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1/29/98 119 C95.3-1991 Revision — 2 nd Draft<br />

10/98 Draft<br />

D5.2 Extended-Boundary-Condition Method (EBCM).<br />

The EBCM is a matrix <strong>for</strong>mulation based on an integral equation <strong>and</strong> expansion of the<br />

EM-fields in spherical harmonics. This method was developed by Waterman [D21] <strong>and</strong><br />

has subsequently been used to calculate the SAR in prolate spheroidal models of<br />

humans <strong>and</strong> animals [D1]. The EBCM is exact within the limits of numerical computation<br />

capabilities, but numerical problems presently limit the method to frequencies below<br />

about 80 MHz <strong>for</strong> prolate spheroidal models of humans. In SAR calculations <strong>for</strong> prolate<br />

spheroidal models of humans, the long-wavelength approximation <strong>and</strong> the EBCM give<br />

identical results up to about 30 MHz, where the long-wavelength approximation begins to<br />

become inaccurate.<br />

D5.3 Iterative Extended-Boundary-Condition Method (IEBCM).<br />

The EBCM has been extended [D11] to a technique called the IEBCM, that is capable of<br />

SAR calculations in prolate spheroidal models of man up to at least 400 MHz. The<br />

IEBCM is different from the EBCM in two main respects. It makes use of more than one<br />

spheroidal harmonic expansion, which allows better convergence <strong>for</strong> elongated bodies at<br />

higher frequencies, <strong>and</strong> it uses iteration, beginning with an approximate solution, to<br />

converge to the solution. These two features of the IEBCM have significantly extended<br />

the range of calculations over that of the EBCM.<br />

D5.4 The Cylindrical Approximation.<br />

The SAR calculated <strong>for</strong> an appropriately long section of an infinitely long cylinder is a<br />

good approximation to the SAR of spheroids in the frequency range where the<br />

wavelength is very short compared with the length of the spheroid. The lowest frequency<br />

at which the approximation is useful depends both on the length of the spheroid <strong>and</strong> on<br />

the ratio of the major axis to the minor axis. For man-sized spheroids, the lower<br />

frequency limit occurs <strong>for</strong> E-polarization when the wavelength is about four-tenths of the<br />

length of the spheroid [D14].<br />

D5.5 Moment-Method Solution.<br />

A moment-method solution of a Green's-function integral equation <strong>for</strong> the electric field<br />

has been used to calculate the internal electric field in block models, so-called because<br />

the mathematical cells of which the model is composed are cubes [D4, D6]. Wholebody<br />

average SARs calculated by this method are very close to those calculated <strong>for</strong><br />

spheroidal models. Although the block model has the advantage that it resembles the<br />

human body better than a spheroid because it has simulated arms, legs, <strong>and</strong> head, the<br />

calculations of the spatial distribution of the internal fields made with the above method<br />

have been found to be of varying accuracy depending on the location of the cell in<br />

question [D15]. Apparently, the calculations are of limited accuracy because the electric<br />

field in each mathematical cell is approximated by a constant, <strong>and</strong> this approximate field<br />

cannot satisfy the boundary conditions <strong>for</strong> cells that touch the curved surface of<br />

interfaces between two dissimilar dielectric materials, or the surface of the body (airtissue<br />

boundary). An improved moment-method uses tetrahedra as mathematical cells<br />

[D18]. Special basis functions are defined within the tetrahedral volume elements to<br />

insure that the normal electric field satisfies the correct conditions at interfaces between<br />

different dielectric media.<br />

Hagmann [D7] has developed improved means <strong>for</strong> predicting regionally averaged SAR<br />

using the block model of man, with the moment-method technique. Since individual<br />

Copyright © 1998 IEEE. All rights reserved. This is an unapproved IEEE St<strong>and</strong>ards Draft,<br />

subject to change.

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