dc.contributor.author |
Uzunoglu, NK |
en |
dc.contributor.author |
Angelikas, EA |
en |
dc.date.accessioned |
2014-03-01T01:06:52Z |
|
dc.date.available |
2014-03-01T01:06:52Z |
|
dc.date.issued |
1987 |
en |
dc.identifier.issn |
0018926X |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/9647 |
|
dc.subject |
Human Body Model |
en |
dc.subject.other |
ANTENNAS, LOOP - Radiation |
en |
dc.subject.other |
HUMAN FORM MODELS - Radiation Effects |
en |
dc.subject.other |
MATHEMATICAL TECHNIQUES - Boundary Value Problems |
en |
dc.subject.other |
MODE-MATCHING PROCEDURE |
en |
dc.subject.other |
SPHEROIDAL WAVE FUNCTIONS |
en |
dc.subject.other |
THREE-LAYER PROLATE SPHEROIDAL HUMAN BODY MODEL |
en |
dc.subject.other |
ELECTROMAGNETIC FIELD EFFECTS |
en |
dc.title |
FIELD DISTRIBUTIONS IN A THREE-LAYER PROLATE SPHEROIDAL HUMAN BODY MODEL FOR A LOOP ANTENNA IRRADIATION. |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1109/TAP.1987.1143991 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1109/TAP.1987.1143991 |
en |
heal.publicationDate |
1987 |
en |
heal.abstract |
Analysis of the field distributions in a three-layer prolate spheroidal human body model is described for loop antenna irradiation. The loop radiator is assumed to be placed symmetrically with respect to the spheroid axis. Spheroidal wave functions are used to expand the field components inside and outside of the prolate spheroid. The boundary conditions on the interface layers are satisfied by using a mode-matching procedure. The loop radiator can be very close to the human body. Numerical results are given for a frequency of 13 MHz. |
en |
heal.journalName |
IEEE Transactions on Antennas and Propagation |
en |
dc.identifier.doi |
10.1109/TAP.1987.1143991 |
en |
dc.identifier.volume |
AP-35 |
en |
dc.identifier.issue |
10 |
en |
dc.identifier.spage |
1180 |
en |
dc.identifier.epage |
1185 |
en |