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WO2008015757A1 - Wind speed radar - Google Patents

Wind speed radar Download PDF

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Publication number
WO2008015757A1
WO2008015757A1 PCT/JP2006/315488 JP2006315488W WO2008015757A1 WO 2008015757 A1 WO2008015757 A1 WO 2008015757A1 JP 2006315488 W JP2006315488 W JP 2006315488W WO 2008015757 A1 WO2008015757 A1 WO 2008015757A1
Authority
WO
WIPO (PCT)
Prior art keywords
radio wave
support member
wind speed
lens
fiber
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.)
Ceased
Application number
PCT/JP2006/315488
Other languages
French (fr)
Japanese (ja)
Inventor
Katsuyuki Imai
Takao Nakagawa
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.)
SEI Hybrid Products Inc
Original Assignee
SEI Hybrid Products Inc
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
Application filed by SEI Hybrid Products Inc filed Critical SEI Hybrid Products Inc
Priority to KR1020097000270A priority Critical patent/KR101283257B1/en
Priority to PCT/JP2006/315488 priority patent/WO2008015757A1/en
Priority to JP2008527628A priority patent/JP4935816B2/en
Priority to CNA2006800550043A priority patent/CN101467066A/en
Priority to TW096102588A priority patent/TWI387776B/en
Publication of WO2008015757A1 publication Critical patent/WO2008015757A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/95Radar or analogous systems specially adapted for specific applications for meteorological use
    • G01S13/951Radar or analogous systems specially adapted for specific applications for meteorological use ground based
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/95Radar or analogous systems specially adapted for specific applications for meteorological use
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P5/00Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/03Details of HF subsystems specially adapted therefor, e.g. common to transmitter and receiver
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01WMETEOROLOGY
    • G01W1/00Meteorology
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q15/00Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
    • H01Q15/02Refracting or diffracting devices, e.g. lens, prism
    • H01Q15/08Refracting or diffracting devices, e.g. lens, prism formed of solid dielectric material
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q19/00Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic
    • H01Q19/06Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using refracting or diffracting devices, e.g. lens
    • H01Q19/062Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using refracting or diffracting devices, e.g. lens for focusing
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q25/00Antennas or antenna systems providing at least two radiating patterns
    • H01Q25/007Antennas or antenna systems providing at least two radiating patterns using two or more primary active elements in the focal region of a focusing device
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A90/00Technologies having an indirect contribution to adaptation to climate change
    • Y02A90/10Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation

Definitions

  • the present invention relates to a wind speed radar that transmits and receives a signal via a lens antenna and measures a wind direction, a wind speed distribution, and the like in an atmospheric layer.
  • These radar devices irradiate a target with high-frequency radio waves such as antenna force microwaves, and receive reflected waves from the target, thereby enabling the size, shape, distance, moving direction, and moving speed of the target. Etc. are detected.
  • the size of the precipitation area and the amount of precipitation are detected by irradiating radio waves to water droplets such as rain and analyzing the received reflected waves. To do.
  • a parabolic antenna or a phased array antenna has been conventionally used.
  • the wind radar needs to be small in size and simple in structure so that it can move easily. Therefore, it is necessary to reduce the number of circuits, components, cables, etc. as much as possible, and to switch the radio waves at high speed in order to ensure the synchronism of force data that needs to be reduced in cost.
  • the zenith angle ⁇ in the direction of the radio wave which is desirable to have a structure that is resistant to wind pressure, is acceptable. It is preferable to change it.
  • parabolic antenna when used as a main component of a wind speed radar, the following two types are adopted. That is, (a) a form using three parabolic antennas, and (b) a form in which one parabolic antenna is moved mechanically.
  • the form (a) is a form in which three parabolic antennas corresponding to each direction of the zenith, north, and east are installed, and each parabolic antenna is switched for observation.
  • it is a type in which three antennas with a diameter of lm or more are installed side by side, it is very bulky and requires a large installation area, which limits the installation location. Therefore, it is difficult to reduce the size of the apparatus, and the cost increases.
  • the antenna antenna has a structure that is susceptible to wind pressure, during strong winds such as typhoons, the antenna shakes due to the influence of the wind and affects the observation data. Therefore, the accuracy and stability of the data are lacking.
  • the antenna antenna is fixedly installed, the zenith angle ⁇ in the radio wave direction cannot be easily changed.
  • the parabolic antenna aperture can be made to correspond to various observation directions by rotational movement, so one parabolic antenna should be installed in all directions. That's fine. Therefore, it is not as bulky as the above-mentioned form (a).
  • an extremely large antenna support mechanism and control mechanism are required for the antenna. Therefore, the size of the device inevitably increases.
  • the antenna direction can be changed by operating the machine, it takes a long time to change the direction. Therefore, the synchronism of observation data between each direction cannot be obtained, and severe weather changes cannot be handled.
  • the format (a) there is a problem that the accuracy and stability of the data are lacking in a strong wind such as a typhoon.
  • a phased array antenna is an antenna that can arbitrarily control the directivity, that is, the transmission / reception direction of radio waves to be transmitted / received, by changing the relative phase of the power supply signal of the element antenna. Then, a system is adopted in which a large number of element antennas are arranged in a plane and the phase planes of radio waves in the direction of transmission and reception are aligned. Therefore, a phase shifter that gives a predetermined phase amount to each element antenna is connected in advance so that the phase of the element antenna is changed based on the position where the element antenna is arranged. [0009] Since this phased array antenna has a flat antenna surface and is parallel to the ground, it can stably acquire data even in strong winds that are not easily affected by wind. In addition, since the beam direction is switched by controlling the phase of each element antenna, high-speed switching is possible.
  • phased array antenna When a phased array antenna is used as a main component of wind speed radar, as a condition for satisfying the characteristics as a wind speed radar, for example, the antenna gain of radio waves transmitted and received must be 30 dBi or more. Become. However, in order to satisfy this condition, it is necessary to arrange 100 or more element antennas. Each element antenna is connected to one phase shifter necessary for switching the beam direction. These phase shifters include a control circuit for changing the necessary phase amount by the phase shifter, A control line or the like is required. Therefore, the structure of the wind speed radar becomes extremely complicated. In addition, since the antenna is configured with multiple element antennas, multiple transmitters and receivers are required, and the phased array antenna is very expensive.
  • this wind speed radar is made up of a spherical radio wave lens formed by using a dielectric material so that the relative permittivity changes at a predetermined rate in the radial direction, and a radio wave lens.
  • a plurality of primary radiators arranged at a focal position of radio waves transmitted and received in a plurality of desired azimuth directions, and a transmitter and a receiver connected to the primary radiator are provided.
  • This radio lens is a radio lens that has long been known as a so-called Luneberg lens. The radio lens is placed on an annular support plate having a diameter slightly smaller than the diameter of the radio lens!
  • the radio wave lens is supported by supporting the support plate with legs. According to such a wind speed radar, data synchronization can be ensured by switching multiple primary radiators at high speed, and it is difficult to be affected by wind pressure. It is described that the entire device can be downsized, the structure can be simplified, and the cost can be reduced (for example, see Patent Document 1).
  • a synthetic resin foam is used as the dielectric material forming the Luneberg lens.
  • the Luneberg lens weighs about 50 kg.
  • the Luneberg lens is formed of a synthetic resin foam, and thus is weak and easily deformed. Therefore, by mounting the Luneberg lens on the annular support plate as described above, the Luneberg lens may be deformed or damaged by the Luneberg lens force due to its own weight. There was a problem that proper support could be difficult.
  • Patent Document 1 JP 2005-61905 A
  • a synthetic resin foam is used as the dielectric material forming the Luneberg lens.
  • the Luneberg lens weighs about 50 kg.
  • the Luneberg lens is formed of a synthetic resin foam, and thus is weak and easily deformed. Therefore, by mounting the Luneberg lens on the annular support plate described above, the Luneberg lens may be deformed or damaged by the Luneberg lens force due to its own weight. There was a problem that it was difficult to support properly.
  • the present invention has been made in view of the above-described problems, and includes a spherical radio wave lens formed using a dielectric material so that the relative permittivity changes at a predetermined rate in the radial direction.
  • An object of the present invention is to provide a wind speed radar that can effectively prevent deformation and breakage of a radio wave lens.
  • a wind speed including a spherical transmission / reception radio lens, a primary radiator for transmission / reception, and a support member that supports the radio lens.
  • Radar is provided.
  • the radio wave lens for transmission and reception is formed by using a dielectric so that the relative permittivity changes at a predetermined rate in the radial direction.
  • the primary radiator for transmission and reception is arranged at the focal position of the radio wave transmitted and received through the radio lens in a plurality of azimuth directions to be observed along the outer periphery of the radio lens.
  • the surface of the support member on which the radio wave lens is placed has a spherical shape that matches the shape of the radio wave lens.
  • the load of the radio wave lens is evenly distributed on the surface of the support member. It becomes possible. Therefore, as a radio wave lens, a spherical Luneberg lens (e.g.
  • the support member is formed with a storage portion for storing the primary radiator. According to this configuration, the primary radiator can be easily arranged at the focal position while the radio wave lens is appropriately supported by the support member.
  • the support member is preferably formed of a fiber reinforced plastic material.
  • the fiber reinforced plastic material is excellent in load resistance, the radio wave lens can be reliably supported by the support member.
  • the thickness of the support member can be reduced, the transmission loss and phase change of the radio wave when the radiation from the primary radiator or the radio wave incident on the primary radiator passes through the support member are effective. Can be suppressed.
  • the fiber reinforced plastic material has excellent heat resistance and a small dimensional change due to a temperature change, the support member can be prevented from being deformed or damaged due to long-term use.
  • the fiber reinforced plastic material is excellent in workability, it becomes easy to process the surface of the support member into a spherical shape that matches the shape of the radio wave lens, and manufacture of the support member is facilitated.
  • the support member is preferably formed of at least one selected from the group consisting of polyolefin resin, polystyrene resin, and fluorine resin. According to this configuration, it is possible to effectively suppress the transmission loss and phase change of the radio wave when the radio wave emitted from the primary radiator or incident on the primary radiator passes through the support member. Furthermore, since these resins are excellent in workability, it is easy to process the surface of the support member into a spherical shape that matches the shape of the radio wave lens. Thus, the support member can be easily manufactured.
  • the support member is formed of a resin foam having a foaming magnification force of 0 or more. According to this configuration, the support member can be formed of the resin foam having a dielectric constant very close to that of air. Therefore, it is possible to more effectively suppress the transmission loss of radio waves in the support member.
  • FIG. 1 is a partial cross-sectional view showing an overall configuration of a wind speed radar according to an embodiment of the present invention.
  • FIG. 2 is a perspective view for explaining a support member that supports a radio wave lens of a wind speed radar.
  • FIG. 3 is a diagram for explaining a method of measuring wind speed and direction by a wind speed radar according to an embodiment of the present invention.
  • FIG. 4 is a partial cross-sectional view showing a modification of the wind speed radar according to the embodiment of the present invention.
  • FIG. 5 is a partially enlarged view of FIG.
  • FIG. 6 is a partial cross-sectional view showing a modification of the wind speed radar according to the embodiment of the present invention.
  • FIG. 7 is a partial sectional view showing a modified example of the wind speed radar according to the embodiment of the present invention.
  • FIG. 8] (a) to (c) are diagrams for explaining the arrangement of wind speed radars according to the embodiment of the present invention.
  • FIG. 1 is a partial cross-sectional view showing an overall configuration of a wind speed radar according to an embodiment of the present invention
  • FIG. 2 is a perspective view for explaining a support member that supports a radio wave lens of the wind speed radar.
  • FIG. 3 is a diagram for explaining a method of measuring the wind speed and direction by the wind speed radar according to the embodiment of the present invention.
  • the wind speed radar 1 includes a radio wave lens 2 for transmission / reception and a plurality of primary radiators 3 for transmission / reception disposed along the outer periphery of the radio wave lens 2 (this embodiment)
  • Reference symbol Z indicates the zenith direction
  • reference symbol N indicates the north direction
  • reference symbol S indicates the south direction
  • reference symbol E indicates the east direction
  • reference symbol W indicates the west direction.
  • the radio wave lens 2 is a Luneberg lens having a spherical shape, and is formed into a spherical lens by a central spherical core 2 and a plurality of different-diameter spherical shells 2, 2, 2 surrounding the spherical core 2.
  • the dielectric constant is used to change the dielectric constant at a predetermined rate in the radial direction.
  • the dielectric here refers to a material that exhibits paraelectricity, ferroelectricity, or antiferroelectricity and does not have electrical conductivity.
  • R is the radius of the sphere
  • r is the distance of the center force of the sphere.
  • the diameter force of the radio wave lens 2 for example, 800 mm, 600 mm, 450 mm can be used.
  • the dielectric for the Luneberg lens for example, a foam of a polyolefin-based synthetic resin such as polyethylene resin or polypropylene resin can be used.
  • an inorganic high dielectric filler such as titanium oxide, titanate or zirconate added to the synthetic resin and foamed from it can also be used.
  • the relative dielectric constant of these dielectric foams is adjusted to the target value by controlling the specific gravity by varying the expansion ratio, and by this adjustment, a higher specific gravity can be obtained with a higher specific gravity. it can.
  • the outer peripheral side requires a magnification of 10 times or more of the center side, so that the addition ratio of the inorganic high dielectric filler is increased on the center side. It is good to add and decrease on the outer peripheral side.
  • the number n of layers of the spherical nuclei is an arbitrary number, in the wind speed radar 1 in the present embodiment, for example, it is set to 16 to 18, and the change in the dielectric constant due to each spherical nuclei is finely and smoothly smoothed. Set to change.
  • a raw material a synthetic resin alone or a mixture of a synthetic resin and an inorganic high dielectric filler
  • a gas such as nitrogen gas.
  • a chemical foaming method in which a foaming agent is added and foamed by placing it in a mold having a desired shape.
  • a pellet-like material impregnated with a volatile foaming agent is pre-foamed in advance, and the obtained pre-foamed beads are filled in a mold having a desired shape, and then heated again with steam or the like to be foamed again, and at the same time.
  • a bead foaming method in which beads are fused to each other.
  • the primary radiator 3 has an electromagnetic hob having an opening having a substantially rectangular or substantially circular cross section.
  • a dielectric antenna or a dielectric rod antenna having a dielectric rod mounted on a waveguide is used.
  • a microstrip antenna, a slot antenna, a linear antenna such as a dipole, a loop antenna, or the like can be used.
  • the directivity (polarization) of the electric field of the radio wave transmitted and received from the primary radiator 3 can be linearly polarized (for example, vertical polarization or horizontal polarization) or circularly polarized (for example, right-handed polarization). It may be a deviation of left-handed polarization.
  • the primary radiator 3 is configured to be supported on support rails 5 and 6 supported by the shaft portion 4.
  • the primary radiator 3 has a focal position of the radio wave lens 2 corresponding to a plurality of desired azimuth directions to be observed in the observation region from the ground to the sky (ie, (Focal position of radio waves transmitted and received via radio lens 2 in a plurality of azimuth directions to be observed) and 5 primary radiators 3Z, 3N, 3S, 3E, and 3W for transmission / reception. is there. More specifically, the focal position of radio waves transmitted and received in the zenith direction and the azimuth angle direction that forms a predetermined zenith angle ⁇ with respect to the north, south, east, and west directions in the observation area up to the ground.
  • the primary radiators 3Z, 3N, 3S, 3E, and 3W are configured to be connected to a transmitter 11 and a receiver 12 of the control unit 9 to be described later by a coaxial cable (not shown).
  • the zenith angle ⁇ is set to an appropriate angle within a range of 10 ° to 15 °.
  • each of the primary radiators 3Z, 3N, 3S, 3E, and 3W is placed on the support rails 5 and 6 at the focal position of the wave lens 2 corresponding to the above-described azimuth directions. It is fixedly installed.
  • Each of the primary radiators 3Z, 3N, 3S, 3E, and 3W is configured to be movable on the support rails 5 and 6 and can be fixed at a predetermined azimuth position. It is preferable that ⁇ can be changed within the above range.
  • the radio wave lens 2 is configured to be supported by a support member 7. More specifically, the radio wave lens 2 is supported by the support member 7 by placing a part of the surface 2 a of the radio wave lens 2 on the surface 7 a of the support member 7. As shown in FIGS. 1 and 2, the surface 7a of the support member 7 on which the radio wave lens 2 is placed has a shape of the radio wave lens 2. It has a spherical shape that matches the shape (ie, spherical shape). With such a configuration, the load of the radio wave lens 2 can be evenly distributed on the surface 7a of the support member 7.
  • the radio wave lens 2 is formed of a synthetic resin foam, and has a diameter of, for example, Even when a Luneberg lens with a weight of 800 mm and a weight of 50 kg is used, deformation or breakage of the Luneberg lens can be effectively prevented.
  • the support member 7 is formed with a storage portion 17 for storing the primary radiator 3 and the like.
  • the primary radiator 3 can be easily placed at the focal position of the radio wave lens 2 while the radio wave lens 2 is appropriately supported by the support member 7.
  • the radio wave is radiated from the primary radiator 3 via the radio wave lens 2, or the primary radiator 3
  • the radio wave passes through the support member 7.
  • the support member 7 needs to have excellent radio wave permeability (that is, a characteristic that the phase change is small with little transmission loss).
  • the support member 7 needs to have strength (that is, load resistance) that can withstand the load of the radio wave lens 2. Therefore, in the present embodiment, in order to ensure excellent radio wave permeability and load resistance, the fiber reinforced plastic composed of a fiber reinforcing material and a matrix resin is used as a material constituting the support member 7. (FRP) material is preferably used.
  • this fiber-reinforced plastic material is excellent in load bearing performance !, it is possible to reliably support the radio wave lens 2 by using the support member 7 formed of the fiber-reinforced plastic material. Is possible. Further, since the fiber reinforced plastic material is excellent in load resistance, the thickness of the support member 7 formed of the fiber reinforced plastic material can be reduced. Furthermore, by selecting a fiber reinforcement or matrix resin that has excellent radio wave transmission (that is, low dielectric constant and low dielectric loss tangent), it is emitted from primary radiator 3 or incident on primary radiator 3. The transmission loss and phase change of the radio wave when the radio wave passes through the support member 7 can be effectively suppressed.
  • the support member 7 can be effectively prevented from being deformed or damaged due to long-term use.
  • fiber reinforced plastic materials are easy to process Therefore, the surface 7a of the support member 7 can be easily processed into a spherical shape matching the shape of the radio wave lens 2, and the manufacture of the support member 7 is facilitated.
  • Examples of the fiber reinforcing material of the fiber reinforced plastic material include glass fiber, aramid fiber, nylon fiber, polyethylene fiber, polytetrafluoroethylene (PTFE) fiber, and the like. Can be used in combination. Of these, the use of glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber as the fiber reinforcement makes it possible to more effectively suppress radio wave transmission loss. Of the glass fibers, quartz (SiO 2) has a high purity (for example, a purity of 9
  • quartz glass fiber or the above-mentioned polytetrafluoroethylene fiber is particularly preferable because transmission loss of radio waves can be minimized.
  • thermosetting resin and thermoplastic resin can be used as the matrix resin of the fiber reinforced plastic material.
  • thermosetting resin include unsaturated polyester resin, phenol resin, epoxy resin, and bismaleimide resin.
  • thermoplastic resin include polyamide resin, polyimide resin, polyamideimide resin, polyetherimide resin, and polyethersulfone resin. These rosins can be used alone or in combination.
  • the thickness of the support member 7 formed of a fiber reinforced plastic material is preferably lmm to 5mm.
  • a synthetic resin can be used instead of the above-described fiber-reinforced plastic material.
  • the resin thermosetting resin and thermoplastic resin can be used. From the viewpoint of effectively suppressing transmission loss of radio waves and phase change, polyolefin resin or polystyrene resin can be used. , And fluorinated resin can be suitably used.
  • these resins are excellent in workability like the above-described fiber-reinforced plastic material, it becomes easy to process the surface 7a of the support member 7 into a spherical shape that matches the shape of the radio wave lens 2. Thus, the support member 7 can be easily manufactured.
  • polystyrene-based resin examples include polystyrene and styrene. N-acrylonitrile copolymer, styrene-butadiene copolymer, styrene-methacrylic acid copolymer, styrene-methyl methacrylate copolymer, and styrene-acrylic acid copolymer.
  • fluorinated resin examples include polytetrafluoroethylene, tetrafluoroethylene monohexafluoropropylene copolymer (FEP), and the like.
  • a resin foam having a high expansion ratio can also be used. From the viewpoint of radio wave transmission, it is preferable that only air having a dielectric constant of 1 exists between the radio wave lens 2 and the primary radiator 3. Therefore, in order to reduce the dielectric constant of the material forming the support member 7 existing between the radio wave lens 2 and the primary radiator 3 to a dielectric constant very close to that of air, it has a high expansion ratio. It is necessary to form the support member 7 using the foam.
  • the support member 7 can be formed of a foamed body having a dielectric constant very close to the dielectric constant of air by using a resin foam having an expansion ratio of 40 or more. Therefore, as in the case of using glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber as the fiber reinforced plastic material, the transmission loss of the radio wave when the radio wave passes through the support member 7, In addition, the phase change can be more effectively suppressed.
  • the resin forming the resin foam having such a high foaming ratio for example, the above-mentioned polyolefin resin, polystyrene resin, and fluorine resin are preferably used. it can.
  • the thickness of the support member 7 formed of a foam having a high expansion ratio is 10 mn! ⁇ 100mm is preferred.
  • the wind speed radar 1 includes a radio lens 2, a primary radiator 3, a support member 7 and the like, and a radome 8 for protecting rain wind and snow accumulation force.
  • the primary radiator 3, the support member 7, etc. are housed inside the radome 8.
  • the radome 8 needs to have excellent radio wave transmissivity, in this embodiment, in order to ensure excellent radio wave transmissibility, as a material constituting the radome 8, for example, the above-described fiber A reinforced plastic (FRP) material is preferably used.
  • the wind speed radar 1 according to the present embodiment includes a control unit 9 that houses a transmitter 11, a receiver 12, and the like, which will be described later, below the radome 8.
  • the control unit 9 of the wind radar 1 includes an oscillator 10 that generates a high-frequency signal, a transmitter 11 that is connected to the oscillator 10 and amplifies the high-frequency signal generated by the oscillator 10, and reflects or It has a receiver 12 that amplifies the weak high-frequency radio signal that has been scattered back and returned.
  • the control unit 9 includes a switch 13 that is connected to the transmitter 11, the receiver 12, and the primary radiator 3 and performs switching of signals to be transmitted and received, and the primary radiator 3 (that is, a plurality of transmitters 11).
  • Each of the primary radiators 3Z, 3N, 3S, 3E, and 3W) is connected to the transmitter 11 and the receiver 12 via the switch 13.
  • the control unit 9 is connected to the receiver 12 and detects a signal received by the receiver 12, and the signal detected by the signal detector 14 is connected to the signal detector 14.
  • a signal processor 15 for calculating the wind speed and direction information of the atmospheric layer T.
  • control unit 9 includes a computer 16 as control means, and by starting a radar device control program, an oscillator 10, a transmitter 11, a receiver 12, a switch 13, a signal detector 14 and the signal processor 15 are controlled.
  • a predetermined high frequency signal is generated by the oscillator 10, and the high frequency signal is sent to the transmitter 11.
  • the high frequency signal is amplified by the transmitter 11 and sent to each of the plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W.
  • the amplified high-frequency signal is converted into a desired high frequency radio wave 20 via the primary radiators 3Z, 3N, 3S, 3E, and 3W, respectively, the radio wave lens 2, and the above-described desired observation to be observed in space. Radiated in multiple azimuth directions.
  • the weak high-frequency radio waves 21 reflected from the atmospheric layer T in the sky and returning from each azimuth angle direction are collected at the focal position by the radio lens 2, and a plurality of primary radiations are transmitted through the radio lens 2. Received in each of 3Z, 3N, 3S, 3E, and 3W.
  • the plurality of azimuth angles to be observed as described above for example, the zenith and the azimuth angle that forms the zenith angle ⁇ with east-west north-south are sent via the radio wave lens 2.
  • Primary radiators 3Z, 3N, 3S, 3E, and 3W are arranged corresponding to the focal position of the received radio wave. Therefore, if radio waves are transmitted from the primary radiators 3Z, 3N, 3S, 3E, and 3W arranged at the respective focal positions, the primary radiators 3Z, 3N, 3S, 3E, and 3W at the respective focal positions are transmitted.
  • the reflected radio wave returns immediately and the radio signal in the specified azimuth direction is obtained.
  • radio wave signals received by each of primary radiators 3Z, 3N, 3S, 3E, and 3W are sent to receiver 12 switched by switch 13.
  • the receiver 12 amplifies the high-frequency signal and sends it to the signal processor 15 via the signal detector 14.
  • the signal processor 15 processes the signal detected by the signal detector 14.
  • each of the plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W that is, five transmitters 11.
  • only one set of transmitter 11 and receiver 12 for multiple primary radiators 3 Z, 3N, 3S, 3E, and 3W ie, one transmitter 11 and one receiver. 12
  • the primary radiator that emits radio waves (or radio waves are incident) is selected from the multiple primary radiators 3Z, 3N, 3S, 3E, and 3W.
  • a configuration may be selected.
  • a pulse-like shape is transmitted from the primary radiator 3S via the radio wave lens 2 toward the azimuth angle direction that forms a predetermined zenith angle ⁇ with respect to the south direction S.
  • the radio wave is radiated, the radio wave is scattered slightly due to the refractive index fluctuation accompanying the atmospheric turbulence in the sky), and returns to the radio wave lens 2 with a time delay corresponding to the altitude.
  • a measurement can be performed using the radio wave signal received by the receiver 12 as described above. It is obtained by calculating in 9.
  • the spherical Luneberg lens described above is used as the radio wave lens 2 when performing this measurement. Therefore, the attenuation rate of radio waves is small and weak. Even radio waves can be sufficiently detected.
  • the radio wave lens 2 that has high strength and is less susceptible to wind pressure. Therefore, even when installed in an area exposed to strong winds, such as a typhoon, it is possible to provide a wind speed radar 1 with excellent wind resistance.
  • the wind speed radar 1 of the present embodiment unlike the phased array antenna described above, it is not necessary to connect a phase shifter to the primary radiator 3, and a large number of element antennas are used. do not need. Therefore, it is possible to reduce the size and weight of the device and simplify the structure, and to reduce the number of circuits, components, cables, and the like as much as possible, thereby reducing the cost.
  • 0 and 0 correspond to, for example, east and west (or north and south).
  • the wind speed and the altitude distribution of the wind direction at each altitude can be obtained.
  • the wind speed radar 1 of the present embodiment can easily and accurately measure the wind direction, wind speed distribution, etc. in the atmospheric layer by using the surface force radio wave, using the lens antenna. It can be widely used for observation.
  • the wind radar 1 of the present embodiment includes a spherical radio wave lens 2 formed using a dielectric so that the relative permittivity changes in a predetermined ratio in the radial direction, and the radio wave lens 2 A support member 7 is provided.
  • the surface 7 a of the support member 7 on which the radio wave lens 2 is placed has a spherical shape that matches the shape of the radio wave lens 2. Therefore, since the load of the radio wave lens 2 can be evenly distributed on the surface 7a of the support member 7, even when a large weight, a Luneberg lens is used, deformation of the Luneberg lens, or Damage can be effectively prevented. As a result, it is possible to appropriately support the radio wave lens 2 in the wind speed radar 1 including the radio wave lens 2.
  • the support member 7 is formed with a storage portion 17 for storing the primary radiator 3. Therefore, the primary radiator 3 can be easily placed at the focal position of the radio wave lens 2 while the radio wave lens 2 is appropriately supported by the support member 7.
  • the support member 7 is formed of a fiber reinforced plastic material having excellent load resistance. Therefore, the radio wave lens 2 is securely attached by the support member 7. It becomes possible to support. Further, since the thickness of the support member 7 can be reduced, the transmission loss of the radio wave when the radio wave radiated from the primary radiator 3 or the radio wave incident on the primary radiator 3 passes through the support member 7, And a phase change can be suppressed effectively. Further, since the fiber reinforced plastic material has excellent heat resistance and a small dimensional change due to a temperature change, the support member 7 can be effectively prevented from being deformed or damaged. Furthermore, since the fiber-reinforced plastic material is excellent in processability, the support member 7 can be easily manufactured.
  • the support member 7 is formed of a polyolefin resin, a polystyrene resin, and a fluorine resin. Therefore, it is possible to effectively suppress transmission loss and phase change of the radio wave when the radio wave emitted from the primary radiator 3 or the radio wave incident on the primary radiator 3 passes through the support member 7. Furthermore, since these resins have excellent processability, the support member 7 can be easily manufactured.
  • the support member is formed of a resin foam having an expansion ratio of 40 or more. Therefore, it is possible to more effectively suppress the transmission loss of radio waves in the support member 7.
  • a plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W are arranged corresponding to the focal positions of radio waves transmitted and received in a plurality of azimuth directions.
  • the primary radiator 3 may be movably disposed so as to correspond to the focal positions of radio waves transmitted and received in a plurality of azimuth directions.
  • the support rails 5 and 6 are provided orthogonal to each other, and for example, the support rail 5 is arranged in the north-south direction. Is installed in the east-west direction.
  • one primary radiator 3 is installed on the support rails 5 and 6 in the direction of the arrow in the figure, and the zenith direction and the north, south, east, and west directions are Stop at the focal position of the radio wave transmitted and received in the azimuth direction that forms the specified zenith angle ⁇ , and at each stop position, wind speed, Measure wind direction data.
  • the method for measuring the wind speed and direction data is the same as in the above embodiment. With such a configuration, it is possible to measure wind speed and wind direction data with one primary radiator 3, thereby suppressing an increase in cost.
  • the support rail 30 that supports the primary radiator 3 is extended only in one direction, and the shaft portion 4 that supports the support rail 30 is rotated. It is good also as a structure provided freely.
  • the primary radiator 3Z is fixedly disposed at the focal position of the radio wave transmitted and received in the zenith direction Z, and one primary radiator 3 is movably provided on the support rail 30. Then, the primary radiator 3 is stopped at the focal position of the radio wave transmitted and received in the azimuth angle direction that forms a predetermined zenith angle ⁇ with respect to the north, south, east, and west directions. Measure wind direction data.
  • the primary radiator 3Z disposed at the focal position of the radio wave transmitted and received in the zenith direction Z is omitted.
  • a configuration in which only one primary radiator 3 is movably provided on the support rail 30 is also possible. In this case, the primary radiator 3 is stopped at the focal position of the radio wave transmitted and received in the zenith direction and the azimuth angle direction that forms the predetermined zenith angle ⁇ with respect to the north, south, east, and west directions. Measure wind speed and direction data at the stop position.
  • the material for forming the support member 7 other materials can be used as long as they have the above-described radio wave permeability, load resistance, and workability.
  • a ceramic material, wood, or the like can be used as a material for forming the support member 7.
  • a plurality of wind speed radars 1 can be used side by side. More specifically, for example, as shown in FIG. 8 (a), four wind speed radars 1 can be arranged, and as shown in FIG. 8 (b), seven wind speed radars are arranged. be able to. Further, as shown in FIG. 8 (c), 13 wind speed radars 1 can be arranged. With such a configuration, the physical area of the radio wave lens 2 can be increased, so that the antenna gain and transmission power can be improved. As a result, the radar performance (for example, observation altitude) can be improved.
  • the oscillator 10, the signal detector 14, the signal processor 15 and the like described in FIG. 3 may be provided for each of the plurality of wind radars 1. Overall, oscillator 10, signal detector 14, and signal Even if only one processor 15 etc. is installed.
  • a wind speed radar that transmits and receives a signal via a lens antenna and measures a wind direction, a wind speed distribution and the like in the atmosphere layer.

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Abstract

A wind speed radar (1) comprises a spherical transmitting/receiving lens antenna (2) so formed of a dielectric that the dielectric constant varies at a predetermined rate in the radial direction and transmitting/receiving primary radiators (3Z, 3N, 3S, 3E, 3W) disposed along the outer periphery of the lens antenna (2) at the focuses of the radio waves transmitted/received through the lens antenna (2) in the direction of azimuths to be observed. The lens antenna (2) is supported by a support member (7). The surface (7a) of the support member (7) on which the lens antenna (2) is placed has a spherical shape matching the shape of the lens antenna (2).

Description

明 細 書  Specification

風速レーダー  Wind speed radar

技術分野  Technical field

[0001] この発明は、レンズアンテナを介して信号を送、受信し、大気層での風向、風速分 布等を測定する風速レーダーに関する。  The present invention relates to a wind speed radar that transmits and receives a signal via a lens antenna and measures a wind direction, a wind speed distribution, and the like in an atmospheric layer.

背景技術  Background art

[0002] 従来、気象観測や航空管制等の目的で、種々のレーダー装置が使用されている。  Conventionally, various radar devices have been used for the purpose of weather observation and air traffic control.

これらのレーダー装置は、アンテナ力 マイクロ波等の高周波電波を対象物に向け て照射し、当該対象物からの反射波を受信することにより、対象物の大きさや形状、 距離、移動方向、移動速度等の検知を行うものである。例えば、気象状態を観測する ための気象レーダー装置の場合は、雨等の水滴に対して電波を照射し、受信した反 射波の解析を行うことにより、降水域の大きさや降水量等を検知する。  These radar devices irradiate a target with high-frequency radio waves such as antenna force microwaves, and receive reflected waves from the target, thereby enabling the size, shape, distance, moving direction, and moving speed of the target. Etc. are detected. For example, in the case of a meteorological radar device for observing weather conditions, the size of the precipitation area and the amount of precipitation are detected by irradiating radio waves to water droplets such as rain and analyzing the received reflected waves. To do.

[0003] また、地表からの放射 ·吸収の影響を、直接的に受ける大気層における大気運動の 観測をすることは、地球環境を知る上で非常に重要であり、その一環として、風速レ 一ダーを使用した高度毎の風向.風速分布の観測が行なわれている。この風速レー ダーでは、風の向き(即ち、風向)を測定するために、電波を、最小限、天頂方向、及 び北、東の各方位に対し、所定の天頂角 Θをなす方位角方向の 3方向に放射して測 定が行われる。また、データの信頼性を向上する際には、天頂方向、及び北、南、東 、西の各方位に対し、所定の天頂角 Θをなす方位角方向の 5方向に電波を放射して 測定が行なわれる。  [0003] Observing atmospheric motion in the atmospheric layer that is directly affected by radiation and absorption from the earth's surface is extremely important for understanding the global environment. Observation of wind direction and wind speed distribution at every altitude using a dar. In this wind speed radar, in order to measure the direction of the wind (ie, the wind direction), the radio wave is at a minimum, the zenith direction, and the azimuth direction forming a predetermined zenith angle Θ with respect to the north and east directions. Measurements are performed by radiating in three directions. In order to improve the reliability of the data, it is measured by radiating radio waves in 5 directions of the zenith direction and the azimuth angle direction Θ that forms the specified zenith angle Θ with respect to the north, south, east and west directions. Is done.

[0004] また、このような風速レーダーの主要構成部材であるアンテナの形式については、 従来、パラボラアンテナやフェーズドアレイ方式のアンテナが用いられている。ここで 、各地の風速 ·風向の観測を簡易に行なうためには、風速レーダーは移動が簡単に 行なえるように装置全体の小型化、構造の簡単ィ匕が必要である。そのため、回路、部 品、ケーブル等を極力減らし、低コストィ匕する必要がある力 データの同時性を確保 するために、電波の切替は、高速に行なう必要がある。また、強風時のデータの安定 性の観点から、風圧を受け難い構造であることが望ましぐ電波方向の天頂角 Θは可 変とするのが好ましい。 [0004] In addition, as a type of an antenna that is a main component of such a wind speed radar, a parabolic antenna or a phased array antenna has been conventionally used. Here, in order to make it easy to observe the wind speed and direction of each region, the wind radar needs to be small in size and simple in structure so that it can move easily. Therefore, it is necessary to reduce the number of circuits, components, cables, etc. as much as possible, and to switch the radio waves at high speed in order to ensure the synchronism of force data that needs to be reduced in cost. In addition, from the viewpoint of the stability of data during strong winds, the zenith angle Θ in the direction of the radio wave, which is desirable to have a structure that is resistant to wind pressure, is acceptable. It is preferable to change it.

[0005] ここで、パラボラアンテナを、風速レーダーの主要構成部材として利用する場合、次 の 2つの形式が採用される。即ち、(a)パラボラアンテナ 3個を用いる形式、(b)パラボ ラアンテナ 1個を機械的に動かす形式である。  [0005] Here, when a parabolic antenna is used as a main component of a wind speed radar, the following two types are adopted. That is, (a) a form using three parabolic antennas, and (b) a form in which one parabolic antenna is moved mechanically.

[0006] (a)の形式は、天頂、北、東の各方位に対応する 3個のパラボラアンテナを設置し、 各パラボラアンテナを切り替えて観測をする形式である。しかし、 lm以上の直径を有 するアンテナを 3個並べて設置する形式であるため、非常に嵩張り、大きな設置面積 が必要となり、設置場所の制限を受ける。従って、装置の小型化を図ることが困難で あり、コスト的にも高くなる。また、ノ ラボラアンテナは風圧を受け易い構造であるため 、台風等の強風時には、風の影響でアンテナが揺れ、観測データに影響を与える。 従って、データの正確性、安定性に欠ける。さらに、ノ ラボラアンテナは固定設置さ れるため、電波方向の天頂角 Θを、容易に変更することができない。  [0006] The form (a) is a form in which three parabolic antennas corresponding to each direction of the zenith, north, and east are installed, and each parabolic antenna is switched for observation. However, because it is a type in which three antennas with a diameter of lm or more are installed side by side, it is very bulky and requires a large installation area, which limits the installation location. Therefore, it is difficult to reduce the size of the apparatus, and the cost increases. In addition, because the antenna antenna has a structure that is susceptible to wind pressure, during strong winds such as typhoons, the antenna shakes due to the influence of the wind and affects the observation data. Therefore, the accuracy and stability of the data are lacking. Furthermore, since the antenna antenna is fixedly installed, the zenith angle Θ in the radio wave direction cannot be easily changed.

[0007] (b)の形式の場合、回転移動により、種々の観測方向に、パラボラアンテナの開口 面を対応させることができるため、全ての方位に対して、 1台のパラボラアンテナを設 置すればよい。従って、上述の(a)の形式ほど嵩張ることはない。しかし、 lm以上の 直径を有する大きなアンテナを傾けて、目的の方位に動かして固定するためには、ァ ンテナに対して、極めて大きなアンテナ支持機構や制御機構が必要となる。従って、 必然的に装置が大型化する。また、機械操作を行うことにより、アンテナの方向を変 える方式であるため、方位の切り替えに長時間必要となる。従って、各方位間での観 測データの同時性が得られず、激しい気象変化には対応できない。さらに、(a)の形 式の場合と同様に、台風等の強風時にデータの正確性、安定性に欠けるという問題 がある。  [0007] In the case of the format (b), the parabolic antenna aperture can be made to correspond to various observation directions by rotational movement, so one parabolic antenna should be installed in all directions. That's fine. Therefore, it is not as bulky as the above-mentioned form (a). However, in order to tilt a large antenna with a diameter of lm or more and move it to the desired orientation and fix it, an extremely large antenna support mechanism and control mechanism are required for the antenna. Therefore, the size of the device inevitably increases. In addition, since the antenna direction can be changed by operating the machine, it takes a long time to change the direction. Therefore, the synchronism of observation data between each direction cannot be obtained, and severe weather changes cannot be handled. Furthermore, as in the case of the format (a), there is a problem that the accuracy and stability of the data are lacking in a strong wind such as a typhoon.

[0008] フェーズドアレイ方式のアンテナは、素子アンテナの給電信号の相対位相を変える ことにより、指向性、即ち、送受信される電波の送受信方向を任意に制御することが できるアンテナである。そして、多数の素子アンテナを平面状に配列して形成し、送 受信される方向の電波の位相面を揃える方式が採用される。従って、予め、素子アン テナの位相を、素子アンテナが配置される位置に基づいて変化させるように、各素子 アンテナに所定の位相量を与える移相器が接続される。 [0009] このフェーズドアレイ方式のアンテナは、アンテナ面が平面であり、かつ、地面に平 行であるため、風の影響を受け難ぐ強風時であっても安定してデータが取得できる 。また、各素子アンテナの位相を制御してビーム方位を切り替えるため、高速切り替 えが可能である。 [0008] A phased array antenna is an antenna that can arbitrarily control the directivity, that is, the transmission / reception direction of radio waves to be transmitted / received, by changing the relative phase of the power supply signal of the element antenna. Then, a system is adopted in which a large number of element antennas are arranged in a plane and the phase planes of radio waves in the direction of transmission and reception are aligned. Therefore, a phase shifter that gives a predetermined phase amount to each element antenna is connected in advance so that the phase of the element antenna is changed based on the position where the element antenna is arranged. [0009] Since this phased array antenna has a flat antenna surface and is parallel to the ground, it can stably acquire data even in strong winds that are not easily affected by wind. In addition, since the beam direction is switched by controlling the phase of each element antenna, high-speed switching is possible.

[0010] フェーズドアレイ方式のアンテナを風速レーダーの主要部材として利用する場合、 風速レーダーとしての特性を満足するための条件として、例えば、送受信される電波 のアンテナ利得が 30dBi以上であることが必要となる。しかし、この条件を満たすため には、 100以上の素子アンテナを並べる必要がある。また、各々の素子アンテナには 、ビーム方位の切り替えに必要な移相器が 1つずつ接続され、これら移相器には、必 要な位相量を移相器で変化させるための制御回路や制御線等が必要となる。従って 、風速レーダーの構造が極めて複雑となる。さらに、アンテナが複数の素子アンテナ 力 構成されているため、送、受信器も複数必要となり、フェーズドアレイ方式のアン テナは非常にコスト高となる。  [0010] When a phased array antenna is used as a main component of wind speed radar, as a condition for satisfying the characteristics as a wind speed radar, for example, the antenna gain of radio waves transmitted and received must be 30 dBi or more. Become. However, in order to satisfy this condition, it is necessary to arrange 100 or more element antennas. Each element antenna is connected to one phase shifter necessary for switching the beam direction. These phase shifters include a control circuit for changing the necessary phase amount by the phase shifter, A control line or the like is required. Therefore, the structure of the wind speed radar becomes extremely complicated. In addition, since the antenna is configured with multiple element antennas, multiple transmitters and receivers are required, and the phased array antenna is very expensive.

[0011] そこで、上述の風速レーダーに対して要求される種々の条件を満たすベぐレンズ アンテナを使用した風速レーダーが開示されている。より具体的には、この風速レー ダ一は、誘電体材料を用いて比誘電率が半径方向に所定の割合で変化するように 形成された球形状の電波レンズと、電波レンズを介して、所望の複数の方位角方向 に送、受信される電波の焦点位置に配置された複数の一次放射器と、当該一次放 射器に接続された送、受信器とを備えている。この電波レンズは、いわゆるルーネべ ルグレンズとして、古くから知られている電波レンズであり、電波レンズの直径よりも若 干小さ!/ヽ径を有する環状の支持板上に電波レンズが載置され、当該支持板を脚材 により支持することにより、電波レンズが支持される構成となっている。このような風速 レーダーによれば、複数の一次放射器の高速切り替えにより、データの同時性を確 保でき、風圧の影響を受け難いため、強風時のデータの安定性を確保でき、また、装 置全体の小型化、構造の簡単化、および低コストィ匕を図ることができると記載されて いる(例えば、特許文献 1参照)。 Accordingly, a wind speed radar using a veg lens antenna that satisfies various conditions required for the above-described wind speed radar is disclosed. More specifically, this wind speed radar is made up of a spherical radio wave lens formed by using a dielectric material so that the relative permittivity changes at a predetermined rate in the radial direction, and a radio wave lens. A plurality of primary radiators arranged at a focal position of radio waves transmitted and received in a plurality of desired azimuth directions, and a transmitter and a receiver connected to the primary radiator are provided. This radio lens is a radio lens that has long been known as a so-called Luneberg lens. The radio lens is placed on an annular support plate having a diameter slightly smaller than the diameter of the radio lens! The radio wave lens is supported by supporting the support plate with legs. According to such a wind speed radar, data synchronization can be ensured by switching multiple primary radiators at high speed, and it is difficult to be affected by wind pressure. It is described that the entire device can be downsized, the structure can be simplified, and the cost can be reduced (for example, see Patent Document 1).

[0012] ここで、下記特許文献 1に記載の風速レーダーにお 、ては、ルーネベルグレンズを 形成する誘電体材料としては、合成樹脂の発砲体が使用される。しかし、例えば、直 径が 800mmのルーネベルグレンズを使用する場合、当該ルーネベルグレンズの重 量は約 50kgにもなる。また、ルーネベルグレンズは、合成樹脂の発砲体により形成さ れているため、強度が弱ぐ変形し易い。従って、上述の、環状の支持板上にルーネ ベルグレンズを載置することにより、当該ルーネベルグレンズを支持する構成では、 ルーネベルグレンズ力 自重により、変形、または破損する場合があり、ルーネベル グレンズを適切に支持することが困難になる場合があるという問題があった。 Here, in the wind speed radar described in Patent Document 1 below, a synthetic resin foam is used as the dielectric material forming the Luneberg lens. But for example, If a Luneberg lens with a diameter of 800 mm is used, the Luneberg lens weighs about 50 kg. In addition, the Luneberg lens is formed of a synthetic resin foam, and thus is weak and easily deformed. Therefore, by mounting the Luneberg lens on the annular support plate as described above, the Luneberg lens may be deformed or damaged by the Luneberg lens force due to its own weight. There was a problem that proper support could be difficult.

特許文献 1 :特開 2005— 61905号公報  Patent Document 1: JP 2005-61905 A

発明の開示  Disclosure of the invention

[0013] ここで、上記特許文献 1に記載の風速レーダーにお 、ては、ルーネベルグレンズを 形成する誘電体材料としては、合成樹脂の発砲体が使用される。しかし、例えば、直 径が 800mmのルーネベルグレンズを使用する場合、当該ルーネベルグレンズの重 量は約 50kgにもなる。また、ルーネベルグレンズは、合成樹脂の発砲体により形成さ れているため、強度が弱ぐ変形し易い。従って、上述の、環状の支持板上にルーネ ベルグレンズを載置することにより、当該ルーネベルグレンズを支持する構成では、 ルーネベルグレンズ力 自重により、変形、または破損する場合があり、ルーネベル グレンズを適切に支持することが困難になる場合があるという問題があった。  Here, in the wind speed radar described in Patent Document 1, a synthetic resin foam is used as the dielectric material forming the Luneberg lens. However, for example, when using a Luneberg lens with a diameter of 800 mm, the Luneberg lens weighs about 50 kg. In addition, the Luneberg lens is formed of a synthetic resin foam, and thus is weak and easily deformed. Therefore, by mounting the Luneberg lens on the annular support plate described above, the Luneberg lens may be deformed or damaged by the Luneberg lens force due to its own weight. There was a problem that it was difficult to support properly.

[0014] 本発明は、上述の問題に鑑みてなされたものであり、誘電体材料を用いて比誘電 率が半径方向に所定の割合で変化するように形成された球形状の電波レンズを備え る風速レーダーにおいて、電波レンズの変形、破損を効果的に防止することができる 風速レーダーを提供することを目的とする。  The present invention has been made in view of the above-described problems, and includes a spherical radio wave lens formed using a dielectric material so that the relative permittivity changes at a predetermined rate in the radial direction. An object of the present invention is to provide a wind speed radar that can effectively prevent deformation and breakage of a radio wave lens.

[0015] 上記目的を達成するために、本発明の一態様では、球形状の送受信用の電波レン ズと、送受信用の一次放射器と、電波レンズを支持する支持部材とを備えている風速 レーダーが提供される。送受信用の電波レンズは、誘電体を用いて比誘電率が半径 方向に所定の割合で変化するように形成されている。送受信用の一次放射器は、電 波レンズの外周に沿って、観測すべき複数の方位角方向に電波レンズを介して送受 信される電波の焦点位置に配設されて ヽる。電波レンズが載置される支持部材の表 面は、電波レンズの形状に合わせた球面形状を有する。  In order to achieve the above object, according to one aspect of the present invention, a wind speed including a spherical transmission / reception radio lens, a primary radiator for transmission / reception, and a support member that supports the radio lens. Radar is provided. The radio wave lens for transmission and reception is formed by using a dielectric so that the relative permittivity changes at a predetermined rate in the radial direction. The primary radiator for transmission and reception is arranged at the focal position of the radio wave transmitted and received through the radio lens in a plurality of azimuth directions to be observed along the outer periphery of the radio lens. The surface of the support member on which the radio wave lens is placed has a spherical shape that matches the shape of the radio wave lens.

[0016] 同構成によれば、支持部材の表面において、電波レンズの荷重を均等に分散させ ることが可能になる。従って、電波レンズとして、誘電体を用いて比誘電率が半径方 向に所定の割合で変化するように形成された球形状のルーネベルグレンズ (例えば[0016] According to the configuration, the load of the radio wave lens is evenly distributed on the surface of the support member. It becomes possible. Therefore, as a radio wave lens, a spherical Luneberg lens (e.g.

、直径力 OOmm、重量が 50kg)を使用する場合であっても、ルーネベルグレンズの 変形、または破損を効果的に防止することができる。その結果、電波レンズを備える 風速レーダーにお 、て、電波レンズを適切に支持することが可能になる。 Even when using a diameter force of OO mm and a weight of 50 kg, deformation or breakage of the Luneberg lens can be effectively prevented. As a result, it is possible to properly support the radio lens in a wind speed radar equipped with the radio lens.

[0017] 上記の風速レーダーにおいて、支持部材には、一次放射器を収納するための収納 部が形成されていることが好ましい。同構成によれば、支持部材により、電波レンズを 適切に支持した状態で、一次放射器を焦点位置に容易に配置することができる。  [0017] In the wind speed radar described above, it is preferable that the support member is formed with a storage portion for storing the primary radiator. According to this configuration, the primary radiator can be easily arranged at the focal position while the radio wave lens is appropriately supported by the support member.

[0018] 上記の風速レーダーにおいて、支持部材が、繊維強化プラスチック材により形成さ れていることが好ましい。同構成によれば、繊維強化プラスチック材は、耐荷重性に 優れているため、支持部材により、電波レンズを確実に支持することができる。また、 支持部材の厚みを薄くすることができるため、一次放射器から放射、または一次放射 器に入射される電波が支持部材を透過する際の、当該電波の透過損失、および位 相変化を効果的に抑制することができる。また、繊維強化プラスチック材は、耐熱性 に優れ、温度変化による寸法変化が小さいため、長期使用による、支持部材の変形 や破損を防止することができる。さらに、繊維強化プラスチック材は、加工性に優れて いるため、支持部材の表面を、電波レンズの形状に合わせた球面形状に加工し易く なり、支持部材の製造が容易になる。  [0018] In the above wind speed radar, the support member is preferably formed of a fiber reinforced plastic material. According to this configuration, since the fiber reinforced plastic material is excellent in load resistance, the radio wave lens can be reliably supported by the support member. In addition, since the thickness of the support member can be reduced, the transmission loss and phase change of the radio wave when the radiation from the primary radiator or the radio wave incident on the primary radiator passes through the support member are effective. Can be suppressed. In addition, since the fiber reinforced plastic material has excellent heat resistance and a small dimensional change due to a temperature change, the support member can be prevented from being deformed or damaged due to long-term use. Furthermore, since the fiber reinforced plastic material is excellent in workability, it becomes easy to process the surface of the support member into a spherical shape that matches the shape of the radio wave lens, and manufacture of the support member is facilitated.

[0019] 上記の風速レーダーにお!/、て、繊維強化プラスチック材の繊維強化材カ ガラス繊 維、ポリエチレン繊維、およびポリテトラフルォロエチレン繊維力もなる群より選ばれる 少なくとも 1種であることが好ましい。同構成によれば、支持部材における電波の透過 損失をより一層効果的に抑制することが可能になる。  [0019] For the above wind speed radar! /, It should be at least one selected from the group consisting of fiber reinforced plastic fiber reinforced plastic fiber glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber strength. Is preferred. According to this configuration, it is possible to more effectively suppress the transmission loss of radio waves in the support member.

[0020] また、上記の風速レーダーにおいて、支持部材が、ポリオレフイン系榭脂、ポリスチ レン系榭脂、およびフッ素系榭脂からなる群より選ばれる少なくとも 1種により形成さ れていることが好ましい。同構成によれば、一次放射器から放射、または一次放射器 に入射される電波が支持部材を透過する際の、当該電波の透過損失、および位相 変化を効果的に抑制することができる。さらに、これらの榭脂は、加工性に優れてい るため、支持部材の表面を、電波レンズの形状に合わせた球面形状に加工し易くな り、支持部材の製造が容易になる。 [0020] In the wind speed radar, the support member is preferably formed of at least one selected from the group consisting of polyolefin resin, polystyrene resin, and fluorine resin. According to this configuration, it is possible to effectively suppress the transmission loss and phase change of the radio wave when the radio wave emitted from the primary radiator or incident on the primary radiator passes through the support member. Furthermore, since these resins are excellent in workability, it is easy to process the surface of the support member into a spherical shape that matches the shape of the radio wave lens. Thus, the support member can be easily manufactured.

[0021] 上記の風速レーダーにお!/、て、支持部材が、発泡倍率力 0以上である榭脂発泡 体により形成されていることが好ましい。同構成によれば、空気の誘電率に極めて近 い誘電率を有する榭脂発砲体により、支持部材を形成することができる。従って、支 持部材における電波の透過損失をより一層効果的に抑制することが可能になる。 図面の簡単な説明  [0021] In the above wind speed radar, it is preferable that the support member is formed of a resin foam having a foaming magnification force of 0 or more. According to this configuration, the support member can be formed of the resin foam having a dielectric constant very close to that of air. Therefore, it is possible to more effectively suppress the transmission loss of radio waves in the support member. Brief Description of Drawings

[0022] [図 1]本発明の実施形態に係る風速レーダーの全体構成を示す部分断面図である。  FIG. 1 is a partial cross-sectional view showing an overall configuration of a wind speed radar according to an embodiment of the present invention.

[図 2]風速レーダーの電波レンズを支持する支持部材を説明するための斜視図であ る。  FIG. 2 is a perspective view for explaining a support member that supports a radio wave lens of a wind speed radar.

[図 3]本発明の実施形態に係る風速レーダーによる風速、風向の測定方法を説明す るための図である。  FIG. 3 is a diagram for explaining a method of measuring wind speed and direction by a wind speed radar according to an embodiment of the present invention.

[図 4]本発明の実施形態に係る風速レーダーの変形例を示す部分断面図である。  FIG. 4 is a partial cross-sectional view showing a modification of the wind speed radar according to the embodiment of the present invention.

[図 5]図 4の部分拡大図である。  FIG. 5 is a partially enlarged view of FIG.

[図 6]本発明の実施形態に係る風速レーダーの変形例を示す部分断面図である。  FIG. 6 is a partial cross-sectional view showing a modification of the wind speed radar according to the embodiment of the present invention.

[図 7]本発明の実施形態に係る風速レーダーの変形例を示す部分断面図である。  FIG. 7 is a partial sectional view showing a modified example of the wind speed radar according to the embodiment of the present invention.

[図 8] (a)〜(c)は、本発明の実施形態に係る風速レーダーの配列を説明するための 図である。  [FIG. 8] (a) to (c) are diagrams for explaining the arrangement of wind speed radars according to the embodiment of the present invention.

発明を実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION

[0023] 以下に、本発明の好適な実施形態について説明する。図 1は、本発明の実施形態 に係る風速レーダーの全体構成を示す部分断面図であり、図 2は、風速レーダーの 電波レンズを支持する支持部材を説明するための斜視図である。また、図 3は、本発 明の実施形態に係る風速レーダーによる風速、風向の測定方法を説明するための 図である。 [0023] Hereinafter, preferred embodiments of the present invention will be described. FIG. 1 is a partial cross-sectional view showing an overall configuration of a wind speed radar according to an embodiment of the present invention, and FIG. 2 is a perspective view for explaining a support member that supports a radio wave lens of the wind speed radar. FIG. 3 is a diagram for explaining a method of measuring the wind speed and direction by the wind speed radar according to the embodiment of the present invention.

[0024] 図 1に示すように、この風速レーダー 1は、送受信用の電波レンズ 2と、当該電波レ ンズ 2の外周に沿って配設された複数の送受信用の一次放射器 3 (本実施形態にお いては、 5個の送受信用の一次放射器 3Z、 3N、 3S、 3E、および 3W)と、を備えてい る。なお、符号 Zは、天頂方向、符号 Nは北方向、符号 Sは南方向、符号 Eは東方向 、および符号 Wは西方向を示す。 [0025] この電波レンズ 2は、球形状を有するルーネベルグレンズであり、中心の球核 2とそ れを取り巻く複数の異径球殻 2、 · · ·、 2 、 2により球形状のレンズとして形成され、 誘電体を用いて比誘電率が半径方向に所定の割合で変化するように形成されたも のである。なお、ここでいう誘電体とは、常誘電性、強誘電性、若しくは反強誘電性を 示し、かつ電気伝導性を有さないものをいう。このルーネベルグレンズからなる電波レ ンズ 2は、各球殻部の比誘電率 ε γ力 およそ ε γ = 2—(rZR) 2の式に従うように 形成されるとともに、中心部の比誘電率を約 2に設定し、当該中心部力 外側へ向か つて誘電率が約 1となるように変化させたものである。なお、上記式において、 Rは球 の半径であり、 rは球の中心力もの距離である。また、本実施形態においては、電波 レンズ 2の直径力 例えば、 800mm, 600mm, 450mmのものが使用できる。 As shown in FIG. 1, the wind speed radar 1 includes a radio wave lens 2 for transmission / reception and a plurality of primary radiators 3 for transmission / reception disposed along the outer periphery of the radio wave lens 2 (this embodiment) In the form, there are five primary radiators 3Z, 3N, 3S, 3E, and 3W) for transmission and reception. Reference symbol Z indicates the zenith direction, reference symbol N indicates the north direction, reference symbol S indicates the south direction, reference symbol E indicates the east direction, and reference symbol W indicates the west direction. The radio wave lens 2 is a Luneberg lens having a spherical shape, and is formed into a spherical lens by a central spherical core 2 and a plurality of different-diameter spherical shells 2, 2, 2 surrounding the spherical core 2. The dielectric constant is used to change the dielectric constant at a predetermined rate in the radial direction. The dielectric here refers to a material that exhibits paraelectricity, ferroelectricity, or antiferroelectricity and does not have electrical conductivity. The radio lens 2 consisting of this Luneberg lens is formed so as to follow the equation of relative permittivity ε γ force of each spherical shell part ε γ = 2-(rZR) 2 , and the relative permittivity of the center part is It is set to about 2 and is changed so that the dielectric constant becomes about 1 toward the outside of the central force. In the above equation, R is the radius of the sphere, and r is the distance of the center force of the sphere. In the present embodiment, the diameter force of the radio wave lens 2, for example, 800 mm, 600 mm, 450 mm can be used.

[0026] このルーネベルグレンズ用の誘電体としては、例えば、ポリエチレン榭脂、ポリプロ ピレン樹脂等のポリオレフイン系の合成樹脂の発泡体を使用することができる。また、 当該合成樹脂に酸化チタン、チタン酸塩、ジルコン酸塩等の無機高誘電フィラーを 加え、それを発泡させたものも使用できる。そして、これらの誘電発泡体の比誘電率 は、発泡倍率を異ならせて比重を制御することにより目標値に調整され、当該調整に より、高比重で、ある程高い比誘電率を得ることができる。  [0026] As the dielectric for the Luneberg lens, for example, a foam of a polyolefin-based synthetic resin such as polyethylene resin or polypropylene resin can be used. In addition, an inorganic high dielectric filler such as titanium oxide, titanate or zirconate added to the synthetic resin and foamed from it can also be used. The relative dielectric constant of these dielectric foams is adjusted to the target value by controlling the specific gravity by varying the expansion ratio, and by this adjustment, a higher specific gravity can be obtained with a higher specific gravity. it can.

[0027] また、この比誘電率の調整を発泡倍率のみを変えて行なうと、外周側では中心側の 10倍以上の倍率が必要となるため、無機高誘電フィラーの添加割合を中心側で増 加させ、外周側で減少させると良い。また、上記球核の層数 nは、任意数であるが、 本実施形態における風速レーダー 1においては、例えば、 16〜18に設定し、各球核 による誘電率の変化を、きめ細かぐ滑らかに変化するように設定する。  [0027] Further, if the relative dielectric constant is adjusted by changing only the expansion ratio, the outer peripheral side requires a magnification of 10 times or more of the center side, so that the addition ratio of the inorganic high dielectric filler is increased on the center side. It is good to add and decrease on the outer peripheral side. In addition, although the number n of layers of the spherical nuclei is an arbitrary number, in the wind speed radar 1 in the present embodiment, for example, it is set to 16 to 18, and the change in the dielectric constant due to each spherical nuclei is finely and smoothly smoothed. Set to change.

[0028] また、誘電発泡体の製造方法としては、例えば、原料 (合成樹脂単体や、合成樹脂 と無機高誘電フィラーの混合物)に対して、加熱により分解して窒素ガス等の気体を 発生する発泡剤を添加し、これを所望の形状の金型に入れて発泡させる化学発泡法 が挙げられる。また、揮発性発泡剤を含浸させたペレット状材料を予め予備発泡させ 、得られた予備発泡ビーズを所望形状の金型に充填した後、水蒸気等で加熱して再 度発泡させると同時に、隣接ビーズを互いに融着させるビーズ発泡法が挙げられる。  [0028] In addition, as a method for producing a dielectric foam, for example, a raw material (a synthetic resin alone or a mixture of a synthetic resin and an inorganic high dielectric filler) is decomposed by heating to generate a gas such as nitrogen gas. There is a chemical foaming method in which a foaming agent is added and foamed by placing it in a mold having a desired shape. In addition, a pellet-like material impregnated with a volatile foaming agent is pre-foamed in advance, and the obtained pre-foamed beads are filled in a mold having a desired shape, and then heated again with steam or the like to be foamed again, and at the same time. There is a bead foaming method in which beads are fused to each other.

[0029] 一次放射器 3は、その断面形状が略矩形状や略円形状の開口部を有する電磁ホ ーンアンテナや、導波管に誘電体ロッドを装着した誘電体ロッドアンテナ等が使用さ れる。また、一次放射器 3として、マイクロストリップアンテナ、スロットアンテナ、ダイポ ール等の線状アンテナ、およびループアンテナ等を使用することもできる。また、一 次放射器 3から送受信される電波の電界の方向性 (偏波)は、直線偏波 (例えば、垂 直偏波や水平偏波)や円偏波(例えば、右旋偏波ゃ左旋偏波)の ヽずれであっても 良い。なお、図 1に示すように、一次放射器 3は、軸部 4に支持された支持レール 5、 6 上に支持される構成となって 、る。 [0029] The primary radiator 3 has an electromagnetic hob having an opening having a substantially rectangular or substantially circular cross section. For example, a dielectric antenna or a dielectric rod antenna having a dielectric rod mounted on a waveguide is used. Further, as the primary radiator 3, a microstrip antenna, a slot antenna, a linear antenna such as a dipole, a loop antenna, or the like can be used. In addition, the directivity (polarization) of the electric field of the radio wave transmitted and received from the primary radiator 3 can be linearly polarized (for example, vertical polarization or horizontal polarization) or circularly polarized (for example, right-handed polarization). It may be a deviation of left-handed polarization. As shown in FIG. 1, the primary radiator 3 is configured to be supported on support rails 5 and 6 supported by the shaft portion 4.

[0030] また、一次放射器 3は、図 1に示すように、地上から上空までの観測領域における、 観測すべき所望の複数の方位角方向に対応する、電波レンズ 2の焦点位置 (即ち、 観測すべき複数の方位角方向に電波レンズ 2を介して送受信される電波の焦点位置 )に、 5個の送受信用の一次放射器 3Z、 3N、 3S、 3E、および 3Wを配設したもので ある。より具体的には、地上力も上空までの観測領域における、天頂方向、及び北、 南、東、西の各方位に対し、所定の天頂角 Θをなす方位角方向に送受信される電波 の焦点位置に対応して、 5個の送受信用の一次放射器 3Z、 3N、 3S、 3E、および 3 Wを配設したものである。なお、これらの一次放射器 3Z、 3N、 3S、 3E、および 3Wは 、図示しない同軸ケーブルにより、後述する制御部 9の送信器 11、および受信器 12 に接続される構成となって 、る。  In addition, as shown in FIG. 1, the primary radiator 3 has a focal position of the radio wave lens 2 corresponding to a plurality of desired azimuth directions to be observed in the observation region from the ground to the sky (ie, (Focal position of radio waves transmitted and received via radio lens 2 in a plurality of azimuth directions to be observed) and 5 primary radiators 3Z, 3N, 3S, 3E, and 3W for transmission / reception. is there. More specifically, the focal position of radio waves transmitted and received in the zenith direction and the azimuth angle direction that forms a predetermined zenith angle Θ with respect to the north, south, east, and west directions in the observation area up to the ground. Corresponding to the above, five primary radiators 3Z, 3N, 3S, 3E, and 3 W for transmission and reception are arranged. The primary radiators 3Z, 3N, 3S, 3E, and 3W are configured to be connected to a transmitter 11 and a receiver 12 of the control unit 9 to be described later by a coaxial cable (not shown).

[0031] また、本実施形態においては、天頂角 Θは、 10° 〜15° の範囲内において、適 当な角度に設定される。図 1においては、一次放射器 3Z、 3N、 3S、 3E、および 3W の各々は、支持レール 5、 6上において、上述の複数の方位角方向に対応する、電 波レンズ 2の焦点位置に、固定して設置されている。なお、一次放射器 3Z、 3N、 3S 、 3E、および 3Wの各々を、支持レール 5、 6上を移動可能に設けるとともに、所定の 方位角位置において固定することができるように構成し、天頂角 Θを、上述の範囲内 にお 、て変化させることができるようにすることが好ま 、。  In the present embodiment, the zenith angle Θ is set to an appropriate angle within a range of 10 ° to 15 °. In FIG. 1, each of the primary radiators 3Z, 3N, 3S, 3E, and 3W is placed on the support rails 5 and 6 at the focal position of the wave lens 2 corresponding to the above-described azimuth directions. It is fixedly installed. Each of the primary radiators 3Z, 3N, 3S, 3E, and 3W is configured to be movable on the support rails 5 and 6 and can be fixed at a predetermined azimuth position. It is preferable that Θ can be changed within the above range.

[0032] また、図 1、図 2に示すように、電波レンズ 2は、支持部材 7により支持される構成とな つている。より具体的には、電波レンズ 2の表面 2aの一部が、支持部材 7の表面 7aに 載置されることにより、電波レンズ 2が、支持部材 7により支持される。そして、図 1、図 2に示すように、電波レンズ 2が載置される支持部材 7の表面 7aが、電波レンズ 2の形 状 (即ち、球形状)に合わせた球面形状を有している。このような構成により、支持部 材 7の表面 7aにおいて、電波レンズ 2の荷重を均等に分散させることが可能になるた め、電波レンズ 2として、合成樹脂の発砲体により形成され、例えば、直径が 800mm 、重量が 50kgのルーネベルグレンズを使用する場合であっても、当該ルーネベルグ レンズの変形、または破損を効果的に防止することができる。 Further, as shown in FIGS. 1 and 2, the radio wave lens 2 is configured to be supported by a support member 7. More specifically, the radio wave lens 2 is supported by the support member 7 by placing a part of the surface 2 a of the radio wave lens 2 on the surface 7 a of the support member 7. As shown in FIGS. 1 and 2, the surface 7a of the support member 7 on which the radio wave lens 2 is placed has a shape of the radio wave lens 2. It has a spherical shape that matches the shape (ie, spherical shape). With such a configuration, the load of the radio wave lens 2 can be evenly distributed on the surface 7a of the support member 7. Therefore, the radio wave lens 2 is formed of a synthetic resin foam, and has a diameter of, for example, Even when a Luneberg lens with a weight of 800 mm and a weight of 50 kg is used, deformation or breakage of the Luneberg lens can be effectively prevented.

[0033] また、本実施形態においては、図 1に示すように、支持部材 7には、一次放射器 3等 を収納するための収納部 17が形成されている。この収納部 17により、支持部材 7に より、電波レンズ 2を適切に支持した状態で、一次放射器 3を電波レンズ 2の焦点位 置に容易に配置することができる。  In this embodiment, as shown in FIG. 1, the support member 7 is formed with a storage portion 17 for storing the primary radiator 3 and the like. With the storage portion 17, the primary radiator 3 can be easily placed at the focal position of the radio wave lens 2 while the radio wave lens 2 is appropriately supported by the support member 7.

[0034] また、このように、一次放射器 3等を支持部材 7の内部に収納する構成においては 、電波レンズ 2を経由して、一次放射器 3から電波を放射、または、一次放射器 3に電 波を入射させる際に、当該電波が支持部材 7を透過することになる。従って、支持部 材 7は、優れた電波透過性 (即ち、透過損失が少なぐ位相変化が小さい、という特性 )を有することが必要になる。また、支持部材 7は、電波レンズ 2の荷重に耐え得る強 度 (即ち、耐荷重性)を有することが必要になる。そこで、本実施形態においては、優 れた電波透過性、および耐荷重性を確保するために、支持部材 7を構成する材料と して、繊維強化材とマトリックス榭脂から構成される繊維強化プラスチック (FRP)材が 好適に使用される。  [0034] Further, in the configuration in which the primary radiator 3 and the like are housed in the support member 7 in this way, the radio wave is radiated from the primary radiator 3 via the radio wave lens 2, or the primary radiator 3 When the electromagnetic wave is incident on the antenna, the radio wave passes through the support member 7. Accordingly, the support member 7 needs to have excellent radio wave permeability (that is, a characteristic that the phase change is small with little transmission loss). Further, the support member 7 needs to have strength (that is, load resistance) that can withstand the load of the radio wave lens 2. Therefore, in the present embodiment, in order to ensure excellent radio wave permeability and load resistance, the fiber reinforced plastic composed of a fiber reinforcing material and a matrix resin is used as a material constituting the support member 7. (FRP) material is preferably used.

[0035] この繊維強化プラスツチク材は、耐荷重性に優れて!/ヽるため、繊維強化プラスツチ ク材により形成された支持部材 7を使用することにより、電波レンズ 2を確実に支持す ることが可能になる。また、繊維強化プラスツチク材は、耐荷重性に優れているため、 繊維強化プラスツチク材により形成される支持部材 7の厚みを薄くすることができる。 更に、電波透過性に優れた (即ち、比誘電率が低ぐ誘電正接が低い)繊維強化材 やマトリックス榭脂を選択することにより、一次放射器 3から放射、または一次放射器 3 に入射される電波が支持部材 7を透過する際の、当該電波の透過損失、および位相 変化を効果的に抑制することができる。また、繊維強化プラスチック材は、耐熱性に 優れ、温度変化による寸法変化が小さいため、長期使用による、支持部材 7の変形 や破損を効果的に防止することができる。さらに、繊維強化プラスチック材は、加工性 に優れているため、支持部材 7の表面 7aを、電波レンズ 2の形状に合わせた球面形 状に加工し易くなり、支持部材 7の製造が容易になる。 [0035] Since this fiber-reinforced plastic material is excellent in load bearing performance !, it is possible to reliably support the radio wave lens 2 by using the support member 7 formed of the fiber-reinforced plastic material. Is possible. Further, since the fiber reinforced plastic material is excellent in load resistance, the thickness of the support member 7 formed of the fiber reinforced plastic material can be reduced. Furthermore, by selecting a fiber reinforcement or matrix resin that has excellent radio wave transmission (that is, low dielectric constant and low dielectric loss tangent), it is emitted from primary radiator 3 or incident on primary radiator 3. The transmission loss and phase change of the radio wave when the radio wave passes through the support member 7 can be effectively suppressed. In addition, since the fiber reinforced plastic material has excellent heat resistance and a small dimensional change due to a temperature change, the support member 7 can be effectively prevented from being deformed or damaged due to long-term use. In addition, fiber reinforced plastic materials are easy to process Therefore, the surface 7a of the support member 7 can be easily processed into a spherical shape matching the shape of the radio wave lens 2, and the manufacture of the support member 7 is facilitated.

[0036] 繊維強化プラスチック材の繊維強化材としては、例えば、ガラス繊維、ァラミド繊維 、およびナイロン繊維、ポリエチレン繊維、ポリテトラフルォロエチレン (PTFE)繊維 等が挙げられ、これらの繊維を単体もしくは組み合わせて使用することができる。この うち、繊維強化材として、ガラス繊維、ポリエチレン繊維、およびポリテトラフルォロェ チレン繊維を使用することにより、電波の透過損失をより一層効果的に抑制すること が可能になる。また、ガラス繊維のうち、石英(SiO )の純度が高い (例えば、純度が 9 [0036] Examples of the fiber reinforcing material of the fiber reinforced plastic material include glass fiber, aramid fiber, nylon fiber, polyethylene fiber, polytetrafluoroethylene (PTFE) fiber, and the like. Can be used in combination. Of these, the use of glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber as the fiber reinforcement makes it possible to more effectively suppress radio wave transmission loss. Of the glass fibers, quartz (SiO 2) has a high purity (for example, a purity of 9

2  2

9%)石英ガラス繊維や、上述のポリテトラフルォロエチレン繊維を使用することにより 、電波の透過損失を最小限まで抑制することができるため、特に好ましい。  9%) The use of quartz glass fiber or the above-mentioned polytetrafluoroethylene fiber is particularly preferable because transmission loss of radio waves can be minimized.

[0037] また、繊維強化プラスチック材のマトリックス榭脂としては、熱硬化性榭脂および熱 可塑性榭脂を用いることができる。熱硬化性榭脂としては、例えば、不飽和ポリエス テル榭脂、フエノール榭脂、エポキシ榭脂、およびビスマレイミド榭脂が挙げられる。 また、熱可塑性榭脂としては、例えば、ポリアミド榭脂、ポリイミド榭脂、ポリアミドイミド 榭脂、ポリエーテルイミド榭脂、およびポリエーテルスルホン榭脂等が挙げられる。な お、これらの榭脂を単体もしくは組み合わせて使用することができる。また、電波透過 性と耐荷重性を両立させるとの観点から、繊維強化プラスチック材により形成された 支持部材 7の厚みは、 lmm〜5mmが好ましい。  [0037] Further, as the matrix resin of the fiber reinforced plastic material, thermosetting resin and thermoplastic resin can be used. Examples of the thermosetting resin include unsaturated polyester resin, phenol resin, epoxy resin, and bismaleimide resin. Examples of the thermoplastic resin include polyamide resin, polyimide resin, polyamideimide resin, polyetherimide resin, and polyethersulfone resin. These rosins can be used alone or in combination. Further, from the viewpoint of achieving both radio wave permeability and load resistance, the thickness of the support member 7 formed of a fiber reinforced plastic material is preferably lmm to 5mm.

[0038] また、本実施形態にぉ 、ては、支持部材 7を形成する材料として、上述の繊維強化 プラスチック材の代わりに、合成樹脂を使用することができる。当該榭脂としては、熱 硬化性榭脂および熱可塑性榭脂を用いることができ、電波の透過損失、および位相 変化を効果的に抑制するとの観点から、ポリオレフイン系榭脂や、ポリスチレン系榭 脂、およびフッ素系榭脂が好適に使用できる。また、これらの榭脂は、上述の繊維強 化プラスツチク材と同様に、加工性に優れているため、支持部材 7の表面 7aを、電波 レンズ 2の形状に合わせた球面形状に加工し易くなり、支持部材 7の製造が容易にな る。ポリオレフイン系榭脂としては、例えば、ポリエチレン、ポリプロピレン、エチレン プロピレン共重合体、エチレンーブテン共重合体、およびプロピレンーブテン共重合 体等が挙げられる。また、ポリスチレン系榭脂としては、例えば、ポリスチレン、スチレ ンーアクリロニトリル共重合体、スチレン ブタジエン共重合体、スチレンーメタクリル 酸共重合体、スチレンーメタクリル酸メチル共重合体、およびスチレン アクリル酸共 重合体等が挙げられる。また、フッ素系榭脂としては、ポリテトラフルォロエチレン、テ トラフルォロエチレン一へキサフルォロプロピレン共重合体 (FEP)等が挙げられる。 [0038] Further, in the present embodiment, as a material for forming the support member 7, a synthetic resin can be used instead of the above-described fiber-reinforced plastic material. As the resin, thermosetting resin and thermoplastic resin can be used. From the viewpoint of effectively suppressing transmission loss of radio waves and phase change, polyolefin resin or polystyrene resin can be used. , And fluorinated resin can be suitably used. In addition, since these resins are excellent in workability like the above-described fiber-reinforced plastic material, it becomes easy to process the surface 7a of the support member 7 into a spherical shape that matches the shape of the radio wave lens 2. Thus, the support member 7 can be easily manufactured. Examples of the polyolefin resin include polyethylene, polypropylene, ethylene propylene copolymer, ethylene-butene copolymer, and propylene-butene copolymer. Examples of the polystyrene-based resin include polystyrene and styrene. N-acrylonitrile copolymer, styrene-butadiene copolymer, styrene-methacrylic acid copolymer, styrene-methyl methacrylate copolymer, and styrene-acrylic acid copolymer. In addition, examples of the fluorinated resin include polytetrafluoroethylene, tetrafluoroethylene monohexafluoropropylene copolymer (FEP), and the like.

[0039] 支持部材 7を形成する材料として、高発泡倍率を有する榭脂発砲体を使用すること もできる。電波透過性の観点から、電波レンズ 2と一次放射器 3の間は、誘電率が 1で ある空気のみが存在することが好ましい。従って、電波レンズ 2と一次放射器 3の間に 存在する支持部材 7を形成する材料の誘電率を、空気の誘電率に極めて近!ヽ誘電 率まで低下させるためには、高発泡倍率を有する発砲体を使用して、支持部材 7を 形成する必要がある。本実施形態においては、発泡倍率が 40以上の榭脂発泡体を 使用することにより、空気の誘電率に極めて近い誘電率を有する発砲体により、支持 部材 7を形成することができる。従って、上述の繊維強化プラスチック材として、ガラス 繊維、ポリエチレン繊維、およびポリテトラフルォロエチレン繊維を使用する場合と同 様に、電波が支持部材 7を透過する際の、当該電波の透過損失、および位相変化を より一層効果的に抑制することができる。  [0039] As a material for forming the support member 7, a resin foam having a high expansion ratio can also be used. From the viewpoint of radio wave transmission, it is preferable that only air having a dielectric constant of 1 exists between the radio wave lens 2 and the primary radiator 3. Therefore, in order to reduce the dielectric constant of the material forming the support member 7 existing between the radio wave lens 2 and the primary radiator 3 to a dielectric constant very close to that of air, it has a high expansion ratio. It is necessary to form the support member 7 using the foam. In this embodiment, the support member 7 can be formed of a foamed body having a dielectric constant very close to the dielectric constant of air by using a resin foam having an expansion ratio of 40 or more. Therefore, as in the case of using glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber as the fiber reinforced plastic material, the transmission loss of the radio wave when the radio wave passes through the support member 7, In addition, the phase change can be more effectively suppressed.

[0040] また、このような高発泡倍率を有する榭脂発泡体を形成する榭脂としては、例えば、 上述の、ポリオレフイン系榭脂や、ポリスチレン系榭脂、およびフッ素系榭脂が好適に 使用できる。また、電波透過性を向上させるとの観点から、高発泡倍率を有する発砲 体により形成された支持部材 7の厚みは、 10mn!〜 100mmが好ましい。  [0040] Further, as the resin forming the resin foam having such a high foaming ratio, for example, the above-mentioned polyolefin resin, polystyrene resin, and fluorine resin are preferably used. it can. In addition, from the viewpoint of improving radio wave transmission, the thickness of the support member 7 formed of a foam having a high expansion ratio is 10 mn! ~ 100mm is preferred.

[0041] また、図 1に示すように、風速レーダー 1は、電波レンズ 2、一次放射器 3、支持部材 7等を雨風や積雪力 保護するためのレドーム 8を備えており、電波レンズ 2、一次放 射器 3、支持部材 7等は、レドーム 8の内部に収納されている。また、レドーム 8は、優 れた電波透過性を有することが必要になるため、本実施形態では、優れた電波透過 性を確保するために、レドーム 8を構成する材料として、例えば、上述の繊維強化プ ラスチック (FRP)材が好適に使用される。なお、本実施形態の風速レーダー 1は、図 1に示すように、当該レドーム 8の下方には、後述の送信器 11、受信器 12等を収納し た制御部 9を備えている。  [0041] Further, as shown in FIG. 1, the wind speed radar 1 includes a radio lens 2, a primary radiator 3, a support member 7 and the like, and a radome 8 for protecting rain wind and snow accumulation force. The primary radiator 3, the support member 7, etc. are housed inside the radome 8. Further, since the radome 8 needs to have excellent radio wave transmissivity, in this embodiment, in order to ensure excellent radio wave transmissibility, as a material constituting the radome 8, for example, the above-described fiber A reinforced plastic (FRP) material is preferably used. As shown in FIG. 1, the wind speed radar 1 according to the present embodiment includes a control unit 9 that houses a transmitter 11, a receiver 12, and the like, which will be described later, below the radome 8.

[0042] 次に、風速レーダー 1による風速、風向の測定方法を、図 3を用いて説明する。図 3 に示す様に、風速レーダー 1の制御部 9は、高周波信号を生成する発振器 10と、当 該発振器 10に接続され、発振器 10により生成された高周波信号を増幅する送信器 11と、反射、または後方散乱されて戻ってきた微弱な高周波電波の信号を増幅する 受信器 12を備えている。また、制御部 9は、送信器 11、受信器 12、および一次放射 器 3に接続され、送受信される信号の切り替えを行う切替器 13を備えており、一次放 射器 3(即ち、複数の一次放射器 3Z、 3N、 3S、 3E、および 3Wの各々)は、切替器 1 3を介して、送信器 11、受信器 12に接続される構成となっている。また、制御部 9は、 受信器 12に接続され、当該受信器 12により受信された信号を検出する信号検出器 14と、信号検出器 14に接続され、当該信号検出器 14により検出された信号を処理 して、大気層 Tの風速、風向の情報を演算する信号処理器 15を備えている。 Next, a method for measuring the wind speed and the wind direction by the wind speed radar 1 will be described with reference to FIG. Fig 3 As shown in FIG. 3, the control unit 9 of the wind radar 1 includes an oscillator 10 that generates a high-frequency signal, a transmitter 11 that is connected to the oscillator 10 and amplifies the high-frequency signal generated by the oscillator 10, and reflects or It has a receiver 12 that amplifies the weak high-frequency radio signal that has been scattered back and returned. The control unit 9 includes a switch 13 that is connected to the transmitter 11, the receiver 12, and the primary radiator 3 and performs switching of signals to be transmitted and received, and the primary radiator 3 (that is, a plurality of transmitters 11). Each of the primary radiators 3Z, 3N, 3S, 3E, and 3W) is connected to the transmitter 11 and the receiver 12 via the switch 13. The control unit 9 is connected to the receiver 12 and detects a signal received by the receiver 12, and the signal detected by the signal detector 14 is connected to the signal detector 14. And a signal processor 15 for calculating the wind speed and direction information of the atmospheric layer T.

[0043] また、制御部 9は、制御手段としてのコンピュータ 16を備えており、レーダー装置制 御プログラムを起動することにより、発振器 10、送信器 11、受信器 12、切替器 13、 信号検出器 14、および信号処理器 15の制御を行う。  [0043] Further, the control unit 9 includes a computer 16 as control means, and by starting a radar device control program, an oscillator 10, a transmitter 11, a receiver 12, a switch 13, a signal detector 14 and the signal processor 15 are controlled.

[0044] 以上の構成の下、風速、風向の観測を行う際には、まず、発振器 10により、所定の 高周波信号が生成され、当該高周波信号が送信器 11に送り出される。次いで、高周 波信号が、送信器 11により増幅されて、複数の一次放射器 3Z、 3N、 3S、 3E、およ び 3Wの各々に送り出される。そして、増幅された高周波信号が、高周波電波 20とし て、一次放射器 3Z、 3N、 3S、 3E、および 3Wの各々力 電波レンズ 2を経由して、 空間における、上述の、観測すべき所望の複数の方位角方向へ向けて放射される。 次いで、上空の大気層 Tで反射され、各方位角方向から戻ってくる微弱な高周波電 波 21を、電波レンズ 2で焦点位置に集めて、電波レンズ 2を経由して、複数の一次放 射器 3Z、 3N、 3S、 3E、および 3Wの各々で受ける。  In the above configuration, when the wind speed and the wind direction are observed, first, a predetermined high frequency signal is generated by the oscillator 10, and the high frequency signal is sent to the transmitter 11. Next, the high frequency signal is amplified by the transmitter 11 and sent to each of the plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W. Then, the amplified high-frequency signal is converted into a desired high frequency radio wave 20 via the primary radiators 3Z, 3N, 3S, 3E, and 3W, respectively, the radio wave lens 2, and the above-described desired observation to be observed in space. Radiated in multiple azimuth directions. Next, the weak high-frequency radio waves 21 reflected from the atmospheric layer T in the sky and returning from each azimuth angle direction are collected at the focal position by the radio lens 2, and a plurality of primary radiations are transmitted through the radio lens 2. Received in each of 3Z, 3N, 3S, 3E, and 3W.

[0045] この際、本実施形態においては、上述のごとぐ観測すべき複数の方位角方向、例 えば、天頂、及び東西南北と天頂角 Θをなす方位角方向に電波レンズ 2を介して送 受信される電波の焦点位置に対応して、一次放射器 3Z、 3N、 3S、 3E、および 3W が配設されている。従って、各々の焦点位置に配設された一次放射器 3Z、 3N、 3S 、 3E、および 3Wから電波を送信すれば、各焦点位置の一次放射器 3Z、 3N、 3S、 3 E、および 3Wへ、直ちに反射された電波が戻り、所定の方位角方向の電波信号を得 ることができる。従って、複数の方位角方向に同時に電波を送受信することが可能に なるため、収集されるデータの同時性の向上を図ることができる。また、データ収集時 間の短縮ィ匕を図ることができる。 At this time, in the present embodiment, the plurality of azimuth angles to be observed as described above, for example, the zenith and the azimuth angle that forms the zenith angle Θ with east-west north-south are sent via the radio wave lens 2. Primary radiators 3Z, 3N, 3S, 3E, and 3W are arranged corresponding to the focal position of the received radio wave. Therefore, if radio waves are transmitted from the primary radiators 3Z, 3N, 3S, 3E, and 3W arranged at the respective focal positions, the primary radiators 3Z, 3N, 3S, 3E, and 3W at the respective focal positions are transmitted. The reflected radio wave returns immediately and the radio signal in the specified azimuth direction is obtained. Can. Therefore, it becomes possible to simultaneously transmit and receive radio waves in a plurality of azimuth directions, so that the simultaneity of collected data can be improved. In addition, it is possible to shorten the data collection time.

[0046] そして、一次放射器 3Z、 3N、 3S、 3E、および 3Wの各々で受けた電波の信号が、 切替器 13により切り替えられた受信器 12に送り出される。次いで、受信器 12におい て、高周波信号が増幅されて、信号検出器 14を経由して信号処理器 15に送り出さ れ、当該信号処理器 15により、信号検出器 14により検出された信号を処理して、大 気層 Tの風速、風向の情報が得られる構成となっている。  [0046] Then, radio wave signals received by each of primary radiators 3Z, 3N, 3S, 3E, and 3W are sent to receiver 12 switched by switch 13. Next, the receiver 12 amplifies the high-frequency signal and sends it to the signal processor 15 via the signal detector 14. The signal processor 15 processes the signal detected by the signal detector 14. Thus, the information on the wind speed and direction of the atmosphere T can be obtained.

[0047] なお、送信器 11、および受信器 12は、複数の一次放射器 3Z、 3N、 3S、 3E、およ び 3Wの各々に対応させて、複数個(即ち、 5個の送信器 11と、 5個の受信器 12)を 設ける構成としても良い。また、送信器 11、および受信器 12を、複数の一次放射器 3 Z、 3N、 3S、 3E、および 3Wに対して 1組のみ(即ち、 1個の送信器 11と、 1個の受信 器 12)設け、切替器 13を制御することにより、複数の一次放射器 3Z、 3N、 3S、 3E、 および 3Wの中から、電波を放射する(または、電波が入射される)一次放射器を選 択する構成としても良い。  [0047] It should be noted that there are a plurality of transmitters 11 and receivers 12 corresponding to each of the plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W (that is, five transmitters 11). A configuration in which five receivers 12) are provided. Also, only one set of transmitter 11 and receiver 12 for multiple primary radiators 3 Z, 3N, 3S, 3E, and 3W (ie, one transmitter 11 and one receiver). 12) By installing and controlling the switch 13, the primary radiator that emits radio waves (or radio waves are incident) is selected from the multiple primary radiators 3Z, 3N, 3S, 3E, and 3W. A configuration may be selected.

[0048] また、本実施形態における風速レーダー 1においては、風速レーダー 1から放射さ れた電波の一部が、大気の乱流により散乱されるとともに、気流の速度によるドッブラ 効果で周波数シフトが生じ、これを観測することにより、大気層 Tの風速、風向の情報 を観測する。  [0048] Further, in the wind speed radar 1 in the present embodiment, a part of the radio wave radiated from the wind speed radar 1 is scattered by the turbulent air flow, and a frequency shift occurs due to the Doppler effect due to the velocity of the air flow. By observing this, information on the wind speed and direction of the atmospheric layer T is observed.

[0049] 即ち、例えば、図 3に示すように、南方向 Sに対し、所定の天頂角 Θをなす方位角 方向に向けて、一次放射器 3Sから、電波レンズ 2を経由して、パルス状の電波が放 射されると、この電波は上空で大気の乱れほ L流)に伴う屈折率の揺らぎにより、僅か ではあるが散乱され、高度に対応する時間遅延を伴って電波レンズ 2へ戻ってくる。 従って、散乱波強度を時間の関数として測定することにより、高度別に風速、風向の データを得ることができ、このような測定は、受信器 12で受信した電波の信号を、上 述の制御部 9において演算することにより得られる。  That is, for example, as shown in FIG. 3, a pulse-like shape is transmitted from the primary radiator 3S via the radio wave lens 2 toward the azimuth angle direction that forms a predetermined zenith angle Θ with respect to the south direction S. When the radio wave is radiated, the radio wave is scattered slightly due to the refractive index fluctuation accompanying the atmospheric turbulence in the sky), and returns to the radio wave lens 2 with a time delay corresponding to the altitude. Come. Therefore, by measuring the scattered wave intensity as a function of time, it is possible to obtain wind speed and direction data at different altitudes. Such a measurement can be performed using the radio wave signal received by the receiver 12 as described above. It is obtained by calculating in 9.

[0050] また、本実施形態においては、この測定を行う際に、上述のごとぐ球形状のルーネ ベルグレンズを電波レンズ 2として使用する。従って、電波の減衰率が小さぐ微弱な 電波であっても十分に検出することができる。また、強度が高ぐかつ風圧も受け難い 電波レンズ 2を提供することが可能になる。従って、台風の襲来など、強風にさらされ る地域に設置される場合においても、耐風性に優れた風速レーダー 1を提供すること ができる。 In this embodiment, the spherical Luneberg lens described above is used as the radio wave lens 2 when performing this measurement. Therefore, the attenuation rate of radio waves is small and weak. Even radio waves can be sufficiently detected. In addition, it is possible to provide the radio wave lens 2 that has high strength and is less susceptible to wind pressure. Therefore, even when installed in an area exposed to strong winds, such as a typhoon, it is possible to provide a wind speed radar 1 with excellent wind resistance.

[0051] また、本実施形態の風速レーダー 1においては、上述のフェーズドアレイ方式のァ ンテナとは異なり、一次放射器 3には移相器を接続する必要がなぐまた、多数の素 子アンテナを必要としない。従って、装置の小型軽量化、及び構造の簡素化を図るこ とができ、また、回路、部品、ケーブル等を極力減少させることができるため、低コスト 化を図ることが可能になる。  [0051] Also, in the wind speed radar 1 of the present embodiment, unlike the phased array antenna described above, it is not necessary to connect a phase shifter to the primary radiator 3, and a large number of element antennas are used. do not need. Therefore, it is possible to reduce the size and weight of the device and simplify the structure, and to reduce the number of circuits, components, cables, and the like as much as possible, thereby reducing the cost.

[0052] 次に、上述の制御部 9における演算について、図 3を参照して説明する。上空の大 気層 Tでの乱流は、大気の乱れ (即ち、風) Kに乗って移動するため、散乱された電 波は、ドッブラ効果により、図 3に示す、散乱点 Aにおける風速 Vに比例した周波数変 位 (即ち、ドッブラシフト) Δ ίを受ける。そして、このドッブラシフト Δ ίと、視線方向風速 (風速の電波放射方向成分) Vrの間には、放射電波の周波数を f、光速を cとすると、 次の(式 1)が成立する。  Next, the calculation in the control unit 9 will be described with reference to FIG. Since the turbulent flow in the upper atmospheric layer T moves on atmospheric turbulence (i.e., wind) K, the scattered wave is caused by the Doppler effect, and the wind speed V at the scattering point A shown in Fig. 3 Is subject to a frequency shift proportional to (ie, Doppler shift) Δ ί. The following (Equation 1) is established between the Doppler shift Δ ί and the line-of-sight wind speed (radio wave radiation direction component) Vr, where f is the frequency of the radiated radio wave and c is the speed of light.

[0053] [数 1]  [0053] [Equation 1]

△ f - - 1 } · · · (式 1 )△ f--1} (Equation 1)

Figure imgf000016_0001
Figure imgf000016_0001

[0054] また、上記 (式 1)において、視線方向風速 Vrは、光速 cに比べると無視できる程小 さいため、上記 (式 1)を展開して、 2次の項以下を無視すると、次の(式 2)を得る。 [0054] In the above (Expression 1), the line-of-sight wind speed Vr is negligibly small compared to the light speed c. Therefore, if the above (Expression 1) is expanded and the second order terms and below are ignored, (Equation 2) is obtained.

[0055] [数 2] [0055] [Equation 2]

V r =c -^— …(式 2) V r = c-^ —… (Formula 2)

[0056] そして、一次放射器 3から放射される電波の方位を、天頂方向 Zに向けた場合、(式 2)より、風速 Vの鉛直成分 Vzを求めることができる。次に、電波の方位を、天頂方向 Zに対して、角度士 Θだけ傾いた方向に変更して、それらの視線方向風速 Vr ( Θ )を 測定することにより、風速 Vの水平成分 Vhを、次の(式 3)より求める。なお、この場合 、電波の測定範囲内における風 Kは、一様であると仮定する。 [0056] Then, when the direction of the radio wave radiated from the primary radiator 3 is directed to the zenith direction Z, (formula From 2), the vertical component Vz of the wind speed V can be obtained. Next, the horizontal component Vh of the wind speed V is changed by changing the direction of the radio wave to a direction inclined by an angle of Θ with respect to the zenith direction Z and measuring the line-of-sight wind speed Vr (Θ). Calculate from the following (Equation 3). In this case, the wind K within the radio wave measurement range is assumed to be uniform.

[0057] [数 3]  [0057] [Equation 3]

V「 (Θ) -V r (-Θ) V '(Θ) -V r (-Θ)

Vh = (式 3) Vh = (Equation 3)

Figure imgf000017_0001
Figure imgf000017_0001

[0058] なお、上記 (式 3)において、 0と 0は、例えば、東と西 (または、北と南)に対応し ている。以上より、各高度における風速、および風向の高度分布を得ることができる。 このように、本実施形態の風速レーダー 1は、地表力 の電波により大気層での風向 、風速分布等を、レンズアンテナを利用して簡易に、かつ正確に測定できるものであ り、大気運動の観測に広く利用することができる。 [0058] In the above (Formula 3), 0 and 0 correspond to, for example, east and west (or north and south). As described above, the wind speed and the altitude distribution of the wind direction at each altitude can be obtained. As described above, the wind speed radar 1 of the present embodiment can easily and accurately measure the wind direction, wind speed distribution, etc. in the atmospheric layer by using the surface force radio wave, using the lens antenna. It can be widely used for observation.

[0059] 以上に説明した本実施形態によれば、以下の効果を得ることができる。  [0059] According to the present embodiment described above, the following effects can be obtained.

[0060] (1)本実施形態の風速レーダー 1は、誘電体を用いて比誘電率が半径方向に所定 の割合で変化するように形成された球形状の電波レンズ 2と、当該電波レンズ 2を支 持する支持部材 7を備えている。そして、電波レンズ 2が載置される支持部材 7の表 面 7aが、電波レンズ 2の形状に合わせた球面形状を有している。従って、支持部材 7 の表面 7aにおいて、電波レンズ 2の荷重を均等に分散させることが可能になるため、 重量の大き 、ルーネベルグレンズを使用する場合であっても、当該ルーネベルグレ ンズの変形、または破損を効果的に防止することができる。その結果、電波レンズ 2を 備える風速レーダー 1にお 、て、電波レンズ 2を適切に支持することが可能になる。  (1) The wind radar 1 of the present embodiment includes a spherical radio wave lens 2 formed using a dielectric so that the relative permittivity changes in a predetermined ratio in the radial direction, and the radio wave lens 2 A support member 7 is provided. The surface 7 a of the support member 7 on which the radio wave lens 2 is placed has a spherical shape that matches the shape of the radio wave lens 2. Therefore, since the load of the radio wave lens 2 can be evenly distributed on the surface 7a of the support member 7, even when a large weight, a Luneberg lens is used, deformation of the Luneberg lens, or Damage can be effectively prevented. As a result, it is possible to appropriately support the radio wave lens 2 in the wind speed radar 1 including the radio wave lens 2.

[0061] (2)本実施形態においては、支持部材 7に、一次放射器 3を収納するための収納 部 17が形成されている。従って、支持部材 7により、電波レンズ 2を適切に支持した 状態で、一次放射器 3を電波レンズ 2の焦点位置に容易に配置することができる。  (2) In the present embodiment, the support member 7 is formed with a storage portion 17 for storing the primary radiator 3. Therefore, the primary radiator 3 can be easily placed at the focal position of the radio wave lens 2 while the radio wave lens 2 is appropriately supported by the support member 7.

[0062] (3)本実施形態にぉ ヽては、支持部材 7を、耐荷重性に優れた繊維強化プラスチッ ク材により形成する構成としている。従って、支持部材 7により、電波レンズ 2を確実に 支持することが可能になる。また、支持部材 7の厚みを薄くすることができるため、一 次放射器 3から放射、または一次放射器 3に入射される電波が支持部材 7を透過す る際の、当該電波の透過損失、および位相変化を効果的に抑制することができる。ま た、繊維強化プラスチック材は、耐熱性に優れ、温度変化による寸法変化が小さいた め、支持部材 7の変形や破損を効果的に防止することができる。さらに、繊維強化プ ラスチック材は、加工性に優れているため、支持部材 7の製造が容易になる。 (3) For the present embodiment, the support member 7 is formed of a fiber reinforced plastic material having excellent load resistance. Therefore, the radio wave lens 2 is securely attached by the support member 7. It becomes possible to support. Further, since the thickness of the support member 7 can be reduced, the transmission loss of the radio wave when the radio wave radiated from the primary radiator 3 or the radio wave incident on the primary radiator 3 passes through the support member 7, And a phase change can be suppressed effectively. Further, since the fiber reinforced plastic material has excellent heat resistance and a small dimensional change due to a temperature change, the support member 7 can be effectively prevented from being deformed or damaged. Furthermore, since the fiber-reinforced plastic material is excellent in processability, the support member 7 can be easily manufactured.

[0063] (4)本実施形態においては、支持部材 7を形成する繊維強化プラスチック材の繊維 強化材として、ガラス繊維、ポリエチレン繊維、および PTFE繊維を使用する構成とし ている。従って、支持部材 7における電波の透過損失をより一層効果的に抑制するこ とが可能になる。 [0063] (4) In the present embodiment, glass fiber, polyethylene fiber, and PTFE fiber are used as the fiber reinforcing material of the fiber reinforced plastic material forming the support member 7. Therefore, it is possible to more effectively suppress the transmission loss of radio waves in the support member 7.

[0064] (5)本実施形態においては、支持部材 7を、ポリオレフイン系榭脂、ポリスチレン系 榭脂、およびフッ素系榭脂により形成する構成としている。従って、一次放射器 3から 放射、または一次放射器 3に入射される電波が支持部材 7を透過する際の、当該電 波の透過損失、および位相変化を効果的に抑制することができる。さらに、これらの 榭脂は、加工性に優れているため、支持部材 7の製造が容易になる。  [0064] (5) In the present embodiment, the support member 7 is formed of a polyolefin resin, a polystyrene resin, and a fluorine resin. Therefore, it is possible to effectively suppress transmission loss and phase change of the radio wave when the radio wave emitted from the primary radiator 3 or the radio wave incident on the primary radiator 3 passes through the support member 7. Furthermore, since these resins have excellent processability, the support member 7 can be easily manufactured.

[0065] (6)本実施形態にぉ 、ては、支持部材を、発泡倍率が 40以上である榭脂発泡体 により形成する構成としている。従って、支持部材 7における電波の透過損失をより一 層効果的に抑制することが可能になる。  [0065] (6) In this embodiment, the support member is formed of a resin foam having an expansion ratio of 40 or more. Therefore, it is possible to more effectively suppress the transmission loss of radio waves in the support member 7.

[0066] なお、上記実施形態は以下のように変更しても良い。  [0066] The embodiment described above may be modified as follows.

[0067] 上記実施形態においては、複数の方位角方向に送受信される電波の焦点位置に 対応して、複数の一次放射器 3Z、 3N、 3S、 3E、および 3Wを配設する構成としたが 、複数の方位角方向に送受信される電波の焦点位置に対応するように、 1個の一次 放射器 3を移動自在に配設する構成としてもよい。より具体的には、図 4、図 5に示す ように、風速レーダー 50において、支持レール 5、 6を、互いに直交して設けるととも に、例えば、支持レール 5を南北方向に、支持レール 6を東西方向に向けて設置する 。そして、 1個の一次放射器 3を、支持レール 5、 6上を、図中の矢印の方向に移動自 在に設けて、天頂方向、及び北、南、東、西の各方位に対し、所定の天頂角 Θをな す方位角方向に送受信される電波の焦点位置に停止させ、各停止位置で、風速、 風向のデータを測定する。なお、風速、風向のデータの測定方法は、上述の実施形 態と同様である。このような構成により、 1個の一次放射器 3により、風速、風向のデー タを測定することができるため、コストアップを抑制することができる。 [0067] In the above embodiment, a plurality of primary radiators 3Z, 3N, 3S, 3E, and 3W are arranged corresponding to the focal positions of radio waves transmitted and received in a plurality of azimuth directions. The primary radiator 3 may be movably disposed so as to correspond to the focal positions of radio waves transmitted and received in a plurality of azimuth directions. More specifically, as shown in FIGS. 4 and 5, in the wind speed radar 50, the support rails 5 and 6 are provided orthogonal to each other, and for example, the support rail 5 is arranged in the north-south direction. Is installed in the east-west direction. Then, one primary radiator 3 is installed on the support rails 5 and 6 in the direction of the arrow in the figure, and the zenith direction and the north, south, east, and west directions are Stop at the focal position of the radio wave transmitted and received in the azimuth direction that forms the specified zenith angle Θ, and at each stop position, wind speed, Measure wind direction data. Note that the method for measuring the wind speed and direction data is the same as in the above embodiment. With such a configuration, it is possible to measure wind speed and wind direction data with one primary radiator 3, thereby suppressing an increase in cost.

[0068] また、図 6に示すように、風速レーダー 51において、一次放射器 3を支持する支持 レール 30を一方位方向にのみ延設するとともに、支持レール 30が支持される軸部 4 を回転自在に設ける構成としても良い。この場合、天頂方向 Zに送受信される電波の 焦点位置に、一次放射器 3Zを固定して配設するとともに 1個の一次放射器 3を、支 持レール 30上を移動自在に設ける。そして、当該一次放射器 3を、北、南、東、西の 各方位に対し、所定の天頂角 Θをなす方位角方向に送受信される電波の焦点位置 に停止させ、各停止位置で、風速、風向のデータを測定する。  Further, as shown in FIG. 6, in the wind speed radar 51, the support rail 30 that supports the primary radiator 3 is extended only in one direction, and the shaft portion 4 that supports the support rail 30 is rotated. It is good also as a structure provided freely. In this case, the primary radiator 3Z is fixedly disposed at the focal position of the radio wave transmitted and received in the zenith direction Z, and one primary radiator 3 is movably provided on the support rail 30. Then, the primary radiator 3 is stopped at the focal position of the radio wave transmitted and received in the azimuth angle direction that forms a predetermined zenith angle Θ with respect to the north, south, east, and west directions. Measure wind direction data.

[0069] また、図 7に示す風速レーダー 52のように、図 6に示した風速レーダー 51において 、天頂方向 Zに送受信される電波の焦点位置に配設された一次放射器 3Zを省略し、 1個の一次放射器 3のみを、支持レール 30上を移動自在に設ける構成としても良!ヽ 。この場合、当該一次放射器 3を、天頂方向、及び北、南、東、西の各方位に対し、 所定の天頂角 Θをなす方位角方向に送受信される電波の焦点位置に停止させ、各 停止位置で、風速、風向のデータを測定する。  [0069] In the wind speed radar 51 shown in FIG. 6, like the wind speed radar 52 shown in FIG. 7, the primary radiator 3Z disposed at the focal position of the radio wave transmitted and received in the zenith direction Z is omitted. A configuration in which only one primary radiator 3 is movably provided on the support rail 30 is also possible. In this case, the primary radiator 3 is stopped at the focal position of the radio wave transmitted and received in the zenith direction and the azimuth angle direction that forms the predetermined zenith angle Θ with respect to the north, south, east, and west directions. Measure wind speed and direction data at the stop position.

[0070] また、支持部材 7を形成する材料は、上述した電波透過性、耐荷重性、および加工 性を有するものであれば、他の材料を使用することができる。例えば、セラミック材料 や、木材等を、支持部材 7を形成する材料として使用することができる。  [0070] As the material for forming the support member 7, other materials can be used as long as they have the above-described radio wave permeability, load resistance, and workability. For example, a ceramic material, wood, or the like can be used as a material for forming the support member 7.

[0071] また、風速レーダー 1を複数個、並べて使用することができる。より具体的には、例 えば、図 8 (a)に示すように、 4個の風速レーダー 1を配列することができ、図 8 (b)に 示すように、 7個の風速レーダーを配列することができる。また、図 8 (c)に示すように 、 13個の風速レーダー 1を配列することができる。このような構成により、電波レンズ 2 の物理的な面積を大きくすることができるため、アンテナ利得と送信電力を向上させ ることが可能になる。その結果、レーダーの性能 (例えば、観測高度)を向上させるこ とが可能になる。なお、この場合、図 3において説明した、発振器 10、信号検出器 14 、および信号処理器 15等は、複数の風速レーダー 1の各々に対して設けてもよぐま た、複数の風速レーダー 1の全体に対して、発振器 10、信号検出器 14、および信号 処理器 15等を 1個のみ設ける構成としてもょ 、。 [0071] Further, a plurality of wind speed radars 1 can be used side by side. More specifically, for example, as shown in FIG. 8 (a), four wind speed radars 1 can be arranged, and as shown in FIG. 8 (b), seven wind speed radars are arranged. be able to. Further, as shown in FIG. 8 (c), 13 wind speed radars 1 can be arranged. With such a configuration, the physical area of the radio wave lens 2 can be increased, so that the antenna gain and transmission power can be improved. As a result, the radar performance (for example, observation altitude) can be improved. In this case, the oscillator 10, the signal detector 14, the signal processor 15 and the like described in FIG. 3 may be provided for each of the plurality of wind radars 1. Overall, oscillator 10, signal detector 14, and signal Even if only one processor 15 etc. is installed.

産業上の利用可能性 Industrial applicability

本発明の活用例としては、レンズアンテナを介して信号を送、受信し、大気層での 風向、風速分布等を測定する風速レーダーが挙げられる。  As an application example of the present invention, there is a wind speed radar that transmits and receives a signal via a lens antenna and measures a wind direction, a wind speed distribution and the like in the atmosphere layer.

Claims

請求の範囲 The scope of the claims [1] 誘電体を用いて比誘電率が半径方向に所定の割合で変化するように形成された球 形状の送受信用の電波レンズと、  [1] A spherical transmission / reception radio wave lens formed using a dielectric so that the relative permittivity changes at a predetermined rate in the radial direction; 前記電波レンズの外周に沿って、観測すべき複数の方位角方向に前記電波レンズ を介して送受信される電波の焦点位置に配設される送受信用の一次放射器と、 前記電波レンズを支持する支持部材と、を備え、  A primary radiator for transmission / reception disposed at a focal position of a radio wave transmitted / received via the radio wave lens in a plurality of azimuth directions to be observed along an outer periphery of the radio wave lens, and supporting the radio wave lens A support member, 前記電波レンズが載置される前記支持部材の表面が、前記電波レンズの形状に合 わせた球面形状を有することを特徴とする風速レーダー。  A wind speed radar, wherein a surface of the support member on which the radio wave lens is mounted has a spherical shape that matches the shape of the radio wave lens. [2] 前記支持部材には、前記一次放射器を収納するための収納部が形成されているこ とを特徴とする請求の範囲 1に記載の風速レーダー。  [2] The wind radar according to claim 1, wherein the support member is formed with a storage portion for storing the primary radiator. [3] 前記支持部材が、繊維強化プラスチック材により形成されて 、ることを特徴とする請 求の範囲 2に記載の風速レーダー。 [3] The wind speed radar according to claim 2, wherein the support member is made of a fiber reinforced plastic material. [4] 前記繊維強化プラスチック材の繊維強化材が、ガラス繊維、ポリエチレン繊維、およ びポリテトラフルォロエチレン繊維力もなる群より選ばれる少なくとも 1種であることを 特徴とする請求の範囲 3に記載の風速レーダー。 [4] The fiber reinforcing material of the fiber reinforced plastic material is at least one selected from the group consisting of glass fiber, polyethylene fiber, and polytetrafluoroethylene fiber strength. The wind speed radar described in 1. [5] 前記支持部材が、ポリオレフイン系榭脂、ポリスチレン系榭脂、およびフッ素系榭脂 力 なる群より選ばれる少なくとも 1種により形成されていることを特徴とする請求の範 囲 2に記載の風速レーダー。 [5] The support member according to claim 2, wherein the support member is formed of at least one selected from the group consisting of polyolefin resin, polystyrene resin, and fluorine resin. Wind speed radar. [6] 前記支持部材が、発泡倍率が 40以上である榭脂発泡体により形成されて ヽること を特徴とする請求の範囲 5に記載の風速レーダー。 6. The wind speed radar according to claim 5, wherein the support member is made of a resin foam having an expansion ratio of 40 or more.
PCT/JP2006/315488 2006-08-04 2006-08-04 Wind speed radar Ceased WO2008015757A1 (en)

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PCT/JP2006/315488 WO2008015757A1 (en) 2006-08-04 2006-08-04 Wind speed radar
JP2008527628A JP4935816B2 (en) 2006-08-04 2006-08-04 Wind speed radar
CNA2006800550043A CN101467066A (en) 2006-08-04 2006-08-04 Wind speed radar
TW096102588A TWI387776B (en) 2006-08-04 2007-01-24 Meteorological radar

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US10224636B2 (en) 2015-08-05 2019-03-05 Matsing Inc. Spherical lens array based multi-beam antennae
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JP2012058193A (en) * 2010-09-13 2012-03-22 Sonic Corp Phased array type doppler sodar system
US10224636B2 (en) 2015-08-05 2019-03-05 Matsing Inc. Spherical lens array based multi-beam antennae
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CN101467066A (en) 2009-06-24
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KR101283257B1 (en) 2013-07-11
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