(19)
(11) EP 0 098 618 A2

(12) EUROPEAN PATENT APPLICATION

(43) Date of publication:
18.01.1984 Bulletin 1984/03

(21) Application number: 83106741.8

(22) Date of filing: 08.07.1983
(51) International Patent Classification (IPC)3H01Q 25/02, H01Q 3/24
(84) Designated Contracting States:
DE FR GB NL SE

(30) Priority: 08.07.1982 IT 4878182

(71) Applicant: SELENIA INDUSTRIE ELETTRONICHE ASSOCIATE S.p.A.
I-00131 Roma (IT)

(72) Inventors:
  • Roveda, Riccardo
    I-00168 Rome (IT)
  • Cattarin, Giuseppe
    I-00125 Rome (IT)
  • Di Gregorio, Carlo
    I-00046 Grottaferrata (IT)
  • Parrucci, Umberto
    I-00145 Rome (IT)
  • Capasso, Giuseppe
    I-00013 Mentana-Rome (IT)

(74) Representative: Gustorf, Gerhard, Dipl.-Ing. 
Patentanwalt Dipl.-Ing. Gerhard Gustorf Bachstrasse 6 A
84036 Landshut
84036 Landshut (DE)


(56) References cited: : 
   
       


    (54) System for the electronical sector scanning of the beam of a monopulse radar antenna


    (57) System for the electronic sector scanning of a bundle of radar antenna monopulses, which allows scanning times in the order of µs by the separation of the R.F. power at a predetermined phase and whith amplitude control.




    Description


    [0001] The present invention relates to a system which allows the fast sectional scanning of a bundle of radar antenna monopulses to be obtained. The invention is used in the field of radar systems for tracking, particularly in the field of the components in waveguides for antennas. Said fast scanning is obtained by the use of an electronic ferrite switch in the waveguide. As no electronic solutions for shifting the bundle were known, the only possibility consisted of very slow electromechanical devices which therefore were not satisfactory when used for radar purposes.

    [0002] The following description of the figures is only an example not restricting the scope of the present invention.

    [0003] Figure 1 shows a basic diagram of the invention in which Pi is the R.F. input power; the block 1 is the electronic ferrite switch; P1 and P2 represent the powers being output at two output terminals of said switch, γ 1 and γ 2 being the corresponding phases; the block 2 represents the monopulse comparator for the sum bundles ( Σ ) and for the difference bundles (Δ) and finally, the block 3 represents the radiating antenna system.

    [0004] Figure 2 represents the block 1 of Figure 1 and is an equivalent circuit diagram of the electronic ferrite switch located in the waveguide. Here, Pi is the input power fed to the switch; A1 and A2 are two hybrid functions interconnected by two ferrite phase shifters A and B. P1 and P2 are the R.F. output powers and γ 1 and γ 2 the corresponding phases.

    [0005] Figure 3 represents the constructional conception in the R.F. ferrite switch in the waveguide, in which the par- ticulars indicated by DRIVER are the control circuits having transistors.

    [0006] The electronic switch which allows the fast scanning of the antenna bundle is based on the monopulse characteristics of the antenna, combining the sum bundle ε with one of the difference bundles Δ

    [0007] The various signal configurations being available at the input terminals of the channels Σ and A of said monopulse comparator are furnished by the electronic switch the essential requirements of which being indicated in the following Table I:

    Said table indicates the correspondence between the input values and the output values which can be derived from the following general formulas of the microwave scheme of Fig. 2:



    Wherein E1, E2 are the output voltages,

    for an incoming voltage



    [0008] The real radiating system and the monopulse comparator are typical embodiments of a Cassegrain system with monopulse function. The electronic switch the equivalent circuit diagram of which being illustrated in Fig. 2 is realized as shown in Fig. 3. A1 and A2 are two hybrid junctions interconnected by two ferrite phase shifters. As the switching over from one status to the other status must be completed within some 10 ps it has been opted in favour of a latching in guide type phase shifter (see e.g. Ref. No. 1x) for the relative reading. The phase shifters are controlled by a transistor driver, which supplies on command the three current couples necessary for the three output situations.

    [0009] As to the materials, use of lithium ferrite for small peak power values and high average power values is convenient; stabilized garnets for high peak power values and moderate average power values; the magnetisation levels are chosen according to the application frequency.

    [0010] The real application of such an antenna is in monopulse systems which require fast sector scanning of such a frequency that no mechanical solution is possible.

    [0011] x) Ref. 1 Cattarin G., Parodi M. "Sfasatori a rimanenza in guida d'onda: teoria, programma di calcolo, alcune applicazioni." Riv. Tec. Selenia, Vol.7, n.l (17 - 26), 1980.


    Claims

    1. System for the fast sectional scanning of a bundle of radar antenna monopulses, characterized by the use of an electronic switch.
     
    2. System according to claim 1, characterized in that said switch consists of a phase shifter with ferrite in the remanence, said phase shifter being inserted between two hybrid connections so that said switch generates output signals having predetermined phases and has amplitude control.
     




    Drawing