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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Slob, Evert
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Topics
Publications (8/8 displayed)
- 2022Physically Constrained 2D Joint Inversion of Surface and Body Wave Tomographycitations
- 2018Theory for 1D full waveform inversion of surface GPR data
- 2016Original and pyrometamorphical altered Bentheimer sandstonecitations
- 2015Determination, by using GPR, of the volumetric water content in structures, substructures, foundations, and soilcitations
- 2011Reconstruction of sub-wavelength fractures and physical properties of masonry media full-waveform inversion of proximal penetrating radarcitations
- 2010Stochastic joint inversion of 2D seismic and seismoelectric signals in linear poroelastic materials: A numerical investigationcitations
- 2007Capillary pressure as a unique function of electric permittivity and water saturationcitations
- 2006Estimating electric permittivity from GPR surface reflection data for water content estimatescitations
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document
Theory for 1D full waveform inversion of surface GPR data
Abstract
In one dimension, full waveform inversion is shown to be a linear problem under several conditions. I show that if the magnetic permeability can be assumed constant and electric conductivity to be zero, measuring the magnetic field at the surface or in the air suffices as input data. I present the theory using integral equations that describe the electric field inside the medium in terms of contrast sources. The electric field inside the medium can be computed from the measured magnetic field by solving a Marchenko equation. Once this field is known only the contrast function is unknown and can be found by matrix inversion. If the electric field is also measured the inverse problem can be solved recursively. In one dimension depth is intrinsically unknown and I use recording time as a replacing coordinate. After the electric permittivity is known as a function of one-way travel time from surface to a depth level inside the medium, the depth level can be found by an integral. This produces electric permittivity as a function of depth and full waveform inversion is complete. A simple numerical example demonstrates the method.