G. Marrocco A. Potenza. L. Mattioni F. Milani. A. Giacomini M. Sabbadini. Work performed under ESA Contract n /08/NL/ST
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1 University of Roma Tor Vergata G. Marrocco A. Potenza L. Mattioni F. Milani A. Giacomini M. Sabbadini Work performed under ESA Contract n /08/NL/ST 1
2 Early satellites were small. Requests for increasing performances! growth in mass and dimensions and cost. Recently, renewed interest in nano and pico satellites with small mass (a few to a few hundreds kilograms), small size (a few centimetres to one meter) - low-cost, rapid timescales - inspector satellites, clusters or formations - experimentation of new payloads - low-cost data-link, surveillance - limited capability of RF section (number and quality of available links) 2
3 - solar cells on almost the whole satellite surface - presence of multiple antennas, sensors, cameras, etc. - bottom plate generally crowded in its centre - antenna radiation properties can not be separated by the satellite effect - possible metallic gaps between solar cells - available space on the edges! Antennas should be integrated on the structure 3
4 Quadrifilar helix (S-Band) wire-like protuding antennas (VHF, UHF) 60x60x65cm Low profile patch antennas (S-Band) Integration with solar cells SOLANT Project (S-band) 4
5 A multiplicity of minimally-invasive exciters placed all over the structure to achieve a distributed control of the radiating currents. The exciters are expected to be greatly coupled and hence they have to be considered as a unique multiport system, designed as a whole When properly sourced, a multi-port system permits to achieve a plurality of service together with a natural redundancy which improves the fault tolerance Reconfigurability may be obtained by dynamically changing the state of the ports (impedance loading, phase/amplitude of the excitation) Input port Imped. load Exciter Solar Panel 5
6 Small (poor) antenna exciters inject radiating currents over the mobile platform working as active part of the antenna system G. Marrocco, L. Mattioni, "Naval structural antenna systems for broadband HF communications", IEEE Trans. Antennas Propagat. vol. 54, n.4, pp , April, 2006
7 7
8 d L C 1 Transmission-line antenna having a form factor such to produce omnidirectional radiation (monopole+ loop mode) h C O GND Lumped capacitors for impedance tuning 8
9 Fine tuning Raw tuning 9
10 E(r) = Pattern shaping N " n =1 e j! n E n (r) Embedded patterns E 1 E 2 E N Active impedance matching [Z in ] = f ([Z],[Z T ],[! ]) V 0 e ja 1 V 0 e ja N... Z in,1 Z in,n [Z] (N+M) Z T,1 Z T,M Exciters Assembly Exciters tuning Optimization parameters - phases! n - Tuning loads Z T,m Phase-only tuning N: number of exciters M: number of exciters tuning loads! Automatic Optimization (Genetic Algorithms) 10
11 C 1 C O GND Cavity ("/2 x "/4) ESA - NANOSAT Starting exciters parameters C 0 =C 1 =0.7pF (exciters matched over # n =n$/4 (octagon) 40x40x35cm (3") Mismatching due to Inter-antenna coupling and Edge/cavity diffraction 11
12 Optimization for maximum CP gain from octagon and active impedance matching C 0 = 0.7 pf C 1 = 1.9 pf Equal exciters tuning ϕ 1 = 0 ϕ 2 = ϕ 3 = ϕ 4 = -135 ϕ 5 = ϕ 6 = ϕ 7 = ϕ 8 = db BW(5dB CP)=40 9% 12
13 Starting parameters C 0 =C 1 =0.7pF # n =[0, 120, 240 ] Optimization [RL, G] ϕ 1 = 0 ϕ 2 = ϕ 3 = 114 C0 1,2 =1.4pF C1 1,2 =0.3pF C0 3 =0.8pF C1 3 =0.6pF 13
14 S-Band: f 0 =2.3 GHz cm 0.8" AMSAT UWE
15 S-Band: f 0 =2.3 GHz z y Monopulse "! cluster satellites 15
16 S-Band: f 0 =2.3 GHz Directive data-link Omnidirectional TT&C CP-patch CP-patch TOT, Gain Gmax = 9.7dB BW(5db)=80 R " L " RCH, Gmax=7.5 db BW(5dB)=45 Exciters - cross TOT, Gain R Exciters - Octagon L 16
17 HAUSAT 2 (Corea) RCH-GAIN 6.1dB 30cm (0.56!) UHF-Band: f 0 =434 MHz Total GAIN No space to place a patch!
18 18
19 2.3 GHz Snn Active Reflection coef. 2.3 GHz C 0 =C 1 =0.7pF (standalone antenna optimized on ground plane) Gn Embedded patterns Theta 19
20 Theoretical and first experimentations demonstrate that the distributed antenna concept can be usefully ported in the micro/nano satellite domain. Electromagnetic simulation and efficient optimization play a key role in the fast system customization for the specific spacecraft. This idea is moreover well suited to electronically controlled tuning, involving electronic switches or self matching networks. The exciter may therefore become a self-configuring device, with the matching and reconfiguration hardware hidden in the antenna module itself. This concept, together with the availability of top-level aided tools for placing and testing will permit in the near future a significant reduction of try and error and measurement effort. 20
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