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Appropriate choices for model and data parameters are interrelated and specific for each data set. Even for full 3-D inversion thorough analysis of dimensionality and strike behaviour of the data set is advisable. In presence of a pronounced geo-electric strike direction, a rotation of data and model grid should be considered. If the coordinate system is not aligned with a dominant strike direction, the outcome of 3-D inversion can be erroneous and misleading. A sensible data-weighting scheme is essential to recover the full information of all inverted components. If the inversion scheme penalizes deviations from a prior model, the set-up of the prior model has to be handled carefully and a range of prior models should be tested. Among the most widely applied, and practical, approaches to inversion of electromagnetic (EM) geophysical data (e.g., magnetotellurics; MT) in two and three dimensions are regularized schemes based on minimizing a penalty functional of the form. It is of course possible to use a GN approach without explicitly forming the normal equations of (2a), but instead solve this symmetric linear system of equations iteratively using conjugate gradients (CG). This approach, which has been used fairly extensively for EM inversion (e.g. Mackie & Madden 1993; Alumbaugh & Newman 1997; Rodi & Mackie 2001) is a variant on the truncated Newton approach to optimization (e.g. Dembo 1982; Nash 2000), with the Hessian replaced by the GN approximation (e.g. Newman & Hoversten 2000). A key point to note here is that the model space vector is just the sensitivity of a particular linear combination of data components, namely u T 1 d (ignoring noise ). 11 October, Tue 04:30 AM palpite gremio x brusque IST.
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