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This study summarizes the findings from the observations of two SG (serial no. 48 and 49) three FG5 (serial no. 224, 228, and 231) and a regional GPS network around Taiwan. The main objectives of this study are:

1. The introductions of SG and AG in Taiwan, including individual devices and the procedures of operation.

2. The analyses of the SG’s critical parameters and the potential applications to related studies, such as solid earth tide, ocean tide loading, atmospheric effect, hydrologic effect, typhoon and earthquake.

3. The preliminary results from the AGTO project in connection to the result of GPS.

The major findings of this study are listed below:

1. Establishing procedures to determine many different types of detided gravity enabling to analyze solid earth tide, ocean tide loading, atmospheric effect, hydrological effect, polar motion effect and other gravity changes caused by environmental changes.

2. The drifting rate of AG and T48 are 2.2±0.3 μgal year-1 and 1.3±0.1 μgal year-1 from the AG and T48 measurements from 2006 to 2011. Based on the parallel observations of AG and SG, the CF and the different rate between AG and T48 were -76.087 ± 0.067 μgal voltage-1 and -0.8 ± 1.3 μgal year-1, respectively. The observed drifting rate of T48 is smaller than the nominal drift-rate of 6 μgal year-1 reported by the SG manufacturer.

3. The north area of HS is a groundwater-rich alluvium with evident gravity variations. A vertical site motion of -0.22±0.97 cm year-1 at HS was found and not directly related to the movement of the Hsinchu Fault.

4. The gravity-atmosphere admittances during typhoons are 30% larger than the mean value. In modeling gravity change due to atmosphere, the global atmospheric pressure model is suitable over a large area, especially for the long period variation. Short period atmosphere-induced gravity change is only well predicted by high frequent atmospheric data.

5. The relative errors between the gravimetric amplitude factors determined with T48 (corrected by NAO.99b) and the model factors of Dehant et al.

(1999) range from 99.95 to 96.07%. The Newtonian part contributes a significant portion to ocean tide loading gravity effects (about 20% for M2 at HS) at HS. The largest Newtonian gravity effect of ocean tide is found around Matzu.

6. The gravity offset generated by the earthquake of September 6, 2007 reached 0.6 μgal, which contributes 0.3 μgal year-1 to the gravity rate at HS over 2006-2011.

7. The mean gravity and vertical rates at AGTO sites are -1.39±4.21 μgal year-1 and 0.50±0.94 cm year-1. The sediment thicknesses changes near AG6 and AG3 due to landslides caused by Typhoon Morakot are 2.45 m and 1.25 m.

8. Using repeated absolute gravimetric measurements to determine gravity changes at islandwide (Taiwan) stations, and the preliminary causes of such changes are identified with the help of GPS and other data. The average rate of gravity change from 2005 to 2008 is -0.58 μgal year-1 in Taiwan.

In this study, the SG and AG gravimeter measurements have been applied to tidal analysis, geodynamics, typhoon and atmosphere. Potential applications of these instruments of methodologies are listed below.

1. The SG gravimeter, T49, is currently at Hsinchu, but it can be deployed in a new location (other than Hsinchu) that has a different geodynamic feature.

With two SG at two locations, many research opportunities can be explored.

For example, a proposed new site for T49 is Mt. Yangming (see Fig. 6-4, YMSG), where possible volcano eruptions can occur and hydrological changes will induce large mass and gravity changes. Records from two SG can be used to study gravity changes in sea level ocean circulation

associated with the Kuroshio Current.

2. Use of gravimetry to study groundwater in central Taiwan. Since 90 % of all unfrozen fresh water is hidden underground, it is difficult to determine its volume. The volume can be estimated with a network of AG sites around central Taiwan.

References

Boy, J.P., J. Hinderer, and P. Gegout, 1998. Global atmospheric loading and gravity, Phys. Earth planet. Inter., 109, 161–177.

Boy, J.P., P. Gegout, and J. Hinderer, 2002. Reduction of surface gravity data from global atmospheric pressure loading. Geophys. J. Int. 149, 534–545.

Boy, J. P., M. Llubes, R. Ray, J. Hinderer, N. Florsch, S. Rosat, F. Lyard, and T.

Letellier, 2004. Non-linear oceanic tides observed by superconducting gravimeters in Europe, J. Geodyn., 38, 391-405.

Boy, J. P., and J. Hinderer, 2006. Study of the seasonal gravity signal in superconducting gravimeter data, J. Geodyn., 41, 227-233.

Chojnicki, T., 1973. Ein Verfahren zur Erdgezeitenanalyse in Anlehnung an das Prinzip der kleinsten Quadrate. Mitt. Inst. F. Theor. Geod. Univ. Bonn, Nr. 15.

Crossley, D., O. Jensen, and J. Hinderer, 1995. Effective barometric admittance and gravity residuals. Phys. Earth planet. Int., 90, 355-358

Dal Moro, G. and M. Zadro, 1998. Subsurface deformations induced by rainfall and atmospheric pressure: tilt/strain measurements in the NE-Italy seismic area.

Earth and Planetary Science Letters, 164, pp. 193-203

Dehant, V., P. Defraigne, and J. M. Wahr, 1999. Tides for a convective Earth. J.

Geophys. Res., 104, 1035-1058.

Dziewonski, A. D., and D. L. Anderson, 1981. Preliminary reference Earth model, Phys. Earth Planet. Inter., 25, 297-356.

Eanes, R., and S. Bettadpur, 1996. The CSR3.0 global ocean tide model: Diurnal and Semi-diurnal ocean tides from TOPEX/POSEIDON altimetry, CRS-TM-96-05, University of Texas, Centre for Space Research, Austin, Texas.

Falk, R., M. Harnisch, G. Harnisch, I. Novak, and B. Richter, 2001. Calibration of the

Superconducting Gravimeter SG 103, C023, CD029 and CD030. Journal of Geodetic Society of Japan, 47, 22−27.

Farrell, W. E., 1972. Deformation of the earth by surface loads, Rev. Geophys. Space Phys., 10, 761-797.

FG5 Absolute Gravimeter User’s Manual, December 2006.

http://www.microglacoste.com/

Francis, O., T. M. Niebauer, G. Sasagawa, F. Klopping, and J. Gschwind, 1998.

Calibration of a superconducting gravimeter by comparison with an absolute gravimeter FG5 in Boulder, Geophys. Res. Lett., 25, 1075-1078.

Fu, G. Y., and W. K. Sun, 2008. Surface coseismic gravity changes caused by dislocations in a 3-D heterogeneous earth, Geophys. J. Int., 172, 479-503, doi:

10.1111/j.1365-246X.2007.03684.x

GWR instruments, inc. 2011. GWR Observatory Superconducting Gravimeter and Support Systems. http://www.gwrinstruments.com/index.html

Hwang, C., R. Kao, C. C. Cheng, J. F. Huang, C. W. Lee, and T. Sato, 2009. Results from parallel observations of superconducting and absolute gravimeters and GPS at the Hsinchu station of Global Geodynamics Project, Taiwan. J. Geophys. Res., 114, B07406, doi: 10.1029/2008JB006195.

Imanishi, Y., T. Higashi, and Y. Fukuda, 2002. Calibration of the superconducting gravimeter T011 by parallel observation with the absolute gravimeter FG5 #210 - a Bayesian approach, Geophys. J. Int., 151, 867-878.

Imanishi, Y., T. Sato, T. Higashi, W. K. Sun, and S. Okubo, 2004. A network of superconducting gravimeters detects submicrogal coseismic gravity changes, Science, 306, 476 – 478, doi: 10.1126/science.1101875.

Jacob, T., R. Bayer, J. Chery, H. Jourde, N. Le Moigne, J. P. Boy, J. Hinderer, B. Luck, and P. Brunet, 2008. Absolute gravimetry monitoring of water storage variation in

a karst aquifer on the larzac plateau (Southern France), J. Hydrol., 359, 105-117.

Jan, S., C. S. Chern, J. Wang, and S. Y. Chao, 2004. The anomalous amplification of M2 tide in the Taiwan Strait, Geophys. Res. Lett., 31, L07308, doi:10.1029/2003/GL019373.

Kim, J. W., J. Neumeyer, T. H. Kim, I. Woo, H. J. Park, J. S. Jeon, and K. D. Kim, 2009.

Analysis of superconducting gravimeter measurements at MunGyung station, Korea. J. Geodyn., 47, 180-190, doi: 10.1016/j.jog.2008.07.008.

Kim, S. Y., and H. Y. Chun, 2011. Impact of typhoon-generated gravity waves in the typhoon development, Geophys. Res. Lett., 38, L01806, doi: 10.1029/

2010GL045719.

Lyard, F., F. Lefevre, T. Letellier, and O. Francis, 2006. Modeling the global ocean tides:

modern insights from FES2004, Ocean Dynamics, 56, 394-415.

Matsumoto, K., T. Takanezawa, and M. Ooe, 2000. Ocean tide models developed by assimilating TOPEX/POSIDON altimeter data into hydrodynamical model: A global model and a regional model around Japan, J. Oceanogr., 56, 567-581.

Mouyen, M., F. Masson, C. Hwang, C.-C. Cheng, R. Cattin, C.W. Lee, N. Le Mogine, J. Hinderer, J. Malavieille, R. Bayer and B. Luck, 2009. Expected temporal absolute gravity change across the Taiwanese Orogen, a modeling approach, J.

Geodynamics, 48, 284-291.

Mukai, A., T. Higashi, S. Takemoto, I. Nakagawa and I. Naito, 1995. Accurate estimation of atmospheric effects on gravity observations made with a superconducting gravity meter at Kyoto, Volume 91, Issues 1-3, pp. 149-159.

Naujoks, M., A. Weise, C. Kroner, and T. Jahr, 2008. Detection of small hydrological variations in gravity by repeated observations with relative gravimeters, J. Geod., 82,543-553.

Nawa, K., N. Suda, I. Yamada, R. Miyajima, and S. Okubo, 2009. Coseismic change

and precipitation effect in temporal gravity variation at Inuyama, Japan: A case of the 2004 off the Kii peninsula earthquakes observed with a superconducting gravimeter. J. Geodyn., 48, 1-5, doi: 10.1016/j.jog.2009.01.006.

Nerem, R. S., E. Leuliette, and A. Cazenave, 2006. Present-day sea-level change: A review, Comptes Rendus Geoscience, 338, 14-15.

Neumeyer, J., J. Hagedoorn, J. Leitloff, and T. Schmidt, 2004. Gravity reduction with three-dimensional atmospheric pressure data for precise ground gravity measurements, J. Geodyn., 38, 437-450.

Neumeyer, J., F. Barthelmes, C. Kroner, S. Petrovic, R. Schmidt, H. Virtanen, and H.

Wilmes, 2008. Analysis of gravity field variations derived from superconducting gravimeter recordings, the GRACE satellite and hydrological models at selected European sites, Earth Planets Space, 60, 505-518.

Peterson, J., 1993. Observations and modelling of background seismic noise.

Open-file report 93-322, U. S. Geological Survey, Albuquerque, New Mexico.

Penna, T. N., M. A. King, and M. P. Stewart, 2007. GPS height time series:

Short-period origins of spurious long-period signals, J. Geophys. Res., 11, B02402, doi: 10.1029/2005JB004047.

Richter, B., H. Wilmes, and I. Nowak, 1995. The Frankfurt Calibration System for Relative Gravimeters. Metrologia, 32, 217−224

Sato, T., Y. Tamura, S. Okubo, and S. Yoshida, 1996. Calibration of scale factor of superconducting gravimeter at Esashi using an absolute gravimeter FG5. Journal of Geodetic Society of Japan, 42, 225−232.

Segall, P., and J. L. Davis, 1997. GPS applications for geodynamics and earthquake studies. Annu. Rev. Earth Planet. Sci. 25, 301–336.

Shiomi, S., 2006. Geophysical test of the universality of free-fall, Phys. Rev. D: Part.

Fields, 74, 027101.

Spratt, R. S., 1982. Modelling the effect of atmospheric pressure variations on gravity, Geophys. J. R. astr. Soc., 71, 173–186.

Tamura, Y., T. Sato, M. Ooe, and M. Ishiguro, 1991. A procedure for tidal analysis with a Bayesian information criterion, Geophys. J. Int., 104, 507-516.

Tamura, Y., T. Sato, Y. Fukuda, and T. Higashi, 2005. Scale factor calibration of a superconducting gravimeter at Esashi Station, Japan, using absolute gravity measurements, J. Geod., 78, 481-488.

Torge, W., 1989. Gravimetry. De Gruyter, Berlin.

TSoft Manual, 2010. http://seismologie.oma.be/TSOFT/tsoft.html

Van Ruymbecke, M., 1989. A calibration system for gravimeters using a sinusoidal acceleration resulting from a vertical periodic movement. Journal of Geodesy, 63, 223−236.

Virtanen, H., and J. Makinen, 2003. The effect of the Baltic sea level on gravity at the Metsahovi station, J. Geodyn., 35, 553-565.

Wang, R. J., F. Lorenzo-Martín, and F. Roth, 2006. PSGRN/PSCMP- a new code for calculating co- and post-seismic deformation, geoid and gravity changes based on the viscoelastic-gravitational dislocation theory, Comput. Geosci., 32, 527-541.

Warburton, R. J., and E. W. Brinton, 1995. Recent developments in GWR Instrument’s superconducting gravimeters, Proc. 2nd Workshop in Non-tidal Gravity Changes: Intercomparison Between Absolute and Superconducting Gravimeters. Cahiers du Centre Européen de Géodynamique et de Séismologie, Luxembourg, ed. Poitevin, C., 11, 23-56.

Warburton, R. J., and Goodkind, J. M., 1977. The influence of barometric pressure variations on gravity. Geophys. J. R. astr. Soc., 48, 281-292.

Wenzel, H. G., 1996. The nanogal software: Earth tide processing package ETERNA 3.30. Bull. d’Inf Marées Terr., 124, 9425-9439.

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