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

ABSTRACT @F>D+=hS  
This book presents a method that allows the use of multiresolution principles in n+p }\msH  
a time domain electromagnetic modeling technique that is applicable to general x1<|hTPk  
structures. The multiresolution time-domain (MRTD) technique, as it is often ,: ^u-b|  
called, is presented for general basis functions. Additional techniques that are presented Fzcwy V   
here allow the modeling of complex structures using a subcell representation +|f@^-  
that permits the modeling discrete electromagnetic effects at individual equivalent ?A0)L27UE&  
grid points. This is accomplished by transforming the application of the effects at }B^tL$k  
individual points in the grid into the wavelet domain. fV~~J2IK  
In this work, the MRTD technique is derived for a general wavelet basis CGFDqCNr-  
using a relatively compact vector notation that both makes the technique easier 6~+
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to understand and illustrates the differences between MRTD basis functions. In X-/]IHDN  
addition, techniques such as the uniaxial perfectly matched layer (UPML) for arbitrary wavelet resolution and non-uniform gridding are presented. Using these 'fW-Y!k%  
techniques, any structure that can be simulated in Yee-FDTD can be modeled (?];VG  
with in MRTD. ; @X<lCk  
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MRTD(Multi Resolution Time Domain) Method in Electromagnetics 54/=G(F  
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part2

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ABSTRACT ]iWRo'  
This book presents a method that allows the use of multiresolution principles in @ZJS&23E  
a time domain electromagnetic modeling technique that is applicable to general YR70BOxK  
structures. The multiresolution time-domain (MRTD) technique, as it is often Zfw,7am/  
called, is presented for general basis functions. Additional techniques that are presented KoRV%@I  
here allow the modeling of complex structures using a subcell representation rjP/l6 ~'  
that permits the modeling discrete electromagnetic effects at individual equivalent 7^Uv7<pw  
grid points. This is accomplished by transforming the application of the effects at "7 yD0T)2  
individual points in the grid into the wavelet domain. >~f]_puT  
In this work, the MRTD technique is derived for a general wavelet basis 2!\DPX  
using a relatively compact vector notation that both makes the technique easier JT?h1v<H]  
to understand and illustrates the differences between MRTD basis functions. In 2eogY#  
addition, techniques such as the uniaxial perfectly matched layer (UPML) for arbitrary wavelet resolution and non-uniform gridding are presented. Using these QPx^_jA  
techniques, any structure that can be simulated in Yee-FDTD can be modeled m'U0'}Ld};  
with in MRTD. =D(j)<9$A  
y7{?Ip4[  
KEYWORDS xo)P?-  
Adaptive Algorithms, MRTD, Wavelets, Adaptive Electromagnetic simulations, RFGff
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Time-/Space-adaptive gridding

MRTD(Multi Resolution Time Domain) Method in Electromagnetics是好书 Wc#24:OKe3  
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