SYSTEM FOR THE CANCELLATION OF INTENTIONAL DISTURBANCE APPLIED TO A MONOPULSE PHASED ARRAY RADAR

Abstract: The invention considers a system for the cancellation of intentional disturbances by means of processing the signals that derive from a group of three beams formed by a planar antenna of a phased array type radar. These three beams are normally available in phased array type radar with electronic scanning both in aximuth and in elevation, to obtain the sum of signals (Σ) and difference (Δ azimuth , Δ elevation ) for the monopulse evaluation of the angular coordinates of a target. The system according to the invention does not there­ fore require the use of auxiliary antennas placed around the antenna and the relative processing channels. It neither requires the multiple processing channels that would be necessary in the case in which it is desired to control all the phased array radiating elements in amplitude and phase. The received signals from the three beams can be still used to calculate the angular coordinates of a target without suffering the damaging effects of the disturbances that are present.

Description: "SYSTEM FOR THE CANCELLATION OF INTENTIONAL DISTURBANCES APPLIED TO A MULTI-BEAM PHASED ARRAY RADAR AND WITH MECHANICAL SCANNING" DESCRIPTION The invention considers a system for the cancellation of intentional disturbantes by means of the processing of the signals derived from a group of three beans formed from a planar antenna of a phased array type radar .#e perfornance of a phased array radar can be notably reduced from the reception, through its antenna side lobes, of disturbances originating from diverse directions in space (jammer). The present invenion concerns a system for the spatial filtering of these disturbances. Up to no# two methods of different complexity and performance have been used. The first method, that is an extension of the one used for mechanical scanning radar, consists in the placing around the phased array antenna re or more auxiliary antennas that in their turn receive the disturbances. The signals originating from these auxiliary antennas are first multiplied j coefficients (weights) that modify their phases and amplitudes and then are summe d between themselves. The resulting signal, that is an estimate e- the signals received from the phased array, is subtracted at the output -- tr. #r that therefore is purged ol disturbances. That is also equivalent to reducing the main antenna gain in the directions from which originate the jammers themselves. This method requires the use of a number of antennas at least equal to the intentional disturbances (jammer) to filter, of an equal number of receiving channels that will allow the disposal of the received signals in the most useful frequency band for their processing, and of an equal number of processing circuits for the weights evaluation. A second method consists in the modification of the amplitudes and phases of the received signals from all the elementary radiators of which is equipped the phased array antenna and then combining them in a way as to still have a beam in a certain direction of interest and at the same time to spatially filter the disturbances reducing the gain in their direction of incidence. This method requires an extremely elevated number of processing channels and weight calculating circuits (equal to the number of the phased array elementary radiators), even if it allows the cancellation of a major number of disturbances. The system according to the present invention permits instead the spatial filtering of the disturbances by use of the signals originating from three antenna beams (indicated by the following symbols EMI2.1 normally available in a phased array radar, with electronic scanning both in azimuth and elevation that performs the "monopulse" evaluation of the polar angular coordinates EMI2.2 of a target. The practical realization of the system according to the present invention does not require the use of auxiliary antennas with the relative processing channels (as said for the first method) because the three available beams EMI2.3 each make up both the part of the main antenna and the part of the auxiliary antenna, and the signals received by them are already available, in the radar, in a band suitable to their processing. Moreover, the system according to the present invention requires only three cancellation circuits, as opposed to the second method that requires as many as are the radiating elements of the phased array antenna. Consequently, the object of the present invention is that of providing a system for the cancellation of directional disturbances for a phased-array radar with three receiving beams that efficiently utilizes the available circuitry and allows the monopulse evaluation of the polar angular coordinates ( p , P ) of a target even in disturbed conditions. The present invention will now be described with reference to an actual preferred realization form presented on an illustrative and not limitative basis, and on the basis of the enclosed design figures, in which: figure 1 shows the block diagram of the receiving part of a multi-beam phased array radar for the evaluation of the angular coordinates ( 6 , f ) of a target, in the presence of intentional disturbances; Figure 2 shows a block diagram of the disturbance cancellation system (block 4 of figure 1) by means of processing the signals originating from the beams; Figure 3 shows the block diagram of the circuit for the evaluation of the channel disturbance (Block 14 of figure 2). A diagram of the principle that permits the reduction of the power relative to the directional disturbances received from the side lobes of a phased array antenna and contemporarily effects the evaluation of the target angular polar coordinates ( # ,f ) is illustrated in Figure 1. The antenna of this type of radar includes a planar phased-array indicated in 1 that can be both mechanically rotational in the azimuth sense or non rotational. The signals received by the elementary antennas, indicated in 2, are linearly combined (that is, multiplied with weights independent of the received signals and therefore summed) in three diverse ways by means of block 3 for furnishing in reception the three beams indicated with the symbols EMI3.1 Thc weight of the linear combination are normally obtained by means of phase shifters inserted after the small elementary antennas. These three beams can explore the space surrounding the antenna 1 either by means of an eventual mechanical rotation of the array, or by control, with a suitable time law, the phase shifters associated to the small antenna 1. The presence of the three beams in reception is requested when it is desired to evaluate with accuracy the angular coordinates ( e, P ) of a target detected by the radar. However, when directional disturbances are present the target detection operation and the evaluation of the coordinates give a low confidence level. To improve the radar performance in this circumstance it is therefore necessary to perform a spatial filtering of the disturbances that, in the spirit of the present invention, is obtained by processing signals EMI4.1 }ip with a cancellation system indicated in its complex with 4 in figure 1. At the output of the cancelling system 4 three signals are still obtained indicated with EMI4.2 corresponding to the input signals of the said cancelling system 4, purged of the directional disturbances. The processed signals EMI4.3 can now be efficiently used for the evaluation of the coordinates ( 8 , P ) of the target itself with the circuitry included in block 5. In figure 2 is shown in detail the structure of block 4 of figure 1. In figure 2 one essentially notices three similar circuits that are indicated with the wording "Adaptive Cancellation Loop" whose purpose is to minimize the effect of the disturbances on the output signals 11 Ae' The cancellation should be carried out in the adaptive fashion, that is, considering the fact that the disturbance direction of incidence origin and intensity is not known, and that the spatial configuration of the antenna-jammers is not stationary in time indue to the antenna rotation,the variations of the antenna side lobes and the movement of the jammers themselves). This objective is obtained by means of the disturbance estimator 14, 17 and 20 that use as feedback signals the respective output signals z @@@ The disturbance estimator that is present in the channel besides using the feedback ss also utilizes the signals from the other two channels Consequently beams aye, 4 , act as two auxiliary antennas relatively to the main antenna. The disturbance estimator on channel ds, utilizes instead, besides the feedback of signal @'@, the signals the originate from t (that this time act as auxiliary antenna) and from @@ 5D. The same holds for the disturbance estimator in channel Consequently, each of the three beams EMI5.1 performes the double function of main antenna (to purge from the disturbance) and of auxiliary antenna that makes it possible to cancel the jammeron another beam considered as main. The output of the three evaluators 14, 17 and 20 are subtracted, by means of block 12, 15 and 18, from the respective signals EMI5.2 furnish outputs @@,@'@,@'@ purged of disturbances. furnish outputs z purged of disturbances. The processing of signal ± . aç, @@ is carried out in analogical manner. It is understood that limitations of principle to the use of digital techniques do not exist. The processing is carried out at an intermediate frequency to reduce the possibility of errors in the operation of the estimator that with reference to figure 3 will be examined in detail. This, besides the direct use of signals EMI5.3 available in the radar system also allows the use of mixers 6,8 and 10 and possibly the local oscillators 7,9 and 11 could not be necessary because being already present before block 4. Passband filters 13, 16 and 19 are adapted to the detected signal, that is, to the echo that originates from the target. These are useful for frequency filtering the disturbances that generally have a power spectrum with a band larger than that of the radar receiver. The block diagram of block 14 is shown in detail in figure 3, that is, of the disturbance estimator that acts on channel z Analogous outlines are also valid for the blocks indicated in 17 and 20. The output signal from estimator 14 is obtained by summing by means of adder 21, the signals that originate from beams X . The amplitudes and phases of these signals are suitably modified by means of mixer 22 and 25 that respectively receive the output signals from the two narrow band filters 24 and 27. The output signals of the two narrow band filters 24 and 27 are non other than the correlation between the feedback signal E and the signals originating from beams EMI6.1 In effect the correlations are obtained by multiplying signals 11 with and : with ¯ respectively amongst themselves by means 23 and 26 and then performing a time integration by means of the two filters 24 and 27 that have a time constant much longer than that of the jammer smallest variational period, that is a much narrower band than that of filters 13, 16 and 19. As much, the disturbance estimator acting on E is non other than the sum of the intercepted signals of the auxiliary beams EMI6.2 multiplied by the correlation coefficient, amongst the auxiliary beams themselves and the z cancellation residual. Because the distances between the phase centers of #E A8 , and of 2i are pratically null there is a strong correlation and therefore a high cancellation value between the main channel received signals and those that come from the auxiliary channels. In conventional systems that use auxiliary antennas that are physically separated from the main antenna, the distance between the phase centers causes a decurrelation between the main and the auxiliary signals produced by a one and only disturbance that travels different distances in order to reach the various antennas, and therefore reduces the system cancellation. The presence in estimator 14 of the two auxiliary signals permits to separately evaluate the effects produced by two independent disturbances or to evaluate with greater precision the effects produced by a single jammer and therefore to more effectively cancel it. The reason for the insertion of the system for the cancellation of disturbances (block 4, figure 1) to the intermediate frequency stage will now be clarified. In principle the cancellation of disturbances can be carried out on video signals that have a null frequency carrier: consequently, the cross correlators of figure 3 can be accomplished with low pass filters rather than with band pass filters. However, this type of realization is very sensible to undesired continuous components (drifts) that can be produced by mixers 23, 26. These drifts alter the optimum value of the correlation coefficients that multiply and therefore drastically reduce the system cancellation. A way of filtering the drifts consists in the realization of the cross correlation with pass band filters that do not permit the passage of continuous components and therefore make the entire system operate at an intermediate frequency. It can be observed that one can obtain a second way in which to realize the invention even though having only two monopulse beams available. Imagine as an example that the phased array antenna is of the mechanical azimuth scanning type and with electronic elevation scanning only and has available two beams EMI7.1 to perform the monopulse evaluation of the target elevation angle. Also, in this case it is possible to cancel the directional disturbances utilizing beam 5 as the main and i as the auxiliary and alternatively beam A as the main and beam 25 as its auxiliary. The layouts for the realization of this form of the invention are analogous to those already described. In particular, in figure 1 circuit of block 3, 4 only the signal couples EMI8.1 come out respectively, while block 5 only generates the monopulse estimator of the target elevation The disturbance cancellation system, illustrated in detail in figure 2, is now made up of only two adaptive loops of cancellation that process the received signals from EMI8.2 cancelling the disturbances by means of the two estimator 14 and 20. The estimator of the disturbance r differs from the one in layout 3 by the fact that the 4 signal processing is missing and that therefore the output of the estimator is made up of the correlation between z only. Analogous considerations are valid for the disturbance estimator on that only calculates the correlation between signals Ar', j Lastly, the cancellation system, object of this present invention can be also used in mechanical scanning radar with a reflector antenna that produces two or three beams for the monopulse evaluation of the target angular coordinates, such as a tracking radar for example. The present invention has been described with reference to its presently preferred realization form but it is to be understood that modifications and variations can in practice be carried out by persons expert in the field without leaving the protective bounds of the present industrial patent.

Claims: CLAIMS 1. A system for the cancellation of directional jammers in phased array type radars, characterized by the fact of including means for the processing of signals that originate from the monopulse beams EMI9.1 available in a phased array radar with electronic azimuth and elevation scanning. 2. A system according to claim 1. characterized by the fact that it includes means for evaluating the disturbances on channel Z by calculating the correlation between channels ss A# and ±' and subtracting said evaluation from signal i in order to obtain the filtered signal zl. 3. A system according to claim 1, characterized by the fact that it includes means for the evaluation of disturbances on channel by calculating the correlations between channels S @@@ and @'@ and subtracting said evaluation from signal de to obtain the filtered signal 4. A system according to claim 1 characterized by the fact that it includes means for the evaluation of disturbances on channel @@ by calculating the correlation between channels z dg and + and subtracting said evaluation from signal @@ to obtain filtered signal at 5. A system for the cancellation of disturbances according to one or more of the claims from 1 to 4 and including a system for the monopulse evaluation of the target angular coordinates by means of monopulse beams E A#0 and @'@ filtered of disturbances. 6. A system for the cancellation of disturbances according to one or more of the claims from 1 to 5 characterized by the fact of utilizing only two monopulse beams EMI10.1 when the phased array antenna is rotating in azimuth and with electronic scanning only in elevation. 7. A system for the cancellation of disturbances according to claim 6 characterized by the fact that it includes a system for the monopulse estimation of the target elevation by means of beams EMI10.2 filtered of disturbances. 8. A system for the cancellation of directional disturbances according to the claim from 2 to 4 applied to mechanical scanning radars with a reflector antenna disposed to produce two or three beams for the monopulse evaluation of the target angular coordinates. 9. A system for the cancellation of disturbances according to claim 8 together with a system for the azimuth monopulse estimate of the evaluation of a target as claimed in claims 5 and 7.

Inventors: FARINA, ALFONSO
Applicants: SELENIA INDUSTRIE ELETTRONICHE ASSOCIATE S.P.A.
Application year: 1982
Main classification: G01S13
IPC codes: G01S13, G01S7, H01Q3