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    • 专利摘要:
    The invention relates to a device for generating complex electromagnetic environments (24) intended to produce electromagnetic test signals to stimulate an electromagnetic sensor (21-22) placed in a test enclosure (11) comprising an anechoic chamber (12). via a radiating panel (14) made up of a plurality of radiating sources (151-15N). The device comprises a set of modules (241, 243, 245i, 246) making it possible to define the electromagnetic environment to be simulated; to determine the characteristics of the signals which would be received by the various reception channels of the electromagnetic sensor under test if it were placed in the electromagnetic environment considered and to synthesize the radiofrequency (RF) signals which the radiating sources must emit to simulate, seen of the sensor (21), the desired electromagnetic environment.
    公开号:FR3082006A1
    申请号:FR1800535
    申请日:2018-05-31
    公开日:2019-12-06
    发明作者:Pierre Bernardi；Julien Canet；Jean Magne
    申请人:Thales SA；
    IPC主号:
    专利说明:

    Method and device for generating complex electromagnetic environments for test benches for electromagnetic sensors
    DOÆO / A / & DE L WVEDT7CW [01] The invention relates to the general field of electromagnetic sensors having one or more reception channels. It relates more particularly to test equipment making it possible to simulate more or less complex electromagnetic environments making it possible to test the performance in terms of detection of such sensors.
    [02] Electromagnetic sensors such as radars, or any other means of detection, are devices which make it possible to detect the position, speed and direction of an object, or target, in its environment. They operate, in a known manner, by emitting an electromagnetic signal in their environment, then by analyzing the signal backscattered by this environment and by all the objects, or targets, which are there.
    [03] The current sensors are mainly pulse sensors operating by acquisition sequences, each sequence consisting of the emission of a train of pulses and the analysis of the signal, backscattered by the environment, following this program. The time difference between two consecutive transmitted pulses, or recurrence period, in known manner defining the ambiguous distance of the sensor and therefore the duration of the reception intervals.
    [04] This environment can consist of fixed or mobile point targets, vehicles or aircraft for example.
    [05] This environment can also consist of elements of terrain, marine areas or atmospheric structures such as clouds or areas of precipitation. In this case we are witnessing the backscattering of more or less diffuse wide echoes which we generally qualify as clutter (soil clutter, sea clutter or atmospheric clutter).
    [06] Very often, the amount of energy backscattered by the geographic and atmospheric environment exceeds the amount of energy backscattered by the target or targets therein, so that, insofar as they are mixed with the signal of higher level backscattered by the environment, the signals backscattered by these objects are sometimes difficult to detect.
    [07] To carry out this detection task, the backscattered signal is recorded and then processed using different algorithms so as to allow the separation of the backscattered signal by the environment from the useful signal which could be masked by it. By useful signal is meant here a signal backscattered by an object of interest that one wishes to detect.
    [08] Testing the proper functioning of an electromagnetic sensor therefore involves testing the operational efficiency of the target detection algorithms implemented by the sensor. This ability to carry out these tests is a determining point in the development of current and future sensors.
    [09] To do this, it is possible to proceed in the field, that is to say by installing the equipment to be tested on, or in, a carrier vehicle (an airplane or a helicopter for example), then by changing different targets in the presumed detection field of the material. The detection, or not, of these targets makes it possible to confirm, or not, that the hardware behaved as expected during its design.
    [10] Conducting field tests can vary the test conditions and in particular the environmental conditions. We can for example move targets above the fields, or above the sea. We can also perform tests in rain or fog, to verify that these climatic conditions do not affect the detection capacity of the equipment tested.
    [11] Unfortunately, the tests carried out in the field are extremely expensive, which is why they are preferred, in some cases, those carried out by means of simulation benches, or test installations, which often prove to be more economical. interesting.
    [12] However, the test installations for electromagnetic sensors currently implemented are generally designed to ensure the simulation of echoes or ORE (Radio Electric Objects) supposed to emanate from point sources or of relatively small extent, such as echoes coming from targets, fixed or mobile, each echo being generated independently of the others.
    [13] Such installations generally comprise a fixed radiating panel, a panel in the form of a spherical cap for example, on which radiating elements are placed, for example RF horns. The axis of this radiant panel is oriented in the direction of the sensor to be tested. They also include various calculation modules, the role of which is to determine the shape and the amplitude of the signals which the horns must emit for a given test.
    [14] The horns are supplied through switching means by radio signal generators capable of generating signals whose amplitude and possibly the phase are controlled, so that by acting on the switching means it is possible to supply a or several radiating elements alternately or alternatively supply a certain number of radiating elements or groups of radiating elements simultaneously.
    [15] However, the number of radiating elements, horns, which can be supplied simultaneously is naturally a function of the number of radio signal generators and switching means available to the installation. However, mainly because of their cost, a test installation includes a limited number of such generators.
    [16] Consequently, even if the radiating panel is large and comprises a large number of radiating elements, the number of radiating elements which can be supplied simultaneously is necessarily limited. The number of point targets that such an installation can generate simultaneously is therefore also limited.
    [17] From a functional point of view, because of their structure designed to independently simulate various point echoes, such installations do not allow realistic simulations of complex electromagnetic scenes, formed in particular of point echoes (of targets) ) operating in a clutter-generating environment, only by considering the signal received by the sensor in such an environment as a multitude of punctual echoes from distinct directions, the combination of which would be capable of constituting an approximation of the clutter in question at the sensor .
    [18] However, simulating such a number of punctual echoes from ORE requires having the necessary material resources, in this case a number of horns and a number of sufficient RF signal generators, which is not generally not the case, because of the number of horns to be activated simultaneously. Consequently, it is generally not possible, with such test installations, to create enough OREs to realistically simulate a complex environment.
    [19] Furthermore, notwithstanding the problem posed by the number of sources required, the principle consisting in carrying out the simulation of clutter from radio sources located on a radiating panel by stimulating each source independently as a function of its position relative to the sensor, does not, in principle, make it possible to carry out a representative simulation of the electromagnetic environment backscattered by a large clutter source, ground or sea clutter, or atmospheric clutter for example.
    [20] Indeed, clutter originating from complex natural phenomena, which can be located anywhere in the space surrounding the sensor and be more or less extensive, simulating a clutter by this principle requires generating an electromagnetic environment s extending over a much larger angular zone (typically extending over 2π steradians) than the angular zone covered by the radiating elements, the horns, necessarily located on the surface of the radiating panel equipping the test installation considered, zone limited to l angular extent covered by the radiating panel.
    [21] It can therefore be seen that the existing test installations which are suitable for the simulation of point radio objects (ORE) do not allow, because of the number of sources that can be activated simultaneously and the position of these sources on a panel of limited scope, to simulate a complex environment realistically. However, future generations of electromagnetic sensors are called upon to implement processing of the received signals making it possible to discern the signals emanating from one or more targets of the background electromagnetic noise, or clutter, emanating from the environment. Consequently, the test facilities which will be used to test these future instruments, must be provided with means enabling them to simulate not only targets, but also clutter.
    [22] An object of the invention is to propose a solution allowing the use of existing test installations, capable of activating a limited number of point radio sources distributed in a limited angular sector compared to the angular sector covered by the equipment. under test, so as to be able to simulate a complex electromagnetic scene corresponding to a clutter-generating environment.
    [23] Another object of the invention is to propose a solution making it possible to simulate an electromagnetic scene including one or more evolving targets in a clutter-generating environment.
    To this end, the subject of the invention is a device for generating complex electromagnetic environments intended for producing electromagnetic test signals to stimulate an electromagnetic sensor comprising N reception channels, said sensor being placed, on a support, in an enclosure test device comprising an anechoic chamber and a radiating panel made up of at least N radiating sources and configured to be connected to an equipment for generating RF excitation signals, and to radiate the corresponding electromagnetic wave inside the anechoic chamber to the material under test. The device according to the invention mainly comprises:
    - an electromagnetic scene definition module which delivers data defining the electromagnetic environment that we want to simulate and to which we want to submit the sensor under test;
    - an electromagnetic scene calculator which produces sets of Doppler - distance cards, each card representing, for a given acquisition sequence and for a given sensor reception channel, the frequency distribution, as a function of the distance, of the signal strength received for the electromagnetic environment defined by the electromagnetic scene definition module;
    - a transfer suppression module which modifies each Doppler-distance card produced by the electromagnetic scene calculator so as to produce a Doppler-distance modified cards, corresponding to the signal which a given radiating source must radiate from the radiating panel to simulate, at the level the sensor reception channels, the electromagnetic environment desired for the corresponding acquisition sequence;
    - modules for synthesis and amplification of radio frequency (RF) signals, each module performing the synthesis of the RF signal corresponding to a Doppler card - given modified distance, produced by the transfer suppression module, the RF signal produced being delivered to a given radiant source.
    According to various arrangements which can be considered separately or in combination with one another, the device according to the invention may include the following technical characteristics.
    According to a first characteristic, the support of the test enclosure being a three-axis table, the device comprises a module for acquiring data from said three-axis table, data which is transmitted to the transfer suppression module.
    According to another characteristic, the device according to the invention comprises a module for acquiring sensor operating data, data which is transmitted to the transfer suppression module and to the electromagnetic scene calculator.
    According to another characteristic, the device according to the invention further comprises switching means making it possible to connect each module for synthesis and amplification of signals to one or the other of the radiating sources of the radiating panel.
    According to another characteristic, the transfer deletion module comprises:
    - a processor configured to build the inverse matrix T -1 of the transfer matrix T which characterizes the propagation of the electromagnetic waves emitted by the radiating sources of the radiating panel up to the reception modules of the sensor for a given Doppler frequency;
    - a multiplier configured to perform the product of the inverse matrix T -1 by a reception vector whose N components correspond, for a given acquisition sequence of the sensor, to the values of the signal amplitude measured in the same doppler cell - distance from each of the N Doppler maps - distance produced by the electromagnetic scene calculator for the acquisition sequence considered. The multiplier delivers an emission vector with N components, each component representing the value of the amplitude of the signal to be emitted by the radiating source considered measured for the same doppler-distance cell of each of the modified doppler-distance cards delivered by the suppression module. transfer.
    According to another characteristic, the processor of the transfer suppression module is configured to calculate a separate inverse matrix T -1 for each of the doppler frequencies defining the doppler-distance cells of the doppler-distance cards produced by the electromagnetic scene calculator.
    According to another characteristic, the processor of the transfer suppression module is configured to calculate a single common inverse matrix T -1 , said matrix being calculated for the Doppler frequency defining the central Doppler-distance cell of the Doppler-distance maps produced by the computer. electromagnetic scenes.
    According to another characteristic, each module for synthesis and amplification of radio frequency (RF) signals of the device according to the invention comprises:
    - a processor configured to implement a transformation operation making it possible to transform the modified Doppler-distance card with which it is associated into a long-time short-time card made up of cells, the amplitude of the signal in each cell corresponding to the amplitude of the signal to be radiated for a given distance cell and a given recurrence of the excitation signal;
    - a synthesizer module configured to generate a time-dependent electromagnetic signal, for each recurrence, of the signal amplitudes in each of the short-time long time cells of the short-time-long time map defined by the same recurrence number on the time axis long.
    The invention also relates to a method for generating complex electromagnetic environments intended to produce electromagnetic test signals to stimulate an electromagnetic sensor under test placed on a support in a test enclosure comprising an anechoic chamber as well as a radiant panel made up of a plurality of radiating sources and configured to be connected to an equipment for generating RF excitation signals, and to radiate the corresponding electromagnetic wave inside the anechoic chamber towards the sensor to be tested. Said method is intended to implement a device for generating complex electromagnetic environments according to the invention. To this end, it includes:
    a first operation consisting in forming, for a given electromagnetic environment scenario, distance Doppler cards such as those which could be formed by the sensor to be tested, for each of its reception channels, in such an environment, from the signals picked up by the reception modules of said sensor;
    a second operation consisting in eliminating, at the level of each Doppler card - distance formed, the transfer through the anechoic chamber, taking into account the position of the sensor to be tested relative to the radiating sources of the radiating panel used, so as to form modified Doppler - distance maps representing the spectra of the signals that the radiating sources must emit so that the sensor perceives an electromagnetic environment corresponding substantially to the scenario developed;
    a third operation consisting, for the signal generators, in converting the spectra of the signals corresponding to the Doppler maps - modified distance into temporal signals, then in radiating these signals towards the sensor, via the radiating sources, through the anechoic chamber.
    According to a particular technical characteristic, the method according to the invention further comprises an additional operation consisting in acquiring the signals picked up by the reception modules of the sensor during the course of the test scenario considered and in forming Doppler - distance cards from the signals recorded, during the test, at the level of the sensor reception modules for each of the reception channels.
    [24] The invention advantageously makes it possible to simulate complex electromagnetic scenes using the equipment available in existing test facilities; in particular by using the anechoic chamber, the three-axis table, and the radiating panel with which such an installation is generally provided.
    [25] It also has the advantage of requiring the implementation only of a number of radiating horns equal to the number N of the reception channel of the sensor under test. This advantageously limits the number of RF signal generators and horns necessary for the simulation of an electromagnetic environment. The invention therefore offers a simple means for simultaneously simulating target echoes and disturbing, clutter or other signals; means which brings into play a lighter material architecture than those used today [26] The proposed invention also makes it possible, advantageously, to simulate electromagnetic scenes without angular limitation.
    [27] It also has a much more flexible configuration than existing installations, depending less on the use of a three-axis table as a support for the equipment to be tested.
    [28] The characteristics and advantages of the invention will be better appreciated from the following description, which description is based on the appended figures which show:
    the figure, the functional schematic representation of a test installation according to the prior art;
    FIG. 2, the functional schematic representation of an example of a test installation in which the device according to the invention is integrated;
    Figure 3, a schematic representation of a distance Doppler card implemented in the context of the invention;
    Figure 4, a block diagram illustrating the structure and operation of the transfer removal module of the device according to the invention;
    Figure 5, a block diagram illustrating the structure and operation of the excitation signal generator module of the device according to the invention;
    [29] It should be noted that, in the appended figures, the same functional or structural element preferably bears the same reference symbol.
    [30] Figure 1 shows a schematic illustration of a test installation 11 of the type known from the prior art.
    [31] Such an installation 11 comprises an anechoic chamber 12, in which is installed a support 13 intended to receive the sensor to be tested. As illustrated in FIG. 1, the support 13 is generally a three-axis table (TTA), or any other equivalent device making it possible to vary the orientation and / or the attitude of an object which is mounted on the latter. However, in a simple embodiment, the installation 11 can simply comprise a fixed support.
    [32] The anechoic chamber 12 has the function of attenuating as much as possible, if not completely eliminating, the parasitic radio signals which may come from the environment of the installation considered.
    [33] The three-axis table 13 is configured so as to be able to accommodate a sensor 21 under test (MST), said sensor then being fixed on the three-axis table (TTA). The sensor 21 under test considered here comprises a modular antenna 22 made up of several reception modules 231 to 23N.
    [34] Such an installation 11 also includes a radiating panel 14 which faces the three-axis table (or the support) 13 and on which radiofrequency radiating horns 151 to 15N are positioned. In the following description, the term “radiant horns” will be used generically, it being understood that, in the context of the invention, these radiating horns can be replaced by any other element capable of radiating a radio wave.
    [35] Cornets 151 to 15N are configured and arranged on the radiating panel 14 so as to transmit radio frequency signals whose wave planes recombine in the vicinity of the reception modules 231 to 23N of the sensor under test 21 when the latter is mounted on the three-axis table (TTA) (or on the support) 13. The recombined signals are assumed to be close to those that a complex electromagnetic environment would have backscattered.
    [36] Depending on the installation considered, the radiating panel may include a number M of horns greater than the number N of reception channels of the sensor under test (MST) 21. However, in the context of the invention, use is made of preferably a number of horns 15 equal to the number of sensor reception channels; knowing that the number of cones must be at least equal to the number of reception channels. In this way, as will appear in the rest of the text, the transfer relation can be written in the form of a linear system whose matrix is square.
    [37] However, when the radiating panel of the installation has more horns 15 than the sensor 21 has reception channels, the horns operated can be chosen according to their positions on the radiating panel 14, so as to minimize the impact of a transmission fault on the signal to be reproduced.
    [38] The Test Installation 11 further comprises a module for generating test signals 16 which ensures the generation of test scenarios and whose role is to generate, as a function of the test scenario considered, the control signals and synchronization intended to drive the radio signal generators 17a to 17N responsible for generating the excitation signals transmitted to the horns 151 to 15N of the radiating panel 14 used to carry out the test.
    [39] These commands and synchronizations depend on the operating mode adopted for the test considered by the sensor under test (MST) 21. This information concerning the operating mode of the sensor can be transmitted to the test signal production unit. 16 by a sensor data acquisition module 18 connected itself to the sensor 21.
    [40] These commands and synchronizations are also a function of the altitude, speed and orientation data of the carrier, the orientation being simulated by means of the three-axis table (TTA) in the case where the support 13 is constituted by such a table, the orientation data being transmitted to the test signal production unit 16 by a module 247 for acquiring data 19 relating to the three-axis table, module connected to the latter by any suitable connection means , wire connection or other.
    [41] The horns are supplied through switching means (not shown in the figure) by the radio signal generators 171 to 17N.
    [42] As can be seen in the diagram in FIG. 1, the test signal production unit 16 carries out the separate control of each of the generators 171 to 17N of radio signals, each generator producing an RF signal intended to supply simultaneously one or more horns, or groups of horns, so as to constitute one or more punctual OREs. As mentioned above, such an installation is therefore in principle designed to simulate occasional or small-scale echoes rather than environments with clutter.
    [43] The following description presents in detail the functional structure of the device 24 for generating complex electromagnetic environments according to the invention, as well as the operating principle of the various modules that make up this device.
    [44] This device can advantageously be integrated into an existing test installation, by replacing a conventional test signal production unit 16 or by operating in parallel with the latter. It can also be part of a test installation specially designed to optimize the sensor test by taking full advantage of the functional advantages which the device provides, in particular in terms of number of horns, for the realization of the envisaged test environments.
    [45] In the embodiment shown diagrammatically in FIG. 2, presented by way of nonlimiting example, the device for generating complex electromagnetic environments 24 according to the invention mainly comprises:
    - an electromagnetic scene calculator 241;
    - a transfer deletion module 243;
    - modules for synthesis and amplification of RF signals 2451 to 245N;
    - a module for defining electromagnetic scenes 246;
    a module 247 for acquiring data from the three-axis table 13;
    a module 248 for acquiring data from the sensor 21.
    [46] It should be noted here that the module 248 for acquiring data from the sensor 21 may be absent from certain embodiments of the device 24 according to the invention. These are in particular the embodiments ensuring a so-called open loop operation for which the simulated environment is a static environment.
    [47] The main function of the electromagnetic scene calculator 241 is to carry out the simulation of a given electromagnetic scene, this simulation being based on physical modeling of a given environment of the sensor 21. The simulation is carried out taking into account input parameters characterizing the electromagnetic scene that one wishes to simulate as well as, preferably, the operating data of the sensor under test 21 itself.
    [48] This simulation takes the form of the estimation and production, by any method known elsewhere and not described here, of sets of Doppler maps - distance, 2421 to 242N, which represent, for each reception module 231 to 23N of the antenna 22 of the sensor, the frequency distribution of the power of the received signal as a function of the distance, for an electromagnetic environment corresponding to the scene considered and for the waveform used by the sensor.
    [49] Thus, for example with regard to a given mobile target simulation, the corresponding distance Doppler map can be determined by considering the evolution model of the target considered (evolution of the velocity and acceleration vectors and of the equivalent surface by example).
    [50] Furthermore, with regard to an environment simulation, the corresponding distance Doppler map can be determined, for example, by discretizing the geometry of the environment into elements, then, for each element, by calculating the backscattered power. by the element considered, by calculating the speed (Doppler) distance coverage of this element, then finally by introducing the power backscattered by this element in the speed - corresponding distance area of the map.
    [51] In the context of an open loop operation of the test installation in which the device is located, the successive distance Doppler cards are memorized and used successively as the simulated electromagnetic scene proceeds. In other words, each group of cards 2421 to 242N relating to a sensor operating sequence is stored in a table, contained in a memory circuit for example, so as to remain available throughout the period of analysis of the scene by the sensor 21 and as long as the simulated electromagnetic scene does not cause modification of this map.
    [52] By open loop operation here is understood an operation for which the kinematic parameters of the sensor and their evolution are determined a priori so that the electromagnetic scene to be simulated can be a scene memorized to be played in due time [53] however in closed loop operation, the Doppler distance maps corresponding to the simulation are generated dynamically for the current analysis period carried out by the sensor and used directly.
    [54] By closed loop operation is meant here an operation for which the kinematic parameters of the sensor are taken into account in real time, the simulated electromagnetic scene having to take these parameters into account as they evolve. The simulated electromagnetic scene is then dependent on the state of these parameters.
    [55] As mentioned above, the clutter originates from complex natural phenomena of which it is generally impossible to carry out a completely exact simulation in a reasonable time, in other words a time less than the time separating two acquisition sequences.
    [56] In general, the input parameters used to generate such Doppler - distance maps can be classified into two categories:
    - the operating parameters of the equipment under test (carrier kinematics, processed waveforms, transmitter parameters, receiver parameters, ...),
    - the environmental parameters that define the operating conditions that we want to simulate.
    [57] Thus, in the case of the simulation of a rain clutter for example, these parameters will concern the properties of the rain, in particular its extent, its flow and its coefficient of attenuation.
    Similarly, in the case of simulating a target, this could be its kinematics and its equivalent surface.
    Similarly, in the case of simulating a soil clutter, these parameters could notably concern, depending on the incidence of the radar wave, the topography of the terrain, the backscatter coefficient of the different topographic areas (forests , sea, fields, snowy surfaces ...).
    [58] From a hardware point of view, the electromagnetic scene calculator 241 may consist of a programmable component of FPGA type or a CPU, possibly associated with storage means.
    [59] The data or parameters characterizing the electromagnetic scene that one wishes to simulate are transmitted to the electromagnetic scene calculator 241 by the definition module 246. The electromagnetic scene data define the electromagnetic environment of the sensor 21 that one wants simulate. In general, they depend on the type of scene that one wishes to simulate.
    [60] Thus, for example, if the test carried out consists in studying the behavior of the sensor 21 in the presence of rain, the electromagnetic scene data supplied by the definition module 246 will relate for example to the position, the speed, the shape, the flow of rain.
    [61] On the other hand, if the test consists in studying the impact of the soil clutter on the detection performance of the sensor, then the electromagnetic scene data may contain the coefficients of soil backscattering and the geographic areas to which these apply. coefficients as well as the topography of the simulated terrain.
    [62] In general, the electromagnetic scene data and, very generally, the operational data specific to the sensor 21 thus constitute the input parameters of the electromagnetic scene calculator 241. These parameters are variable depending on the type of simulated environment and the degree of interdependence of the sensor and the installation.
    [63] The module 246 which allows the scene computer 241 to develop the Doppler - distance cards can, for example, consist of a memory block containing the scene data, addressed directly by the scene computer.
    [64] The operating data of the sensor 21 is transmitted to the electromagnetic scene computer 241 by the module 248 for acquiring the operating data of the sensor. The data acquired may consist in particular of the direction of the antenna vector as well as of the characteristics of the waveform used by the sensor.
    This module performs the acquisition of this data periodically for each analysis period of the sensor 21. The operating data flow of the sensor 21 can indeed change with each new acquisition sequence of the received radio signal. The sensor data acquisition module 248 therefore carries out their acquisition for each new acquisition sequence of the radio signal by the sensor and transmits this data to the computer 241 with this same periodicity.
    [65] Figure 3 graphically shows a Doppler distance 242 map. This map is made up of boxes or cells each defined by a Doppler frequency band and by a distance interval, the extent of the Doppler frequency band and the distance interval defining the resolution of the cells forming the map [66] Each cell thus defined contains a signal sample, a pixel p, the value of which represents the amplitude of the corresponding spectral component of the signal received for the distance considered.
    [67] Within the framework of the invention, and according to the operating mode considered, the Doppler-distance cards 2421 to 242N produced by the electromagnetic scene calculator 241 can have an excursion in frequency and in distance sufficient to cover the whole of the Doppler spectrum and the space necessary for the creation of the electromagnetic environment to be simulated. In this case, however, the Doppler-distance cards 2421 to 242N to be produced have a large number of cells so that their production requires more computing time [68] Alternatively, knowing that the sensor to be tested has a certain ambiguity in distance and Doppler and that for Doppler distances and frequencies located beyond the unambiguous zones there is a folding in Doppler and in distance of the received signal, the Doppler-distance cards 2421 to 242N produced by the electromagnetic scene calculator 241 can have frequency and distance excursions simply limited to unambiguous areas.
    [69] In this second case, however, since the distances of the unambiguous areas in distance and in Doppler are likely to vary depending on the operating mode adopted by the sensor for a given analysis period, it is necessary to take into account, for the generation of the simulated electromagnetic environment, the operating parameters of the sensor, such as its frequency and its ambiguity distance, and to size the Doppler maps - distance so as to cover the Doppler frequency ranges and corresponding distances, so that the generation of these maps is made more complex.
    [70] The function of the transfer suppression module 243 is, as illustrated in FIG. 4, to convert the estimated Doppler maps - distance 2421 to 242N, produced by the electromagnetic scene calculator 241 at the reception modules 231 to 23N of sensor 21, in modified Doppler maps - distance 2441 to 244N, representative of the signals that the horns 151 to 15N must transmit so that sensor 21 perceives a signal equivalent to that which the scene simulated by the electromagnetic scene calculator would have 241; in other words, so that the signals effectively perceived by the reception modules 231 to 23N of the antenna 22 of the sensor 21 are substantially equal to the signals perceived that the electromagnetic scene simulated by the electromagnetic scene calculator 241 would have backscattered.
    [71] To estimate the Doppler cards - distance 2441 to 244N, the transfer suppression module 243 calculates and applies to the Doppler cards - distance 2421 to 242N the reverse transfer of the transfer introduced by the space between the horns 151 to 15N and the reception modules 231 to 23N of the antenna 22 of the sensor 21. To do this, the transfer suppression module 243 uses the data 19 coming from the three-axis table 13, as well as the data 18 coming from the sensor 212.
    [72] To perform this operation, the transfer suppression module 243 implements, as illustrated in FIG. 3, a processor 31 and a multiplier 32, these two elements being able to consist of two separate electronic components or alternatively be integrated into the same electronic component, a microprocessor or an FPGA for example.
    Alternatively, the processor 31 and the multiplier 32 can consist of two functions integrated into the electronic circuit constituting the electromagnetic scene calculator 241.
    [73] The transfer suppression operation consists firstly in constructing the inverse matrix T -1 33 of the transfer matrix T characterizing the transit of the signals from the horns 151 to 15N from the radiating panel to the reception modules 231 to 23N of the antenna 22 of the sensor 21 for a given Doppler frequency, a different matrix being able to be constructed for each of the Doppler frequencies of the card considered.
    [74] However, due to the small variation observed in the coefficients of the different matrices, the device according to the invention can, in a simplified embodiment, calculate and use only a single matrix or a limited number of matrices for the 'whole of the considered card, the matrix corresponding to the central Doppler frequency for example. This operation is carried out by the processor 31.
    [75] The coefficients of the matrix T depend on the working frequency of the sensor 21 and on the position of the reception modules 231 to 23N with respect to the horns 151 to 15N. We show indeed that, from a theoretical point of view, the Maxwell equations which govern the propagation of electromagnetic waves in space being linear, we can write:
    R = T-E [001]
    In equation [001], E is the vector resulting from the concatenation of the amplitude of the signals transmitted by the horns 151 to 15N and R is the vector resulting from the concatenation of the amplitude of the signals recorded by the reception modules 231 to 23N of the antenna 22 of the sensor 21.
    [76] As a result, we can write reciprocally:
    E = T ^ -R [002] as far as it makes sense.
    [77] It should be noted here that the values of the coefficients of the matrix
    7] depend on the relative positions of the horns 151 to 15N and of the reception modules 231 to 23N as well as of the transmission characteristics of the horns and of the reception characteristics of the antenna modules.
    [78] Consequently, for equation [002] to present a solution T -1, it suffices therefore to arrange the RF emission horns 151 to 15N in such a way that the following condition is satisfied:
    Det (T) Φ 0 [003] [79] Consequently, the condition [003] being satisfied, and knowing the position of the RF emission horns 151 to 15N, The matrix T -1 can be estimated in different ways.
    [80] The matrix T -1 can thus be determined analytically, from linear relations expressing the amplitude of the signals received at each antenna module as the sum of the signals transmitted by the different horns, each signal being affected by '' a phase shift depending on the distance between the module considered and the horn.
    [81] Alternatively, the matrix T -1 can also be determined by simulation from the orientation data of the three-axis table 13 on which the sensor 21 is placed and knowledge of the waveform emitted by the sensor.
    [82] Alternatively also, the matrix T -1 can be stored in a database developed during a calibration operation consisting in determining and storing, for different orientations of the three-axis table 13 and for different groups horns (in the case where, the radiating panel comprising more than N horns, it is possible to choose the N horns used by the device), the coefficients of the matrix T -1 .
    [83] The identification of the coefficients of the matrix T -1 by calibration can then consist in exciting the RF emission horns 151 to 15N in turn. The measurements of the signals received by the sensor at each reception module 231 to 23N then define the columns of the transfer matrix T. This matrix is then inverted to obtain the matrix T -1 .
    [84] This identification can, alternatively, be carried out, when technically possible, by exciting the reception modules 231 to 23N one by one. The measurements of the signals received at each RF horn 151 to 15N then directly define the columns of the matrix T -1 , so that no matrix inversion is to be carried out.
    [85] Once the matrix T -1 has been determined, the transfer suppression operation continues by constructing, for each distance Doppler cell, a reception vector 34 whose N components correspond to the amplitude values taken by the signal in the cell. considered for each of the N Doppler-distance cards 2421 to 242N produced by the electromagnetic scene calculator 241, then by multiplying the vector 34 thus formed by the matrix T -1 . The product vector thus obtained, or emission vector 35, is a vector with N components.
    [86] Obtaining an emission vector for each pixel (distance Doppler) considered then makes it possible to construct N corrected distance Doppler maps 2441 to 244N, of dimensions identical to those of the Doppler-distance maps produced by the electromagnetic scene calculator 241 , each corrected card of rank i comprising the component of rank i of each of the transmission vectors 35.
    [87] The scalar product of the inverse transfer matrix T -1 , 33, with the reception vector 34 is performed in the multiplier 32. The multiplier 32 returns an emission vector 35, each component of the emission vector 35 corresponding to the amplitude of a pixel from one of the Doppler maps - distance 2441 to 244N.
    The Doppler maps - distance 2441 to 244N are thus estimated by scanning all the pixels of the maps 2421 to 242N by applying the method described above. These corrected cards 2441 to 244N have the same dimensions as the initial Doppler-distance cards 2421 to 242N produced by the electromagnetic scene calculator 241. They constitute a frequency representation of the signal which each horn 151 to 15N must emit.
    [88] The function of signal generators 2451 to 245N is, as illustrated in Figure 4, to convert the Doppler maps - distance 2441 to 244N into time signals intended to excite the horns 151 to 15N.
    [89] The conversion of the Doppler-distance representation into a temporal representation is effected by each calculation module 41 i which applies to the pixels forming a same line of the Dopplerdistance map (iso-distance line) an inverse Fourier transform TFI so which leads to obtain a card 42i representing the signal in a long time - short time space, the long time representing the successive periods of acquisition of the signals by the sensor 21 (recurrence periods) and the short time representing the distance samples taken by the sensor 21 during the same acquisition period (distance samples).
    [90] A long time - short time map 42i is thus formed of cells, each cell being identified on the map by a recurrence number on the long time axis and a distance box number (a distance interval) on the short time axis and containing a signal sample or pixel p 'whose amplitude corresponds to the amplitude of the signal backscattered by the scene for the distance and the recurrence considered.
    [91] The values of the amplitudes of the pixels of a column of the map
    Recurrence number - Distance sample number 42i represent the energy of the wave packets recorded by the sensor at different times during the corresponding recurrence.
    [92] Each of the long time - short time cards 42i is used by a calculation module 43i which receives the information relating to the operating data of the sensor, the characteristics of the waveform emitted in particular. From this data, the calculation module 43i considered, delivers to the corresponding horn 15i, recurrence after recurrence, a time signal which corresponds to the concatenation of the pixels forming a same acquisition period (ie the same recurrence), the pixels being delivered at the rate of the sampling period with which the sensor 21 samples the signals picked up by the reception modules 231 to 23N.
    [93] The time signals thus formed are transmitted to the horns 151 to 15N and then emitted in the anechoic chamber 12 towards the sensor 21. The spatial distribution of the signal emitted at the plane of the antenna 22 of the sensor 21 resulting from the recombination of the signals emitted by the horns 151 to 15N is close to the signal backscattered by the electromagnetic scene estimated by the electromagnetic scene calculator 2411.
    [94] As described structurally and functionally in the preceding paragraphs, the device 24 for generating complex electromagnetic environments according to the invention implements a certain number of operations.
    [95] The first operation consists of the scene computer 241 forming, for a given simulated electromagnetic scene (environmental scenario), Doppler maps - distance such as those which could be formed from the signals picked up by the modules of reception 231 to 23N of the antenna 22 of the sensor 21, for each of its reception channels, in this environment.
    This electromagnetic scene is produced by implementing software for generating environmental simulation scenarios which produces, for each acquisition channel of the sensor 21 and for each acquisition sequence, Doppler-distance maps which correspond to the simulated environment.
    [96] The second operation implemented by the transfer suppression module 243 consists in suppressing, at the level of the Doppler card - current distance considered, the transfer through the anechoic chamber. Knowing the position of the sensor 21 to be tested relative to the horns 151 to 15N of the radiating panel 14 used to carry out the test, we can indeed estimate the transfer in amplitude and in phase due to the space separating the sensor from the latter. The elimination of this transfer provides an estimate of the spectra of the signals that the horns 151 to 15N must emit so that the sensor 21 perceives an electromagnetic environment corresponding substantially to the scenario developed by simulation.
    [97] The third operation consists, for signal generators 2451 to 245N, of converting the spectra of the signals intended to excite the horns into time signals, then of transmitting these time signals to the sensor 21, via the horns, through the anechoic chamber 12.
    [98] These operations can be followed, in a particular implementation mode, by an additional operation consisting in acquiring the signals picked up by the antenna modules of the sensor during the course of the test scenario considered, of form a Doppler - distance card from the signals recorded, during the test, at the antenna modules for each of the reception channels. The map obtained can advantageously be compared to that produced by simulation.
    [99] Advantageously, the device according to the invention treats all radioelectric objects (ORE) identically, the structure and behavior of which can be described using distance Doppler maps. The invention therefore provides a means of having only one generation mode for all the existing OREs (clutter, rain, targets, jammers ...).
    [100] If we consider a test installation comprising a device for generating complex electromagnetic environments according to the invention, it can be seen that it can be implemented in different ways.
    [101] According to a nominal implementation mode, the installation uses the orientation commands of the three-axis table 13 to be able, if necessary, to reproduce the dynamics of a carrier vehicle. In this use case, the transfer suppression module 243 uses the data 19 coming from the three-axis table 13 which must be transmitted to it by the data acquisition module 247 at each new analysis in order to determine the coefficients of the reverse transfer matrix 33.
    [102] According to a lightened mode of implementation, the three-axis table 13 is maintained in a fixed position throughout the test scenario. In this mode of implementation, the characteristics describing the state of the three-axis table 13 are transmitted to the transfer suppression module 243 at the start of the test scenario. The inverse transfer matrix 33 is estimated only once and remains the same for the duration of the scenario.
    [103] The device according to the invention advantageously makes it possible to reproduce, in the vicinity of the sensor, a signal equivalent to that generated by a complex electromagnetic scene. The electromagnetic scene generated can include complex natural objects such as for example a terrain area, a marine area or even a rainy atmospheric area accompanied by targets.
    [104] As such, the module according to the invention can advantageously be integrated into an existing test installation 11 such as that illustrated in FIG. 1 and come to replace the means for generating existing test echoes, means generally configured to generate ORE simulating echoes of fixed or moving point targets.
    [105] Alternatively, however, the device according to the invention can also complement these means and support the simulation of complex objects generating clutter while the means for generating existing test echoes remain used for the simulation of fixed or mobile occasional echoes. In this case, insofar as the device according to the invention requires for its implementation only a number N of radiating horns equal to the number of reception channels of the sensor under test, it is advantageously possible to use the other horns forming the radiant panel for emitting radio signals corresponding to point target echoes.
    权利要求:
    Claims (10)
    [1" id="c-fr-0001]
    1. Device for generating complex electromagnetic environments (24) intended to produce electromagnetic test signals to stimulate an electromagnetic sensor (21-22) comprising N reception channels, placed on a support (13) in a test enclosure ( 11) comprising an anechoic chamber (12) and a radiating panel (14) consisting of at least N radiating sources (151-15N) and configured to be connected to an equipment for generating RF excitation signals, and to radiate the corresponding electromagnetic wave inside the anechoic chamber towards the material under test, characterized in that it mainly comprises:
    - an electromagnetic scene definition module (246) which delivers data which define the electromagnetic environment that we want to simulate and to which we want to submit the sensor under test:
    - an electromagnetic scene calculator (241) which produces sets of Doppler - distance cards (2421-242N), each card representing, for a given acquisition sequence and for a given reception channel (231-23N), frequency distribution, as a function of distance, of the signal strength received for the electromagnetic environment defined by the electromagnetic scene definition module (246);
    - a transfer suppression module (243) which modifies each Doppler - distance card (2421-242N) produced by the electromagnetic scene calculator (241) so as to produce a modified Dopplerdistance cards (2441 to 244N), corresponding to the signal that must radiate a given radiating source (151-15N) from the radiating panel (14) to simulate, at the level of the reception channels (231-23N) of the sensor (21), the electromagnetic environment desired for the corresponding acquisition sequence;
    - modules (2451-245N) for synthesis and amplification of radio frequency (RF) signals, each module performing the synthesis of the RF signal corresponding to a Doppler card - modified distance - data (2441 to
    244N) produced by the transfer suppression module (243), the RF signal produced being delivered to a given radiating source (151-15N).
    [2" id="c-fr-0002]
    2. Device according to claim 1, characterized in that the support (13) of the test enclosure (11) being a three-axis table, the device comprises a module (247) for acquiring data from said table three axes (13), this data being transmitted to the transfer deletion module (243);
    [3" id="c-fr-0003]
    3. Device according to one of claims 1 or 2, characterized in that it comprises a module (248) for acquiring operating data of the sensor (21-22), this data being transmitted to the transfer suppression module (243) and to the electromagnetic scene calculator (241).
    [4" id="c-fr-0004]
    4. Device according to one of claims 1 to 3, characterized in that it further comprises switching means making it possible to connect each module (2451-245N) for synthesis and amplification of signals to one or the other. 'other of the radiating sources (151-15N) of the radiating panel (14).
    [5" id="c-fr-0005]
    5. Device according to any one of claims 1 to 4, characterized in that the transfer suppression module (243) comprises:
    - A processor (31) configured to build the inverse matrix T ~ l (33) of the transfer matrix 7 which characterizes the propagation of the electromagnetic waves emitted by the radiating sources (151-15N) from the radiating panel (14) to the modules receiving (231-23N) the sensor (21) for a given Doppler frequency;
    - a multiplier (32) configured to perform the product of the inverse matrix Γ 1 (33) by a reception vector (34) whose N components correspond, for a given acquisition sequence of the sensor, to the values of the amplitude of signal measured in the same doppler-distance cell of each of the N Doppler-distance cards (2421 to 242N) produced by the electromagnetic scene calculator (241) for the acquisition sequence considered; the emission vector (35) thus obtained being a vector with N components, each component representing the value of the amplitude of the signal to be emitted by the radiating source considered measured for the same doppler-distance cell of each of the modified doppler-distance cards ( 2441-244N) delivered by the transfer deletion module (243).
    [6" id="c-fr-0006]
    6. Device according to claim 5, characterized in that the processor (31) is configured to calculate a separate inverse matrix T -1 for each of the doppler frequencies defining the doppler-distance cells of the doppler-distance cards (2421-242N) produced by the electromagnetic scene calculator (241).
    [7" id="c-fr-0007]
    7. Device according to claim 5, characterized in that the processor (31) is configured to calculate a single common inverse matrix T -1 , said matrix being calculated for the Doppler frequency defining the central Doppler cell-distance of the Doppler maps (2421 -242N) produced by the electromagnetic scene calculator (241).
    [8" id="c-fr-0008]
    8. Device according to any one of the preceding claims, characterized in that each module (2451-245N) for synthesis and amplification of radiofrequency (RF) signals comprises:
    - a processor (41 i) configured to implement an inverse Fourier transformation operation making it possible to transform the modified doppler-distance card (2441-244N) with which it is associated into a short time-long time card (42) consisting cells, the amplitude of the signal in each cell corresponding to the amplitude of the signal to be radiated for a given distance cell and a given recurrence of the excitation signal;
    - a synthesizer module configured to generate a temporal electromagnetic signal which is a function, for each recurrence, of the signal amplitudes in each of the short time long time cells of the short time long time card (42) defined by the same recurrence number on the 'long time axis.
    [9" id="c-fr-0009]
    9. Method for generating complex electromagnetic environments intended to produce electromagnetic test signals to stimulate an electromagnetic sensor under test (21-22) placed on a support (13) in a test enclosure (11) comprising an anechoic chamber ( 12) and a radiating panel (14) made up of a plurality of radiating sources (151-15N) and configured to be connected to an equipment for generating RF excitation signals, and to radiate the corresponding electromagnetic wave inside from the anechoic chamber to the sensor to be tested, said method implementing a device (24) for generating complex electromagnetic environments according to any one of claims 1 to 8, characterized in that it comprises:
    a first operation consisting in forming, for a given electromagnetic environment scenario, distance Doppler cards such as those which could be formed by the sensor to be tested (21), for each of its reception channels, in such an environment, from the signals picked up by the reception modules (231 to 23N) of said sensor;
    - a second operation consisting in removing, at each Doppler card - distance formed, the transfer through the anechoic chamber, taking into account the position of the sensor (21) to be tested relative to the radiating sources (151 to 15N) of the panel radiant (14) used, so as to form modified Doppler maps - distance (2441-244N) representing the spectra of the signals which the radiating sources (151 to 15N) must emit so that the sensor (21) perceives a corresponding electromagnetic environment substantially the scenario developed;
    - a third operation consisting, for the signal generators (245a to 245N), in converting the spectra of the signals corresponding to the modified Doppler - distance cards (2441244N) into time signals, then in radiating these signals towards the sensor (21) radiant sources (151 to 15N), through the anechoic chamber (12).
    [10" id="c-fr-0010]
    10. A method of generating complex electromagnetic environments according to claim 9, characterized in that it further comprises an additional operation consisting in acquiring the signals picked up by the reception modules (231 to 23N) of the sensor 5 during the course of the test scenario considered and to form Doppler - distance cards (2421-242N) from the signals recorded, during the test, at the level of the reception modules (231 to 23N) of the sensor for each of the reception channels.
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    同族专利:
    公开号 | 公开日
    EP3575821A1|2019-12-04|
    FR3082006B1|2020-06-19|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US4467327A|1981-09-22|1984-08-21|The Boeing Company|Active millimeter wave simulator for missile seeker evaluations|
    US6114985A|1997-11-21|2000-09-05|Raytheon Company|Automotive forward looking sensor test station|
    CN111458577B|2020-03-04|2022-03-08|中国工程物理研究院应用电子学研究所|Complex electromagnetic environment construction method|
    CN111521893A|2020-03-23|2020-08-11|中国工程物理研究院应用电子学研究所|Complex electromagnetic environment generation system and method capable of simulating space-time evolution process|
    CN113064125B|2021-03-23|2021-08-31|北京航空航天大学|Complex electromagnetic environment construction method based on radio frequency port response equivalence|
    法律状态:
    2019-04-29| PLFP| Fee payment|Year of fee payment: 2 |
    2019-12-06| PLSC| Search report ready|Effective date: 20191206 |
    2020-05-05| PLFP| Fee payment|Year of fee payment: 3 |
    2021-04-26| PLFP| Fee payment|Year of fee payment: 4 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1800535A|FR3082006B1|2018-05-31|2018-05-31|METHOD AND DEVICE FOR GENERATING COMPLEX ELECTROMAGNETIC ENVIRONMENTS FOR TEST BENCHES OF ELECTROMAGNETIC SENSORS|
    FR1800535|2018-05-31|FR1800535A| FR3082006B1|2018-05-31|2018-05-31|METHOD AND DEVICE FOR GENERATING COMPLEX ELECTROMAGNETIC ENVIRONMENTS FOR TEST BENCHES OF ELECTROMAGNETIC SENSORS|
    EP19176756.5A| EP3575821A1|2018-05-31|2019-05-27|Method and device for generating complex electromagnetic environments for electromagnetic sensor test benches|
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