The presently disclosed subject matter relates to the field of target detection.
In accordance with certain aspects of the presently disclosed subject matter, there is provided a sensor configured to transmit electromagnetic waves towards a target, wherein the sensor is operable to detect, in response to the electromagnetic waves, first electromagnetic waves reflected by the target towards the sensor, second electromagnetic waves received by at least one redirecting device from the target and redirected by the redirecting device towards the sensor, wherein the first and second electromagnetic waves are usable to determine data representative of at least one of a position and a velocity of the target.
In addition to the above features, the sensor according to this aspect of the presently disclosed subject matter can optionally comprise one or more of features (i) to (xv) below, in any technically possible combination or permutation:
According to another aspect of the presently disclosed subject matter there is provided a system including a sensor as described above, and a first redirecting device, configured to redirect second electromagnetic waves received from the target towards the sensor.
According to some embodiments, the system includes a second redirecting device, configured to redirect third electromagnetic waves received from the target towards the sensor.
According to some embodiments, the system includes more than two redirecting devices, each configured to redirect electromagnetic waves received from the target towards the sensor.
In accordance with other aspects of the presently disclosed subject matter, there is provided a method including transmitting, by a sensor, electromagnetic waves towards a target, detecting first electromagnetic waves reflected by the target towards the sensor, detecting second electromagnetic waves received by a first redirecting device from the target and redirected by the first redirecting device towards the sensor, wherein the first and second electromagnetic waves are usable to determine data representative of at least one of a position and a velocity of the target.
In addition to the above features, the method according to this aspect of the presently disclosed subject matter can optionally comprise one or more of features (xvi) to (xxxi) below, in any technically possible combination or permutation:
In accordance with other aspects of the presently disclosed subject matter, there is provided a non-transitory computer readable medium comprising instructions that, when executed by a processor and memory circuitry (PMC), cause the PMC to perform operations comprising obtaining data representative of first electromagnetic waves reflected by a target towards a sensor in response to electromagnetic waves sent by the sensor, obtaining data representative of second electromagnetic waves received by a first redirecting device from the target and redirected by the first redirecting device towards the sensor, and using the first and second electromagnetic waves to determine data representative of at least one of a position and velocity of the target.
According to some embodiments, the operations comprise obtaining data representative of third electromagnetic waves received by a second redirecting device from the target and redirected by the second redirecting device towards the sensor, and using the first, second and third electromagnetic waves to determine data representative of at least one of a position and velocity of the target.
According to some embodiments, the operations can optionally comprise one or more of features (xvi) to (xxxi) above, in any technically possible combination or permutation.
According to some embodiments, the proposed solution enables determination of data representative of a position of a target in a more precise and efficient way.
According to some embodiments, the proposed solution improves performance of an array configured to detect a target. In particular, according to some embodiments, the proposed solution eliminates the stringent constraints present in prior art systems involving an array, such as precise clock synchronization (in time and frequency) between multiple devices of the array.
According to some embodiments, the proposed solution improves operation of a multi-static array.
According to some embodiments, the proposed solution provides position and/or velocity of a target using an array including simple and efficient components.
In order to understand the invention and to see how it can be carried out in practice, embodiments will be described, by way of non-limiting examples, with reference to the accompanying drawings, in which:
In the following detailed description, numerous specific details are set forth in order to provide a thorough understanding of the invention. However, it will be understood by those skilled in the art that the presently disclosed subject matter can be practiced without these specific details. In other instances, well-known methods have not been described in detail so as not to obscure the presently disclosed subject matter.
Unless specifically stated otherwise, as apparent from the following discussions, it is appreciated that throughout the specification, discussions utilizing terms such as “detecting”, “obtaining”, “determining”, “controlling”, “sending” or the like, refer to the action(s) and/or process(es) of a processor and memory circuitry that manipulate and/or transform data into other data, said data represented as physical data, such as electronic, quantities and/or said data representing the physical objects.
The term “processor and memory circuitry” covers any computing unit or electronic unit with data processing circuitry that may perform tasks based on instructions stored in a memory, such as a computer, a server, a chip, a processor, etc. It encompasses a single processor or multiple processors, which may be located in the same geographical zone or may, at least partially, be located in different zones and may be able to communicate together.
Embodiments of the presently disclosed subject matter are not described with reference to any particular programming language. It will be appreciated that a variety of programming languages can be used to implement the teachings of the presently disclosed subject matter as described herein.
System 100 includes a sensor 120 (in particular an active sensor 120), configured to transmit electromagnetic waves 130 towards a target 110 and to receive an electromagnetic signal reflected by the target 110. According to some embodiments, sensor 120 includes a radar equipped by antennas (e.g. collocated or divided antennas) for transmitting and receiving signals and/or a LIDAR. Electromagnetic waves 130 can be located e.g. in the radiofrequency or optical band, but this is not limitative.
In some embodiments, the sensor 120 is configured to scan space in order to detect a target, such as target 110.
Target 110 reflects at least some of the electromagnetic waves 130. According to some embodiments, at least some of the first electromagnetic waves reflected by the target 110 (referred to as 140) are sent back directly to the sensor 120 (e.g. along a direct path between the target 110 and the sensor 120, as shown e.g. in
System 100 further includes at least two redirecting devices 151 and 152 (this is not limitative, and a larger number of redirecting devices can be used). As shown in
Similarly, a second redirecting device 152 receives third electromagnetic waves 175 from the target 110. At least some of the second electromagnetic waves 175 are redirected by the second redirecting device 152 towards the sensor 120.
Sensor 120 detects therefore at least the first electromagnetic waves 140 (directly from the target 110), the second electromagnetic waves 170 (redirected by the first redirecting device 151) and the third electromagnetic waves 175 (redirected by the second redirecting device 152).
According to some embodiments, the redirecting device(s) (e.g. 151 and/or 152) can include e.g. mechanical antenna(s), reflector(s) (such as an electro-mechanical mirror and/or a horn) or electronically steerable antenna(s) (such as a phased array antenna).
According to some embodiments, the redirecting device(s) (e.g. 151 and/or 152) are passive devices that do not generate electromagnetic waves by themselves, but rather redirect the received electromagnetic waves to a different direction.
As explained hereinafter, the first electromagnetic waves 140, the second electromagnetic waves 170 and the third electromagnetic waves 175 are usable to determine data representative of at least one of a position and a velocity of the target 110. In particular in some embodiments, a three dimensional position and/or a three dimensional velocity vector can be determined at each instant of time (in contradiction to a classical radar which cannot determine a velocity vector along certain directions),
According to some embodiments, sensor 120 can include and/or can communicate with a processor and memory circuitry (see processing unit 180 and associated memory 190), which can perform various processing tasks, as explained hereinafter.
According to some embodiments, system 100 includes a single active sensor, and does not require additional active sensors to detect the target and determine data representative thereof.
Attention is now drawn to
In this example, the redirecting device 251 is a mirror. Orientation 202 of the mirror 251 is controlled along two axes (e.g. pan and tilt) by a motor 201. The motor 201 can receive commands to modify orientation of the mirror 251.
In a first orientation of the mirror 251 (
In a second orientation of the mirror 251 (see
As explained hereinafter, the redirection axis of the mirror 251 can be controlled (by controlling orientation of the mirror along one or more axes) such that the electromagnetic waves received from the target and redirected by the redirecting device, are redirected towards the sensor 120.
Attention is drawn to
In this non-limitative example, the redirecting device 350 is a phased array antenna. Upon reception of electromagnetic waves 370 reflected by the target, the phased array antenna can be controlled such that the redirection axis (in this case this corresponds to the axis 371 of the beam emitted by the phased array antenna) is oriented towards the sensor 120. Steering of the beam emitted by the phased array antenna can be carried out electronically, without requiring moving the individual antennas 374 of the phased array antenna. This can be performed by controlling the phase of the individual elements 374 using one or more phase shifters 304 controlled by a controller 303, such that the electromagnetic waves (e.g. radio waves) from the individual elements 374 work together to increase the radiation in the redirection axis, while cancelling radiation in other directions.
According to some embodiments, the phased array antenna is a passive phased array.
Attention is now drawn to
The method includes (operation 400) transmitting electromagnetic waves from a sensor (such as sensor 120) towards a target (e.g. 110). According to some embodiments, the method can include directly illuminating the target with the electromagnetic waves (without a relay between the sensor and the target).
The method includes detecting (operation 410), by the sensor, first electromagnetic waves reflected by the target towards the sensor (as mentioned above, according to some embodiments, at least some of the first electromagnetic waves are reflected by the target along a direct path between the target and the sensor).
The method includes detecting (operation 420), by the sensor, second electromagnetic waves received by a first redirecting device from the target and redirected by the first redirecting device towards the sensor (as mentioned above, at least some of the electromagnetic waves received by the first redirecting device from the target, are redirected towards the sensor).
The method includes detecting (operation 430), by the sensor, third electromagnetic waves received by a second redirecting device from the target and redirected by the second redirecting device towards the sensor (as mentioned above, at least some of the electromagnetic waves received by the second redirecting device from the target, are redirected towards the sensor).
According to some embodiments, in order to ensure that the second electromagnetic waves are redirected towards the sensor, the method can include controlling (operation 425) a redirection axis of the first redirecting device.
According to some embodiments, in order to ensure that the third electromagnetic waves are redirected towards the sensor, the method can include controlling (operation 435) a redirection axis of the second redirecting device.
In some embodiments, this control is performed by the sensor, which sends a command (e.g. through wireless communication) to the first and second redirecting devices. This is not limitative, and in some embodiments, the redirecting devices can be controlled by a processor and memory circuitry (which can be external to the sensor and can e.g. communicate, directly or indirectly, with the sensor).
According to some embodiments, controlling of redirection by the redirecting device(s) can be performed as a two-phase process. In a first phase, first commands (see reference 415 in
In a second phase, subsequent commands (see reference 445 in
In some embodiments, a continuous control of the redirecting axis of the redirecting device is performed, and in other embodiments, a control is performed from time to time (frequency of the control can depend, in particular, on the angular velocity of a line of sight from the redirecting device to the target).
As mentioned above, in some embodiments, a first indication of the position of the target is obtained by the sensor, and can be used to adjust the redirection axes of the redirecting devices. For example, in the case of a mirror, and as shown in
The method can further include (operation 440) using the first, the second and the third electromagnetic waves sensed by the sensor to determine data representative of at least one of a position and a velocity of the target. Since the first, second and third electromagnetic waves are sensed by the same sensor, there is no need to perform an accurate clock synchronization between a clock of the sensor and a clock of another devices in the array. Operation 440 can be performed e.g. by a processor and memory circuitry located in the sensor, and/or by an external processor and memory circuitry.
According to some embodiments, data representative of a position of the target is determined based on a range measured by the sensor (e.g. radar) 120, a time difference of arrival between the first and second electromagnetic waves detected by the sensor, and a time difference of arrival between the first and the third electromagnetic waves detected by the sensor.
According to some embodiments, a full 3D instantaneous position of the target at a given point of time can be determined using the following equations (these equations are not limitative):
c|t
2
−t
1|=2R1 (Equation 1)
c|t
3
−t
1
|=R
1
+R
2
+D
1 (Equation 2)
c|t
4
−t
1
|=R
1
+R
3
+D
2 (Equation 3)
In these equations, c is the velocity of light, t1 is the time at which the electromagnetic waves are transmitted by the sensor, t2 is the time at which the first electromagnetic waves are sensed by the sensor, t3 is the time at which the second electromagnetic waves (redirected to the sensor by the first redirecting device 151 in
Determination of target position by usage of R1, R1+R2 and R1+R3 has a following geometry interpretation: R1 defines the radius of a sphere (which centre is sensor 120) of target possible locations, R1+R2 defines a first ellipsoid of target possible locations (sensor 120 and the first redirecting device 151 are the foci of the first ellipsoid), and R1+R3 defines a second ellipsoid of target possible locations (sensor 120 and the second redirecting device 152 are the foci of the second ellipsoid).
The intersection of the sphere and each of the two ellipsoids generates two circles of possible target locations. The intersection of these two circles provides two points corresponding to the possible target positions. One of the points (called “ghost target”) is eliminated by a constraint on Earth surface (one of a target possible location points is located above Earth surface and the second under the plane defined by sensor 120, first redirecting device 151 and second redirecting device 152).
Algebraic equations are provided hereinafter in order to determine 3D position and/or 3D velocity of the target (these equations are not limitative).
Attention is now drawn to
Assume that the origin of a canonical right Cartesian coordinates system (defined by axes X, Y, Z) is located at sensor 120 (see
In this coordinate system, sensor 120 has coordinates (0,0,0), the first redirecting device 151 has coordinates (D1,0,0) and the second redirecting device 152 has coordinates (X2,Y2,0).
Coordinate Y2 can be obtained by usage of a Heron formula for triangle area. The area SΔ of a triangle defined by points 120, 151 and 152 can be expressed in as follows:
In Equation 4,
As a consequence:
The sign of coordinate Y2 depends on a deployment of the second redirecting device 152 relatively to the X axis.
Coordinate X2 can be obtained by following expression:
X2 is positive if the triangle (as shown in
Attention is now drawn to
The following set of equations expresses the relationships between the target coordinates and tetrahedron edges:
R
1
2
=X
t
2
+Y
t
2
+Z
2
2 (Equation 7)
R
2
2=(Xt−D1)2+Yt2+Zt2 (Equation 8)
R
3
2=(Xt−X2)2+(Yt−Y2)+Zt (Equation 9)
X2 and Y2 are obtained by Equations 5 and 6.
X5 coordinate of the target can be extracted from Equations 7 and 8:
Yt coordinate of the target can be extracted from Equations 7 and 9:
Zt coordinate of the target can be extracted from Equation 7 as follows (Xt and Yt have been determined based on Equations 10 and 11):
Z
t=±√{square root over (R12−Xt2−Tt2)} (Equation 12)
A positive sign of Zt coordinate corresponds to the fact that the target is located above the plane which includes sensor 120, the first redirecting device 151 and the second redirecting device 152. A negative sign of Zt coordinate corresponds to the fact that the target is located below the above mentioned plane. If the sensor 120 is located on ground, a negative sign is indicative of a ghost target.
According to some embodiments, a full 3D instantaneous vector of velocity of the target at a given point of time can be determined based on three Doppler sifts Δf1, Δf2 and Δf3 measured by a sensor 120. A Doppler shift Δf1 is defined as a difference between a frequency f0 of the electromagnetic waves 130 transmitted by the sensor 120 towards the target 110 and a frequency f1 of the first electromagnetic waves 140 detected by the sensor 120. A Doppler shift Δf2 is defined as a difference between frequency f0 and a frequency f2 of the second electromagnetic waves 170 redirected by the first redirecting device 151 and detected by the sensor 120. A Doppler shift Δf3 is defined as a difference between frequency f0 and a frequency f3 of the third electromagnetic waves 175 redirected by the second redirecting device 152 and detected by the sensor 120.
Doppler shift can be calculated by the following equation:
In Equation 13, c is speed of light and V is a projection of target velocity. In Equation 13, the relevant projection V1 of the target velocity measured for the first electromagnetic waves 140 is a projection of the target velocity on a line of sight between the sensor 120 and the target 110. The relevant projection V2 of the target velocity for the second electromagnetic waves 170 is a projection of the target velocity on a line from the middle point between the sensor 120 and the first redirecting device 151 to the target (similar to the Doppler shift measured by bi-static radars). The relevant projection V3 of the target velocity for the third electromagnetic waves 175 is a projection of the target velocity on the line of sight from the middle point between the sensor 120 and the second redirecting device 152 to the target 110.
Assume that target velocity is Vt, for which three components Vtx, Vty and Vtz need to be determined.
The three projections V1, V2 and V3 of the target velocity provide a set of linear equations allowing reconstruction of target velocity Vt components:
The projection V1 of target velocity Vt on the line of sight from the sensor 120 to the target 110 can be expressed as follows:
The projection V2 of target velocity Vt on the line from the middle point between the sensor 120 and the first redirecting device 151 to the target 110 can be expressed as follows:
The projection V3 of target velocity Vt on the line from the middle point between the sensor 120 and the second redirecting device 152 to the target 110 can be expressed as follows:
Vtx can be extracted from Equations 15 and 16:
Vty can be extracted from Equations 15 and 17:
In Equation 19, Vtx is obtained from Equation 18.
Vtz can be extracted from Equation 15:
In Equation 20, Vtx and Vty are obtained from Equations 18 and 19 respectively.
It is understood that data sensed by the sensor over time (first, second and third electromagnetic waves) is usable to determine data representative of at least one of position and velocity of the target over time.
In particular, the method depicted in
Attention is now drawn to
There are several cases in which kinematic behaviour of the target is associated with several constraints and therefore the measurement system is not required to obtain 3D position and/or 3D vector velocity. For example, a constraint of see surface alleviates the need of determining “Z coordinate” of a vessel's position and/or upper component of vessel's velocity. Several aerial and/or space applications also have some constraints that eliminate a need for full (3D) state vector measurements. Examples of such constraints may include e.g. assuming of non-manoeuvrability of a target, assuming that the target is maintained at a predefined altitude and/or within a predefined plane during its flight, etc. According to some embodiments, in these examples, determination of four parameters (e.g. two position coordinates and two components of velocity vector) are enough for target state vector definition.
System 100 includes a sensor 820, similar to sensor 120, which is therefore not described again (one can refer to the description above). Sensor 820 is configured to transmit electromagnetic waves 830 towards a target 810.
Target 810 reflects at least some of the electromagnetic waves 830. According to some embodiments, at least some of the first electromagnetic waves reflected by the target 810 (referred to as 840) are sent back directly to the sensor 820 (e.g. along a direct path between the target 810 and the sensor 820, as shown e.g. in
In this embodiment, system 810 includes a single redirecting device 851. The redirecting device 851 is similar to the redirecting device 151 and is therefore not described again. As shown in
As explained hereinafter, the first electromagnetic waves 840 and the second electromagnetic waves 870 are usable to determine data representative of at least one of a position and a velocity of the target 810. By tracking the target over time, a 2D position and/or 2D velocity vector can be determined as explained hereinafter.
According to some embodiments, system 800 includes a single active sensor, and does not require additional active sensors to detect the target and determine data representative thereof.
Attention is drawn to
The method includes (operation 900) transmitting electromagnetic waves from a sensor (such as sensor 820) towards a target (e.g. 810). According to some embodiments, the method can include directly illuminating the target with the electromagnetic waves (without a relay between the sensor and the target).
The method includes detecting (operation 910), by the sensor, first electromagnetic waves reflected by the target towards the sensor (as mentioned above, according to some embodiments, at least some of the first electromagnetic waves are reflected by the target along a direct path between the target and the sensor).
The method includes detecting (operation 920), by the sensor, second electromagnetic waves received by a redirecting device from the target and redirected by the redirecting device towards the sensor (as mentioned above, at least some of the electromagnetic waves received by the first redirecting device from the target, are redirected towards the sensor).
According to some embodiments, in order to ensure that the first electromagnetic waves are redirected towards the sensor, the method can include controlling (operation 925) a redirection axis of the redirecting device. According to some embodiments, and as mentioned above, the first commands of a redirection axis of the first redirecting device (see reference 915 in
In some embodiments, control of the redirecting device is performed by the sensor, which sends a command (e.g. through wireless communication) to the redirecting device. This is not limitative, and in some embodiments, the redirecting device can be controlled by a processor and memory circuitry (which can be external to the sensor and can e.g. communicate, directly or indirectly, with the sensor).
This control can be performed e.g. while the target is tracked by the sensor. In some embodiments, a continuous control of the redirecting axis of the redirecting device is performed, and in other embodiments, a control is performed from time to time (frequency of the control can depend, in particular, on the angular velocity of a line of sight from the redirecting device to the target).
As mentioned above, in some embodiments, a first indication of the position of the target is obtained by the sensor, and can be used to adjust the redirection axis of the redirecting devices. For example, in the case of a mirror, and as shown in
The method can further include (operation 930) using the first and the second electromagnetic waves sensed by the sensor to determine data representative of at least one of a position and a velocity of the target.
According to some embodiments, data representative of a position of the target is determined based on a time difference between transmitting electromagnetic waves by the sensor and receiving first electromagnetic waves by the sensor and a time difference between receiving the first electromagnetic waves by the sensor and receiving the second electromagnetic waves by the sensor.
According to some embodiments, and as shown in
According to some embodiments, data representative of a position of the target is determined based on a range measured by the sensor (e.g. radar) 820 and a time difference of arrival between the first and second electromagnetic waves detected by the sensor.
According to some embodiments, a 2D instantaneous position of the target at a given point of time can be determined using the following equations (these equations are not limitative):
c|t
2
−t
1|=2R1 (Equation 20)
c|t
3
−t
1
|=R
1
+R
2
+D
1 (Equation 21)
Assume that the origin of a canonical right Cartesian coordinates system (defined by axes X, Y) is located at sensor 820 (see
In this coordinate system, sensor 820 has coordinates (0,0), the redirecting device 851 has coordinates (D1,0) and the target 810 has coordinates (Xt, Yt).
Coordinates of the target (Xt,Yt) can be obtained e.g. according the method described above by usage of a Heron formula for triangle area. The area SΔ of a triangle defined by points 820, 851 and 810 can be expressed in as follows:
In Equation 22, p=½*(D1+R1+R2).
As a consequence:
The sign of coordinate Yt depends on a position of the target 810 relatively to the X axis.
Coordinate Xt can be obtained by following expression:
Xt is positive if the triangle (as shown in
According to some embodiments, a 2D instantaneous vector of velocity of the target at a given point of time can be determined based on two Doppler shifts Δf1 and Δf2 measured by sensor 820. A Doppler shift Δf1 is defined as a difference between a frequency f0 of the electromagnetic waves 830 transmitted by the sensor 820 towards the target 810 and a frequency f1 of the first electromagnetic waves 840 detected by the sensor 820. A Doppler shift Δf2 is defined as a difference between frequency f0 and a frequency f2 of the second electromagnetic waves 870 redirected by the redirecting device 851 and detected by the sensor 820.
Doppler shift can be calculated by Equation 13 mentioned above.
The relevant projection V1 of the target velocity measured for the first electromagnetic waves 840 is a projection of the target velocity on a line of sight between the sensor 820 and the target 810. The relevant projection V2 of the target velocity for the second electromagnetic waves 870 is a projection of the target velocity on a line from the middle point between the sensor 820 and the redirecting device 851 to the target (similar to the Doppler shift measured by bi-static radars).
Assume that target velocity is Vt, for which two components Vtx and Vty need to be determined.
The two projections V1 and V2 of the target velocity provide a set of linear equations allowing reconstruction of target velocity Vt components:
The projection V1 of target velocity Vt on the line of sight from the sensor 820 to the target 810 can be expressed as follows:
The projection V2 of target velocity Vt on the line from the middle point between the sensor 820 and the redirecting device 851 to the target 810 can be expressed as follows:
Vtx can be extracted from Equations 26 and 27:
Vty can be extracted from Equation 26:
In Equation 29, Vtx is obtained from Equation 28.
Therefore, both Vtx and Vty, which are the components of the target vector velocity Vt, are obtained.
As already mentioned above, position and/or velocity of the target determined over time can be used as a raw data for different filters and/or trackers. These filters and/or trackers can be used for different tasks, such as, but not limited to, reduction of measurement noise, classification of the target, detection of the target manoeuvers, etc.
The invention contemplates a computer program being readable by a computer for executing at least part of one or more methods of the invention. The invention further contemplates a machine-readable memory tangibly embodying a program of instructions executable by the machine for executing at least part of one or more methods of the invention.
It is to be noted that the various features described in the various embodiments can be combined according to all possible technical combinations.
It is to be understood that the invention is not limited in its application to the details set forth in the description contained herein or illustrated in the drawings. The invention is capable of other embodiments and of being practiced and carried out in various ways. Hence, it is to be understood that the phraseology and terminology employed herein are for the purpose of description and should not be regarded as limiting. As such, those skilled in the art will appreciate that the conception upon which this disclosure is based can readily be utilized as a basis for designing other structures, methods, and systems for carrying out the several purposes of the presently disclosed subject matter.
Those skilled in the art will readily appreciate that various modifications and changes can be applied to the embodiments of the invention as hereinbefore described without departing from its scope, defined in and by the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
276015 | Jul 2020 | IL | national |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/IL2021/050833 | 7/7/2021 | WO |