JPH0252286B2 - - Google Patents
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- Publication number
- JPH0252286B2 JPH0252286B2 JP56170065A JP17006581A JPH0252286B2 JP H0252286 B2 JPH0252286 B2 JP H0252286B2 JP 56170065 A JP56170065 A JP 56170065A JP 17006581 A JP17006581 A JP 17006581A JP H0252286 B2 JPH0252286 B2 JP H0252286B2
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- JP
- Japan
- Prior art keywords
- distance
- flying object
- signal
- tracking
- target
- Prior art date
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- Expired - Lifetime
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- Aiming, Guidance, Guns With A Light Source, Armor, Camouflage, And Targets (AREA)
- Control Of Position, Course, Altitude, Or Attitude Of Moving Bodies (AREA)
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】
本発明は、飛しよう体の比例航法用ホーミン
グ・シーカの追尾機能改善に関するもので、特に
飛しよう体搭載デイジタル計算機で情報処理をほ
どこすことによりシーカの角度追尾機能、距離追
尾機能の改善ならびに飛しよう体のミスデイスタ
ンス改善を目的としたものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improving the tracking function of a homing seeker for proportional navigation of a flying object, and in particular improves the angular tracking function of the seeker by performing information processing on a digital computer mounted on the flying object. The purpose is to improve the distance tracking function and to improve the miss distance of the flying object.
飛しよう体の誘導制御には比例航法がよく採用
されている。この比例航法は、飛しよう体より標
的をみた標的目視線角度が一定であれば両者は衝
突するという原理に基くものであり、標的目視角
度が常に一定になる如く飛しよう体を誘導制御す
る。従つて、その目視線角度が変化しない限り飛
しよう体の進路は一定であり、目視線角度が変化
したときの横加速度指令値は以下の如くなる。 Proportional navigation is often used to guide and control flying objects. This proportional navigation is based on the principle that if the viewing angle of the target from the flying object is constant, the two will collide, and the flying object is guided and controlled so that the viewing angle of the target is always constant. Therefore, the course of the flying object is constant unless the line-of-sight angle changes, and the lateral acceleration command value when the line-of-sight angle changes is as follows.
(横加速度指令値)=(航法定数)×(飛しよう体と
標的との相対速度)×(標的目視線角速度)
第1図に2次元平面で表した標的目視線及びシ
ーカ・アンテナ・ボアサイト軸との関係を示す。
図でX軸は基準軸、1Aは標的目視線、1Bはア
ンテナ・ボアサイト軸、2Aは追尾誤差角、2B
は目視線角を示し、3Aが飛しよう体のシーカ・
アンテナ位置、3Bが標的位置を表す。第2図に
アンテナ座標系及び標的目視線座標系との関係を
示す。図において(r,e,d)直交3軸はアン
テナ座標系を示し、(r′,e′,d′)直交3軸は標的
目視線座標系を示す。ここで4Aは方位角追尾誤
差、4Bは仰角追尾誤差を表す。(Lateral acceleration command value) = (navigation constant) x (relative velocity between flying object and target) x (target line-of-sight angular velocity) Figure 1 shows the target line-of-sight and the seeker antenna boresight on a two-dimensional plane. Indicates the relationship with the axis.
In the figure, the X axis is the reference axis, 1A is the target line of sight, 1B is the antenna boresight axis, 2A is the tracking error angle, and 2B
indicates the line of sight angle, and 3A is the seeker who is about to fly.
The antenna position, 3B, represents the target position. FIG. 2 shows the relationship between the antenna coordinate system and the target eye line coordinate system. In the figure, three orthogonal axes (r, e, d) indicate the antenna coordinate system, and three orthogonal axes (r', e', d') indicate the target eye line coordinate system. Here, 4A represents an azimuth tracking error, and 4B represents an elevation tracking error.
さて、従来の飛しよう体の比例航法用ホーミン
グ・シーカに用いられてきている角度追尾制御方
式は、コニカルスキヤン方式又はモノパルス方式
による飛しよう体と標的との角度誤差信号を、利
得補正回路を通した後アンテナ空間安定ループに
送り、アンテナ空間安定ループは、このレート指
令値に基づき油圧又は電動によるアンテナ・ジン
バル・サーボを駆動することによつて角度誤差を
零にするアナログ負帰還方式であつた。 Now, in the angle tracking control system used in conventional homing seekers for proportional navigation of flying objects, the angular error signal between the flying object and the target using the conical scan method or the monopulse method is passed through a gain correction circuit. After that, it was sent to the antenna space stability loop, and the antenna space stability loop was an analog negative feedback method that reduced the angle error to zero by driving the antenna gimbal servo hydraulically or electrically based on this rate command value. .
第3図は従来のアナログ追尾系を用いた飛しよ
う体の誘導系のブロツク図を示す。5は標的の空
間運動を示し、6は標的と飛しよう体との相対運
動を表わしている。7A,7Bはそれぞれ第2図
のd′軸,e′軸まわりの標的目視線角速度すなわち
ωLSd′,ωLSe′を表し、いわゆるδx,δy成分と呼ば
れるものである。20A,20Bはシーカ・アン
テナの空間角速度のd軸,e軸成分すなわち
ωAd,ωAeを表し、7Aと20Aとの差及び7B
と20Bとの差、すなわち8A,8Bはそれぞれ
追尾誤差角εd,εeの微分値を示す。従つて9A,
9Bで示される積分器の出力10A,10Bはそ
れぞれ方位角追尾誤差、仰角追尾誤差εd,εeを示
す。点線で囲まれた12はシーカの角度誤差受信
部・フイルタ部を示し、11A,11Bはそれぞ
れのチヤンネル(方位角追尾用及び仰角追尾用)
の受信機雑音を示す。13A,13Bはそれぞれ
の追尾チヤンネルのループ利得を示し、その出力
はアンテナ空記安定装置14の空間角速度指令値
を作る。15は飛しよう体の空間角速度運動を表
し、14の出力は、シーカ・アンテナの空間角速
度成分20A,20Bすなわち、ωAd,ωAeを作
り出す。一方、13A,13Bの出力であるアン
テナ空間角速度指令値は、16A,16Bで示さ
れる比例航法を用いた誘導法則により飛しよう体
の横加速度指令信号を作る。ここで17は飛しよ
う体と標的との距離及び距離レートを測定するた
めの距離/距離レート受信部から得られる距離レ
ートゲート出力信号である。16A,16Bによ
つて作られた飛しよう体横加速度指令信号は、そ
れぞれ18A,18Bで示される飛しよう体オー
トパイロツト機体横方向の運動を通じて飛しよう
体に横加速度を発生させ、飛しよう体は19A,
19Bで示される機体のG−リミツタの制限下に
於ける空力飛しよう運動を行い、6の標的とミサ
イルの相対運動に基づく標的目視線角速度を一定
に保つように比例航法により誘導される。一方標
的との相対距離、距離レートはそれぞれ24A,
24BすなわちR,R〓で示され、21の点線で囲
まれた距離/距離レート受信部で測定されそれぞ
れ25,17で示される距離ゲート出力、距離レ
ートゲート出力信号によつて追尾される。ここ
で、22,23は、距離/距離レート受信部の受
信機雑音を示す。 FIG. 3 shows a block diagram of a flying object guidance system using a conventional analog tracking system. 5 represents the spatial movement of the target, and 6 represents the relative movement between the target and the flying object. 7A and 7B represent the target eye line angular velocities around the d' and e' axes in FIG. 2, ie, ω LSd ' and ω LSe ', respectively, and are so-called δ x and δ y components. 20A and 20B represent the d-axis and e-axis components of the spatial angular velocity of the seeker antenna, namely ω Ad and ω Ae , and the difference between 7A and 20A and 7B
The difference between and 20B, ie, 8A and 8B, indicates the differential values of the tracking error angles ε d and ε e , respectively. Therefore 9A,
Outputs 10A and 10B of the integrator indicated by 9B indicate the azimuth tracking error and the elevation tracking error ε d and ε e , respectively. 12 surrounded by a dotted line indicates the angle error receiving section/filter section of the seeker, and 11A and 11B are the respective channels (for azimuth angle tracking and elevation angle tracking).
shows the receiver noise of 13A and 13B indicate the loop gain of each tracking channel, and the output thereof creates a spatial angular velocity command value of the antenna air recording stabilizer 14. 15 represents the spatial angular velocity motion of the flying object, and the output of 14 produces the spatial angular velocity components 20A, 20B of the seeker antenna, ie, ω Ad , ω Ae . On the other hand, the antenna spatial angular velocity command value outputted from 13A and 13B produces a lateral acceleration command signal for the flying object according to the guidance law using proportional navigation shown at 16A and 16B. Here, 17 is a distance rate gate output signal obtained from a distance/distance rate receiving section for measuring the distance between the flying object and the target and the distance rate. The flying body lateral acceleration command signals generated by 16A and 16B generate lateral acceleration on the flying body through the lateral movement of the flying body autopilot aircraft indicated by 18A and 18B, respectively. 19A,
The aircraft performs an aerodynamic flight motion under the limitations of the G-limiter of the aircraft, indicated by 19B, and is guided by proportional navigation so as to keep the target line-of-sight angular velocity constant based on the relative movement of the target and the missile in 6. On the other hand, the relative distance to the target and the distance rate are 24A, respectively.
24B, that is, R, R〓, which are measured by the distance/distance rate receiving section surrounded by the dotted line 21 and tracked by the distance gate output and distance rate gate output signals shown at 25 and 17, respectively. Here, 22 and 23 indicate receiver noise of the distance/distance rate receiving section.
このような従来の方式は、標的とシーカを搭載
する飛しよう体との相対運動によつてもたらされ
る角度誤差信号を検出し、その誤差を零にするよ
うに帰還をかけるもので、追尾系としては一次遅
れ系を構成する。従つて、標的の激しい運動によ
る目視線角速度が大きい時、追尾誤差角が大きく
なり追尾をはずす恐れがある。そこで追尾ループ
の応答を早めるため利得補正回路を含めたループ
の時定数を小さくしたり、ループ利得を高める
と、受信機雑音によつて追尾ループが不安定にな
るという欠点を持ち、おのずからその追尾機能に
は制限を有していた。 This conventional method detects the angular error signal caused by the relative movement between the target and the flying object carrying the seeker, and applies feedback to reduce the error to zero, and is used as a tracking system. constitutes a first-order lag system. Therefore, when the angular velocity of the eye's line of sight due to intense movement of the target is high, the tracking error angle becomes large, and there is a risk that tracking may be lost. Therefore, if you reduce the time constant of the loop including the gain correction circuit or increase the loop gain in order to speed up the response of the tracking loop, this has the disadvantage that the tracking loop becomes unstable due to receiver noise, and the tracking loop naturally becomes unstable. It had limited functionality.
本発明は、上記の点に鑑み、デイジタル計算機
を飛しよう体に搭載し、生の角度誤差信号、距離
信号、距離レート信号をデイジタル信号に変換す
るとともにその時の受信レベルにおける受信機雑
音の推定値を用いて、標的目視線角度の変化率の
推定値、角度誤差の推定値、距離及び距離レート
の推定値を演算し、これらの推定値を用いて比例
航法による誘導を行つて、ミスデイスタンス及び
追尾機能の改善を図つた飛しよう体誘導制御方法
を提供しようとするものである。 In view of the above points, the present invention mounts a digital calculator on a flying body, converts a raw angle error signal, a distance signal, and a distance rate signal into digital signals, and generates an estimated value of receiver noise at the reception level at that time. is used to calculate the estimated rate of change of the target eye gaze angle, the estimated angular error, the estimated distance and distance rate, and use these estimated values to perform guidance by proportional navigation to avoid misdistance. The present invention also aims to provide a flying object guidance control method that improves the tracking function.
以下、本発明に係る飛しよう体誘導制御方法の
実施例を図面に従つて説明する。 Embodiments of the flying object guidance and control method according to the present invention will be described below with reference to the drawings.
本発明と従来のアナログ追尾系との大きな相違
は、角度追尾系、距離/距離レート追尾系の各受
信部の後に最適フイルタが搭載デイジタル計算機
のソフトウエアとして組込まれている点にある。
第4図に本発明の実施例のブロツク図を示す。こ
の第4図において、26は標的の空間運動を示
し、27の標的と飛しよう体との相対幾何学的運
動を表わす線形近似ダイナミクス方程式は、角度
追尾系、距離/距離レート追尾系についてそれぞ
れ次式の如く記述される。 The major difference between the present invention and conventional analog tracking systems is that an optimum filter is incorporated as software in the on-board digital computer after each receiving section of the angle tracking system and distance/distance rate tracking system.
FIG. 4 shows a block diagram of an embodiment of the present invention. In this figure, 26 indicates the spatial motion of the target, and the linear approximate dynamics equations representing the relative geometric motion between the target and the flying object in 27 are as follows for the angle tracking system and the distance/distance rate tracking system, respectively. It is written as follows.
d〓A/dt=〓〓A+〓A+〓A〓A …(1)
但し
ここで、状態変数〓Aの要素;εd,εeは方位角
追尾誤差、仰角追尾誤差、ωLSd′,ωLSe′は標的目
視線角速度のd′軸,e′軸成分、aT-d′,aTe′は標的
加速度の−d′軸、e′軸成分を示し、いずれも確率
変数である。確定ベクトル〓Aの要素;ωAd,ωAe
はシーカ・アンテナの空間角速度のd軸,e軸成
分、aId,aIeは飛しよう体の加速度のd軸,e軸
成分を示す。〓Aは入力制約行列を示し追尾対象
の性質で定まる。追尾対象への入力ベクトル〓A
の要素;Wd′,We′は標的加速度モデルを駆動す
る白色雑音を示す。また、係数行列〓の要素;
ωArはシーカ・アンテナの空間角速度のr軸成
分、Rは距離、R〓は距離レート、τd′,τe′は標的
旋回時定数を表わす。同様に距離/距離レート追
尾系は、
d〓R/dt=〓・〓R+〓R+〓R・Wr′ …(2)
但し、
〓T R=[R,R〓,aTr′]
〓T R=[0,−aIr,0]
〓T R=[0,0,1]
〓=0
ω2 Ls
01
0
00
1
−1/τr′
ここで、状態変数〓Rの要素;aTr′は標的加速
度のr′軸成分、確定ベクトル〓Rの要素;aIrはミ
サイルの加速度のr軸成分、〓Rは入力制約行列
を示し追尾対象の性質で定まり、Wr′は標的加速
度モデルを駆動する白色雑音を示す。また、係数
行列〓の要素;ω2 Lsは、ω2 Ls=ω2 Lsd′+ω2 Lse′で
与え
られる。τr′は標的加速度に関する旋回時定数を
表わす。ここで飛しよう体のホーミング・シーカ
が3軸ジンバルを持つか又は飛しよう体のオート
パイロツトのロール安定が充分であるとすると、
(1)式で与えられるダイナミクス方程式の係数行列
〓の要素ωAr、すなわちシーカ・アンテナの空間
角速度のr軸成分は無視することができる。従つ
て(1)式は、方位角チヤネルと仰角チヤネルを分離
することができ、それぞれ次式の如く表わせる。 d〓 A /dt=〓〓 A +〓 A +〓 A 〓 A …(1) However Here, the elements of the state variable A ; ε d and ε e are the azimuth tracking error and the elevation tracking error, ω LSd ′, ω LSe ′ are the d′-axis and e′-axis components of the target eye line-of-sight angular velocity, a Td ′ , a Te ′ indicate the −d′-axis and e′-axis components of the target acceleration, both of which are random variables. Elements of deterministic vector 〓 A ; ω Ad , ω Ae
are the d-axis and e-axis components of the spatial angular velocity of the seeker antenna, and a Id and a Ie are the d-axis and e-axis components of the acceleration of the flying object. 〓 A indicates the input constraint matrix, which is determined by the characteristics of the tracking target. Input vector to tracking target〓 A
The elements; W d ′ and W e ′ represent white noise that drives the target acceleration model. Also, the elements of the coefficient matrix 〓;
ω Ar is the r-axis component of the spatial angular velocity of the seeker antenna, R is the distance, R〓 is the range rate, and τ d ′ and τ e ′ are the target rotation time constants. Similarly, the distance/distance rate tracking system is d〓 R /dt=〓・〓 R +〓 R +〓 R・Wr′ …(2) However, 〓 T R = [R, R〓, a Tr ′] 〓 T R = [0, −a Ir , 0] 〓 T R = [0, 0, 1] 〓 = 0 ω 2 Ls 01 0 00 1 −1/τ r ′ Here, state variable 〓 Element of R ; a Tr ′ is the r′-axis component of the target acceleration, the element of the deterministic vector 〓 R ; a Ir is the r-axis component of the missile acceleration, 〓 R is the input constraint matrix, which is determined by the properties of the tracking target, and W r ′ is the target acceleration Shows white noise driving the model. Also, the element of the coefficient matrix 〓; ω 2 Ls is given by ω 2 Ls = ω 2 Lsd ′+ω 2 Lse ′. τ r ′ represents the turning time constant with respect to the target acceleration. If the homing seeker of the flying object has a 3-axis gimbal or the roll stability of the flying object's autopilot is sufficient, then
The element ω Ar of the coefficient matrix 〓 of the dynamics equation given by equation (1), that is, the r-axis component of the spatial angular velocity of the seeker antenna can be ignored. Therefore, equation (1) can be separated into an azimuth channel and an elevation channel, which can be expressed as the following equations.
d/dt〓A′=〓′〓A′+〓A′+〓A′We′ …(3)
但し
〓T A′=[εd,ωLsd′,aTe′]
〓T A′=[−ωAd,−aIe/R,0]
〓′=0
0
01
−2R/R
00
1/R
−1/τe′
〓T A′=[0,0,1]
同様に、
d/dt〓A″=〓″〓A″+〓A″+〓A″Wd′ …(4)
但し
〓T A″=[εe,ωLse′,aT-d′]
〓T A″=[−ωAe,aId/R,0]
〓=0
0
01
−2R〓/R
00
1/R
−1/τe′
〓T A″[0,0,1]
さて、27の角度追尾系のダイナミクス方程式
(3),(4)式の標的目視線角速度;ωLsd,,ωLse′は、
28A,28Bで示され、シーカ・アンテナの空
間角速度ωAd,ωAeは、50A,50Bで示され
る。28Aと50Aの差及び28Bと50Bとの
差、すなわち29A,29Bは、アナログ追尾系
の場合と同様追尾誤差角εd,εeの微分値を示す。
従つて追尾誤差εd,εeは29A,29Bを積分器
70A,70Bで一回積分した30A,30Bで
表わされる。点線で囲まれた32はシーカの角度
誤差受信部を示し、31A,31Bはそれぞれの
チヤネルの受信機雑音を示す。角度誤差の観測値
はS・W1が閉じられた時に得られる。この観測
値は、1点鎖線で囲まれた33で示される搭載デ
イジタル計算機のソフトウエアとして構成された
34で示される最適フイルタ()(カルマンフ
イルタとも呼ばれる)の入力信号となる。最適フ
イルタ()34には、(3),(4)式で表わされる標
的と飛しよう体との相対幾何学的運動を表わす連
続系ダイナミクス方程式から変換された離散値系
ダイナミクス方程式に基づき推定誤差2乗を最小
にする規範を満足する繰返し形式の離散値系フイ
ルタが構成されている。離散値系ダイナミクス方
程式は、方位角チヤネルの場合次式で与えられ
る。 d/dt〓 A ′=〓′〓 A ′+〓 A ′+〓 A ′W e ′ …(3) However, 〓 T A ′=[ε d , ω Lsd ′, a Te ′] 〓 T A ′= [−ω Ad ,−a Ie /R,0] 〓′=0 0 01 −2R/R 00 1/R −1/τ e ′ 〓 T A ′=[0,0,1] Similarly, d/ dt〓 A ″=〓″〓 A ″+〓 A ″+〓 A ″W d ′ …(4) However,〓 T A ″=[ε e , ω Lse ′, a Td ′] 〓 T A ″=[− ω Ae ,a Id /R,0] 〓=0 0 01 −2R〓/R 00 1/R −1/τ e ′ 〓 T A ″[0,0,1] Now, the dynamics of the 27 angle tracking system equation
The target eye line angular velocity in equations (3) and (4); ω Lsd, , ω Lse ′ is
The spatial angular velocities ω Ad and ω Ae of the seeker antenna are shown as 50A and 50B. The difference between 28A and 50A and the difference between 28B and 50B, ie, 29A and 29B, represent the differential values of the tracking error angles ε d and ε e as in the analog tracking system.
Therefore, the tracking errors ε d and ε e are represented by 30A and 30B obtained by integrating 29A and 29B once by integrators 70A and 70B. 32 surrounded by a dotted line indicates the angle error receiving section of the seeker, and 31A and 31B indicate receiver noise of each channel. The observed value of angular error is obtained when S·W1 is closed. This observed value becomes an input signal to an optimal filter ( ) (also called a Kalman filter) indicated by 34 configured as software of the on-board digital computer indicated by 33 surrounded by a dashed line. The optimal filter ( ) 34 calculates the estimation error based on the discrete-value system dynamics equation converted from the continuous-system dynamics equation representing the relative geometric motion between the target and the flying object expressed by equations (3) and (4). A repeating type discrete value filter is constructed that satisfies the criterion of minimizing the square. The discrete-value system dynamics equation is given by the following equation for the azimuthal channel.
〓A′(K+1)=ΦA′(K+1,K)〓A′(K)
+〓A′(K)+〓A′(K)We′(K) …(5)
ここで、ΦA′(K+1,K)は遷移行列を示し
次式の如く与えられる。 〓 A ′ (K + 1) = Φ A ′ (K + 1, K) 〓 A ′ (K) + 〓 A ′ (K) + 〓 A ′ (K) W e ′ (K) …(5) Here, Φ A '(K+1,K) represents a transition matrix and is given as shown in the following equation.
(但し、Δt=tk+1−tk)
同様に確定ベクトル;〓A′(K)、入力制約ベ
クトル;〓A′(K)も次式の如く与えられる。 (However, Δt=t k+1 −t k ) Similarly, the deterministic vector 〓 A ′(K) and the input constraint vector 〓 A ′(K) are also given as follows.
仰角チヤネルも同様にして与えられることが自
明であり省略する。 It is obvious that the elevation channel is also given in the same way, so the description thereof will be omitted.
また、フイルタ入力35は、角度誤差の観測値
を示し方位角チヤネルの場合次式で与えられる。 Further, the filter input 35 indicates the observed value of the angular error, which is given by the following equation in the case of the azimuthal channel.
〓A′(K+1)=〓A〓A′(K+1)+〓A′(K
+1) …(6)
又は、
ZA′(K+1)=εd(K+1)+nd(K+1)
ここで〓Aは観測行列を示し、この場合次式で
与えられる。〓A′(K+1)は観測雑音を示す。 〓 A ′(K+1)=〓 A 〓 A ′(K+1)+〓 A ′(K
+1) ...(6) Or, Z A ′ (K+1)=ε d (K+1)+n d (K+1) where 〓 A represents the observation matrix, which in this case is given by the following equation. 〓 A ′(K+1) indicates observation noise.
〓A=[100]
フイルタ入力36も同様にして、仰角チヤネル
の場合次式で与えられることがわかる。 〓 A = [100] Similarly, it can be seen that the filter input 36 is given by the following equation in the case of the elevation channel.
〓A″(K+1)=〓A〓A″(K+1)+〓A″(K
+1) …(7)
又は、
ZA″(K+1)=εe(K+1)+ne(K+1)
(5),(6)式が与えられたとき、最適フイルタ
()34は次式の如く与えられることが知られ
ている。 〓 A ″(K+1)=〓 A 〓 A ″(K+1)+〓 A ″(K
+1) ...(7) Or, Z A ″(K+1)=ε e (K+1)+n e (K+1) When the equations (5) and (6) are given, the optimal filter ( ) 34 is given as the following equation. It is known that
〓A′(K+1)|K+1)=〓A′(K+1|K)
+〓A(K+1){〓A′(K+1)−〓A〓A′(K+
1|K)} …(8)
〓A′(K+1|K)=Φ^A′(K+1,K)〓A′
(K|K)+〓A′(K) …(9)
〓A(K+1)=〓A(K+1|K)〓T A[〓A〓A
(K+1|K)〓T A+RA(K+1)]-1 …(10)
〓A(K+1|K)ΔE[〓1 A(K+1|K)
〓′T A(K+1|K)] …(11)
但し、
〓A′(K+1|K)=〓A′(K+1)−〓A′(K
+1|K) …(12)
(11)式で定義される事前推定誤差共分散行列〓A
(K+1|K)は次式を満足する。 〓 A ′(K+1)|K+1)=〓 A ′(K+1|K)
+〓 A (K+1) {〓 A ′(K+1)−〓 A 〓 A ′(K+
1|K)} …(8) 〓 A ′(K+1|K)=Φ^ A ′(K+1,K)〓 A ′
(K|K)+〓 A ′(K) …(9) 〓 A (K+1)=〓 A (K+1|K)〓 T A [〓 A 〓 A
(K+1|K)〓 T A +R A (K+1)] -1 …(10) 〓 A (K+1|K) Δ E[〓 1 A (K+1|K)
〓′ T A (K+1|K)] …(11) However, 〓 A ′(K+1|K)=〓 A ′(K+1)−〓 A ′(K
+1 | K) …(12) Prior estimation error covariance matrix defined by equation (11) 〓 A
(K+1|K) satisfies the following equation.
〓A(K+1|K)=Φ^A′(K+1,K)〓A
(K|K) ×Φ^′T A(K+1,K)+〓A′(K)QA
(K)〓′T A(K) …(13)
(13)式の事後推定誤差共分散行列〓A(K|
K)は次式の如く定義される。 〓 A (K+1|K)=Φ^ A ′(K+1,K)〓 A
(K|K) ×Φ^′ T A (K+1,K)+〓 A ′(K)Q A
(K)〓′ T A (K) …(13) Posterior estimation error covariance matrix of equation (13)〓 A (K|
K) is defined as follows.
〓A(K|K)ΔE[〓A′(K|K)〓′T A(K|
K) …(14)
但し
〓A′(K|K)=〓A′(K)−〓A(K|K)
…(15)
又(14)式で定義される〓A(K|K)は次式
を満足する。 〓 A (K|K) Δ E[〓 A ′(K|K)〓′ T A (K|
K) …(14) However, 〓 A ′ (K | K) = 〓 A ′ (K) − 〓 A (K | K)
...(15) Also, A (K|K) defined by equation (14) satisfies the following equation.
〓A(K|K)=[−〓A(K)〓A]〓A(K|
K−1) …(16)
ここで、(9)式、(13)式に出てくるΦ^A′(K+
1,K),〓A′(K),〓A′(K)はそれぞれ(5)式
のΦ^A′(K+1,K),〓A′(K),〓A′(K)の
要素R及びR〓が距離/距離レート追尾系の最適フ
イルタ()すなわち57の出力R(K),R(K)
によつて置換えられていることを意味する。(10)式
のRA(K+1)は次式に示されるような観測雑音
の分散を示す。すなわち
[E[nd(K+1)]=0
E[nd(K+1) nd(K+1+J)]
=RA(K+1)δK+1 〓 A (K | K) = [−〓 A (K)〓 A ]〓 A (K |
K−1) …(16) Here, Φ^ A ′(K+
1, K), 〓 A ′(K), 〓 A ′(K) are the elements of Φ^ A ′(K+1, K), 〓 A ′(K), 〓 A ′(K) in equation (5), respectively. R and R〓 are the optimal filters () for the distance/distance rate tracking system, that is, the outputs R(K) and R(K) of 57
means that it has been replaced by . R A (K+1) in equation (10) represents the variance of observation noise as shown in the following equation. That is, [E[n d (K+1)] = 0 E[n d (K+1) n d (K+1+J)] = R A (K+1) δ K+1
Claims (1)
信号と距離信号と距離レート信号とを用いて飛し
よう体を比例航法により誘導する飛しよう体誘導
制御方法において、前記ホーミング・シーカが標
的を検知し追尾モードに入つた時、追尾を維持す
るための雑音を含んだ生の角度誤差信号と生の距
離信号と生の距離レート信号とをデイジタル信号
に変換し、前記追尾モードにおける受信機の受信
レベルでのS/N比を推定して予め当該飛しよう
体に搭載のデイジタル計算機にプログラムされて
いる状態推定のアルゴリズムの中の受信機雑音の
分散(電力値)を推定し、前記生の角度誤差信号
と生の距離信号と生の距離レート信号と前記受信
機雑音の分散の推定値とを用いて前記計算機で前
記標的とシーカ・アンテナとの目視線角度の変化
率の推定値、角度誤差の推定値、距離及び距離レ
ートの推定値を求め、これらの推定値を用いて比
例航法による誘導を実行することを特徴とする飛
しよう体誘導制御方法。1. In a flying object guidance control method in which a flying object is guided by proportional navigation using an angular error signal, a distance signal, and a distance rate signal of a homing seeker of a flying object, the homing seeker detects and tracks a target. When entering the tracking mode, the raw angle error signal containing noise for maintaining tracking, the raw distance signal, and the raw distance rate signal are converted into digital signals, and the reception level of the receiver in the tracking mode is The variance (power value) of the receiver noise in the state estimation algorithm programmed in advance in the digital computer mounted on the flying object is estimated by estimating the S/N ratio of the raw angular error signal. and the raw range signal, the raw range rate signal, and the estimate of the variance of the receiver noise. 1. A method for guiding and controlling a flying object, characterized in that the estimated values of the distance, distance, and distance rate are obtained, and these estimated values are used to execute guidance by proportional navigation.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56170065A JPS5872897A (en) | 1981-10-26 | 1981-10-26 | Method of inducing and controlling missile |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56170065A JPS5872897A (en) | 1981-10-26 | 1981-10-26 | Method of inducing and controlling missile |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5872897A JPS5872897A (en) | 1983-04-30 |
| JPH0252286B2 true JPH0252286B2 (en) | 1990-11-13 |
Family
ID=15897973
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56170065A Granted JPS5872897A (en) | 1981-10-26 | 1981-10-26 | Method of inducing and controlling missile |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5872897A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0523460U (en) * | 1991-06-25 | 1993-03-26 | ウイトコオブジユピター電通株式会社 | Connector with feedthrough capacitor |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61184476A (en) * | 1985-02-12 | 1986-08-18 | Mitsubishi Electric Corp | Tracking filter |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5676809A (en) * | 1979-11-28 | 1981-06-24 | Mitsubishi Heavy Ind Ltd | Induction system applying kalman filter |
-
1981
- 1981-10-26 JP JP56170065A patent/JPS5872897A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0523460U (en) * | 1991-06-25 | 1993-03-26 | ウイトコオブジユピター電通株式会社 | Connector with feedthrough capacitor |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5872897A (en) | 1983-04-30 |
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