Airborne Gravity 2010 - Geoscience Australia
Airborne Gravity 2010 - Geoscience Australia
Airborne Gravity 2010 - Geoscience Australia
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<strong>Airborne</strong> <strong>Gravity</strong> <strong>2010</strong><br />
3D imaging of subsurface structures using<br />
migration and regularized focusing inversion of<br />
gravity and gravity gradiometry data<br />
Introduction<br />
Michael S. Zhdanov 1 , Glenn A. Wilson 2 , and Xiaojun Liu 3<br />
1 University of Utah & TechnoImaging (mzhdanov@technoimaging.com)<br />
2 TechnoImaging (glenn@technoimaging.com)<br />
3 University of Utah (xiaojun.liu@utah.edu)<br />
Since gravity and gravity gradiometry can provide an independent measure of the subsurface density<br />
distribution, they have come to be routinely integrated into exploration workflows. The advantage of<br />
gravity gradiometry over other gravity methods is that the data are extremely sensitive to localized<br />
density contrasts within regional geological settings. Moreover, high quality data can now be acquired<br />
from either air- or ship-borne platforms over very large areas at relatively low cost.<br />
Here, we present the results from two different methods of interpretation for gravity and gravity<br />
gradiometry data. We introduce potential field migration that is a direct integral transformation of the<br />
observed gravity fields and/or their gradients into 3D images of density distribution. Unlike ill-posed<br />
and unstable transforms such as downward analytic continuation or higher order differentiation,<br />
migration is a well-posed and stable transformation. Migration does not assume nor require any a<br />
priori information about the type of the source of the fields. When implemented, potential field<br />
migration is fast and robust, and can be used for real-time imaging as well as for producing a priori<br />
models for a subsequent inversion.<br />
We then introduce 3D regularized focusing inversion, whereby the use of focusing stabilizers allows<br />
the recovery of subsurface models with sharper density contrasts than can be obtained using<br />
traditional smooth stabilizers. Our inversion is based on the re-weighted regularized conjugate<br />
gradient method. Compression and FFT matrix multiplications further reduce memory requirements<br />
and runtimes, so as to make it practical to invert entire airborne or marine datasets to models with<br />
millions of cells.<br />
The combination of migration and inversion makes it is feasible to run multiple interpretation scenarios<br />
based on different data combinations and various regularization parameters so as to build confidence<br />
in the robustness of features in the recovered models. It also allows us to discriminate any artifacts<br />
that may arise from any single interpretation. Here, we demonstrate these methods using a case study<br />
for the inversion of marine gravity gradiometry data for salt mapping in the Norwegian Barents Sea.<br />
Potential Field Migration<br />
A variety of fast imaging techniques related to Euler decomposition have been developed. Most of<br />
these are based on the superposition of analytical responses from specific sources. These imaging<br />
methods estimate the positions and some parameters of the sources based on field attenuation<br />
characteristics. We developed a different approach to imaging, one which we base on the idea of<br />
potential field migration as originally introduced by Zhdanov (2002) and first applied to gravity<br />
gradiometry data by Zhdanov et al. (<strong>2010</strong>). The concept of the migration was developed for seismic<br />
wave fields (e.g., Schneider, 1978; Berkhout, 1980; Claerbout, 1985). Since, it has been demonstrated<br />
that the same concept can also be extended to electromagnetic and potential fields (Zhdanov, 1988,<br />
2002, 2009a). Potential field migration is based on a special form of downward continuation of the<br />
potential field or one of its gradients. This downward continuation is obtained as the solution of the<br />
boundary value problem to Laplace’s equation in the lower half-space where the boundary values of<br />
the migration field on the Earth’s surface are determined from the observed data. It is important to<br />
stress that potential field migration is not the same as analytic continuation. It transforms the observed<br />
field into a migration field, and does not attempt to reconstruct the true potential field. However, the<br />
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