How to design the imperfect Berenger PML

被引:16
作者
Wittwer, DC
Ziolkowski, RW
机构
[1] Electromagnetics Laboratory, Department of Electrical and Computer Engineering, University of Arizona, Tucson, AZ
关键词
D O I
10.1080/02726349608908491
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
In contrast to the previously popular second order Mur absorbing boundary condition (ABC), the recently introduced Berenger Perfectly Matched Layer (PML) ABC can be designed to lower the numerical reflection coefficient associated with mesh truncation by several orders in magnitude. Nonetheless the PML ABC is not perfect; it does have a numerical reflection coefficient. This reflection coefficient is characterized in the time and frequency domains for narrow and broad bandwidth pulses from several points of view including specifically its behavior in terms of the magnitude of the loss tangent in the PML and the thickness of the PML. It is demonstrated that for broad bandwidth pulses the PML ABC exhibits a low frequency increase in its reflection coefficient that is associated with the actual thickness of the PML layer in terms of the longest wavelengths contained in the signal incident upon it. Moreover, it is shown that the effectiveness of the PML ABC saturates when the loss parameters of the PML are significantly increased and that this behavior is connected with the size of the first discontinuity in the material properties encountered by a pulse as it propagates into the PML region. An optimal operating point for the design of the PML region is thus obtained.
引用
收藏
页码:465 / 485
页数:21
相关论文
共 10 条
[1]   A COMPARISON OF THE BERENGER PERFECTLY MATCHED LAYER AND THE LINDMAN HIGHER-ORDER ABCS FOR THE FDTD METHOD [J].
ANDREW, WV ;
BALANIS, CA ;
TIRKAS, PA .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1995, 5 (06) :192-194
[2]   A PERFECTLY MATCHED LAYER FOR THE ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
BERENGER, JP .
JOURNAL OF COMPUTATIONAL PHYSICS, 1994, 114 (02) :185-200
[3]   A 3D PERFECTLY MATCHED MEDIUM FROM MODIFIED MAXWELLS EQUATIONS WITH STRETCHED COORDINATES [J].
CHEW, WC ;
WEEDON, WH .
MICROWAVE AND OPTICAL TECHNOLOGY LETTERS, 1994, 7 (13) :599-604
[4]   VALIDATION AND EXTENSION TO 3 DIMENSIONS OF THE BERENGER PML ABSORBING BOUNDARY-CONDITION FOR FD-TD MESHES [J].
KATZ, DS ;
THIELE, ET ;
TAFLOVE, A .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1994, 4 (08) :268-270
[5]   A NEW LOOK AT THE PERFECTLY MATCHED LAYER (PML) CONCEPT FOR THE REFLECTIONLESS ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
MITTRA, R ;
PEKEL, U .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1995, 5 (03) :84-86
[6]   ABSORBING BOUNDARY-CONDITIONS FOR THE FINITE-DIFFERENCE APPROXIMATION OF THE TIME-DOMAIN ELECTROMAGNETIC-FIELD EQUATIONS [J].
MUR, G .
IEEE TRANSACTIONS ON ELECTROMAGNETIC COMPATIBILITY, 1981, 23 (04) :377-382
[7]   A perfectly matched anisotropic absorber for use as an absorbing boundary condition [J].
Sacks, ZS ;
Kingsland, DM ;
Lee, R ;
Lee, JF .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 1995, 43 (12) :1460-1463
[8]  
WITTWER DC, 1995, UNPUB IEEE T ELECTRO
[9]  
YEE KS, 1966, IEEE T ANTENN PROPAG, VAP14, P302
[10]  
ZIOLKOWSKI RW, 1996, IN PRESS IEEE T ANTE