𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Numerical integration method in analysis of wire antennas

✍ Scribed by Yang Shaolin; Ke Hengyu; Hou Jiechang


Publisher
Wuhan University
Year
1998
Tongue
English
Weight
472 KB
Volume
3
Category
Article
ISSN
1007-1202

No coin nor oath required. For personal study only.


πŸ“œ SIMILAR VOLUMES


Accurate modeling of thin-wire antennas
✍ M. Douglas; M. Okoniewski; M. A. Stuchly πŸ“‚ Article πŸ“… 1999 πŸ› John Wiley and Sons 🌐 English βš– 154 KB πŸ‘ 1 views

The nonreciprocal phenomena of a gyrotropic thin-film waveguide with a grating configuration have been analyzed by the singular perturbation technique with multiple space scales. The analyzed structure can perform both as a grating coupler and an isolator. With low gyrotropy, the beam deflection is

Numerical aspects in time domain modelli
✍ G. Cerri; S. Chiarandini; P. Russo πŸ“‚ Article πŸ“… 1999 πŸ› John Wiley and Sons 🌐 English βš– 243 KB πŸ‘ 2 views

This paper deals with the numerical modelling of arbitrarily shaped curved antennas by marching on in time (MoT) technique. This time domain version of the method of moments (MoM) is particularly suitable for transient analysis and, in this respect, is more e$cient than the frequency domain approach

Time-domain analysis of conducting wire
✍ Baek Ho Jung; Tapan Kumar Sarkar; Zhong Ji; Young-seek Chung πŸ“‚ Article πŸ“… 2003 πŸ› John Wiley and Sons 🌐 English βš– 104 KB

## Abstract In this work, a new method is presented for analyzing the transient electromagnetic response from conducting wire structures using the time‐domain integral equation (TDIE). Instead of the conventional marching‐on in time (MOT) technique, this solution method is based on Galerkin's metho

Analysis of a coil-loaded wire antenna
✍ Mitsuo Taguchi; Kiyomi Yamashita; Kazumasa Tanaka; Toshiyuki Tanakas πŸ“‚ Article πŸ“… 1993 πŸ› John Wiley and Sons 🌐 English βš– 616 KB

An analysis method using Pocklington's integral equation is presented for wire antennas with lumped inductive loading along its arm. In the formulation of the integral equation, using the equivalence principle, the equivalent electric and magnetic currents on the coil surface are expressed instead o