Fractional Derivatives Based Scheme for FDTD Modeling of nth-Order Cole-Cole Dispersive Media

被引:20
|
作者
Abdullah, Haythem Hussein [1 ]
Elsadek, H. A. [1 ]
ElDeeb, H. E. [1 ]
Bagherzadeh, N. [2 ]
机构
[1] Elect Res Inst, Giza 12622, Egypt
[2] Univ Calif Irvine, Henri Samuli Sch Engn, Dept Elect Engn & Comp Sci, Irvine, CA 92697 USA
关键词
Cole-Cole model; dispersive media; finite-difference time domain (FDTD); fractional derivatives; WAVE-PROPAGATION;
D O I
10.1109/LAWP.2012.2190029
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
A finite-difference time-domain (FDTD) modeling of the wave propagation in a Cole-Cole dispersive media is presented. Since the empirical Debye and Lorentz models are not accurate for the representation of the frequency dependence of some dispersive media terms, the Cole-Cole dispersion relation was used to model the electromagnetic properties of biological tissues. The main problem in time-domain modeling of the Cole-Cole model is the approximation of the fractional derivatives that appear in the model equation. Researchers face this problem by approximating the Cole-Cole terms (poles) by a sum of Debye terms or by a sum of decaying exponentials or by polynomials. The accuracy of these models depends on the number of terms needed to model each Cole-Cole term, which may consume large amounts of time and memory. In this letter, all the FDTD fields are approximated by a linear function of time that has a closed form for its fractional derivative. The proposed scheme is considered the more general scheme that has the capability to model nth-order Debye and Cole-Cole models. The scheme is a straightforward extension that can deal with other models such as Lorenz, Drude, and the chiral media. Promising results are observed when calculating the reflection coefficient at an air/muscle material interface. The SAR distribution within a Cole-Cole equivalent brain spherical material excited by an infinitesimal dipole is calculated and compared to the normal FDTD at 900 MHz.
引用
收藏
页码:281 / 284
页数:4
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