Truncation of open boundaries of cylindrical waveguides in 2.5-dimensional problems by using the convolutional perfectly matched layer

被引:91
作者
Wang, JG [1 ]
Wang, Y
Zhang, DH
机构
[1] NW Inst Nucl Technol, Xian 710024, Shaanxi, Peoples R China
[2] Xian Jiaotong Univ, Sch Elect & Informat Engn, Xian 710049, Peoples R China
关键词
convolutional perfectly matched layer (CPML); finite-difference time-domain (FDTD); particle simulation; truncation; waveguide structure; two-and-a-half-dimensional (2.5-D) problem;
D O I
10.1109/TPS.2006.875830
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
In order to solve the problem of truncating the open boundaries of cylindrical waveguides used in the simulation of high-power microwave (HPM) sources, this paper studies the convolutional perfectly matched layer (CPML) in the cylindrical coordinate system. The electromagnetic field's finite-difference time-domain (FDTD) equations and the expressions of axis boundary conditions are presented. Numerical experiments are conducted to validate the equations and axis boundary conditions. The performance of CPML is simulated when it is used to truncate the cylindrical waveguide excited by the sources with different frequencies and modes in the two-and-a-half-dimensional. (2.5-D) problems. Numerical results show that the maximum relative error is less than -95 dB, and demonstrate that the property of CPML is much better than that of the Mur-type absorbing boundary condition when they are used to truncate the open boundaries of waveguides. The CPML is especially suitable for truncating the open boundaries of the dispersive waveguide devices in the simulation of HPM sources.
引用
收藏
页码:681 / 690
页数:10
相关论文
共 16 条
[1]  
Barker R. J., 2001, HIGH POWER MICROWAVE, DOI 10.1109/9780470544877
[2]  
BENFORD J, 1992, HIGH POWER MICROWAVE
[3]   Evanescent waves in PML's:: Origin of the numerical reflection in wave-structure interaction problems [J].
Bérenger, JP .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 1999, 47 (10) :1497-1503
[4]   A PERFECTLY MATCHED LAYER FOR THE ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
BERENGER, JP .
JOURNAL OF COMPUTATIONAL PHYSICS, 1994, 114 (02) :185-200
[5]  
Birdsall C. K., 2018, Plasma Physics via Computer Simulation
[6]   USER-CONFIGURABLE MAGIC FOR ELECTROMAGNETIC PIC CALCULATIONS [J].
GOPLEN, B ;
LUDEKING, L ;
SMITHE, D ;
WARREN, G .
COMPUTER PHYSICS COMMUNICATIONS, 1995, 87 (1-2) :54-86
[7]   Frequency dependence of the constitutive parameters of causal perfectly matched anisotropic absorbers [J].
Kuzuoglu, M ;
Mittra, R .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1996, 6 (12) :447-449
[8]   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
[9]   A modified perfectly matched layer implementation for use in electromagnetic PIC codes [J].
Pasik, MF ;
Seidel, DB ;
Lemke, RW .
JOURNAL OF COMPUTATIONAL PHYSICS, 1999, 148 (01) :125-132
[10]  
POZAR DM, 1998, MICROWAVE ENG, P139