Novel TLM-based time-domain wave propagator

被引:19
作者
Özyalçin, MO
Akleman, F
Sevgi, L
机构
[1] Turkish Airforce Acad, TR-34152 Istanbul, Turkey
[2] Istanbul Tech Univ, Elect & Commun Engn Dept, TR-80626 Istanbul, Turkey
[3] Dogus Univ, Elect & Commun Engn Dept, TR-81010 Istanbul, Turkey
关键词
finite difference time domain (FDTD); ground wave; split-step parabolic equation (SSPE); terrain scattering; time domain simulation; TLM; wave propagator;
D O I
10.1109/TAP.2003.813624
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 this letter, a novel time-domain wave propagator, based on the transmission line matrix (TLM) technique, is introduced. A two-dimensional (2-D) TLM algorithm is modified and the sliding window technique is applied to analyze ground wave propagation characteristics. The longitudinal propagation region over earth's surface is covered by a finite-size TLM computation space, as if the space slides from source to observation point. A short pulse is injected into the TLM computation space as a vertical initial source distribution near the left end and is traced within an adjustable window while propagating toward right. Perfectly matched layer (PML) blocks on the left, top and right terminate the TLM computation space to simulate semi-open propagation region, The ground at the bottom is a perfectly electrical conductor (PEC). The PML blocks absorb field components that scatter back and top. The ground wave components (i.e., the direct, ground-reflected and surface waves) are traced longitudinally toward right. Transient propagation can be observed at any range/altitude by accumulating time history of the desired field components and any steady-state vertical and/or horizontal field profile at a desired frequency can be extracted by applying off-line discrete Fourier transformation (DFT).
引用
收藏
页码:1680 / 1682
页数:3
相关论文
共 9 条
[1]   A novel implementation of Berenger's PML for FDTD applications [J].
Akleman, F ;
Sevgi, L .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1998, 8 (10) :324-326
[2]   A novel finite-difference time-domain wave propagator [J].
Akleman, F ;
Sevgi, L .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 2000, 48 (05) :839-841
[3]   A PERFECTLY MATCHED LAYER FOR THE ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
BERENGER, JP .
JOURNAL OF COMPUTATIONAL PHYSICS, 1994, 114 (02) :185-200
[4]  
ESWARAPPA C, 1995, ELECT LETT, V31
[5]   NUMERICAL SOLUTION OF 2-DIMENSIONAL SCATTERING PROBLEMS USING A TRANSMISSION-LINE MATRIX [J].
JOHNS, PB ;
BEURLE, RL .
PROCEEDINGS OF THE INSTITUTION OF ELECTRICAL ENGINEERS-LONDON, 1971, 118 (09) :1203-+
[6]  
Sevgi L, 1998, INT J NUMER MODEL EL, V11, P87, DOI 10.1002/(SICI)1099-1204(199803/04)11:2<87::AID-JNM291>3.0.CO
[7]  
2-6
[8]   Groundwave propagation modeling: Problem-matched analytical formulations and direct numerical techniques [J].
Sevgi, L ;
Akleman, F ;
Felsen, LB .
IEEE ANTENNAS AND PROPAGATION MAGAZINE, 2002, 44 (01) :55-75
[9]   EQUIVALENCE OF PROPAGATION CHARACTERISTICS FOR THE TRANSMISSION-LINE MATRIX AND FINITE-DIFFERENCE TIME-DOMAIN METHODS IN 2 DIMENSIONS [J].
SIMONS, NRS ;
BRIDGES, E .
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, 1991, 39 (02) :354-357