Compact Antenna Replacements for C-Band Global Horns

G.A.E. Crone, K. Markus* (1); J. Martinez (2); J. Vazquez(3); A.G. Roederer (4)

(1) Electromagnetics Division, ESTEC, * Now with VTT (SF)
(2) RYMSA (E)
(3) IRSA (E),
(4) Electromagnetics Division, ESTEC.

Résumé

Les satellites de télécommunications mobiles sont équipés d'antennes en bande C pour les échanges avec les stations fixes connectées au réseau téléphonique. Ces antennes sont présentement des cornets en fibre de carbone d'une longueur allant jusqu'au mètre. L'objet du développement décrit dans cet article est de remplacer ces cornets par une antenne beaucoup plus compacte. Il s'agit d'une évolution d'un concept ancien dû à von Trentini, où le rayonnement d'une source placée au-dessus d'un disque conducteur est rendu plus directif en disposant un disque semi-transparent devant la source. Ici le disque semi-transparent diélectrique de von Trentini est remplacé par deux plaques métalliques perforées, plus résistantes à l'environnement spatial. Les performances obtenues avec le modèle décrit dans l'article démontrent clairement le potentiel de ce type d'antennes pour les satellites futurs.

Contractors:
RYMSA (E), IRSA (E)

Funding:
Basic Technology Research Programme

Introduction

Many satellite communication services employ horn antennas to achieve wide area coverage. These antennas radiate a symmetrical beam within a cone of 9 degrees from geostationary orbit. In particular, satellites used by both Inmarsat and Intelsat use such antennas at C-band. In the case of Inmarsat, where the bandwidth requirements are narrower, there is a strong possibility that a much more compact design can meet requirements.

Figure 1 shows a photograph of the 4-GHz horn antenna manufactured in carbon fibre material by RYMSA for Matra-Marconi. Although this antenna has low mass, its overall length, including the launching and polariser section, approaches one metre. The antennas described in this article are greatly reduced in volume and mass yet offer potentially similar performance.

A configuration based on the Von Trentini antenna (Figure 2) was studied. This antenna consists of a waveguide feed, positioned in the centre of a perfectly-reflecting circular ground plane. In front of the feed are placed one or more semi- transparent circular sheets of material, each of which may be a dielectric or, as is shown in Figure 2, an artificial dielectric screen, comprising a pattern of holes in a conducting plate. The gain of the openended waveguide feed is increased by selecting an appropriate value for the (effective) dielectric constant of the sheets. Rays incident on the screen are partially reflected and partially transmitted. The value of the reflection coefficient C determines the aperture distribution over the sheet. The distance between the screen and ground plane is chosen such that the rays transmitted into space have equal phases in the desired direction of maximum radiation, usually normal to the sheet.

Several configurations of this antenna were studied and prototypes were tested.

Horn Antenna
Figure 1. A 4-GHz horn antenna manufactured for Inmarsat by RYMSA

Von Trentini Antenna
Figure 2. The configuration of a Von Trentini antenna

Electrical requirements, design and reference

The study was based on requirements detailed in Table 1. These are comparable to those for the horn antennas of Inmarsat III, taking the receive antenna as a specific case. The launching section of the antenna is the same as that used for horn antennas and consists of a square septum polariser feed in the ground plane with two rectangular waveguide inputs, one for each direction of circular polarisation. The septum polariser has the following characteristics:

Axial ratio 	< 0.3 dB 
Isolation 	> 30 dB
Return loss 	> -25 dB

The first prototypes used artificial dielectric screens consisting of holes drilled in a metal plate; the final design used a double screen. The antenna was analysed using the principles of geometrical optics. The finally selected prototype was 5.5 wavelengths in diameter and is shown alongside an equivalent horn antenna in Figure 3. The performance is summarised in the Table 2. The observed minor non-compliances in cross polarisation and gain are capable of correction.

The Von Trentini antenna has an open structure, and to obtain improved mechanical and electrical properties, it was decided to investigate a closed cavity design which offered a stiffer structure and a further reduction in aperture size. The electrical design of this antenna, based on Harrington's method-of-moments, led to the close cavity design shown in Figure 4 whose aperture was five wavelengths. The electrical performance shown in Table 2 complies with specifications.

Antennae
Figure 3. Compact Von Trentini antenna (left) and global horn antenna (right)

Compact antenna
Figure 4. A closed-cavity compact antenna

Table 1. Antenna design requirements.


Central Frequency		6.44 GHz
Bandwidth			32.6 MHz
Polarisation			Dual cicular
Cross polarisation		-31 dB
Isolation at I/P ports		-20 dB
Coverage			±9°
Edge of coverage gain		-7.15 dB
V.S.W.R.			< 1.15

Table 2. Comparison of prototype antennas with requirements.

				          Compliance
Parameter	  	Requirements	  Von Trentini	  Closed-cavity
________________________________________________________________________
Bandwidth	   	 32.6 MHz		Yes		Yes
Polarisation  		    ---			---		Yes
Cross polarisation 	-31 dB (±9°)          -28 dB	        Yes
(EOC)		   
Isolation input ports	-20 DB			Yes		Yes
Gain (EOC)		17.15 dB (±9°)        16.5 dB	        Yes
V.S.W>R.		< 1.15			Yes		Yes

Conclusions

It is feasible for a compact antenna to replace a narrow-band global coverage horn antenna. However future work is required to improve electrical performance. and to widen the bandwidth over which a compliant input match is obtained, creating additional margin to accommodate thermal variations. This activity together with a full development of a flight compatible design is strongly recommended.


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Right Left Up Home TTP homepage Preparing for the Future Vol. 5 No. 2.
Published June 1995.
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