RF currents induced in an anatomically-based model of a human for plane-wave exposures (20-100 MHz).

The three-dimensional finite-difference time-domain (FDTD) method has been used to calculate local, layer-averaged and whole-body averaged specific absorption rates (SARs) and internal radiofrequency (RF) currents in a 5628-cell, anatomically-based model of a human for plane-wave exposures from 20-100 MHz. The conditions of exposure of the human considered are: 1) isolated from ground, and 2) feet in contact with ground. Also considered are various separations of the model from ground and the use of insulating, rubber-soled footwear close to the grounded resonance frequency of 45 MHz. The calculated results are in agreement with the experimental data of Hill and others. While the existence of large foot currents has been known previously, substantial RF currents (600-800 mA) induced over much of the body are obtained for E-polarized fields suggested in the 1982 ANSI RF safety guideline.

[1]  J. Mautz Reviews and abstracts - Computer program for the Mie series solution for a sphere , 1978, IEEE Antennas and Propagation Society Newsletter.

[2]  Allen Taflove,et al.  Application of the Finite-Difference Time-Domain Method to Sinusoidal Steady-State Electromagnetic-Penetration Problems , 1980, IEEE Transactions on Electromagnetic Compatibility.

[3]  Om P. Gandhi,et al.  Use of the Finite-Difference Time-Domain Method in Calculating EM Absorption in Human Tissues , 1987, IEEE Transactions on Biomedical Engineering.

[4]  Stuchly,et al.  DIELECTRIC PROPERTIES OF BIOLOGICAL SUBSTANCES–TABULATED , 1980 .

[5]  R. Holland THREDE: A Free-Field EMP Coupling and Scattering Code , 1977, IEEE Transactions on Nuclear Science.

[6]  O. Gandhi,et al.  Numerical calculation of electromagnetic energy deposition in models of man with grounding and reflector effects , 1979 .

[7]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[8]  A. Taflove,et al.  Use of the finite-difference time-domain method for calculating EM absorption in man models , 1988, IEEE Transactions on Biomedical Engineering.

[9]  Om P. Gandhi,et al.  Calculation of EM power deposition for operator exposure to RF induction heaters , 1988 .

[10]  Om P. Gandhi,et al.  Electromagnetic deposition in an anatomically based model of man for leakage fields of a parallel-plate dielectric heater , 1989 .

[11]  A. Guy,et al.  Nonionizing electromagnetic wave effects in biological materials and systems , 1972 .

[12]  O. Gandhi,et al.  Currents Induced in a Human Being for Plane-Wave Exposure Conditions 0-50 MHz and for RF Sealers , 1986, IEEE Transactions on Biomedical Engineering.

[13]  Allen Taflove,et al.  A Novel Method to Analyze Electromagnetic Scattering of Complex Objects , 1982, IEEE Transactions on Electromagnetic Compatibility.

[14]  O. Gandhi,et al.  Likelihood of high rates of energy deposition in the human legs at the ANSI recommended 3-30-MHz RF safety levels , 1985, Proceedings of the IEEE.

[15]  A. C. Eycleshymer,et al.  A cross-section anatomy , 1970 .

[16]  Karl Kunz,et al.  A Three-Dimensional Finite-Difference Solution of the External Response of an Aircraft to a Complex Transient EM Environment: Part I-The Method and Its Implementation , 1978, IEEE Transactions on Electromagnetic Compatibility.