Current and SAR induced in a human head model by the electromagnetic fields irradiated from a cellular phone

The near field finite-difference time-domain method was used to calculate the current and specific absorption rate (SAR) distributions in an inhomogeneous model of a human head exposed to the electromagnetic waves irradiated from a cellular phone. The human head was simulated by a model of 57,263 block cells with inhomogeneous dielectric constant and conductivity. The cellular phone was modeled by an equivalent dipole antenna with an equivalent resistor of 120 ohms located at the center gap between the two arms of this dipole antenna. The transmitted power of the cellular phone was assumed to be 0.6 watts at a frequency of 835 MHz. For the head near the dipole antenna in the range of 1.0/spl sim/2.5 cm, the maximum currents and SAR's induced in the head were found in the ranges of 356/spl sim/551 mA and 1.23/spl sim/2.63 W/kg, respectively. It was also found that the maximum SAR induced in the head was below the IEEE's upper safety limit of 1.6 W/kg for the head to keep a distance from the dipole antenna by longer than 2.0 cm. >

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

[2]  R. Luebbers,et al.  FDTD calculation of wide-band antenna gain and efficiency , 1992 .

[3]  C.H. Durney,et al.  Computer-aided design of two dimensional electric-type hyperthermia applicators using the finite-difference time-domain method , 1991, IEEE Transactions on Biomedical Engineering.

[4]  G. Mur Absorbing Boundary Conditions for the Finite-Difference Approximation of the Time-Domain Electromagnetic-Field Equations , 1981, IEEE Transactions on Electromagnetic Compatibility.

[5]  Raj Mittra,et al.  A study of the nonorthogonal FDTD method versus the conventional FDTD technique for computing resonant frequencies of cylindrical cavities , 1992 .

[6]  A. Taflove,et al.  Computation of the Electromagnetic Fields and Induced Temperatures Within a Model of the Microwave-Irradiated Human Eye , 1975 .

[7]  C. Taylor,et al.  Electromagnetic pulse scattering in time-varying inhomogeneous media , 1969 .

[8]  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.

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

[10]  W. Scott,et al.  Accurate computation of the radiation from simple antennas using the finite-difference time-domain method , 1989, Digest on Antennas and Propagation Society International Symposium.

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

[12]  O. Gandhi,et al.  Currents induced in an anatomically based model of a human for exposure to vertically polarized electromagnetic pulses , 1991 .

[13]  Cynthia Furse,et al.  Improvements to the finite-difference time-domain method for calculating the radar cross section of a perfectly conducting target , 1990 .

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

[15]  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.

[16]  P.J. Dimbylow Finite-difference time-domain calculations of absorbed power in the ankle for 10-100 MHz plane wave exposure , 1991, IEEE Transactions on Biomedical Engineering.