Introduction Directory UMM :Data Elmu:jurnal:J-a:Journal Of Applied Geophysics:Vol46.Issue1.2001:

Ž . Journal of Applied Geophysics 46 2001 45–54 www.elsevier.nlrlocaterjappgeo Full 3-D inversion of electromagnetic data on PC Yutaka Sasaki Department of Earth Resources Engineering, Graduate School of Engineering, Kyushu UniÕersity, Hakozaki, Higashi, Fukuoka 812-8581, Japan Received 5 August 1999; accepted 31 October 2000 Abstract Ž . Ž . Three-dimensional 3-D electromagnetic EM inversion might be believed to require high-performance computers. Ž . However, with the rapid progress of recent computer technology, running 3-D inversions on personal computers PC is becoming a rational choice. This paper describes an attempt to carry out full 3-D inversions of synthetic frequency-domain EM data on a PC. In the inversion, a staggered-grid finite difference scheme is used to solve for the secondary electric field. Ž . The system of equations is solved using the incomplete Cholesky biconjugate gradient ICBCG method. By applying the w Ž . x static divergence correction proposed by Smith Geophysics 61 1996 1319–1324 , the rates of convergence are dramatically improved, and the forward calculation per source location on a medium-size grid takes only a few minutes on a PC. The sensitivities of the EM responses to subsurface resistivity changes are calculated from forward solutions using the reciprocity relation. An inverse problem is formulated so that a model is found that has a smooth structure and at the same time is close to an initial model, and is solved with an iterative least-squares method. A synthetic example for an airborne EM survey shows that the lateral extents of 3-D bodies are well resolved, and the vertical coil coaxial system gives a better lateral resolution than the horizontal coil coplanar system. An example for a ground EM survey shows that expanding the survey coverage or aperture is needed to improve the resolution at depth. q 2001 Elsevier Science B.V. All rights reserved. Keywords: 3-D inversion; Finite difference method; Biconjugate gradient method; Electromagnetics

1. Introduction

Ž . Inverting electromagnetic EM data for three-di- Ž . mensional 3-D electrical conductivity structures has been a major challenge in applied geophysics for many years. Full 3-D inversions involve rigorous forward modelings for general 3-D structures, which are computationally very time-consuming compared to 1-D and 2-D cases. Despite this difficulty, several Fax: q81-92-642-3614. Ž . E-mail address: sasakimine.kyushu-u.ac.jp Y. Sasaki . attempts have been made to carry out 3-D inversions using different forward numerical solutions. Eaton Ž . Ž . 1989 and Pellerin et al. 1993 both used the integral equation approach to formulate 3-D inverse problems for controlled-source EM surveys. Mackie Ž . and Madden 1993 developed an inversion proce- dure for magnetotelluric data that is based on the finite difference and conjugate gradient methods. Xie Ž . et al. 1995 derived a new integral equation in terms of the magnetic field and applied it to invert for Ž . conductivities and permittivities. Ellis 1995 per- formed a 3-D inversion on airborne EM data using Ž . the finite element method. Newman 1995 presented 0926-9851r01r - see front matter q 2001 Elsevier Science B.V. All rights reserved. Ž . PII: S 0 9 2 6 - 9 8 5 1 0 0 0 0 0 3 8 - 0 an inversion scheme in which the finite difference method is used for the forward modeling and the integral equation method for the inverse formulation. Ž . Later, Newman and Alumbaugh 1997 modified their inversion scheme for use on a massively paral- lel computer. These inversion methods required powerful higher-end workstations or supercomputers. Thus, it is commonly accepted that 3-D EM inversions are too expensive and cannot be a practical interpretation tool for most field geophysicists. However, due to the ever increasing power of personal computers Ž . PC , running 3-D inversion schemes on PC is be- coming a rational choice. The purpose of this paper is to demonstrate using synthetic examples that full 3-D EM inversions are feasible on PC. The inversion method consists of three key components: inversion algorithm, forward modeling, and sensitivity calcula- tion. In this paper, these key points are first dis- cussed and then the accuracy of the finite-difference solution used in the inversion routine is verified. Finally, two synthetic examples of 3-D inversions involving airborne and ground EM methods are pre- sented.

2. Linearized inversion