HR: 09:30h
AN: GP31A-07 [Abstracts]
TI: A new method for mapping depth to the Curie-temperature isotherm in the Great Basin from aeromagnetic anomalies
AU: * Bouligand, C
EM: cbouligand@usgs.gov
AF: U.S. Geological Survey, 345 Middlefield Rd., MS989, Menlo Park, CA 94025, United States
AU: Glen, J
EM: jglen@usgs.gov
AF: U.S. Geological Survey, 345 Middlefield Rd., MS989, Menlo Park, CA 94025, United States
AU: Blakely, R
EM: blakely@usgs.gov
AF: U.S. Geological Survey, 345 Middlefield Rd., MS989, Menlo Park, CA 94025, United States
AB:
We have revisited the problem of using aeromagnetic data to map depth to the Curie-temperature isotherm and
tested our new methodology in an attempt to provide an independent estimate of heat flow in the Great Basin.
Such methods typically assume that the depth-extent of crustal magnetic sources corresponds to the temperature
at which rocks lose their spontaneous magnetization (e.g., 580°C for magnetite). They usually operate in
the Fourier domain by analyzing the shape of the power-density spectrum calculated from aeromagnetic
anomalies and critically depend on assumptions about the distribution of crustal magnetization. Early methods
assumed that crustal magnetization is a completely random function of position characterized by a flat power-
density spectrum. In this study, we attempted to incorporate more realistic geologic models for crustal
magnetization and applied the method to newly released aeromagnetic compilations for Nevada and North
America. We assume that crustal magnetization has fractal properties, as suggested previously by others, so that
the power-density spectrum of the magnetization is proportional to the wavenumber raised to a power -β,
where β is related to the geologic terrane. In this case, the theoretical power spectrum, as derived by Maus
et al. (Geophys. J. Int., 129, 163-168, 1997), depends on three independent parameters: the depths to the top and
bottom of the magnetic source layer and the fractal exponent β. We estimate these parameters by first
calculating a three-dimensional matrix representing the misfit between the power spectrum computed from
observed data and a variety of theoretical spectra calculated from a range of realistic parameter values. We then
search the matrix for the set of parameters that leads to the minimum misfit. This operation was performed on
overlapping sliding windows that were swept across the entire magnetic map. A matrix was developed for each
window, thereby providing lateral variations in the depth to the bottom of magnetic sources. We tested this
methodology on synthetic aeromagnetic data and applied it to aeromagnetic compilations from the Great Basin.
Preliminary results obtained by assuming β is constant throughout the Great Basin show spatial variations
in the depth to the bottom of magnetic sources that, in general, do not depend on the assumed value of β or
on the size of the window. However, our observed variations also do not correlate to large extent with observed
surface heat-flow anomalies. They may reflect real variations in crustal magnetic thickness, due either to
undulations of the depth to the Curie-temperature isotherm not reflected in surface heat-flow measurements, or
to lateral variations of shallower magnetic interfaces. Alternatively, they may be artifacts caused by variations in
geologic terrane (i.e., variations in β). Future studies will attempt to include β explicitly, using
mapped geology as a guide to help distinguish which of the observed patterns reflect real variations in depth to
Curie-temperature isotherm.
DE: 1517 Magnetic anomalies: modeling and interpretation
DE: 1545 Spatial variations: all harmonics and anomalies
DE: 5418 Heat flow
SC: Geomagnetism and Paleomagnetism [GP]
MN: 2007 Fall Meeting