GB2284899A - Inclination angle detector - Google Patents

Inclination angle detector Download PDF

Info

Publication number
GB2284899A
GB2284899A GB9503113A GB9503113A GB2284899A GB 2284899 A GB2284899 A GB 2284899A GB 9503113 A GB9503113 A GB 9503113A GB 9503113 A GB9503113 A GB 9503113A GB 2284899 A GB2284899 A GB 2284899A
Authority
GB
United Kingdom
Prior art keywords
inclination
axis
antenna
filter
output
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB9503113A
Other versions
GB9503113D0 (en
GB2284899B (en
Inventor
Kouichi Eguchi
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Japan Radio Co Ltd
Original Assignee
Japan Radio Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from JP3057070A external-priority patent/JP2549470B2/en
Priority claimed from JP31502091A external-priority patent/JP3182185B2/en
Application filed by Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority claimed from GB9206013A external-priority patent/GB2256318B/en
Publication of GB9503113D0 publication Critical patent/GB9503113D0/en
Publication of GB2284899A publication Critical patent/GB2284899A/en
Application granted granted Critical
Publication of GB2284899B publication Critical patent/GB2284899B/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/12Supports; Mounting means
    • H01Q1/18Means for stabilising antennas on an unstable platform

Landscapes

  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

An inclination angle detector (52) for a stabilised antenna system is mounted on an AZ (azimuth) frame (26) and detects an inclination angle around an elevation (EL). The inclination angle detector (52) includes a reciprocal combination filter (142) for combining outputs of an inclinometer (72) and a rate sensor (74). The reciprocal combination filter (142) includes two reciprocal filters (144, 146), and parameters thereof are adaptively controlled depending on frequency and amplitude of the inclination to ensure the reciprocity in a necessary frequency range. <IMAGE>

Description

STABILISED ANTENNA SYSTEM DESCRIPTION The present invention relates to a stabilised antenna system including an antenna having a fan beam directivity, that is, a wide beam width around a longitudinal axis of the antenna.
Conventionally, a directive antenna has been used for satellite communication on a ship or the like. Such a satellite communication system is typified by the MARISAT satellite of the U.S.A. which has been in use since 1976, and has been operated by an international organisation called INMARSAT, since 1982. In such a ship satellite communication system, an antenna having a certain directivity is required.
For example, the technical requirements document for an INMARSAT standard A ship earth station require as of June 1987 that the G/T of the ship earth station is at least -4 dBK. In order to construct an antenna satisfying this requirement as a parabolic antenna, a diameter of approximately 80cm is needed.
For the ship satellite communication system, a stabilised antenna system has been used. This stabilised antenna system is provided with a stabilisation function in addition to a satellite tracking function.
That means that in order that an antenna mounted on a moving platform in a ship or the like can keep receiving a radio wave sent from a satellite, it is necessary to drive the antenna so that it tracks the satellite. Such antenna driving and control functions can be constructed so as to carry out the stabilisation of the antenna. Bearing in mind that the ship may be inclined to the vertical due to waves on the sea, then a good satellite tracking system must compensate for such inclination. The inclination of the ship may include, for example, a roll, a pitch and the like. In order to stabilise the antenna against the roll and pitch, it is necessary to mechanically or electronically drive the antenna or its beam direction sideways or lengthways. Hence, conventionally, a variety of techniques for driving the antenna have been developed.
One- example of a conventional stabilised antenna system is disclosed in Japanese Patent Laid-Open No. Sho 51-115757.
This antenna system uses a parabolic antenna having a pencil beam directivity, and supported by a mount.
This mount enables the parabolic antenna to be simultaneously moved angularly around axes in three mutually perpendicular dimensions, i.e. around a vertical axis, an elevation axis and a cross elevation axis. This is explained in more detail later with reference to Figure 29. By angularly moving the parabolic antenna around the vertical axis, an azimuth the parabolic antenna directs to can be controlled. Hence, this vertical axis is usually called an azimuth (AZ) axis.
In this conventional stabilised antenna system, an attitude sensor is arranged on the vertical axis so as to rotate therewith. The attitude sensor detects inclinations around the other two axes. By applying this detected result to drive controls for the other axes, the inclinations can be compensated for or stabilised while the parabolic antenna is satisfactorily tracking the satellite.
As described above, all three axes can be formed by mechanical axes. However, in this case, the structural designing is complicated, and thus the entire antenna system is apt to be expensive. In order to solve this problem, the axis structure is preferably improved so that two mechanical axes are sufficient.
One example of a mechanical axis antenna system with two axes is disclosed in "Development of a Compact Antenna System for INMARSAT Standard-B SEs in Maritime Satellite Communication", Shiokawa et al., Institute of Electronics and Communication Engineers of Japan, SANE 84-19, pp 17-24. In this antenna system, a short backfire antenna of 40cm, having a beam width of ±150 is used.
On the basis of this structure, a stabilised antenna system can be implemented by a simpler mechanical structure.
However, in such a structure, a singular point is caused. The singular point, for instance, appears in the zenith direction, and, when the antenna faces in this direction under the inclined condition, a tracking error is caused. In order to deal with the singular point properly, a light and solid material is used for the antenna and its support frame to reduce the load of a drive motor.
Alternatively, a relatively high performance AC servo motor is adopted and accordingly a high performance AC servo control circuit is used to drive the antenna by a high performance servo system. Furthermore, by improving software, the tracking error near the singular point can be reduced.
However, these countermeasures require a particular material, an expensive circuit and the like, and the antenna system is still expensive. Furthermore, even when these countermeasures are applied, a tracking error of approximately 100 is reported at the singular point.
In order to solve such problems, it is effective to use an electronic beam steering for any of the axes. The electronic axis can be implemented by a phased array antenna.
The phase array antenna, for example, is formed by arranging a plurality of antenna elements as electrodes in a square lattice form on an antenna plane. Furthermore, a phase shifter is provided for each antenna element, and by controlling an amount of phase shift of a signal for each antenna element, the beam direction of the antenna can be controlled. Also, as described in Japanese Patent Application No. Hei 2-339317 in the name of the present applicant, by providing a phase shifter for each column of antenna elements arranged in a matrix form, the electronic axis can be implemented by a relatively simple construction.
By using two mechanical axes and one electronic axis, as described above, the singular point can be avoided and the stabilisation can be carried out by a relatively simple and inexpensive construction. However, in this stabilisation, control of two to three axes is required, Such control is effected by performing matrix operations on co-ordinate representations of the ship's roll and pitch.
This is described in more detail with reference to Figures 30 to 33 of the accompanying drawings.
However, this matrix operation is complex and if it can be omitted or eliminated, the construction of the antenna system can be simplified, and made less expensive.
The construction has been simplified and the cost reduced by using an antenna system having a fan beam directivity. This can be achieved using a array of antennas arranged so that the directivity of the array is narrow around the elevation axis but wide around a virtual cross elevation axis perpendicular to the elevation axis.
However, even using an array antenna having fan beam directivity, it is necessary to perform some matrix operations and so the necessary control calculations are still complicated.
The present invention seeks to overcome some of the problems of the known systems.
According to the present invention, there is provided an inclination angle detecting device for use in a stabilised antenna system to be mounted on a moving platform, comprising a rate sensor for detecting an angular velocity around an elevation axis of the moving platform, an inclinometer for detecting an inclination around the elevation axis of the moving platform, a reciprocal combination filter for combining outputs -of the rate sensor and the inclinometer and outputting an inclination angle around the elevation axis, and parameter adaptive control means for adaptively controlling parameters of the reciprocal combination filter depending on a frequency of the inclination, the reciprocal combination filter including a first filter means for filtering the output of the rate sensor, the first filter means including a feedback loop of a feedback gain factor Kb, second filter means for filtering the output of the inclinometer, the second filter means having a reciprocal transfer function including a term of the 1st order of Laplace operator s in a numerator with reference to the first filter means, and adding means for combining outputs of the first filter means and the second filter means to output the inclination angle around the elevation axis, the parameter adaptive control means including means for detecting the frequency of the inclination, and correction means for determining a correction factor a (a < 1) depending on the detected frequency and correcting the term of the 1st order of Laplace operator s by the correction factor a.
Preferably the parameter adaptive control means further includes means for detecting an amplitude of the inclination, and means for determining the feedback gain factor depending on the detected amplitude and for adaptively controlling the feedback gain factor.
According to another aspect of the invention there is provided an inclination angle device for use in a stabilised antenna system to be mounted on a moving platform, comprising a rate sensor for detecting an angular velocity around an elevation axis of the moving platform, an inclinometer for detecting an inclination around the elevation axis of the moving platform, a reciprocal combination filter for combining outputs of the rate sensor and the inclinometer and outputting an inclination angle around the elevation axis, the reciprocal combination filter including a first filter means for filtering the output of the inclinometer, the second filter means having a reciprocal transfer function with reference to the first filter means, and adding means for combining outputs of the first filter means and the second filter means to output the inclination angle around the elevation axis.
In a system constructed according to the present invention, there is no need for calculations of the stabilisation required around a virtual cross elevation axis.
This is why the antenna has the fan beam directivity.
It is sufficient only to carry out the stabilisation calculation for the inclination component q1 around the elevation axis.
Accordingly, the detection output of the inclination sensing means can be used for the stabilisation control, as it is. For example, assuming that the elevation of the satellite is defined el with reference to the horizontal plane when no inclination occurs, the beam direction of the antenna can be controlled by using the following control amount with reference to the zenith: 8 = 900 -el + q1 Hence, in a system according to the first aspect of the present invention, not only does the control algorithm become simple, but also, since it is enough to detect the inclination component of only one axis, the inclination sensing means can be constructed for less cost and made light in weight.
In another preferred embodiment there is an adaptive control of a correction factor a (a < 1) based on the inclination frequency. If the transfer functions of the first and second filter means are determined so as to satisfy the reciprocity at least the necessary frequency range, as described above, corresponding to the provision of the feedback loop in the first filter means, a differential term appears in the numerator of the transfer function of the second filter means. This term of the 1st order of Laplace operator s emphasises the error (inclination acceleration error) of the inclinometer caused by the accelerations of ship's inclinations. By controlling the influence of the a term of the 1st order of Laplace operator s by the correction factor a, the inclination acceleration error can be reduced.
Furthermore, for this reduction, the inclination frequency is detected and the parameter control of the correction factor a is carried out to reduce the error depending on the inclination conditions.
According to another preferred embodiment, the inclination amplitude is detected and adaptive control of the feedback gain factor Kb is carried out. This is a consequence of the fact that by enlarging the feedback gain factor bt the inclination acceleration error becomes remarkable.
Furthermore, such an inclination angle sensor, that is, an inclination sensing means including parameter adaptive control means proposed above is applicable to the stabilised antenna system. In this respect, the structure is the same as described above, and thus the detailed description can be omitted for brevity.
The above and other objects, features and advantages of the present invention will more fully appear from the hollowing description of the preferred embodiments with reference to the accompanying drawings, in which: Fig. 1 is a schematic cross section of a first embodiment of a stabilized antenna system according to the present invention; Fig. 2 is a block diagram of an entire circuit structure of the stabilized antenna system shown in Fig. 1; Fig. 3 is a block diagram of an array antenna shown in rig 2; Fig. 4 is a block diagram of a controller shown in Fig.
2; Fig. 5 is a block diagram of a uniaxial inclination sensor shown in Fig. 4; Fig. 6 is a block diagram showing a transfer function model of the uniaxial inclination sensor shown in Fig. 5; Fig. 7 is a circuit diagram of an inclinometer shown in Fig. 5; Fig. 8 is a block diagram of an azimuth and elevation input portion shown in Fig. 2; Fig. 9 is a block diagram of an antenna output processor shown in Fig. 2; Fig. 10 is a block diagram of a second embodiment of a stabilized antenna system according to the present invention; Fig. 11 is a block diagram of an array antenna shown in Fig. 10; Fig. 12 is a graphical representation of a beam position around a supplementally EL axis of the array antenna shown in Fig. 11 when N = 3; Fig. 13 is a block diagram of a controller shown in Fig. 10; rig. 14 is a block diagram of an azimuth and elevation input portion of a third embodiment of a stabilized antenna system according to the present invention; Fig. 15 is a block diagram of an antenna output rocessor of the third embodiment of the stabilized antenna system according to the preset invention; Fig. 16 is a schematic cross section of a fourth embodiment of a stabilized antenna system according to the present invention; Fig. 17 is a block diagram of a circuit structure of an array antenna shown in rig. 16; Fig. 8 is a block diagram of a co-phase combination circuit shown in Fig. 17; Fig. 19 is a block diagram of a detailed transfer function model of a uniaxial inclination sensor to be applicable to the first to fourth embodiment of a stabilized antenna system according to the present invention; Fig. 20 is a block diagram of a uniaxial inclination sensor of a fifth embodiment of a stabilized antenna system according to the present invention; Fig. 21 is a block diagram of a parameter adaptive controller shown in Fig. 20; Fig. 22 is a block diagram showing a transfer function model of the uniaxial inclination sensor shown in Fig. 20; Figs. 23A, 23B and 23C are graphical representations of a simulation result of an inclination acceleration error, when Kb = 5.0, 10.0 and 15.0, respectively, obtained in the fifth embodiment of the stabilized antenna system according to the present invention; Fig. 24 is a graphical representation of a simulation result of a drift error obtained in the fifth embodiment of the stabilized antenna system according to the present invention; Fig. 25 is a graphical representation showing an adaptive control in the fifth embodiment of the stabilized antenna system according to the present invention; Fig. 26 is a block diagram of a uniaxial inclination sensor of a sixth embodiment of a stabilised antenna system according to the present invention; Fig. 27 is a block diagram of a uniaxial inclination sensor of a seventh embodiment of a stabilised antenna system according to the present invention; Fig. 28 is a block diagram of a uniaxial inclination sensor of an eighth embodiment of a stabilised antenna system according to the present invention; Fig. 29 is a conventional stabilised antenna system; Fig. 30 is a schematic view showing a principle of a conventional stabilisation of an inclination; Fig. 31 is another conventional stabilised antenna system; and Figs. 32 and 33 are graphical representations of antenna patterns around a virtual XEL and EL axes, respectively, of a conventional antenna having a fan beam directivity.
Figures 29 to 33 will be described first to make clear the features of conventional antenna systems.
In Fig. 29 a conventional stabilised antenna system is shown, similar to that disclosed in Japanese Patent No. Sho 51-115757. This antenna system uses a parabolic antenna 10 having a pencil-beam directivity and a mount composed of members 12-16 for supporting the parabolic antenna 10.
This mount enables the parabolic antenna 10 to be simultaneously moved angularly around axes 12, 14 and 16.
Axis 16 being vertical, by angularly moving the parabolic antenna 10 around axis 16, an azimuth which the parabolic antenna 10 points to can be controlled. Hence this vertical axis 16 is usually called an azimuth (AZ) axis.
In this conventional stabilised antenna system, an attitude sensor 18 is arranged on the vertical axis 16 so as to rotate therewith. The attitude sensor 18 detects inclinations around the other two axes 12 and 14. By applying this detected result to drive controls for the other axes 12 and 14, the inclinations can be compensated for or stabilised while the parabolic antenna is satisfactorily tracking a satellite.
In this known system, all three axes are formed mechanically. This makes the structural designing complicated and thus the entire antenna system expensive.
In general, an inclination of a ship can be represented as a coordinate transformation, as shown in Fig. 30, wherein a coordinate system X(O)Y(O)Z(O) is represented by X(O) in the bow direction and ZvO) in the zenith direction when the ship is not included.
In this case, when a pitch occurs, the coordinate system is moved to X(l)Y(1)Z(1).
In turn, when a roll happens, the coordinate system is moved to X(2)Y(2)Z(2).
In Fig. 30, an angle v representing the inclination of the ship can be resolved into a component q1 around the elevation (EL) and a component q2 around the cross elevation (XEL) perpendicular to the EL axis. Each component ql or q2 can be obtained by a matrix operation on the basis of the roll r or the pitch p.
For instance, when the EL and XEL axes are constructed as the mechanical and electronic axes respectively, the controls of the EL and XEL axes are carried out on the basis of the respective components ql and q2.
In Fig. 31, there is shown another conventional stabilised antenna system using an array antenna having a fan beam directivity. In the stabilised antenna system, as shown in fig. 31, the array antenna 22 includes four antenna elements 20 aligned longitudinally. the array antenna 22 possesses a fan beam directivity, as hereinafter described in detail, and is supported by an EL axis 24 so that the antenna elements may be arranged around the EL axis 24.
The EL axis 24 is rotatably supported by a U-shaped AZ axis frame 26. The gear 28 is mounted to one end of the EL axis 24, and an EL axis motor 30 is mounted to the AZ axis frame 26. A belt 32 is suspended between the gear 28 and the EL axis motor 30. Accordingly, by driving the EL axis motor 30, the EL axis 24 is rotated to turn the array antenna around the EL axis 24.
An AZ axis 34 is integrally secured to the AZ axis frame 26 on its central position and is rotatably held by a pedestal 36 having a T-shaped cross section, and a gear 38 is attached to the lower end of the AZ axis 34. An AZ axis motor 40 is mounted to the pedestal 36, and a belt 42 is extended between the gear 38 and the AZ axis motor 40. Hence, by driving the AZ axis motor 40, the AZ axis 34 is rotated to turn the array antenna 22 around the AZ axis 34.
The pedestal 36 eccentrically supports the AZ axis frame 26, the EL axis 24, the array antenna 22 and the like. That is, the pedestal 36 is mounted to a radome base 44 in an eccentric position from the centre of the radome base 44. An access hatch 48 having a sufficient size for operation is provided to the radome base 44 through a hinge 46 so as to be openable. The access hatch 48 is formed for an operator to insert his hand through the opened access hatch 48 for carrying out maintenance and inspection of the array antenna 22, its peripheral circuits and the like. As a result, the maintainability of the antenna system can be secured.
The radome base 44 constitutes the bottom part of a radome 50. The radome 50 for protecting the components of the antenna system from a rainfall or the like is made of a material such as FRP or the like through which the radio wave can pass.
In Figs. 32 and 33, there are shown antenna patterns of the array antenna 22 around the virtual XEL axis and the EL axis 24, respectively. The virtual XEL axis is a virtual axis perpendicular to the EL axis 24 and is not actually present in the antenna system shown in Fig. 31.
As apparent from Figs, 32 and 33, the directivity of the array antenna 22 is wide around the virtual XEL axis and narrow around the EL axis 24. This property is generally called a fan beam directivity. By using the fan beam directivity around virtual XEL axis, the stabilisation of the component q2 is not required.
However, even using an array antenna having fan beam directivity, it is necessary to perform some matrix operations and so the necessary control calculations are still complicated.
The present invention will now be described in connection with its preferred embodiments with reference to Figures 1 to 28, wherein like reference characters designate like or corresponding parts throughout the views and thus the repeated description thereof can be omitted for brevity.
In Fig. 1, there is shown the first embodiment of a stabilised antenna system according to the present invention, in which members 20 to 50 are the same as those in the conventional stabilised antenna system shown in Fig. 31. In this embodiment, a uniaxial inclination sensor 52 is mounted on an AZ frame 26. Hence, by the rotation of an AZ axis 34, the uniaxial inclination sensor 52 is rotated together with the AZ frame 26. Furthermore, the uniaxial inclination sensor 52 is arranged on the AZ frame 26 so as to detect an inclination component around an EL axis 24. and on the basis of the output of the uniaxial inclination sensor 52. a control of an EL axis motor 30 can be carried out.
In Fig. 2, there is shown the entire circuit structure of tie stabilized antenna system shown in rig. 1, which comprises an array antenna 22, a controller 54, an azimuth and elevation input portion 56 andean antenna output processor 58. The array antenna 22 includes four antenna elements 20 aligned along a longitudinal side of the antenna, as shown in Fig. 1, and realizes antenna patterns shown in Figs. 32. and 33. The controller 54 drives the array antenna 22 on the basis of satellite elevation (EL) and satellite azimuth (AZ) output from the azimuth and elevation input portion 56 to allow the array antenna 22 to track a satellite (S). The controller 54 also includes a stabilization function of the inclination. The azimuth and elevation input portion 56 inputs a moving platform azimuth (azimuth of a moving platform such as a ship or the like mounting the antenna system) from a gyrocompass or the like, and outputs the elevation (EL) and the relative azimuth (AZ) of the satellite to the controller 54. The antenna output processor 58 inputs the output of the array antenna 22 and conducts a predetermined processing to output a step track angle.
In Fig. 3, there is shown the circuit structure of the array antenna 22 shown in Fig. 2, including- four antenna elements 4 longitudinally aligned.
An array antenna, for example, includes an antenna substrate supporting antenna elements, and a feeding substrate laminated with the antenna substrate via dielectric layer. The array antenna 22 also include a combiner 60 connected to the four antenna elements 22.
Tiiat is, in this embodiment, the outputs of the antenna elements 20 are combined in the combiner 60 to output a combined signal to the antenna output processor 58. Hence, in this case. a single antenna pattern as shown in Fig. 33 around the EL axis 24 is obtained.
In rig. 4, there is shown the structure of the controller 54. The controller 54 includes the EL axis 24, the EL axis motor 30, tie AZ axis 34 and the AZ axis motor 40 shown in Fig. 31. That is. the controller 54 is a circuit having a function for mechanically driving the array antenna 22.
The controller 54 further includes an EL axis angle detector 62 for detecting the angle of the EL axis 24. The controller 54 similarly includes an AZ axis angle detector 64 for detecting the angle of the AZ axis 34.
The detection results of the EL axis angle detectors 62 and 64 are fed back to an EL axis control circuit 66 and an AZ axis control circuit 68, respectively. An EL axis control processor 70 takes in the elevation of the satellite to be tracked, that is, the satellite elevation from the azimuth and elevation input portion 56, and calculates an EL axis control amount for controlling the. EL axis motor 30.
The calculation result of the EL axis control processor 70 is given to the EL axis control circuit 66, and the EL axis control circuit 66 controls the EL axis motor 30 according to the calculation result of the EL axis control processor 70. The EL axis angle detector 62 feeds back the detected result to the EL axis control circuit 66. Thus, a servo loop for the EL axis is formed.
On the other hand, the AZ axis control circuit 68 takes in the relative azimuth of the satellite from the azimuth and elevation input portion 56, and controls the AZ axis motor 40 on the basis of the input azimuth. The AZ axis angle detector 64 feeds back the detected result to the AZ axis control circuit 68. Thus, another servo loop for the AZ axis 34 is also formed. The controller 54 can directly take in the relative azimuth of the satellite to the AZ axis control circuit 68 without requiring a member corresponding to the EL axis control processor 70 becaiise the array antenna 22 has the pattcrn shown in rig. 32.
Furthermore, the controller 54 is provided with a uniaxial inclination sensor 52. The uniaxial inclination sensor 52 is mounted on the AZ frame 26, as described above, and detects the inclination angle around the EL axis 24.
'rhe output of the uniaxial inclination sensor 52 is given to ishe EL axis control processor 70, and the EL axis control processor 70 calculates the EL axis control amount by using the output of the uniaxial inclinatton sensor 52 together with the satellite elevation. The calculation formula of the EL axis control amount is as follows as described above 6 = 90' - el + ql wherein e is tlle EL axis control amount, el is the satellite elevation and ql is the inclination component around the EL axis 24 of the detected result of the uniaxial inclination - sensor 52.
In Fig. 5, there is shown the structure of the uniaxial inclination sensor 52, and Fig. 6 illustrates a transfer function model thereof. In this embodiment, the uniaxial inclination sensor 52 includes aninclinometer 72, a rate sensor 74 and a combination filter 76. The inclinometer 72 is a sensor for detecting the inclination of the moving platform and outputting an inclination signal to the combination filter 76. For instance, a pendulum inclinometer can be used.
In Fig. 7, there is shown one embodiment of a pendulum inclinometer. In this instance, two resistors R and two magnetoresistance elements Rx and Ry are connected in a bridge form, an a magnet 80 supported as a pendulum is arranged near the magnetoresistance elements Rx and Hy.
When the ship is inclined in this state, the magnet 80 is inclined accordingly, and the bridge is unbalanced to generate an output electric potential e between terminals A and B. This output electric potential e represents the inclination angle of the ship.
In turn, the rate sensor 74 is a sensor for detecting an angular velocity of the moving platform. For the rate sensor 74, for example, a solid state type can be used. and a rate signal output from the rate sensor 74 is fed to the combination filter 76.
No, assuming that the input to the inclinometer 72 and the rate sensor 74 is the inclination angle of the moving platform in a predetermined direction, the transfer function of the inclinometer 72 is 1 and the transfer function of the rate sensor added to the moving platform azimuth in the azimuth and elevation input portion 56.
For carrying out this operation, the azimuth and elevation input portion 56 takes in a moving platform azimuth variation from a device such as a gyrocompass or the Like. in order to execiite the moving platform azimuth. t))e roving platform azimuth register 90 for storing the present moving platform azimuth. and tie adder 92 arranged before the moving platform azimuth register 90 for adding the output of the moving platform azimuth register 90.with the moving platform azimuth variation are provided.
In the adder 94 arranged after the moving platform azimuth register 90, the moving platform azimuth stored in the register 90 is subtracted from the absolute azimuth (AZ) fed from the satellite azimuth and elevation input means 88.
The satellite elevation register 96 once stores the satellite elevation (EL) output from the satellite azimuth and elevation input means 88. The satellite relative azimuth register 98 once stores the relative azimuth of the satellite, obtained by the adder 94.
The elevation.stored in the register 96 and the relative azimuth stored in the register 98 are supplied to the controller 54, and thus the tracking of the satellite by the array antenna 22 is carried out.
In this instance, as to the satellite elevation register 96 and the moving platform azimuth register 90, a so-called step track control is conducted. The step track control is performed by a step track angle output from the antenna output processor 58.
In Fig. 9, there is shown the structure of the antenna output processor 58 for carrying ont the step track control.
The circuit shown in Fig. 9 shows a part of receiver equipment for the satellite communication or for the satellite broadcasting, and particularly only shows a construction relating to a detection of an azimuth error.
The antenna output processor 58 includes a receiver 1.00, a receiving level signal generator 102 and a step track control circuit 104. Tlse receiver 100 takes in the output of the array antenna 22.
The receiving leveJ signal generator 102 generates a receiving level signal depending on the output of the receiver 100. The receiver 100 converts the antenna output into a lower frequency, and outputs an IF signal to the receiving level signal generator 102. The receiving level signal generator 102 takes in the IF signal output from the receiver 100, and estimates the carricr to noise density ratio C/NO from the carrier levcl or the like contained in the IF signal. The recciving level signal generator 102 produces a receiving level signal of a monotone increase value against the estimated C/NO. The produced receiving level signal is input to the step track control circuit 104.
The step track control circuit 104 produces the step track angles for the elevation and azimuth on the basis of the receiving level signal output from the receive level signal generator 102. That is. the step track angle output from the step track control circuit 104 is supplied to the satellite elevation register 96 and the moving platform azimuth register 90. When the step track angle is given to these registers 96 and 90, their contents are slightly adjusted or corrected.
In this instance, a specific structure of the step track control circuit 104 is basically disclosed in Japanese Patent Application No.e 2-175014 and No.Hei 2-240413 applied by the present applicant, and thus the detail of the step track control circuit i04 can be omitted.
Next, the particular operation of the stabilized antenna system described above according to the present invention will now be described.
In this embodiment, when the inclination is caused on the ship during the satellite tracking controlling, the inclination component around the EL axis 24 is detected by the uniaxial inclination sensor 52. This detection result is obtained by the combination filter 76 for realizing the reciprocal transfer functions and the accuracy can he ensured in the necessary frequency band. The output of the biaxial inclination sensor 52 is given to the EL axis control processor 70, alld the EL axis control processor 70 executes the subtraction for tile satellite elevation to calculate the EL axis control amount. In other words, only the subtraction for the output of tize uniaxial inclination sensor 52 is carried out, and the EL axis 24 is rotated so as to compensate or stabilize the inclination component Therefore, in this embodiment, the stabilization of the moving platform such as the ship or te like can be practiced by an extremely simpler arithmetic algorithm compared with the conventional stabilized antenna system.
This is the reason why the fan beam directivity is realized by the array antenna 22, and the uniaxial inclination sensor 52 is mounted on the AZ frame 26 so as to detect the inclination angle around the EL axis 24. Furthermore, since the inclination detector means as the uniaxial inclination sensor 52 is constructed so as to detect only the inclination angle around the EL axis 24, there is no need to carry out the detection of the drive components in the two directions like the conventional attitude sensor 18 shown in Fig. 29, and the above-described effects can be realized by the inexpensive inclination detector means implemented by approximately the half cost of the conventional one. Furthermore, by properly determining the number such as 4 to 5 of the antenna elements 20, the influence of the sea surface reflection can be reduced.
In Fig. 10, there is shown a whole circuit structure of the second embodiment of a stabilized antenna system according to the present invention, having the same construction as the first embodiment shown in Fig. 2, except an array antenna 22a ad a controller 54a which outputs a phase shifter control signal (p.s. control) for controlling a phase shift amount in the array antenna 22a.
In Fig. 11, there is shown the structure of the array antenna 22a shown in Fig. 10. The array antenna 22a includes three antenna elements 20 longitudinally aligned, a combiner 60 coupled to the middle antenna element 20, two hase sifters 106-1 and 106-3 connected to the upper and Lower antenna elements 20. respectively, and a phase shifter drive circuit 108 for driving the two phase shifters 106-1 and 106-3.
In this embodiment, by controJling the phase shift amounts by the phase shifters 106-1 and 106-3, the beam positions of the array antenna 22a can be switched around the EL axis 24. In order to enable the beam position switching, the phase shifter drive circuit 108 for driving the phase shifters 106- and 1C6-3 is provided.
The phase shifter drive circuit 108 executes the control of the phase shifters 106-] and 106-3 according to the phase shifter control signal supplied from the controller 54a. More specifically, the digital signal is supplied to the phase shifters 106-1 and 106-3 depending on the bit numbers of the phase shifters 106-1 and 106-3. The outputs of the phase shifters 106-1 and 106-3 along with the output of the middle antenna element 20 are fed to the combiner 60 and are combined thereiIl, and the combined signal is output from the combiner 60 to the antenna output processor 58. At thins time, when the phase shifters 106-1 and 106-3 are controlled by the phase shifter drive circuit 108, for example, the beam positions around the EL axis 24 of the array antenna 22a are switched. as shown in Fig. 12.
In this embodiment, the bit number for the phase shifters 106-1 and 106-3 is 2 bits, and thus the bcam position can be controlled to be switched into three types. Since the beam position switching is carried out around the EL axis 24. this can be called a supplementary EL axis. That is, the actual EL axis 24 is tie mechanical axis driven to be rotated by the EL axis motor 30, and the beam position switching by the control of the phase shifters 106-1 and L06-3 can assist the EL axjs 24. ln this embodiment. the inclination can be solely compensated or stabilized by this supplemcntary El axis.
In Fig. 13, there is shown the construction of the controller 54a shown in Fig. 10 for supplying the phase shifter control signal (p.s. control) to the phase shifter drive circuit 108 of the array antenna 22a In this embodiment, the controller 54a has the same construction as the controller 54 of the first embodiment shown in Fig. 4, except that an output of a uniaxial inclination sensor 52 is fed to a phase shifter control amount processor 110, and the satellite elevation output from the azimuth and elevation input part 56 is directly input to an EL axis control circuit 66. The phase shifter control amount processor 110 produces the phase shifter control signal for compensating or stabilizing the inclination component around the EL axis 24 and outputs the phase shifter control signal to the phase shifter drive circuit 108. That is, in this embodiment, the AZ axis 34 and the EL axis 24 are driven only for allowing the array antenna 22a to track the satellite, and the stabilization of the inclination is carried out solely by the phase shifter control signal output from the phase shifter control amount processor 110.
Accordingly, in this embodiment, the same effects and advantages as those resulted in the first embodiment can be obtained. In addition, the stabilization of the inclination of the moving platform can be performed only by the phase shifter control signal, and thus the servo loop in respect of the AZ axis 34 and the AZ axis 34 can be of a relatively low speed. This is the reason why the variation of the satellite elevation and the variation of the relative azimuth of the satellite are caused by the variation of the azimuth, the movement and the like of the moving platform such as the ship and are of a lower speed than the inclination. Hence, the controller 54a can be produced at a low cost, and the response to the inclination can be kept to relatively high speed.
In Fig. 14, there is shown a structure of an azimuth and elevation input portion 56 of the third embodiment of a stabilized antenna system according to the present invention. In this embodiment, the azimuth and elevation input portion includes an adder 92, a satellite elevation register 96, a satellite relative azimuth register 98 and a search controller 116 ip place of the satellite azimuth and elevation input means 88 of the first embodiment shown in Fig. 8. The feature of this embodiment is to use a controlling in respect of the relative azimuth in the azimuth and elevation input portion.
That is, as shown in Fig. 14, the search controller 116 carries out a search operation in response to a power on, asearch instruction and the like. In this instance, the structure of the search controller 116 is formed by adapting a structure of an azimuth search control circuit disclosed in Japanese Patent Application No.Hei 2-240413 applied by the present applicant. In this embodiment, the output such as the satellite elevation and the relative azimuth of the satellite of the search controller 116 is fed to the satellite elevation register 96 and the satellite relative azimuth register 98, and the search control of both the satellite elevation and the relative azimuth of the satellite is performed. The step track control is practiced to both the satellite elevation register 96 and the satellite relative azimuth register 98.
In Fig. 15: there is shown a construction of an antenna output processor for producing a carrier detection signal (CD) to be input to the azimuth and elevation input portion shown in Fig. 14 in the third embodiment. In this embodiment, the antenna output processor has the same structure as the first embodiment as shown in Fig. 9, except that a decoder 118 is further provided. The decoder 118 takes in the IF signal from the receiver 100, detects a farrier from the IF signal and outputs the carrier detection signal (CD) for representing whether or not a desired signal is received by at least a fixed level. The carrier detection signal is fed to the search controller 116 of the azimuth and elevation input portion, and the search controller 116 carries out the search control accordingly.
Hence, in this embodiment, the same effects and advantages as those of the first and second embodiments can be obtained.
As described above, in the above-described embodiments, although 3 to 4 antenna elements 20 are arranged around the.
EL axis 24 in the array antenna, however, the present invention is not restricted to the arrangements. For example, a plurality of antenna elements can be aligned along two lines. In this instance, the beam width around tlie virtual XEL axis becomes narrower compared with one line alignment, and hence the inclination becomes apt to somewhat give an influence. However, on the contrary, the height of the array antenna is reduced compared with the one line alignment that the number of the antenna elements 20 is the same and thus the combined gain is substantially equal.
Accordingly, such a structure can be effective on a ship of which an inclination component to be stabilized is small, for example, a ship in an inland water channel, a large ship or the like.
In Fig. 16, there is shown the fourth embodiment of a stabilized antenna system according to the present invention, having the same construction as the first embodiment shown in Fig. 1, except that an array antenna 22b includes antenna elements 20 aligned in a 4 x 2 matrix form.
Figs. 17 and 18 show a part of a circuit structure of the fourth embodiment of the stabilized antenna system shown in Fig. 16. That is, lig. 17 shows a circuit structure of the array antenna 22b, and Fig. 18 shows a circuit structure of a co-phase combination circuit shown in Fig. 17.
In Fig. 17, since the antenna elements 20 are arranged in 4 lows x 2 columns in the array antenna 22b, as shown in lig. 16, the structure of the output processing of the array antenna 22b is different froni the array antenna 22 of the first embodiment shown in Fig. 2. That is, although the beam width around the virtual XEL axis is narrowed due to the two line arrangement of the antenna elements. by the structure shown in Fig. 17, the fan beam di-rectivity equivalent to the one line arrangement of the antenna elements can be realized.
As shown in Fig. )7, in the array antenna 22b, one combiner 60 is provided for each line of four-antenna elements 20. The outputs (antenna outputs A and B) of the two combiners 60 are sent to a pair of receiver front-ends 120 for performing a processing such as amplification and the like. The receiver front-ends 120 each include the LNA and the like, are arranged near the array antenna 22h, and separately bear a partial function of the receiver 100. The array antenna 92b further includes a frequency converter 122 for converting the output of each receiver front-end 120 into a predetermined IF signal A or B, and a co-phase combination circuit 124 for executing a co-phase combination of the IF signals A and B output from the frequency converter 122 and outputting a combined IF signal to the receiver 100.
That is, at the receiving time, the gain is improved.
For example, compared with a case of 6 antenna elements 20 arranged along one line, in case of 8 antenna elements 20 arranged along two lines, by the increase of the number of the antenna elements 2(), the combined gain is increased.
Furthermore, the number of the antenna elements 20 arranged around the EL axis 24 for each line is reduced from six to four, and the system is lowered in height and becomes compact in size. When the number of the antenna elements 20 per line is equal, the receive gain of the two line arrangement is increased by the maximum of 3 dB compared with the one line arrangement.
In order to obtain this effect, the co-phase combination circuit 124 is constructed, as shown in Fig. 18.
'rhe co-phase combinatio, circuit 124 includes a pair of mixers 126 and 128 corresponding to the respective IF signals A and B, and a combiner 130 for combining the outputs of the mixers 126 and 128 to output a combined IF signal. In the co-phase combination circuit 124, a local oscillator 132 for generating a signal having predetermined frequency and phase is connected to the mixer 128, and a phase comparator 134 compares the output phase of the mixer 126 and the phase of te IF signal B to output a signal exhibiting a phase difference between the two signals to a loop filter 136. Furthermore, Tn the co-phase combination circuit 124, the loop filter 136 extracts the signal exhibiting the phase difference from the output of the phase comparator 134 and outputs it to a VCO (voltage controlled local oscillator) 138, and the VCO 138 controls the oscillation phase depending on the output signal value (voltage) of the loop filter 136 and oscillates at the same frequency as the local oscillator 132 to output a signal to the mixer 126. The mixer 126 and the VCO 138 constitute a phase shifter 140.
That is, in this embodiment, the IF signals A and B are mixed with the output signals of the VCO 138 and the local oscillator 132 in the mixers 126 and 128, respectively, and the outputs of the mixers 126 and 128 are combined in the combiner 130. The output phase of the VCO 138 is adjusted depending on the comparison result of the phase comparator 134 so that the 'output phase of the mixer 126 may be equal to the output phase of the mixer 128.
Hence, in this embodiment, at the receiving time, by the co-phase combination, the satellite can be electronically tracked around the virtual XEL axis, and in spite of the narrow beam width around the virtual XEL axis, the fan beam directivity equivalent to that of the one line arrangement of the antenna elements can be obtained. The tracking range can be determined depending on the beam width of the individual antenna clement 20, the C/NO, the performance of the co-phase combination circuit 124, and the like. Since the phase comparison operation is required, such effects can be expected only at the receiving time.
According to the present invention, as described above, although the AZ axis 34 and the radome 50 are separately constructed, these two members can be integrally formed with the same effects as those obtained in the embodiments. One example of an antenna system including the AZ axis 34 and the radome 50 integrally constructed is disclosed in Japanese Patent Application No.Hei 3-040297 applied by the present applicant. In other words, the azimuth axis structure of this antenna system can be applied to the antenna system according to the present invention. In this case, the radome 50 can be small-sized. Furthermore, the uniaxial inclination sensor 52 can be mounted on a supplementary rotation mount rotating in synchronism with the AZ axis 34.
As described above, according to the present invention, the antenna having the fan beam directivity is rotatably supported by two mechanical axes, and the inclination sensor means for detecting the inclination component around the EL axis is mounted onto the AZ frame. Therefore, the stabilization of the antenna can be performed by using the simple control algorithm, and the structure of the inclination sensor means can be more simplified. As a result, an inexpensive and small-sized stabilized antenna system can be implemented. Furthermore, the fan beam directivity can be also obtained by the array antenna.
According to the present invention, further, the reciprocal transfer functions are realized and the detection of the inclination component is carried out by using both the inclinometer and the rate sensor. Hence, the accurate inclination detection can be performed by a simple structure, and the small-sizing and the cost reduction of the antenna system can l)e remarkably achieved.
In Fig. 19, there is shown a detailed transfer function model of the uniaxial ijiclination sensor 52 to be applicable to the above-described embodiments.
The rate sensor 74 is formed of a piezoelectric type rate sensor or the like and possesses the following transfer function: Glo(s) = K1.s (Kl: constant) That is, the rate sensor 74 is a sensor which outputs a differential of an inclination angle #1(s) to be added. In Fig. 19, Gll(s) and do(s) represent a parasitic element having an LPF characteristic and an offset and its drift, respectively, and are expressed as follows: 2 s + 2#1#1s + #1 do do(s) = s wherein 1 and #1 represent a cutoff frequency and a damping factor, respectively, of second order lag elements of the rate sensor 74, and do represents an offset voltage of the rate sensor 10. The formula G11(s) models the parasitic element as the second order LPF.
Furthermore, the inclinometer 72 possesses the following transfer function: G20(s) = K2 (K2: constant) In Fig. 19, G21(s) and G22(s) represent a parasitic element having an LPF characteristic and an influence of acceleration, respectively, and are expressed as follows: 2 #2 G21(s) = s + 2#2#2s + w2 -(L/g)s.#2.K2 G22(s) = s + 2#2#2s + #2 wherein 02 and 52 represent a cutoff frequency and a damping factor, respectively, or second order lag elements of the inclinometer 72, L represents a distance from the inclination center of the moving platform to the inclinometer 72 and g represents the acceleration of gravity. The formula G21(s) models the parasitic element as the second order LPF.
According to these formulas, the transfer functions of the rate sensor 74 and the inclinometer 72, containing the influences of the offset and acceleration, are expressed as follows: G10(s).G11(s) + do(s) G20(s) G2l(s) + G22(s) The reciprocal combination filter 76 is a filter for reciprocally combining the outputs of the rate sensor 74 and the inclinometer 72 so that the frequency characteristic may not appear in the output e0(s) in the necessary frequency band.
Now, when the offset and the parasitic element are not considered, the transfer function of the rate sensor 74 is represented by a formula of Go(s) = Kls. Also, when the influence of the acceleration and the parasitic element are not considered, the transfer function of the inclinometer 72 is represented by a formu]a of G20(s) = K2. In order to reciprocally combining the outputs of both the members, in principle, it is necessary to meet the following relationship: Grate(0)(s) + Gincl(0)(s) = 1 wherein Grate(0)(s) is a transfer function including the rate sensor 74 and tie reciprocal filter 82, and GinciCO,(s) is a transfer function including the inclinometer 72 and the reciprocal filter 84.
The reciprocal filters 82 and 84 are connected in series to the rate sensor 74 and the inc3inometer 72, respectively, and the adder 86 adds the outputs of both the reciprocal filters 82 and 84 to output the detection result eO(s). The transfer function Frate(0)(s) of the reciprocal filter 82 and the transfer function Ft,,ciCO)(s) of the reciprocal filter 84 arc specifically determined as follows: FrateC '(s) = Fincl(0)(s) = Now, when Ka = l/Kl and Kb = /K2, the following formula is obtained.
Ka/(s+#a).K1.s + Kb/(s+#a).K2 = 1 It is readily understood that the reciprocal combination is carried out.
However, the inclinometer 72 iiicludes the pendulum for obtaining the standard in the gravity direction, as shown in Fig. 7. The error due to the influence of the acceleration (error due to G22(s) in the above-described example) becomes large. Furthermore, the rate sensor 74 has the offset, and its temperature drift is large (do(s) in the above-described example). The inclination angle output error (offset error) caused by the offset of the rate sensor 74 is DR0 CO) = d0/(K1.#a) as the limit value of s ' O of s.d0(s).G10(s) according to the final value theorem. A presently available low cost vibration gyro type rate sensor has characteristics such as K1 = 1.26 (V/rad/sec) and do = -0.2 to 0.2 (V) (by temperature), and thus there is a practical problem of DRo eo) except a case of using within a thermostatic chamber.
In Fig. 20, there is shown a structure of a uniaxial inclination sensor of I.he fifth embodiment of a stabilized antenna system according to the present invention. Fig. 21 shows a structure of a parameter adaptive controller shown in Fig. 20, and'Fig. 22 shows a transfer function model of the uniaxial inclination sensor shown in Fig. 20.
In this embodiment, as shown in Fig. 20, the uniaxial inclination sensor 52 includes an inclinometer 72, a rate sensor 74, a parameter adaptive controller 140 and a parameter adaptive reciprocal combination filter 142 having a reciprocal filter with a feedback loop 144, a reciprocal filter 146 and an adder 86.
The reciprocal filter with the feedback loop 144 and the reciprocal filter 146 are connected to the rear stages of the rate sensor 74 atld the inclinometer 72, respectively, and the adder 86 adds tie outputs of both the reciprocal filter with the feedback )oop 144 and 146.
The different points of the structure of the parameter adaptive reciprocal combination filter 142 from the same of the first to fourth embodiments are as follows. First, the reciprocal filter 144 includes the feedback loop so as to enable reducing of an offset error DRoCi)., as shon in Fig. 22.
As shown in Fig. 22, when a transfer function of the feedback loop of the reciprocal filter 144 is defined as follows, Hb(s) = a transfer function Frate(1)(s) of the reciprocal filter 144 is obtained as the following combination value Frate(1)(s) = G2(s)/(1+G2(s).Hb(s))
wherein #b represents a cutoff frequency of the feedback loop and Kb represents a feedback gain factor of the feedback loop, of the following transfer function G2(s) = Ka/(s+#a) and the transfer function Hb(S) of the feedback loop. Kb is controlled by the parameter adaptive controller 140 depending on the conditions of the inclination, as hereina 74, that is, the offset error DRo ( ) is obtained from 7rate(1 (s) by the final value theorem as follows.
DR0Cl? = do/(K1.#a + Ko) It can be understood from this formula that the offset error DR0 Cl) becomes small by increasing the feedback gain factor Kb of the feedback loop. That is, in this embodiment, the offset error DR0(1) can be reduced by providing the feedback loop with feedback gain factor Kb in the reciprocal filter 144.
In this embodiment, the transfer function of the reciprocal filter 146 is different from that of the filter 82 of the first to fourth embodiments, as shown in Fig. 6.
In order to satisfy the reciprocity in a predetermined frequency band, it is required to satisfy the following relationship: K1.s.Frate(1)(s) + K2.Fincl(1)(s) = 1 F1nciCl)(S): a transfer function of the reciprocal filter 146 However, at this time, the parasitic elements of the rate sensor 74 and the inclinometer 72, the drift of the rate sensor 74, and the influence of the acceleration in the inclinometer 72 are neglected.
On the other hand, since the transfer function Frate(1)(s) of the reciprocal filter 144 is expressed by the formula, as described above, the transfer function FinClcl'(s) of the reciprocal filter 146 can be expressed by the modification of the above-described formulas as follows.
#as + #b(#a+KaKb) Fincl(1)(s) = K2{s + (#a+#b)s + #b(#a+K1Kb)} In this formula, a 1st order term of the Laplace operator s appears in the numerator. By this term, the inclination error is caused.
That is, the inclination acceleration error is an error appearing in the output e0(s) by the influence of the acceleration to the inc)inometer 72. When the period of inclination is short and the installation height L is large, it is considered that the influence of G22(s) is emphasized by the term of the 1st order of Laplace operator s -s and thus the error becomes large.
Accordingly, in this embodiment, for reducing the contributory part of the term of the 1st order of Laplace operator s, a correction factor a (a < 1) is introduced in the transfer function Fincl(1)(s) as follows.
&alpha;.#as + #b(#a+KaKb) Fincl(1)(s) = K2{s + (#a+#b)s + #b(#a+KaKb)} As described above, by enlarging the feedback gain factor Kb, the offset error is reduced, and by introducing the correction factor a, the inclination acceleration error is reduced. However, when the feedback gain factor Kb is enlarged, the inclination acceleration error is enlarged regardless of the correction factor a. Hence, in order to reduce both the offset error and the inclination acceleration error at the same time, it is necessary to carry out an adaptive control of the correction factor a and the feedback gain factor Kg.
In this embodiment, for the adaptive control, the parameter adaptive controller 140 is provided. The parameter adaptive controller 140 detects the frequency and amplitude of the inclination from the output e0(s) of the parameter adaptive reciprocal combination filter 142 and outputs a parameter control (ctrl) signal (a, Kb) on the basis of the detection result to the parameter adaptive reciprocal combination filter 142. In the parameter adaptive reciprocal combination filter 142, a parameter (a, Kb) is switched depending on the parameter control signal (a, K ) fed from the parameter adaptive controller 140.
In Fig. 21, there is shown one embodiment of the parameter adaptive controller 140 shown in Fig. 20. The parameter adaptive controller 140 includes an inclination frequency detector 148, an inclination amplitude detector L50 and a parameter (a, Kb) controller 152. The inclination Frequency detector 148 and the inclination amplitude detector 150 detect the respective frequency and amplitude of the inclination e0(s) from the parameter adaptive reciprocal combination filter 142, and output the detection results to the parameter (-a, K ) controller 152. This frequency and amplitude detection is executed by using, for example, the FFT (fast Fourier transform) or the DFT (discrete Fourier transform). The method for obtaining the frequency and the amplitude of the input signal.by the FFT or the DFT is a known algorithm.
The parameter (a, Kb) controller 152 controls the parameter (a, Kb) to the corresponding value according to the frequency and the amplitude of the inclination, detected by the incAination frequency detector 148 and the inclination amplitude detector 150.
By this parameter control, both the offset error and the inclination acceJeration error can be reduced at the same time. In this instance, when the correction factor a becomes far less than one by the adaptive control of the correction factor a, the reciprocity at a low frequency is partially destroyed. Accordingly, there is a possibility of increasing of the error at the low frequency, but this can be controlled to a negligible amount compared with the error reduction by the correction factor a.
Furthermore" in practice, the reciprocity is disturbed due to a phase delay of the rate sensor 74 in a high range (around one Hz or more when the system mounted on the ship and its inclination is detected). Hence, the characteristics of the rate sensor 74 should be checked depending on uses. In this embodiment, it is assumed that the reciprocity in the high range can be almost satisfied in a necessary range for its use, and the terms such as a reciprocal filter and the like are still used in the following description. A model of the present embodiment will be called a reciprocal model. Also, a case of a = 1 will be called a complcte rcciprocal model, and a case of a # 1 will be called an incomplete reciprocal model.
Prior to carrying out the adaptive control of the correction factor a and the feedback gain factor Rb, it is necessary to know how te errors change by the variations of the correction factor a and the feedback gain factor Rb.
That is, by conducting a simulation or the like, the contents (the switch stage number, the value and the like) of the adaptive control of the correction factor a and the feedback gain factor Kb are determined so that the errors may be the minimum values.
Figs. 23A to 23C show the simulation results of the inclination acceleration error. In Figs. 23A to 23C, as to a sine wave of an inclination amplitude of 20 (deg) ad an inclination period of 1 to 33 (sec), an inclination acceleration error is obtained. The conditions are determined as follows. That is, the feedback gain factor Kb = 5.0 (Fig. 23A), 10.0 (Fig. 23B) and 15.0 (Fig. 23C), the installation height L = 20 (m) of th inclinometer 72, fl = 1/2r = 7.0 (Hz), #1 = 1.0, f2 = 2/2r = 1.0 (Hz), #2 = 1.0, and the correction factor a = -0.5, 0, 0.5 and 1.0.
It is understood from Figs. 23A to 23C that, when the inclination period is short, as the correction factor a is smaller compared with 1, the inclination acceleration error is small, and, as the correction factor a is more close to 1, the inclinati,on acceleration error is large.
Furthermore, as the feedback gain factor Rb is large, the inclination acceleration error is large.
Fig. 24 shows a simulation result of a ramp response (an error due to a drift of an offset of the rate sensor 74, that is, a drift error) of the transfer function Frat.Cl)(S). A used ramp input is started from 0 (v) and reaches 50 (mV) in 10 (min) (corresponding to an angular speed of approximately 2 (deg/sec)), and the ramp response of three cases of feedback gain factor Kb = 5.0, 10.0 and 15.0 is obtained. It is understood from Figs. 23A to 23C that as the feedback gain factor Kb is enlarged, the drift error can be diminished.
From these simulation results, for example, the contents of te adaptive control of the correction factor a and the feedback gain factor Kb can be determined as follows.
Fig. 25 shows one example of the adaptive control, in which a correction factor a and a feedback gain factor Kb of a parameter (a, Kb) are varied. In this instance, the parameter (a, Kb) controller 152 controls the correction factor c by switching the correction factor a at the following two stages depending on the frequency (1/period of inclination) of the inclination, detected by the inclination frequency detector 148.
Period of inclinat.ion # 12 (sec) a = 0.5 Period of inclination < 12 (sec) a = 0 The parameter (a, Kb) controller 152 also controls the feedback gain factor Kb by switching the feedback gain factor Kb at the following three stages depending on the amplitude (rms value) of the inclination, detected by the inclination amplitude detector 150.
Amplitude of inclination < 5 (deg) Kb = 15.0 5 (deg) C amplitude of inclination < 15 (deg) Kb = 10.0 Amplitude of inclination # 15 (deg) Kb = 5.0 In this case, as regards the determination of the feedback gain factor Kb, the cutoff frequencies Wa and Wb and the like, it is not sufficient by the aforementioned simplified transfer function formulae, and it is necessary to determine by carrying out a time series analysis using more detailed formulae.
First, when the transfer function Gll(s) of the parasitic element is considered, the transfer function Grate'1'(s) of a combination system of the rate sensor 74 and the reciprocal filter 144, hereinafter referred to as a rate sensor system is expressed from Grate(1)(s) = G10(s).G11(s).Frate(1)(s) as follows.
Grate(1)(s) K1#1s Ka(s+#b) = . s + 2#1#1s + #1 s + (#a+#b)s + #b(#a+KaKb) Furthermore, considering the transfer function G21(s) of the parasitic element and the transfer function G22(s) of the acceleration. the transfer function Gincl(1)(s) = {G20(s).G21(s) + G22(s)}Fincl(1)(s) of a combination system of the inclinometer 72 and the reciprocal filter 146, hereinafter referred to as an inclination sensor system is expressed as follows.
Gincl(1)(s) K2{1-(L/g)s}#2 &alpha;#as + #b(#a+KaKb) = . s + 2#2#2s + #2 s + (#a+#b)s + #b(#a+KaKb) Therefore, the total transfer function Gtotal(1)(s) of the circuit is expressed as follows: Gtotal(1)(s) = Grate(1)(s) + Gincl(1)(s) r2s (s+#b) a0s +a1s+a2s+a3 = + (s+r1s+r2)(s+b1s+b2) (s+p1s+p2)(s+b1s+b2) wherein r1 = 2#1#1, r2 = #1, p1 = 2#2#2, p2 = #2, b1 = #a + #b, b2 = #b(#a + KaKb), a0 = &alpha;KLgp2#a, a1 = KLgp2b2, a2 = &alpha;p2#a, a3 = P2b2. KLg = -L/g.
In this embodiment, as described above, the offset error, the drift error and the inclination acceleration error can be reduced.
First, when the offset error is compared with the example in Fig. 5, in Fig. 5; offset error D,(O) = 0.126 (rad) = 7.24 (deg) in Fig. 20; offset error DR0(1) = 0.010 (rad) = 0.57 (deg) the offset error can be remarkably reduced. This data are obtained under the following conditions: K1 = 1.26 (V/rad/sec) dO = 0.1 (V) #a(0) = 2# X 0.1 (rad), #a(1) = 2# X 0.002 (rad) Rb = 10.0 Hence, in this embodiment, by the feedback loop, the offset error can be reduced, and the rate sensor 74 having a large offset error can be used.
Furthermore, relating to the drift error and the inclination acceleration error, as apparent from the results shown in Figs. 23A to 23C and Fig. 24, by the adaptive control of the correction factor a and the feedback gain factor Kb, they can be reduced as a whole.
In Fig. 26, there is shown a structure of a uniaxial inclination sensor of the sixth embodiment of a stabilized antenna system according to the present invention. In this embodiment, a parameter adaptive controller 154 does not detect the frequency and amplitude of the inclination from the output 60 of the parameter adaptive reciprocal combination filter 142 but detect the same from the output of the inclinometer 72 to output the parameter control signal (a, Kb) to the parameter adaptive reciprocal combination filter 142. The function of the parameter adaptive controller 154 is almost the same as the parameter adaptive controller 140 of the fifth embodiment shown in Fig. 20. In this embodiment, of course, the same effects and advantages as those of the above-described embodiments can be obtained.
In Fig. 27, there is shown a structure of a uniaxial inclination sensor 52 of the seventh embodiment of a stabilized antenna system according to the present invention. In this embodiment, a parameter adaptive controller 156 inputs a receiving level signal from a receiver and outputs a parameter control signal (a, Kb) to the parameter adaptive reciprocal combination filter 142 to properly control feedback gain factor Kb and the correction factor a.
In this embodiment, the receiving level signal output -from this receiver exhibits the signal level received from the communication satellite. The parameter adaptive controller 156 executes the step track on the basis of the receiving level signal.
That is, the parameter adaptive controller 156 generates the step track signal having a minute value and determines the sign(+/-) of this signal to the direction so that the receiving level may be more enlarged, to output as the parameter control signal (a, Rub). By this signal, the values of the correction factor a and the feedback gain factor Kb are gradually increased or decreased, and as a result, the output 0o having a small error can be obtained from the parameter adaptive reciprocal combination filter 142.
In Fig. 28, there is shown a structure of a uniaxial inclination sensor 52 of the eighth embodiment of a stabilized antenna system according to the present invention. In this embodimeiit, two reciprocal filters 158 and 160 are implemented as digital filters, and hence to output sides of a rate sensor 162 and an inclinometer 164, two A/D (analogdigital) converters 166 and 168 are connected. The output of the A/D converter 166 is fed to the reciprocal filter 158 via an adder 172, and the output of the A/D converter 1B8 is input to the reciprocal filter 160. An offset correction register 170 for correcting the offset of the output of the rate sensor 182 is coupled to the adder 172. A parameter adaptive controller 140 has almost the same structure as the fifth embodiment shown in Figs. 20 and 21.
In this embodiment, in case that the reciprocal filters 158 and 160 are implemented as the digital filters, the parameter control can be readily carried out (the control of the correction factor a and the feedback gain factor Kb is relatively easy). In this embodiment, an implementation by digital filters can be carried out by a bilinear transformation as follows.
First, an implementation of the reciprocal filter 158 will be described. By using an operator u = z-l representing a unit time T (one bit) of delay, a bilinear transformation of a transfer function Frate(1)(s) using a Laplace operator by s = h(1-u)/(l+u) and h = 2/T is carried out to obtain the following formula: Frate(1)(s) = (H0.u + H1.u + H2)/(N0.u + N1.u + N2) = Z(u)/R(u) wherein R(u): input series to reciprocal filter 158 Z(u): output series from reciprocal filter 158 H0 = Ka(-h + Wa) HI 1 = 2K,ob H2 = Ka(h + #b) N0 = h - b1h + b2 N1 = -2h2 + 2b2 N2 = h2 + b1h + b2 In this formula, by expressing that R(u).u = R-1 and Z(u).u = Z-l, the output series Z(u) is expressed in the following difference equation: Z(u) = H00R-2+H10R-1+H20R(u) - (N00-R-2+N10R-1+N20R(u)) wherein Moo = Ho/N2 Hlo = 1120 = H2/N2 Noo = No/N2 Nlo = N1/N2 N20 = N2/N2 This difference equation can be readily implemented by a logic circuit or a program of a microprocessor.
Similarly, a bilinear transformation of a transfer function Fincl(1)(s) of the reciprocal filter 160 is carried out to obtain the following formula: Fincl(1)(s) = (Mo u2 + M1,u + M2)/(N0,u2 + N1.u + N2) = Y(u)/X(u) wherein X(u): input series to reciprocal filter 160 Y(u): output series from reciprocal filter 160 M0 = (-&alpha;#ah + b2)/K2 M1 = 2b2/K2 M2 = (&alpha;#ah + b2)/K2 In this formula, by expressing that X(u).uL X-1 and Y(u)*ul = Y-1, the output series Y(u) is expressed in the following difference equation: Y(u) = M00R-2+M10R-1+M20R(u) - (N00R-2+N10R-1+N20R(u)) wherein Moo = Mo/N2 Mlo = Ml/N2 M20 = M2/N2 This difference equation can be readily implemented by a logic circuit or a program of a microprocessor as well.
Furthermore, in this embodiment, the adder 172 subtracts the content of the offset correct register 170 from the output of the A/D converter 166 and outputs the subtracted value to the reciprocal filter 158. The offset correct register 170 stores the offset of the rate sensor 162, and, when the content of the offset correct register 170 is subtracted from the output of the A/D converter 166, the offset corrected value is input to the reciprocal filter 158. As a result, the error can be further reduced.
In the offset correct register 170, the receive level signal is input 'from the receiver. The offset correct register 170 is provided with the step track function, and thus gradually increases or decreases the offset value depending on the value change of the recciving level signal.
As an initial value to be set to the offset correct register 170, a normal temperature value can be preferably used.
As described above, when the offset correct register 170 is used, the feedback gain factor Kb can be settled to a relatively small value, for example, Rb 5 5.
Accordingly, in this embodiment, since the reciprocal filters 158 and 160 are implemented as the digital filters, the feedback gain factor Kb and the correction factor c can be relatively readily controlled, and further, since by the step track in the offset correct register 170, not only the offset error can be reduced but also the feedback gain factor Kb can be determined to be rLelatively small, the inclination acceleration error can be also reduced.
Furthermore, by using the offset correct register 170, the improvement of the tracking function by the array antenna can be performed.
Although the present invention has been described in its preferred embodiments with reference to the accompanying drawings, it it readily understood that the present invention is not restricted to the preferred embodiments and that various changes and modifications can be made by those skilled in the art without departing from the scope of the present invention as defined by the claims.
For instance, in the example of the control shown in Fig. 25, the correction factor a and the feedback gain factor Kb are switched into 2 to 3 Stages. As shown in this example, the adaptive control according to the present invention does not necessarily mean only high level adaptive algorithm, and a control such as switching into 2 to 3 steps can be sufficiently practicable.
In the above-described embodiments, although the adaptive control of the correction factor a and the feedback gain factor Kb hFs been described with reference to the a-Kb adaptation model, by an a adaptation model for adaptively switching or controlling only the correction factor a. the reduction of the inclination acceleration error can be achieved.
Furthermore, although the DFT method or the like and the step track method or the like have been used for the detection of tfie frequency and amplitude of the inclination and the parameter control, other methods such as a mean square method, a mean absolute value method or a zerocrossing method can be also used. In the mean square method, a mean square value of the input signals (an output 60 or the like) is obtained, and based on the obtained mean square value, the feedback gain factor Kb is determined. In the mean absolute value method, a mean value of absolute values of the input signals, and on the basis of the obtained mean value, the feedback gain factor Kb is determined. In the zero-crossing method, from a zero-cross of the input signal, its frequency is obtained, and the correction factor a is determined. The mean square method, the mean absolute value method and the zero-crossing method are already known, and thus the detail of these methods can be omitted.
As described above, according to the present invention, by setting the feedback gain factor Rb, the offset error can be reduced, and by introducing the correction factor a and its adaptive control, the inclination acceleration error can be reduced.
Furthermore, in addition to the adaptive control of the correction factor a, by enlarging the feedback gain factor Rb, the drift error can be reduced.

Claims (5)

CLAINS
1. An inclination angle detecting device for use in a stabilised antenna system to be mounted on a moving platform, comprising a rate sensor for detecting an angular velocity around an elevation axis of the moving platform, an inclinometer for detecting an inclination around the elevation axis of the moving platform, a reciprocal combination filter for combining outputs of the rate sensor and the inclinometer and outputting an inclination angle around the elevation axis, and parameter adaptive control means for adaptively controlling parameters of the reciprocal combination filter depending on a frequency of the inclination, the reciprocal combination filter including a first filter means for filtering the output of the rate sensor, the first filter means including a feedback loop of a feedback gain factor Kb, second filter means for filtering the output of the inclinometer, the second filter means having a reciprocal transfer function including a term of the 1st order of Laplace operator s in a numerator with reference to the first filter means, and adding means for combining outputs of the first filter means and the second filter means to output the inclination angle around the elevation axis, the parameter adaptive control means including means for detecting the frequency of the inclination, and correction means for determining a correction factor a (a < 1) depending on the detected frequency and correcting the term of the 1st order of Laplace operator s by the correction factor a.
2. A device according to claim 1, wherein the parameter adaptive control means further includes means for detecting an amplitude of the inclination, and means for determining the feedback gain factor depending on the detected amplitude and for adaptively controlling the feedback gain factor.
3. An inclination angle device for use in a stabilised antenna system to be mounted on a moving platform, comprising a rate sensor for detecting an angular velocity around an elevation axis of the moving platform, an inclinometer for detecting an inclination around the elevation axis of the moving platform, a reciprocal combination filter for combining outputs of the rate sensor and the inclinometer and outputting an inclination angle around the elevation axis, the reciprocal combination filter including a first filter means for filtering the output of the inclinometer, the second filter means having a reciprocal transfer function with reference to the first filter means, and adding means for combining outputs of the first filter means and the second filter means to output the inclination angle around the elevation axis.
4. An inclination angle detecting device substantially as hereinbefore described with reference to Fig. 19 or Figs.
20 to 25 or Fig. 26, 27 or 28.
5. Stabilised antenna system comprising an inclination angle detecting device according to any one of claims 1 to 4.
GB9503113A 1991-03-20 1992-03-19 Inclination angle measuring device Expired - Fee Related GB2284899B (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP3057070A JP2549470B2 (en) 1991-03-20 1991-03-20 Oscillation compensation antenna device
JP31502091A JP3182185B2 (en) 1991-11-28 1991-11-28 Motion angle detector
GB9206013A GB2256318B (en) 1991-03-20 1992-03-19 Stabilised antenna system

Publications (3)

Publication Number Publication Date
GB9503113D0 GB9503113D0 (en) 1995-04-05
GB2284899A true GB2284899A (en) 1995-06-21
GB2284899B GB2284899B (en) 1995-09-06

Family

ID=27266104

Family Applications (1)

Application Number Title Priority Date Filing Date
GB9503113A Expired - Fee Related GB2284899B (en) 1991-03-20 1992-03-19 Inclination angle measuring device

Country Status (1)

Country Link
GB (1) GB2284899B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2021122617A1 (en) * 2019-12-17 2021-06-24 Rheinmetall Electronics Gmbh Accessory platform

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
WPI Abstract Accession No:N83-228274 & SU 1002844 A (Ocean- logy) 10.3.83 (see abstract) *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2021122617A1 (en) * 2019-12-17 2021-06-24 Rheinmetall Electronics Gmbh Accessory platform

Also Published As

Publication number Publication date
GB9503113D0 (en) 1995-04-05
GB2284899B (en) 1995-09-06

Similar Documents

Publication Publication Date Title
US5227806A (en) Stabilized ship antenna system for satellite communication
JP2579070B2 (en) Array antenna and swing compensation type antenna device
US5359337A (en) Stabilized antenna system
GB2295493A (en) Tracking array antenna system
US5948044A (en) Hybrid GPS/inertially aided platform stabilization system
US4334226A (en) Antenna system for satellite communication
US5587714A (en) Spacecraft antenna pointing error correction
WO2008132141A1 (en) Device and method for controlling a satellite tracking antenna
JPH0568881B2 (en)
BG107622A (en) Following system for flat mobile aerial system
JP2549470B2 (en) Oscillation compensation antenna device
US4803490A (en) Horizon stabilized antenna beam for shipboard radar
JPS6057702A (en) 3-axis antenna trestle for ship
US4680521A (en) Stabilization aid for a vehicle-or vessel-borne search unit
GB2284899A (en) Inclination angle detector
US3432856A (en) Doppler inertial navigation system
JP3957628B2 (en) Target tracking apparatus and method
Bigley et al. Wideband base motion isolation control for a mobile platform
JPH04315301A (en) Rocking compensation type antenna system
JPH05259722A (en) Antenna directive device
JP2596376B2 (en) Antenna drive control device
JPH06104621A (en) Antenna directivity device
JPH05259721A (en) Antenna directive device
JPH08211140A (en) Monopulse tracking antenna
Chernodarov et al. A SPATIALLY DISTRIBUTED MICRONAVIGATTION SYSTEM FOR A SYNTHETIC–APERTURE RADAR

Legal Events

Date Code Title Description
PCNP Patent ceased through non-payment of renewal fee

Effective date: 19990319