In the preceding paper, the author assumed the density distribution of the subterranean structure was the eq. (4) and he deduced the coefficient
Cm from the boundary conditions, these were the gravity and the density both observed on the earth surface.
By this method, he showed the actual structure was reasonably explained by the gravity anomaly.
Consulting the eqs. (2) and (6), he now assumes the distribution of excess mass on the surface ρ
em and their compensated subterranean mass ρ
em. They are the eqs. (8) and (9).
He takes this model for that of isostasy and calculates some quantities which are shown in Table 1, and Fig. 1.
When the surface topography are represented by the eq. (17) and the density on the surface is ρ
o, the isostatic anomaly is the eq. (28) in his model of isostasy.
These results are agreed with that of the
Tsuboi's model which is identically independent from this model.
The relation between the isostatic anomaly and the
coefficient of the rate of change of density λ is shown by the eq. (29).
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