An Equivalent Source Method for Modelling the Lithospheric Magnetic Field Using Satellite and Airborne Magnetic Data

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Downloaded from orbit.dtu.dk on: Oct 03, 2018 An Equivalent Source Method for Modelling the Lithospheric Magnetic Field Using Satellite and Airborne Magnetic Data Kother, Livia Kathleen; D. Hammer, Magnus; C. Finlay, Christopher; Olsen, Nils Publication date: 2015 Document Version Peer reviewed version Link back to DTU Orbit Citation (APA): Kother, L. K., D. Hammer, M., C. Finlay, C., & Olsen, N. (2015). An Equivalent Source Method for Modelling the Lithospheric Magnetic Field Using Satellite and Airborne Magnetic Data [Sound/Visual production (digital)]. 2014 AGU Fall Meeting, San Francisco, CA, United States, 15/12/2014 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim.

An Equivalent Source Method for Modelling the Lithospheric Magnetic Field Using Satellite and Airborne Magnetic Data Livia Kother 1, Magnus D. Hammer 2, Christopher C. Finlay 1, Nils Olsen 1 1 Division of Geomagnetism, DTU Space, Technical University of Denmark Diplomvej, Building 371, 2800 Kgs. Lyngby, Denmark 2 Copenhagen, Denmark

Importance of lithospheric magnetic field models Lithospheric structure and composition Resource exploration Directional drilling High resolution models require combination of both satellite and airborne/marine measurements http://geomag.org/models/wdmam.html

Applied Geomagnetic Data Satellite data Airborne data www.ngu.no Data combination Global field structure defined by satellite data http://www.astrium.eads.net/en/programme/champ-cta.html CHAMP Solar quiet period Altitude ~ 300 km Global model Resolution ~ 400 km Local surveys Norwegian coast Local model Resolution ~ 5 km Local high resolution data provided by airborne data Better description of short wavelength structures

Applied Modelling Method - Equivalent Sources Model values are transferable to spherical harmonic representation Icosahedron grid of magnetic point sources q Divergence-free constraint

Inverse Modelling Scheme Observed magnetic field data Removal of core and large-scale magnetospheric sources + data selection Estimate of lithospheric field at measurement location Combination with icosahedron grid of equivalent sources Inverse modelling (regularized IRLS algorithm) to determine model values

Model Estimation Uniqueness problem regularization

Model Result: CHAMP Data Quadratic Regularization

Model Result: CHAMP Data Entropy Regularization

Model Result: CHAMP Data RMS misfit Br = 1,6051 nt = 1,6079 nt = 1,6625 nt

Model Result: Airborne Data Survey 1 - Viking Year: 1993 Sensor elevation: 150 m Line spacing: 0.5 2 km Survey 2 - Fairey Year: 1971 Sensor elevation: 500 m Line spacing: 2 7,5 km Aeromagnetic survey data are kindly provided by NGU

Model Result: Airborne Data Modelled values [nt] at Earth surface

Conclusion Lithospheric field modelling based on equivalent potential field source estimation Robust, regularized, least squares estimation scheme Successful tests using satellite data on a global scale and local airborne data Advantages of the method: Combined local and global applications are possible Model regularization can be easily implemented Downward / upward continuation Method is not sensitive to polar gap problem

Swarm mission www.esa.int Launched: 22th Nov 2013 Mission duration: 4yrs Orbit: 2 satellites orbit side-byside at an initial altitude of 460 km, decaying naturally to 300 km; the third satellite orbits at about 530 km Instruments: Vector field magnetometer, absolute scalar magnetometer, electric field instrument, accelerometer, GPS receiver, startrackers and laser retroreflector