[FDTD][eBook]MRTD(Multi Resolution Time Domain) Method in Electromagnetics

ABSTRACT Pa8E.<>  
This book presents a method that allows the use of multiresolution principles in a&?SRC'x  
a time domain electromagnetic modeling technique that is applicable to general vzr?#FG  
structures. The multiresolution time-domain (MRTD) technique, as it is often mHiV};$  
called, is presented for general basis functions. Additional techniques that are presented 6G^x%s  
here allow the modeling of complex structures using a subcell representation Rfk8trD B  
that permits the modeling discrete electromagnetic effects at individual equivalent 2!7)7wlj0  
grid points. This is accomplished by transforming the application of the effects at \Y4>_Mk  
individual points in the grid into the wavelet domain. T@S\:P  
In this work, the MRTD technique is derived for a general wavelet basis W$I^Ej}>$  
using a relatively compact vector notation that both makes the technique easier 9}=]oX!+V  
to understand and illustrates the differences between MRTD basis functions. In #jc+2F,+{  
addition, techniques such as the uniaxial perfectly matched layer (UPML) for arbitrary wavelet resolution and non-uniform gridding are presented. Using these '#;%=+=;  
techniques, any structure that can be simulated in Yee-FDTD can be modeled EINjI:/D  
with in MRTD. .:`+4n  
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MRTD(Multi Resolution Time Domain) Method in Electromagnetics jHU5>Gt-}  
5i<E AKL  
part2

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ABSTRACT `Cv@16  
This book presents a method that allows the use of multiresolution principles in p?#%G`dm  
a time domain electromagnetic modeling technique that is applicable to general _ft)e3Gf  
structures. The multiresolution time-domain (MRTD) technique, as it is often ,xzSFs>2  
called, is presented for general basis functions. Additional techniques that are presented IuW5LS  
here allow the modeling of complex structures using a subcell representation EYaX@|)  
that permits the modeling discrete electromagnetic effects at individual equivalent Fb^Ae6/i  
grid points. This is accomplished by transforming the application of the effects at (UGmbRf&  
individual points in the grid into the wavelet domain.
Li{R?Osx  
In this work, the MRTD technique is derived for a general wavelet basis )2YZ [~3  
using a relatively compact vector notation that both makes the technique easier Bt?.8H6Y  
to understand and illustrates the differences between MRTD basis functions. In :8CYTEc  
addition, techniques such as the uniaxial perfectly matched layer (UPML) for arbitrary wavelet resolution and non-uniform gridding are presented. Using these YZHqy++x  
techniques, any structure that can be simulated in Yee-FDTD can be modeled f'-) 3T  
with in MRTD. @8$3Q,fF(  
l(fStpP  
KEYWORDS V1 :aR3*!  
Adaptive Algorithms, MRTD, Wavelets, Adaptive Electromagnetic simulations, "x"y3v'  
Time-/Space-adaptive gridding

MRTD(Multi Resolution Time Domain) Method in Electromagnetics是好书 TM1D|H  
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