity at Stations
- Select the gravity values on the surface at the
stations - Average all stations for each day (mean surface)
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38Select Central Stations
39New Surface Using Central Stations
40Central Stations, 6-Month Intervals
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42Northward Event 99
Apr 99
Jan 99
Mar 99
Feb 99
May 99
43Northward Event 99
Jun 99
May 99
Aug 99
Jul 99
44So far
- GGP data shows clear annual signal for 3 years
(97-00), but not for 2000-01 - Accuracy at 0.8 mgal, comparable to predicted
GRACE (0.4 mgal) at 300 km. - Atmospheric loading - difference between global
(p,T) and local p - affects the mean gravity
field at about the 0.5 mgal level. - No attempt yet to estimate secular changes over
Europe
45Interpretation of Annual Signals
- Local
- Instrument effects, thermal anomalies,
vegetation, groundwater, surface water, soil
moisture - Regional and global
- Atmospheric pressure (3-D) attraction / loading
- Ocean circulation, loading
- Hydrology
- Soil compaction
- Zerbini S., B. Richter, M. Negusini, C.
Romagnoli, D. Simon, F. Domenichini, W. Schwahn
(2001) EPSL 192. - C. Romagnoli, S. Zerbini, L. Lago, B. Richter, D.
Simon, F. Domenichini, C. Elmi, and M. Ghirotti
(2003) in press.
46Annual Signals at Medicina
47GPS and Gravity at Medicina
- GPS (upper), gravity (lower)
- Expected anti-correlation
- Reasonable admittance -18 mm vs 6 mgal (peak to
peak)
48Continental Water Storage
- Model uses estimated precipitation, downwelling
radiation and near surface atmospheric conditions - Soil saturates and recharges groundwater that
partially recharges surface water model includes
evaporation - Monthly water storage is convolved with a Greens
function to estimate gravity attraction and
elastic deformation. - van Dam, T., Wahr, J. Milly, C., and Francis
O., (2001) J. Geodet. Soc Japan.
49Global loading results
- Model results from some GGP stations
- Includes attraction and loading
- Note maxima usually in winter
50Water Storage Statistics
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52Comment
- Residual annual gravity in Europe has a similar
amplitude 2.5 mgal - and phase (probably)
- as estimated water loading
- To proceed further, we need CHAMP and GRACE
satellite data
53Other Possibilities (1) Japan (2) Greenland
54Japan Ocean Hemisphere Project
National Astronomical Observatory, Misuzawa
(Esashi, Canberra and Ny-Alesund) Kyoto
University (Bandung) National Institute for Polar
Research, Tokyo (Syowa)
55GGP Stations - W. Pacific
BA Bandung CB Canberra ES Esashi KY Kyoto MA
Matsushiro WU Wuhan
56Greenland Uplift
Kellyville
- Post-glacial uplift from 3 different models
- ICE-3G Greenland component only
- HUY2 ignoring ice changes during last 4000 yr
- ICE-3G - variability outside Greenland
- J. Wahr, T. van Dam, K. Larson, and O. Francis,
(2001) JGR, 106
Kulusuk
57Greenland GPS
58Greenland AG
59Greenland Interpretation
- GPS uplift rate as a function of increasing data
length - Kellyville multi-day averages
- Kellyville daily averages
- , (d) same for Kulusuk
60New Greenland Proposal
- Network of 5 new SGs around coast
- Should confirm gravity variations to lt 1 mgal
- Tied to AG measurements
- Monitored by GRACE
61New GWR field instrument
(requires no He refills)
62Larger European GGP Array
- New sites would be useful in Europe to fill gap
between ME and existing stations - e.g. Central France, Denmark, Southern Sweden,
Poland -
63Conclusions
- GGP database will monitor gravity variations for
satellite missions - Both SGs and AGs are required to confirm drift
and offsets at the 1 mgal level - GPS measurements required to correct for ground
vertical deflection requires gt 4 years to define
secular trends - Atmospheric loading should be done with full 3-D
modeling, as for GRACE - More hydrological studies, including soil
moisture and continental water loading, are
required.
64Thanks to all members of the GGP Support
Groups who have dedicated their efforts to
maintaining the gravity stations