Abstract

We present a compressed implicit Jacobian scheme for the regularized Gauss-Newton (GN) inversion algorithm for reconstructing three-dimensional conductivity distribution from electromagnetic data. In this scheme, the Jacobian matrix, whose storage usually requires a large amount of memory, is decomposed in terms of electric fields excited by sources located and oriented identically to the physical sources and receivers. As a result, the memory usage for the Jacobian matrix reduces from O (N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S</sub> N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">R</sub> N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</sub> ) to O [(N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S</sub> + N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">R</sub> )N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</sub> ], in which N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S</sub> is the number of sources, NR is the number of receivers and N <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</sub> is the number of parameters to be inverted. Further we applied the adaptive cross approximation (ACA) to compress these fields in order to further reduce the memory usage and to improve the efficiency of the GN method. In addition, the ACA error criterion is linked to the data misfit cost function so that we obtain a higher compression rate in early GN iterations. This compressed implicit Jacobian scheme provides a good balance between the memory usage and the computational time and makes the GN algorithm more efficient. We demonstrate the benefits of this scheme using synthetic and field data for geophysical electromagnetic applications.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call