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Crustal magnetization Kathy Whaler University of Edinburgh

Crustal magnetization

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Crustal magnetization. Kathy Whaler University of Edinburgh. Why study the Martian Magnetic Field?. Satellite data - Earth. Earth POGO (1960s and 1970s): scalar field MAGSAT (1979/80): vector Ørsted (current): vector (high altitude) - PowerPoint PPT Presentation

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Page 1: Crustal magnetization

Crustal magnetization

Kathy Whaler

University of Edinburgh

Page 2: Crustal magnetization

Why study the Martian Magnetic Field?

Page 3: Crustal magnetization
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Satellite data - Earth

• Earth– POGO (1960s and 1970s): scalar field – MAGSAT (1979/80): vector– Ørsted (current): vector (high altitude)– CHAMP (current): vector, but I’ve just worked

with scalar data so far

• Need to extract small crustal anomaly field from data dominated by the main field

Page 5: Crustal magnetization

Scalar data

• The anomaly field is a tiny fraction of the main field generated in the core, Bc

• Thus we can linearize the relationship between the scalar and vector fields:

• Hence any methods developed to treat vector data will work with minor modifications on scalar data

)(c

η

)(

c

BBB

1B

Page 6: Crustal magnetization

Satellite data - Mars• Mars Global Surveyor

– current– vector– aerobraking phase provided data as low as 120km

above surface– used data in the 120-600km altitude range

• No main field– field is due to remanent magnetization of the crust

and external field– difficult to use scalar data

Page 7: Crustal magnetization

Martian magnetic field

• The internal magnetic field amplitude is surprisingly high

• The field is much stronger over the heavily cratered region south of the dichotomy

• Greater external field contamination in the horizontal components

Page 8: Crustal magnetization
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Data and Technique• Low-altitude coverage is sparse, suitable for

analysis to degree 50 globally.• Spatially varying magnetization, linear

combination of Green’s functions relating predicted magnetization to observed magnetic field.

• Minimize RMS magnetization within the Martian crust.

• Data by data information matrix is sparse (preconditoned CG).

• Damping controls relative importance of fit and RMS magnetization.

Page 10: Crustal magnetization
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Methodology

• Relate a magnetic field satellite measurement to the magnetic field or magnetization in the crust, e.g.

V jjjj

dVB )(.),(.ˆ)()()( sMsrHlr

r

where (η) denotes the component, rj is the satellite datum position, s positionwithin the magnetized crust, H a known geometrical function, and M magnetization

Page 12: Crustal magnetization

Methodology

• Express the model as a linear combination of the data kernels

• Find the multipliers that minimize e.g.

so-called minimum norm solutions

• Hence model continuously-varying functions, either downward continued B, or M within the crust

dVV

2M

Page 13: Crustal magnetization

Numerical considerations

• Minimum norm solutions require solving a data-by-data system of equations - too big

• Reduce by:– expanding in terms of data kernels at a limited

number of points– taking advantage of peaked nature of data

kernels - matrix effectively sparse• Calculation parallelises effectively• Use iterative conjugate gradient algorithm on

resulting sparse system• Improve convergence by Jacobi preconditioning

Page 14: Crustal magnetization

Green’s function showing how the surface magnetic field contributes to a satellite measurement at 400km altitude. Solid/dashed line: vertical/horizontal component

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Its interpretation

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A magnetic chronology

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Interpretation caveats

• Residuals to our model are strongly non-normal: external fields and unmodelled sources

• Varying misfit by a factor of 3 alters the RMS magnetization by two orders of magnitude: model does not constrain magnetization strength, only direction

Page 27: Crustal magnetization

Comparison with other magnetization models

•Discrete model of magnetization (Langlais et al., 2003): correlation coefficients are in excess of 0.8.

•Ideal body theory (Parker, 2003) demonstrates that magnetization must be at least 4.76 A/m for a 50 km thick crust.

•Ten isolated bodies described by Arkani-Hamed and Boutin (2003): Five of their ten paleomagnetic poles are within 30º of our poles. The others are at angular distances of 32º, 41º, 59º, 66º and 69º.

Page 28: Crustal magnetization

Power spectra for downward continued Magsat model (diamonds) and aeromagnetic compilation (crosses) over Africa

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This rendition of the North American

compilation has had wavelenths longer

than 500 km replaced with the

Comprehensive model (Sabaka et al., 2002), utilizing a technique

developed by Ravat et al. (2002). The data is

on a 1 km grid projected with a

spherical transverse Mercator. The grid

size is 8901 by 8511.

Page 38: Crustal magnetization
Page 39: Crustal magnetization

Inversion for magnetization

directions based on satellite and near-

surface data

Page 40: Crustal magnetization

Depth-independent magnetization

• Satellite data ‘see’ magnetized crust as a thin sheet

no point in trying to resolve depth dependence• Allowing depth variation seems to cause

problems when integrating aeromagnetic data• Almost finished implementing code to calculate M constant with depth through magnetized layer

Page 41: Crustal magnetization

Conclusions

• Satellite data have provided a new perspective on the magnetic fields of both Earth and Mars

• The long wavelength crustal magnetization of both planets aids structural and tectonic interpretation