LOD-BOR-FDTD Algorithm for Efficient Analysis of Circularly Symmetric Structures

The unconditionally stable locally 1-D (LOD) scheme is used to develop an efficient implicit body-of-revolution (BOR) finite-difference time-domain (FDTD) method. In the LOD-BOR-FDTD, the number of arithmetic operations of the resultant finite-difference equations is significantly reduced, when compared with the alternating-direction implicit (ADI) BOR-FDTD. Numerical results of circular cavity resonators reveal that the LOD-BOR-FDTD provides resonance frequencies identical to the ADI counterparts, with the computational time being reduced to 70%.

[1]  Raj Mittra,et al.  Finite-difference time-domain algorithm for solving Maxwell's equations in rotationally symmetric geometries , 1996 .

[2]  Zhizhang Chen,et al.  An efficient unconditionally stable three-dimensional LOD-FDTD method , 2008, 2008 IEEE MTT-S International Microwave Symposium Digest.

[3]  Zhizhang Chen,et al.  A three-dimensional unconditionally stable ADI-FDTD method in the cylindrical coordinate system , 2002 .

[4]  J. Yamauchi,et al.  Efficient implicit FDTD algorithm based on locally one-dimensional scheme , 2005 .

[5]  Kyung-Young Jung,et al.  An Iterative Unconditionally Stable LOD–FDTD Method , 2008, IEEE Microwave and Wireless Components Letters.

[6]  A Novel Body-of-Revolution Finite-Difference Time-Domain Method With Weakly Conditional Stability , 2008, IEEE Microwave and Wireless Components Letters.

[7]  Richard W. Ziolkowski,et al.  Body-of-revolution finite-difference time-domain modeling of space–time focusing by a three-dimensional lens , 1994 .

[8]  O. Ramadan Unsplit field implicit PML algorithm for complex envelope dispersive LOD-FDTD simulations , 2007 .

[9]  D. Pozar Microwave Engineering , 1990 .

[10]  E. L. Tan,et al.  Unconditionally Stable LOD–FDTD Method for 3-D Maxwell's Equations , 2007, IEEE Microwave and Wireless Components Letters.

[11]  The stability analysis of the three-dimensional LOD-FDTD method , 2008, 2008 Asia-Pacific Symposium on Electromagnetic Compatibility and 19th International Zurich Symposium on Electromagnetic Compatibility.

[12]  F. Teixeira,et al.  Split-field PML implementations for the unconditionally stable LOD-FDTD method , 2006, IEEE Microwave and Wireless Components Letters.

[13]  Allen Taflove,et al.  Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .

[14]  J. Yamauchi,et al.  Performance evaluation of several implicit FDTD methods for optical waveguide analyses , 2006, Journal of Lightwave Technology.

[15]  Eng Leong Tan,et al.  Development of split-step FDTD method with higher-order spatial accuracy , 2004 .

[16]  Erping Li,et al.  Convolutional Perfectly Matched Layer for an Unconditionally Stable LOD-FDTD Method , 2007, IEEE Microwave and Wireless Components Letters.

[17]  Yansheng Jiang,et al.  A hybrid implicit‐explicit FDTD scheme with weakly conditional stability , 2003 .

[18]  Weng Cho Chew,et al.  PML-FDTD in cylindrical and spherical grids , 1997 .

[19]  Bin Chen,et al.  Anisotropic-Medium PML for ADI-BOR-FDTD Method , 2008, IEEE Microwave and Wireless Components Letters.

[20]  Eng Leong Tan,et al.  Fundamental Schemes for Efficient Unconditionally Stable Implicit Finite-Difference Time-Domain Methods , 2008, IEEE Transactions on Antennas and Propagation.

[21]  C. Balanis Advanced Engineering Electromagnetics , 1989 .

[22]  Zhizhang Chen,et al.  A finite-difference time-domain method without the Courant stability conditions , 1999 .

[23]  T. Namiki,et al.  A new FDTD algorithm based on alternating-direction implicit method , 1999 .

[24]  Da-Gang Fang,et al.  Unconditionally Stable ADI–BOR–FDTD Algorithm for the Analysis of Rotationally Symmetric Geometries , 2007, IEEE Microwave and Wireless Components Letters.