## Abstract The finiteβelement method (FEM) is applied to the analysis of phasedβarray antennas. Curvilinear tetrahedral elements are used for domain discretization and highβorder vector basis functions are used for field expansion. Periodic boundary and radiation conditions are enforced on a singl
Analysis of finite phased arrays of arbitrary-shaped linear microstrip antennas
β Scribed by Ahmed M. Attyia; Essam A. El-Diwany; Fatma M. El-Hefnawi
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 519 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0895-2477
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β¦ Synopsis
In this article the analysis of finite phased arrays of arbitrary shaped linear microstrip antennas is presented in detail. The analysis is based on solving the electic field integral equation with the moment method to find the current distribution along the array elements, the input impedance
of the array elements, and the radiation pattern of the array. The main problem in the moment-method solution is the large matrix. In this article a unified approach i s presented to reduce both the computational time and the storage to a minimum by making use of the similarities of the elements of the moment-method matrix.
π SIMILAR VOLUMES
## Abstract Analysis of Hβshaped patch is carried out using equivalent circuit model. It is found that the antenna exhibits dual resonance behavior which is very sensitive to the dimensions of the notch. The theoretical results of proposed method are compared with experimental and theoretical resul
In this article an integral equation for a microstrip antenna on a finite ground plane is deri¨ed with the use of the reaction theory and the dyadic Green's function. The integral equation is sol¨ed with the use of the Galerkin method, and the current densities on the patch and the ground plane are
An approach is developed to analyze microstrip antennas on finite chiral substrates using the finite-element method (FEM). The perfectly matched layers (PMLs) in the chiral media is employed in this work. First, the characteristics of microstrip antennas on infinite conventional, ferrite, and chiral
wavenumbers because the subradical expression becomes negative. The same takes place for the second wave when the values of the parameters satisfy the condition Ε½ . The conditions 11 and 12 correspond to the wave propagation within certain angular domains in space defined by the anglesandfor the fi