Experiment provides the most convincing justification of numerical studies. A frequency selective surface (FSS) with Type-2 gangbuster array is fabricated and measured. The measurement results agree well with numerical results. An FSS with regular y-directed dipole array is also fabricated and measured. The bandwidth of the former isobserved much wider than that of the latter. © 2006 Wiley Periodicals, Inc. Microwave Opt Technol Lett 48: 2421-2425, 2006; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/ mop.21967Key words: frequency selective surfaces; gangbuster
INTRODUCTIONA frequency selective surface (FSS) with gangbuster array was put forward by Kornbau in his dissertation in 1984. It was introduced to the public by Munk [1, 2]. Since then, it has attracted increasing attention due to its unique and outstanding property. Numerous numerical studies on its performance and applications have been conducted [3][4][5][6][7][8][9][10][11][12]. However, literature survey shows that little experimental study has been reported.In this article, FSS with gangbuster array is experimentally investigated. An FSS with Type-2 gangbuster array is fabricated and measured. The measured reflection and transmission coefficients agree well with numerical results.For comparison, an FSS with regular y-directed dipole array is also fabricated and measured. The band of FSS with gangbuster array is observed much wider.
ANALYSIS OF FREQUENCY SELECTIVE SURFACESAnalysis of FSS is very crucial for both design and application engineers. Many approaches such as the periodic moment method [1, 2], the standard SDM [13], the equivalent circuit model [14], the finite element method [15], the finite difference time domain method [16], the recursive T-matrix method [17], etc., have been proposed. Commercial software such as Ansoft HFSS is also applicable.Among various methods for the analysis of FSS, the standard SDM is usually the method of choice. However, it is not imme-
FABRICATIONAn FSS with Type-2 gangbuster array is fabricated. First, PCB technology is used to generate the array pattern as shown in Figure 1. Thin copper dipoles (width: 80 m, thickness: 17.5 m) are printed on Kapton substrate (relative permittivity:Ϸ3.5, thickness: 40 m). Dipole length (9.18 mm) is chosen so that the resonant frequency is approximately 10 GHz. A sandwich structure as shown in Figure 2 is then obtained by putting four Kevlar sheets (relative permittivity: Ϸ3.65 Ϫ j0.1, each sheet is 230 m thick) on both sides of the PCB. Finally, the sandwich structure is vacuum bagged and cured in autoclave for 1 h (7 bars, 175°C). The final panel (424 ϫ 424 ϫ 1.7 mm 3 , tolerance of thickness: Ϯ0.1 mm) with gangbuster array embedded is shown in Figure 3.For comparison, a panel with regular y-directed dipole array as shown in Figure 4 is also fabricated in the same way.
EXPERIMENTAL SETUPThe experimental setup is shown in Figure 5. Figure 6 is a photo of the panel holder. Its height is 100 cm and the top surface is 60 ϫ 60 cm 2 . ...