This paper deals with the atmospheric effects involved in the time variations of grav ity measured by asuperconducting gravimeter. The atmospheric effects on the gravity changes are two-fold, i.e., the effect from the Newtonian attraction caused by the mass of the atmosphere and that from the loading effect caused by the deformation and density change of the Earth. The former effect was evaluated by assuming that the density change of the atmosphere with altitude follows an exponential function. The latter effect was evaluated using Farrell's Green function. One problem is that there is a singular point in the Green's functions of both effects at the angular distance ψ=0 measured from the gravimeter site. However, we proved that the both gravity changes converge at ψ=0. We obtained a closed formula for the Newtonian attraction, and a linear asymptotic solution for the loading effect. The total atmospheric effect thus ob tained is about 12 Fugal: Its 90% is caused by the atmosphere between ψ=0 and 0°43, the effect from the atmosphere between 0°43 and 2°7 is zero in all because the two effects cancel one another, and the global effect from outside ψ=2°7 is about 1 Fugal. Our superconducting gravimeter is installed at the past geophysical facility attached to the Faculty of Sciences, University of Tokyo, located at Kakioka, Ibaragi Prefecture (36°D233 N, 140°183 E, Elevation 31.7 m). The data used for evaluating the atmospheric effects are the pressure at the gravimeter site at the interval of 30 minutes, the local pressure data reported by the Japan Meteorological Agency, at the interval of 3 hours, and the global data distributed by the same agency at the interval of 24 hours. In this study the gravity data for one month in January 1990 were processed and corrected for the atmospheric effects. The result shows that the residual gravity change after corrections were made is 1 μgal in amplitude. When this correction was made assuming Non-Inverted Barometer Model the standard deviation of the residual was 1.07 μgal, whereas, when it was made assuming Inverted Barometer Model the standard deviation was somewhat lowered to 0.78 μgal.
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