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REGULARIZED SOLUTIONS OF AN INTEGRAL EQUATION OF GRAVIMETRY

Dinh Ngoc Thanh 1
Chu Van Tho 2
Volume & Issue: Vol. 5 No. 9 (2002) | Page No.: 43-54 | DOI: 10.32508/stdj.v5i9.3441
Published: 2002-09-30

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This article is published with open access by Viet Nam National University, Ho Chi Minh City, Viet Nam. This article is distributed under the terms of the Creative Commons Attribution License (CC-BY 4.0) which permits any use, distribution, and reproduction in any medium, provided the original author(s) and the source are credited.

Abstract

We consider the problem of determining the relative density ρ of a body in the interior of the earth from surface gravity anomalies created by this body. Let ρ_1, be the mass density, and ρ_2 be the density of the surrounding medium, the relative density of the body is ρ=ρ_1-ρ_2. The earth is represented by a half-space (x,z), -∞ <z≤ H, H > 0. The body Ω is represented by Ω = {(x; y): 0<x<1 ; 0<z< σ(x)} where σ: [0, 1] → IR is piecewise C1 function such that với 0<x<1; α>0. In general, with , the problem of determining the relative density p of a body in the interior of the earth from surface gravity anomalies is no uniqueness. In the case of , the above problem admits at most one solution. Then ρ satisfies a nonlinear integral equation of the first kind. In the case of , the nonlinear integral equation is changed to the convolution equation. The solution of the convolution equation is regularized by the Tikhonov method.

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