The complete ellipsoidal shell-model in EEG imaging

This work provides the solution of the direct Electroencephalography (EEG) problem for the complete ellipsoidal shell-model of the human head. The model involves four confocal ellipsoids that represent the successive interfaces between the brain tissue, the cerebrospinal fluid, the skull, and the sk...

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Main Authors: S. N. Giapalaki, F. Kariotou
Format: Article
Language:English
Published: Hindawi Limited 2006-01-01
Series:Abstract and Applied Analysis
Online Access:http://dx.doi.org/10.1155/AAA/2006/57429
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spelling doaj-99f9edd6b3904636bfbbb8a131bc878b2020-11-24T20:58:43ZengHindawi LimitedAbstract and Applied Analysis1085-33751687-04092006-01-01200610.1155/AAA/2006/5742957429The complete ellipsoidal shell-model in EEG imagingS. N. Giapalaki0F. Kariotou1Department of Chemical Engineering, University of Patras, Patras 26504, GreeceHellenic Open University, 16, Sahtouri Street & Ag. Andreou Street, Patras 262 22, GreeceThis work provides the solution of the direct Electroencephalography (EEG) problem for the complete ellipsoidal shell-model of the human head. The model involves four confocal ellipsoids that represent the successive interfaces between the brain tissue, the cerebrospinal fluid, the skull, and the skin characterized by different conductivities. The electric excitation of the brain is due to an equivalent electric dipole, which is located within the inner ellipsoid. The proposed model is considered to be physically complete, since the effect of the substance surrounding the brain is taken into account. The direct EEG problem consists in finding the electric potential inside each conductive space, as well as at the nonconductive exterior space. The solution of this multitransmission problem is given analytically in terms of elliptic integrals and ellipsoidal harmonics, in such way that makes clear the effect that each shell has on the next one and outside of the head. It is remarkable that the dependence on the observation point is not affected by the presence of the conductive shells. Reduction to simpler ellipsoidal models and to the corresponding spherical models is included.http://dx.doi.org/10.1155/AAA/2006/57429
collection DOAJ
language English
format Article
sources DOAJ
author S. N. Giapalaki
F. Kariotou
spellingShingle S. N. Giapalaki
F. Kariotou
The complete ellipsoidal shell-model in EEG imaging
Abstract and Applied Analysis
author_facet S. N. Giapalaki
F. Kariotou
author_sort S. N. Giapalaki
title The complete ellipsoidal shell-model in EEG imaging
title_short The complete ellipsoidal shell-model in EEG imaging
title_full The complete ellipsoidal shell-model in EEG imaging
title_fullStr The complete ellipsoidal shell-model in EEG imaging
title_full_unstemmed The complete ellipsoidal shell-model in EEG imaging
title_sort complete ellipsoidal shell-model in eeg imaging
publisher Hindawi Limited
series Abstract and Applied Analysis
issn 1085-3375
1687-0409
publishDate 2006-01-01
description This work provides the solution of the direct Electroencephalography (EEG) problem for the complete ellipsoidal shell-model of the human head. The model involves four confocal ellipsoids that represent the successive interfaces between the brain tissue, the cerebrospinal fluid, the skull, and the skin characterized by different conductivities. The electric excitation of the brain is due to an equivalent electric dipole, which is located within the inner ellipsoid. The proposed model is considered to be physically complete, since the effect of the substance surrounding the brain is taken into account. The direct EEG problem consists in finding the electric potential inside each conductive space, as well as at the nonconductive exterior space. The solution of this multitransmission problem is given analytically in terms of elliptic integrals and ellipsoidal harmonics, in such way that makes clear the effect that each shell has on the next one and outside of the head. It is remarkable that the dependence on the observation point is not affected by the presence of the conductive shells. Reduction to simpler ellipsoidal models and to the corresponding spherical models is included.
url http://dx.doi.org/10.1155/AAA/2006/57429
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