It is possible to detect the non-Newtonian gravity due to the Earth's mass by measuring gravity gradient over a wide range of altitude since there is a characteristic pattern in the relation between the value of the non-Newtonian gradient and the altitude on a logarithmic scale. The value of the non-Newtonian gravity gradient on the Earth is estimated at about a×10
-6s
-2 where α is the coefficient of the additional YUKAWA term. The effects of harmonics of gravity potential with degrees higher than 3 and uncertainty of density of the Earth's interior, on the other hand, are less than 10
-10s
-2 and they can be corrected to as small as in the range of 10-
12s
-2 with an reliable Earth model, which is equivalent to the non-Newtonian gravity gradient in the case of α=10
-6. A gravity gradiometer with a couple of superconducting accelerometer or that with high sensitive Fabry-Perot interferometer can have the sensitivity better than 10-13s-2 and it is the most effective for the detection of the non-Newtonian gravity on the Earth . The non-Newtonian gravity gradient due to the Earth is detectable if the coefficient α is larger than 10
-6 and the range λ is shorter than 10
5 m by the gravity gradient measurement.
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