Abstract
Physical principles of electric field tomography—a contactless method making it possible to obtain, using a quasi-static electric field, information about the spatial distribution of the conductivity and permittivity of an object—are considered. Features of this method are discussed, a planar system is simulated, and the results obtained are analyzed.
References
Korjenevsky, A.V., Radiotekh. Elektron. (Moscow), 2004, vol. 49, no. 6, p. 761.
Korjenevsky, A.V., Physiol. Meas., 2005, vol. 26, no. 2, p. 101.
Korjenevsky, A.V., Physiol. Meas., 2004, vol. 25, no. 1, p. 391.
Korjenevsky A., Tuykin T., Proc. 7th Conf. Biomedical Applications of Electrical Impedance Tomography, Seoul, 2006, p. 177.
Korjenevsky, A.V., and Tuikin, T.S., Biomed. Tekhnol. Radioelektron., 2007, no. 1, p. 60.
Gabriel, C. and Gabriel, S., Report of Physics Department, King’s College, London, 1996, no. AL/OE-TR-1996-0037; http://www.brooks.af.mil/AFRL/HED/hedr/reports/dielectric.
FTDTRro Program for Finite-Difference Simulation; http://zfdtd.narod.ru.
Author information
Authors and Affiliations
Corresponding author
Additional information
Original Russian Text © A.V. Korjenevsky, T.S. Tuykin, 2008, published in Izvestiya Rossiiskoi Akademii Nauk. Seriya Fizicheskaya, 2008, Vol. 72, No. 1, pp. 100–103.
About this article
Cite this article
Korjenevsky, A.V., Tuykin, T.S. Planar measuring system for experiments on electric-field tomography. Bull. Russ. Acad. Sci. Phys. 72, 89–92 (2008). https://doi.org/10.3103/S1062873808010218
Published:
Issue Date:
DOI: https://doi.org/10.3103/S1062873808010218