JPS62879A - Electric wave and optical system composite seeker - Google Patents

Electric wave and optical system composite seeker

Info

Publication number
JPS62879A
JPS62879A JP13907785A JP13907785A JPS62879A JP S62879 A JPS62879 A JP S62879A JP 13907785 A JP13907785 A JP 13907785A JP 13907785 A JP13907785 A JP 13907785A JP S62879 A JPS62879 A JP S62879A
Authority
JP
Japan
Prior art keywords
antenna elements
seeker
optical system
radio wave
electric wave
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP13907785A
Other languages
Japanese (ja)
Other versions
JPH077050B2 (en
Inventor
Osami Yoshizawa
吉沢 修身
Yoshihiro Yano
義弘 矢野
Tadashi Adachi
忠司 足立
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Japan Steel Works Ltd
Nissan Motor Co Ltd
Technical Research and Development Institute of Japan Defence Agency
Original Assignee
Japan Steel Works Ltd
Nissan Motor Co Ltd
Technical Research and Development Institute of Japan Defence Agency
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 Japan Steel Works Ltd, Nissan Motor Co Ltd, Technical Research and Development Institute of Japan Defence Agency filed Critical Japan Steel Works Ltd
Priority to JP13907785A priority Critical patent/JPH077050B2/en
Publication of JPS62879A publication Critical patent/JPS62879A/en
Publication of JPH077050B2 publication Critical patent/JPH077050B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Aerials With Secondary Devices (AREA)
  • Radar Systems Or Details Thereof (AREA)
  • Aiming, Guidance, Guns With A Light Source, Armor, Camouflage, And Targets (AREA)

Abstract

PURPOSE:To store antenna elements in an airframe by forming the reflection path of an electric wave by utilizing a light convergence path characteristic to an optical system seeker. CONSTITUTION:An infrared-light detector 43 equipped with a primary reflector 41, a secondary reflector 42, a reticle 44, a condenser lens 45, and an infrared- light detector 46 is united to constitute a gyro optical system. Two couples of antenna elements 31 of an electric wave system seeker 30, on the other hand, have their base ends arranged at the peripheral edge part of a luminous flux area and are united with the gyro optical system to constitute the horn antenna of a monopulse system. The reflection path of infrared light reaching the peripheral edge pat becomes the reflection path of the electric wave, so a radiation zone Z corresponding to respective antenna elements 31 is formed from the peripheral part of the primary reflector 41 and when the radio wave from a target crosses the zone Z, each couple of antenna elements 31 have a gain difference according to the azimuth angle and elevation or depression angle of the radio wave. Thus, the radio wave is transmitted or received as well as a system which have antenna elements arranged at the periphery of the head of the airframe.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電波系シーカと光学系シーカとを兼備する複
合シーカ、特に機体回転式ミサイル等のホーミングシス
テムに用いられる複合シーカに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a composite seeker that has both a radio wave seeker and an optical seeker, and particularly relates to a composite seeker used in a homing system for a rotating body missile or the like.

〔従来の技術〕[Conventional technology]

複合シーカは、目標から発せられる。あるいは反射され
る電波および光(赤外光)を探知しながら、当該ミサイ
ル等を主に電波系シーカを用いて債幣ロm表裡hl−z
−^1Cノ毒−ラ1ご片書  を爪後、主に光学系シー
カを用いて追尾させるものであって、前記機体回転1式
ミサイルは例えばAviation Week & 5
pace Technology (1978年12月
11日刊行)にRamミサイルとして紹介されており、
また電波系シーカおよび光学系シーカの概要が誘導武器
概論(昭和56年11月25日、防衛技術協会発行)に
説明されている。
A compound seeker emanates from the target. Alternatively, while detecting reflected radio waves and light (infrared light), the missile, etc. can be detected using a radio wave seeker.
-^1C no Poison - La 1 Notes The system mainly uses an optical seeker to track the aircraft, and the aircraft rotation type 1 missile is, for example, Aviation Week & 5.
It was introduced as a Ram missile in pace Technology (published December 11, 1978).
Additionally, an overview of radio wave seekers and optical seekers is explained in Introduction to Guided Weapons (November 25, 1980, published by the Defense Technology Association).

第2図は上記R五iミ・サイルにおける複合シーカを略
示したもので、1は・ミ゛サイルの機体、2は機体頭部
のレドーム、10は電波系シーカ、20は光学系シーカ
であって、該ミサイルは例えば30RPM程度でローリ
ングをしつつ飛翔する。
Figure 2 schematically shows the composite seeker in the R5i missile, where 1 is the missile body, 2 is the radome on the head of the aircraft, 10 is the radio seeker, and 20 is the optical seeker. Therefore, the missile flies while rolling at, for example, about 30 RPM.

電波系シーカlOにおいて、11は機体の頭部周辺から
前方へ突出させた1対(2本)あるいは2対(4本)の
アンテナ素子で、これらのアンテナ素子を用いてモノパ
ルスアンテナを構成している。12は加算器、13はミ
キサ、14は検波増巾器で、いま目標からの電波が機体
の座標系に対して成る方位角および上下角をもって前記
アンテナのラジエーシ厘ンゾーン21に入射すると、対
をなすアンテナ素子11にゲイン差が生じる。加算器1
2はこのゲイン差の発生状態(ディファレンシャルモー
ド)にもとづいて方位差ΔX、上下差Δyおよび和Σを
刻々と算出する。ミキサ13はこの算出値とジャイロか
らの姿勢運動信号とを要素として方位角誤差と上下角誤
差とを演算する。検波増巾器14はこの演算結果を処理
して方位角誤差信号δX′および上下角誤差信号δy′
を発信し、位相検波器15へ入力する。
In the radio seeker IO, 11 is one pair (two) or two pairs (four) of antenna elements protruding forward from around the head of the aircraft, and these antenna elements are used to configure a monopulse antenna. There is. 12 is an adder, 13 is a mixer, and 14 is a detection amplifier. When a radio wave from a target enters the radiation zone 21 of the antenna at an azimuth angle and an up/down angle relative to the coordinate system of the aircraft, the pair is A gain difference occurs between the antenna elements 11 . Adder 1
2 calculates the azimuth difference ΔX, the vertical difference Δy, and the sum Σ every moment based on the state of occurrence of this gain difference (differential mode). The mixer 13 calculates the azimuth angle error and the vertical angle error using this calculated value and the posture motion signal from the gyro as elements. The detection amplifier 14 processes this calculation result to generate an azimuth angle error signal δX' and an up/down angle error signal δy'.
is transmitted and input to the phase detector 15.

また光学系シーカ20において、21は凹状の反射面を
有する1次反射鏡、22は平面の反射面をそなえる2次
反射鏡、23は赤外光検知器で、これらが一体化されて
ジャイロ光学系を構成し、トルカ28の回転により安定
に保持されている。
In the optical system seeker 20, 21 is a primary reflecting mirror with a concave reflecting surface, 22 is a secondary reflecting mirror with a flat reflecting surface, and 23 is an infrared light detector, which are integrated into a gyro optical system. It constitutes a system and is stably held by the rotation of the torquer 28.

入射赤外光IRは1次お・よび2次反射鏡により反射さ
れて1次反射鏡21の中央部附近に集束し、入射赤外光
IHの方位角および上下角に応じた部位に焦点を結ぶ、
赤外光検知器23において。
The incident infrared light IR is reflected by the primary and secondary reflecting mirrors and is focused near the center of the primary reflecting mirror 21, focusing on a portion corresponding to the azimuth and up/down angle of the incident infrared light IH. tie,
In the infrared light detector 23.

24はレティクル、25は集光レンズ、26は赤外光検
出器である。レティクル24は上記の焦点部位に置かれ
て通常ジャイロと同一速度で回転駆動され、この焦点の
位相に応じた変調光パルスを発生し、集光レンズ25が
この光パルスを集束して検出器26上に集光する。検出
器26は変調光パルスを電気信号に変換し、検波増巾器
27がこの信号を基に方位角誤差δX″および上下角誤
差δy″を演算してその結果を前記位相検波器15へ入
力する。そして位相検波器15はこれらの入力δx′、
δx#、およびδ、I、δy#を処理して操舵角信号δ
Xおよびδyを発信する。
24 is a reticle, 25 is a condenser lens, and 26 is an infrared light detector. The reticle 24 is placed at the focal point and rotated at the same speed as the gyro, and generates a modulated optical pulse according to the phase of the focal point. Focus the light upward. The detector 26 converts the modulated optical pulse into an electrical signal, and the detection amplifier 27 calculates the azimuth error δX'' and the vertical angle error δy'' based on this signal, and inputs the results to the phase detector 15. do. Then, the phase detector 15 receives these inputs δx',
δx#, and δ, I, δy# are processed to generate a steering angle signal δ.
Transmits X and δy.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところで、斯かる従来の複合シーカにあっては、赤外光
の入射範域の外方にアンテナ素子を突出させていたので
、これがミサイル等の空力特性を低下させ、あるいはア
ンテナ素子を発射筒に干渉させないために、機体外径を
必要以上に大きくしなければならない等の問題があった
のである。
By the way, in such conventional composite seekers, the antenna element protrudes outside the incident range of infrared light, which deteriorates the aerodynamic characteristics of the missile, etc., or prevents the antenna element from attaching to the launch tube. In order to prevent interference, there were problems such as the need to make the outer diameter of the aircraft larger than necessary.

そこで本発明の課題は、これらのアンテナ素子を機体の
外に突出させないようにすることにある。
Therefore, an object of the present invention is to prevent these antenna elements from protruding outside the aircraft body.

〔発明の手段〕[Means of invention]

上記課題を解決した本発明の手段は1反射鏡によって集
光される光の光束域の周縁部分に前記アンテナ素子を配
設したものである。
A means of the present invention that solves the above problems is that the antenna element is disposed at the periphery of the luminous flux area of the light condensed by one reflecting mirror.

〔作用〕[Effect]

上記手段によれば、−次反射鏡の周辺部から2次反射鏡
を経て光束域の周縁部へ至る赤外光の反射径路が、この
周縁部に配設したアンテナの電波反射径路ともなるので
、機体の頭部周辺にアンテナ素子を配設した従来のもの
と同様にして電波の発信あるいは受信をおこなうことが
できる。
According to the above means, the reflection path of infrared light from the periphery of the -order reflector to the periphery of the luminous flux area via the secondary reflection mirror also serves as the radio wave reflection path of the antenna disposed at this periphery. , it is possible to transmit or receive radio waves in the same manner as the conventional antenna element arranged around the head of the aircraft.

〔実施例〕〔Example〕

第1図において、3は前記Ramミサイルの機体、4は
レドーム、30および40はそれぞれ本発明に係る電波
系シーカおよび光学系シーカである。
In FIG. 1, 3 is the body of the Ram missile, 4 is a radome, and 30 and 40 are a radio wave seeker and an optical seeker, respectively, according to the present invention.

〜ム M  −+lj、  −ゝ−−−−4啼 A  
^ +4 aう 身\ 哨−Julふ  1 1し は
 ^↓鏡、42は2次反射鏡、43はレティクル44と
集光レンズ45と赤外光検出器46とをそなえる赤外光
検知器で、これらが一体化されてジャイロ光学系を構成
し、トルカ48の回転により安定に保持されていること
は従来の場合と同様である。
~Mu M -+lj, -ゝ----4 A
^ +4 Aう \ \ \ \ \ \ \ \ \ \ ^↓Mirror, 42 is a secondary reflecting mirror, 43 is an infrared light detector comprising a reticle 44, a condensing lens 45, and an infrared light detector 46. , these are integrated to constitute a gyro optical system, and are stably held by the rotation of the torquer 48, as in the conventional case.

然して、この実施例は、2次反射鏡42を凸面鏡として
1次反射鏡41の中央部に集束される光束域を従来のも
のより少し拡げてあり、49は赤外光検知器43の前端
部に配設した集光レンズで、上記光束域の中央部分に反
射されてきた赤外光をこの集光レンズにより集光してレ
ティクル44上に焦点を結ばせる。そしてレティクル4
4が変調光パルスを発生し、検出器46がこれを電気信
号に変換し、検波増巾器47がこの電気信号を受けて方
位角誤差δX“および上下角誤差δy″を演算すること
は前記従来の場合と同様である。
However, in this embodiment, the secondary reflecting mirror 42 is used as a convex mirror, and the luminous flux area focused on the central part of the primary reflecting mirror 41 is slightly expanded compared to the conventional one, and 49 is the front end of the infrared light detector 43. A condenser lens disposed in the reticle 44 condenses the infrared light reflected at the center of the luminous flux area and focuses it on the reticle 44. and reticle 4
4 generates a modulated optical pulse, the detector 46 converts this into an electrical signal, and the detection amplifier 47 receives this electrical signal and calculates the azimuth error δX" and the vertical angle error δy" as described above. This is the same as the conventional case.

電波系シーカ30において、31は2対(4本)のアン
テナ素子で、それらの基端を前記光束域の周縁部に配置
して前記ジャイロ光学系と一体となし、これらのアンテ
ナ素子を後方へ対向的に延ばしてモノパルス系のホーン
アンテナを構成している。したがって、該周縁部へ至る
赤外光の反射径路が即ち電波の反射径路となるから、1
次反射鏡の周辺部から各アンテナ素子31に対応するラ
ジエーシ璽ンゾーンZが形成され、目標からの電波が該
ゾーンをよぎると、その方位角および上下角に応じて6
対のアンテナ素子31に前記ゲイン差が生じる。
In the radio wave seeker 30, reference numeral 31 denotes two pairs (four antenna elements), the base ends of which are arranged at the periphery of the luminous flux area to be integrated with the gyro optical system, and these antenna elements are arranged rearward. They extend oppositely to form a monopulse horn antenna. Therefore, since the reflection path of infrared light reaching the peripheral portion becomes the reflection path of radio waves, 1
A radiation zone Z corresponding to each antenna element 31 is formed from the periphery of the next reflector, and when radio waves from the target cross this zone, 6
The gain difference occurs between the paired antenna elements 31.

以後、これらのゲイン差を加算器32、ミキサ33およ
び検波増巾器34で処理して方位角誤差δX′と上下角
誤差δy′とを演算し、位相検波器35がこれらの演算
結果および光学系からの前記方位角誤差δX“および上
下角誤差δy″を入力して操舵角信号δXおよびδyを
発信することは従来と同様であって、この場合、ミキサ
33は加算器32の算出値ΔX、Δy、Σ、および機体
3と前記ジャイロ光学系との相対姿勢運動の信号を演算
要素とする。
Thereafter, these gain differences are processed by the adder 32, the mixer 33, and the detection amplifier 34 to calculate the azimuth error δX' and the vertical angle error δy', and the phase detector 35 uses these calculation results and the optical Inputting the azimuth error δX" and the vertical angle error δy" from the system and transmitting the steering angle signals δX and δy is the same as in the conventional system, and in this case, the mixer 33 uses the calculated value ΔX of the adder 32. , Δy, Σ, and a signal of the relative attitude movement between the aircraft body 3 and the gyro optical system as calculation elements.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、光学系シーカが固有する
集光径路を利用して電波の反射径路を形成したので、こ
れによってアンテナ素子を機体内に収納することができ
る。よってアンテナ素子の突出にもとづく前記従来の問
題を解消しうるちのである。
As explained above, in the present invention, the radio wave reflection path is formed by using the condensing path unique to the optical system seeker, so that the antenna element can be housed inside the fuselage. Therefore, the above-mentioned conventional problems caused by the protrusion of the antenna element can be solved.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の1実施例を示す説明図、第2図は従来
装置の説#1図である。 !、3・・・機体 10.30・・・電波系シーカ 11.31・・・アンテナ素子 20.40・・・光学系シーカ 21.41・・・1次反射鏡 22.42・・・2次反射鏡 23.43・・・赤外光検知器 24.44・・・レティクル 26.46・・・赤外光検出器 IR・・・赤外光
FIG. 1 is an explanatory diagram showing one embodiment of the present invention, and FIG. 2 is a diagram #1 of a conventional device. ! , 3...Airframe 10.30...Radio wave system seeker 11.31...Antenna element 20.40...Optical system seeker 21.41...Primary reflecting mirror 22.42...Secondary Reflector 23.43...Infrared light detector 24.44...Reticle 26.46...Infrared light detector IR...Infrared light

Claims (1)

【特許請求の範囲】[Claims] 電波系シーカを構成するための複数のアンテナ素子と、
光学系シーカを構成するための集光用反射鏡とをそなえ
るシーカにおいて、集光される光の光束域の周縁部分に
前記アンテナ素子を配設した電波系・光学系複合シーカ
multiple antenna elements for configuring a radio wave seeker;
A radio wave system/optical system composite seeker, which is equipped with a condensing reflector for configuring an optical system seeker, and the antenna element is disposed at a peripheral portion of a luminous flux area of condensed light.
JP13907785A 1985-06-27 1985-06-27 Radio wave / optical system composite seeker Expired - Lifetime JPH077050B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13907785A JPH077050B2 (en) 1985-06-27 1985-06-27 Radio wave / optical system composite seeker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13907785A JPH077050B2 (en) 1985-06-27 1985-06-27 Radio wave / optical system composite seeker

Publications (2)

Publication Number Publication Date
JPS62879A true JPS62879A (en) 1987-01-06
JPH077050B2 JPH077050B2 (en) 1995-01-30

Family

ID=15236949

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13907785A Expired - Lifetime JPH077050B2 (en) 1985-06-27 1985-06-27 Radio wave / optical system composite seeker

Country Status (1)

Country Link
JP (1) JPH077050B2 (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0213798A (en) * 1988-06-30 1990-01-18 Mitsubishi Heavy Ind Ltd Composite guiding system for missile
US5214438A (en) * 1990-05-11 1993-05-25 Westinghouse Electric Corp. Millimeter wave and infrared sensor in a common receiving aperture
US5298909A (en) * 1991-12-11 1994-03-29 The Boeing Company Coaxial multiple-mode antenna system
US5307077A (en) * 1990-12-14 1994-04-26 Hughes Missile Systems Company Multi-spectral seeker antenna
US8094081B1 (en) 2007-10-25 2012-01-10 The Johns Hopkins University Dual band radio frequency (RF) and optical communications antenna and terminal design methodology and implementation

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0213798A (en) * 1988-06-30 1990-01-18 Mitsubishi Heavy Ind Ltd Composite guiding system for missile
US5214438A (en) * 1990-05-11 1993-05-25 Westinghouse Electric Corp. Millimeter wave and infrared sensor in a common receiving aperture
US5307077A (en) * 1990-12-14 1994-04-26 Hughes Missile Systems Company Multi-spectral seeker antenna
US5298909A (en) * 1991-12-11 1994-03-29 The Boeing Company Coaxial multiple-mode antenna system
US8094081B1 (en) 2007-10-25 2012-01-10 The Johns Hopkins University Dual band radio frequency (RF) and optical communications antenna and terminal design methodology and implementation

Also Published As

Publication number Publication date
JPH077050B2 (en) 1995-01-30

Similar Documents

Publication Publication Date Title
US5973309A (en) Target-tracking laser designation
US4383663A (en) Active optical terminal homing
US8164037B2 (en) Co-boresighted dual-mode SAL/IR seeker including a SAL spreader
US7183966B1 (en) Dual mode target sensing apparatus
US4009393A (en) Dual spectral range target tracking seeker
US8049869B2 (en) Dual FOV imaging semi-active laser system
JP3222837B2 (en) Imaging self-referencing tracking device and related method
US4439012A (en) Dual-secondary mirror cassegrain optical system
US6279478B1 (en) Imaging-infrared skewed-cone fuze
US5478028A (en) Tracking and guidance techniques for semi-ballistic rounds
US4093154A (en) Target seeking gyro for a missile
JPS58127100A (en) Guidance method at final orbit stage and guidance missile operated according to said method
EP2989410B1 (en) Multimode shared aperture seeker
US7952688B2 (en) Multi-waveband sensor system and methods for seeking targets
US6268822B1 (en) Dual-frequency millimeter wave and laser radiation receiver
IL140232A (en) Method and system for active laser imagery guidance of intercepting missiles
JPS62880A (en) Electric wave and optical system composite seeker
JP3157148B2 (en) Optical system for missile target detection tracking device
US6552318B1 (en) Sensor system with rigid-body error correcting element
JPS62879A (en) Electric wave and optical system composite seeker
US7175130B2 (en) Missile steering using laser scattering by atmosphere
KR101968330B1 (en) Homing apparatus with multiple sensor
US7247852B2 (en) Methods and apparatus for sensor systems
JPH0766049B2 (en) Aircraft optical system device
US4309003A (en) Target seeking gyro

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term