JPH0549070B2 - - Google Patents
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- Publication number
- JPH0549070B2 JPH0549070B2 JP8343886A JP8343886A JPH0549070B2 JP H0549070 B2 JPH0549070 B2 JP H0549070B2 JP 8343886 A JP8343886 A JP 8343886A JP 8343886 A JP8343886 A JP 8343886A JP H0549070 B2 JPH0549070 B2 JP H0549070B2
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- Japan
- Prior art keywords
- phase
- fixed
- signals
- radio waves
- element antennas
- Prior art date
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- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は到来電波の方向を検出する方探装置
に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a direction finding device that detects the direction of incoming radio waves.
[従来の技術]
第3図は従来の方探装置のブロツク図であつ
て、1,2は到来電波を受信する素子アンテナ、
3は位相検波器、4はコンソール、5,6は素子
アンテナ1,2と位相検波器3の間を接続する信
号ケーブルである。[Prior Art] Fig. 3 is a block diagram of a conventional direction finding device, in which 1 and 2 are element antennas for receiving incoming radio waves;
3 is a phase detector, 4 is a console, and 5 and 6 are signal cables connecting between the element antennas 1 and 2 and the phase detector 3.
次にこの装置の動作を説明する。素子アンテナ
1,2で受信した到来電波は信号ケーブル5,6
を経由して位相検波受信機3に導かれる。 Next, the operation of this device will be explained. The incoming radio waves received by the element antennas 1 and 2 are sent to the signal cables 5 and 6.
The signal is guided to the phase detection receiver 3 via.
位相検波受信機3の一方の端子に入力する信号
を
V1=E1sinωt ……(1)
他方の端子に入力する信号を
V2=E2sin(ωt+φ) ……(2)
とすると、出力信号Voutは(3)式で示されるよう
に素子アンテナ(1)及び
Vout=K(E1E2)cosφ ……(3)
(2)で受信した到来電波の位相差φの関数で表わさ
れる。コンソール(4)では(3)式で示されるVoutを
読みとり、Voutからただちに位相差φに換算す
る。 If the signal input to one terminal of the phase detection receiver 3 is V 1 = E 1 sinωt ...(1) and the signal input to the other terminal is V 2 = E 2 sin (ωt + φ) ...(2), As shown in equation (3), the output signal Vout is expressed as a function of the phase difference φ of the incoming radio waves received by the element antenna (1) and Vout=K(E 1 E 2 ) cosφ ...(3) (2) It can be done. The console (4) reads Vout expressed by equation (3), and immediately converts Vout to a phase difference φ.
一方第3図からも明らかな如く位相差φと電波
の到来方向θとの間には(4)式の関係があり、コン
ソール(4)で
θ=sin-1[λ・φ/2πd] ……(4)
λ:波長
上式を演算することにより、到来電波の方向を求
め表示することが出来る。 On the other hand, as is clear from Fig. 3, there is a relationship between the phase difference φ and the arrival direction θ of the radio wave as shown in equation (4), and in the console (4), θ=sin -1 [λ・φ/2πd]... ...(4) λ: By calculating the above equation, the direction of the arriving radio wave can be determined and displayed.
[発明が解決しようとする問題点]
従来の方探装置は以上のように構成されており
素子アンテナ1,2で受信する到来電波の位相を
位相検波受信機3を用いて測定している。位相測
定は振幅測定にくらべて一般的に難かしく、素子
アンテナ1,2や位相検波受信機3の周波数特性
や信号ケーブル5,6のひねり、曲り温度特性等
が位相測定時の誤差となり、到来電波の方向を精
度よく検出出来ない欠点があつた。[Problems to be Solved by the Invention] The conventional direction finding device is configured as described above, and the phase of the incoming radio waves received by the element antennas 1 and 2 is measured using the phase detection receiver 3. Phase measurement is generally more difficult than amplitude measurement, and the frequency characteristics of the element antennas 1 and 2 and the phase detection receiver 3, as well as the twisting and bending temperature characteristics of the signal cables 5 and 6, cause errors during phase measurement. There was a drawback that the direction of radio waves could not be detected accurately.
この発明は、上記のような問題点を解消する為
になされたもので、従来のように位相検波受信機
3を用いて直接、到来電波の位相を検出するのを
廃し、素子アンテナ1,2での受信電界を複数個
に合成し、振幅受信機でその複数個の振幅を同一
時間面内で計測することにより、計算で精度よく
両素子アンテナ1,2で受信する到来波の位相を
求めることを目的とする。 This invention was made to solve the above-mentioned problems, and eliminates the need to directly detect the phase of an incoming radio wave using the phase detection receiver 3 as in the past, and instead uses the element antennas 1 and 2. By combining the received electric fields into multiple fields and measuring the amplitudes of the multiple fields in the same time plane with an amplitude receiver, the phase of the arriving wave received by both element antennas 1 and 2 is calculated with high precision. The purpose is to
[問題点を解決するための手段]
この発明に係る方探装置は素子アンテナ1,2
に到来する電波の位相を複数の振幅受信機を用い
て、一方あるいは他方のいずれかの素子アンテナ
に接続された複数の半固定又は固定位相器の位相
をあらかじめ異なるように設定しておき、その時
の複数の合成受信ベクトルの振幅変化から計算に
より素子アンテナ1,2に到来する電波の位相を
求め、その位相から前記(4)式を用いて電波の到来
方向を計算により求めようとするものである。[Means for solving the problem] A direction finding device according to the present invention includes element antennas 1 and 2.
Using multiple amplitude receivers, the phases of multiple semi-fixed or fixed phase shifters connected to either one or the other element antenna are set to be different in advance, and the phase of the radio waves arriving at This method calculates the phase of the radio waves arriving at the element antennas 1 and 2 from the amplitude changes of multiple composite reception vectors, and calculates the direction of arrival of the radio waves from the phase using equation (4) above. be.
[作用]
この発明に係る方探装置は素子アンテナ1,2
に到来する電波の位相を求める場合、位相受信機
を用いることなく複数の振幅受信機を用いること
により、位相を直接測定する方式にくらべ安定に
かつ精度よく振幅を測定することができるので従
来の位相比較方探方式の問題点であつた位相測定
の精度を飛躍的に向上させることが出来るととも
に、従来の方式の特徴である瞬探性をも維持させ
ることができる。[Function] The direction finding device according to the present invention has element antennas 1 and 2.
When determining the phase of radio waves arriving at The accuracy of phase measurement, which was a problem with the phase comparison method, can be dramatically improved, and the instantaneous detection characteristic of the conventional method can also be maintained.
[実施例]
以下、この発明の一実施例を図について説明す
る。[Example] Hereinafter, an example of the present invention will be described with reference to the drawings.
第1図は、この発明の一実施例を示す図であり
1は第1の素子アンテナ、2は第2の素子アンテ
ナ、4はコンソール、5,6は信号ケーブル、7
は第1の電力分配器、8は第2の電力分配器、9
a,9b,9cは第1、第2、第3の結合器、1
0a,10b,10cは第1、第2、第3の振幅
受信機、11a,11b,11cは第1、第2、
第3の半固定又は固定位相器、12,13,14
はT1,T2,T3受信チヤンネルである。 FIG. 1 is a diagram showing an embodiment of the present invention, in which 1 is a first element antenna, 2 is a second element antenna, 4 is a console, 5 and 6 are signal cables, and 7 is a diagram showing an embodiment of the present invention.
is the first power divider, 8 is the second power divider, 9
a, 9b, 9c are first, second and third couplers, 1
0a, 10b, 10c are first, second, third amplitude receivers; 11a, 11b, 11c are first, second,
third semi-fixed or fixed phaser, 12, 13, 14
are the T 1 , T 2 , and T 3 receiving channels.
上記のように構成された、この発明の方探装置
の一実施例の動作について説明する。 The operation of one embodiment of the direction finding device of the present invention configured as described above will be described.
第1の素子アンテナ1で受信した信号をS1、
第2の素子アンテナ2で受信した信号をS2とす
る。 The signal received by the first element antenna 1 is S1,
The signal received by the second element antenna 2 is assumed to be S2.
信号S1は信号ケーブル5を経由し第1の電力
分配器7で分配され、複数の結合器9a,9b,
9cの一方の端子に入力する。 The signal S1 is distributed by the first power divider 7 via the signal cable 5, and is distributed to a plurality of couplers 9a, 9b,
Input to one terminal of 9c.
信号S2は信号ケーブル6を経由し第2の電力
分配器8で分配され、位相が既知の複数の半固定
又は固定位相器11a,11b,11cを経由し
て、それぞれ前記複数の結合器9a,9b,9c
の他方の端子に入力される。複数の半固定又は固
定位相器11a,11b,11cによりそれぞれ
位相偏位されたそれぞれの信号をS2a,S2b,S2c
とする。 The signal S2 is distributed by the second power divider 8 via the signal cable 6, and then passed through a plurality of semi-fixed or fixed phase shifters 11a, 11b, 11c whose phases are known, and then connected to the couplers 9a, 11c, respectively. 9b, 9c
is input to the other terminal of The respective signals phase-shifted by a plurality of semi-fixed or fixed phase shifters 11a, 11b, 11c are converted into S 2a , S 2b , S 2c
shall be.
それぞれの結合器9a,9b,9cでは前記信
号S1と前記信号S2a,S2b,S2cそれぞれがベク
トル合成され、振幅の異なる信号T1,T2,T3を
出力する。複数の振幅受信機10a,10b,1
0cでは前記結合器9a,9b,9cからの出力
信号T1,T2,T3を受信する。コンソール4はこ
れらのレベルの異なる信号T1,T2,T3の信号を
同一時間面内に読みとり、演算処理して第1の素
子アンテナ1と第2の素子アンテナ2で受信する
到来電波の相対的位相を算出する。 In each of the combiners 9a, 9b, and 9c, the signal S1 and the signals S2a , S2b , and S2c are vector-synthesized to output signals T1 , T2 , and T3 having different amplitudes. Multiple amplitude receivers 10a, 10b, 1
At 0c, output signals T 1 , T 2 and T 3 from the couplers 9a, 9b and 9c are received. The console 4 reads the signals T 1 , T 2 , and T 3 with different levels within the same time plane, processes them, and calculates the incoming radio waves received by the first element antenna 1 and the second element antenna 2. Calculate relative phase.
この結果からただちに前記(4)式の演算がコンソ
ール4でおこなわれ到来電波の方向を知ることが
できる。 Immediately from this result, the calculation of equation (4) is performed on the console 4, and the direction of the incoming radio wave can be determined.
第2図は到来電波の相対的位相の演算方法を説
明する為の図でS1とS2a,S2b,S2cを振幅と位
相をもつたベクトルで表わし、振幅受信機10
a,10b,10cそれぞれの受信レベルをT1,
T2,T3で表わしている。 Figure 2 is a diagram for explaining the method of calculating the relative phase of incoming radio waves.
The reception level of each of a, 10b, and 10c is T 1 ,
It is expressed as T 2 and T 3 .
観測値p、q、rは第2図の01を中心にS2が
回転し、これに伴つて合成ベクトルT1,T2,T3
が0を固定点として伸縮したものである。 The observed values p, q, r are rotated by S2 around 01 in Fig. 2, and along with this, the resultant vectors T 1 , T 2 , T 3
is expanded and contracted using 0 as a fixed point.
従つて観測値p、q、rが同図破線の円周上に
存在し、かつαは半固定又は固定位相器11bと
11aの位相差、又βは半固定又は固定位相器1
1cと11bとの位相差に相当した値となること
から観測値p、q、rから逆に円C及びS2の回
転中心01が計算により求まる。これにより任意の
位相に対する合成ベクトルTも求めることができ
る。 Therefore, the observed values p, q, and r exist on the circumference indicated by the broken line in the figure, and α is the phase difference between the semi-fixed or fixed phase shifters 11b and 11a, and β is the phase difference between the semi-fixed or fixed phase shifts 11b and 11a.
Since the value corresponds to the phase difference between 1c and 11b, the center of rotation 01 of the circles C and S2 can be calculated from the observed values p, q, and r. Thereby, the composite vector T for any phase can also be determined.
Tの振幅の最大値と最小値及び最大値と最小値
となる時の位相からS1とS2の相対位相が計算
により求めることができる。 The relative phase of S1 and S2 can be calculated from the maximum and minimum values of the amplitude of T and the phases when the maximum and minimum values are reached.
具体的には第2図において合成ベクトルTが最
大値を与える位相をΔ0とすると、到来電波の相
対位相(S1とS2の相対位相X=φo−φ0)は次式
を用いて計算により求めることができる。 Specifically, in Figure 2, if the phase at which the combined vector T gives the maximum value is Δ 0 , then the relative phase of the incoming radio waves (relative phase of S 1 and S 2 X = φ o - φ 0 ) can be calculated using the following formula. It can be obtained by calculation.
X=tan-1sinΔ0/cosΔ0+S2/S1 ……(5)
S1とS2の相対位相が計算できれば直ちに(4)式を
用いて電波の到来方向を知ることができる。 X=tan -1 sinΔ 0 /cosΔ 0 +S 2 /S 1 (5) If the relative phase of S 1 and S 2 can be calculated, the direction of arrival of the radio wave can be immediately determined using equation (4).
ここでS1とS2の相対位相Xの導出過程について
以下に説明する。 Here, the process of deriving the relative phase X of S 1 and S 2 will be explained below.
第2図において初期状態の合成電界ベクトル
T〓2の振幅、位相をE0、φ0、着目する第n番目の
ベクトルS〓2bの振幅、位相をEo、φoとする。 In Fig. 2, the composite electric field vector in the initial state
The amplitude and phase of T〓 2 are E 0 and φ 0 , and the amplitude and phase of the n-th vector S〓 2b of interest are E o and φ o .
この第n番目のベクトルS〓2bの位相をφo+βに
設定固定とした時の合成ベクトルT〓3は次式で表
わされる。 When the phase of this n-th vector S〓 2b is set and fixed at φ o +β, the composite vector T〓 3 is expressed by the following equation.
T〓3=〔E0ej〓0−Eoej〓n〕+Eoej(〓n+〓)
X=φo−φ0とおくと
T〓3={E0−Eoej(〓n-〓0) +Eoej(〓n-〓0+〓)
}ej〓0
={E0+EoejX〔ej〓−1〕}ej〓0
={E0e-jX+Eo〔ej〓−1〕}ej(〓0+X)
=(E0cosX+Eocosβ−Eo)+j(−E0sinX
+Eosinβ)ej(X+〓0)
|T3|2=(E0cosX−Eo)2+2Eo(E0cosX
−Eo)cosβ+Eo 2+E0 2sin2X
−2E0EosinXsinβ
従つて
|T3|2/T2 2=〔cosX−Eo/E0〕2+sin2X+〔Eo
/E0〕2+2〔Eo/E0〕{〔cosX−Eo/E0〕cosβ−sinX
sinβ}
ここでk=Eo/E0
とおきY2=(cosX−k)2+sin2Xとすれば
|T3|2/T2 2=Y2+K2+2k{(cosX−k)cosβ−sin
Xsinβ)
|T3|2/T2 2=Qとおくと
Q=Y2+k2+2kYcos(β+Δ0) (5)
但し
tanΔ0=sinX/cosX−k (6)
が得られる。T〓 3 = [E 0 e j 〓 0 −E o e j 〓 n ]+E o e j( 〓 n+ 〓 ) If we set X=φ o −φ 0 , then T〓 3 = {E 0 −E o e j ( 〓 n- 〓 0) +E o e j( 〓 n- 〓 0+ 〓 )
}e j 〓 0 = {E 0 +E o e jX [e j 〓−1]}e j 〓 0 = {E 0 e -jX +E o [e j 〓−1]}e j( 〓 0+X) = (E 0 cosX + E o cosβ−E o ) + j (−E 0 sinX + E o sinβ) e j(X+ 〓 0) |T 3 | 2 = (E 0 cosX−E o ) 2 +2E o (E 0 cosX − E o ) cosβ + E o 2 + E 0 2 sin 2 _ _ _
/E 0 ] 2 + 2 [E o /E 0 ] {[cosX−E o /E 0 ]cosβ−sinX
sinβ } Here , if k = E o / E 0 and Y 2 = (cosX−k) 2 + sin 2 −sin
Xsinβ) |T 3 | 2 /T 2 2 =Q, then Q=Y 2 +k 2 +2kYcos (β+Δ 0 ) (5) where tanΔ 0 = sinX/cosX−k (6) is obtained.
Qの最大と最小の比をγとすると(5)式より
γ2=(Y+k)2/(Y−k)2
従つて
γ=±〔Y+k/Y−k〕 (7)
(7)式の右辺の符号が正の場合について(6)、(7)式
より、未知数であるk、Xを求める。 If the ratio of the maximum and minimum of Q is γ, then from equation (5), γ 2 = (Y+k) 2 / (Y-k) 2 Therefore, γ = ± [Y+k/Y-k] (7) In equation (7), When the sign on the right side is positive, the unknowns k and X are found from equations (6) and (7).
(7)式より Y=〔γ+1/γ−1〕k 展開して (cosX−k)2−sin2X=〔γ+1/γ−1〕2k2 (8) となる。 From equation (7), Y=[γ+1/γ−1]k is expanded to become (cosX−k) 2 −sin 2 X=[γ+1/γ−1] 2 k 2 (8).
(6)、(8)式より連立方程式を解くと、
k=Γ/(1+ΓcosΔ0+Γ2)1/2 (9)
X=tan-1〔sinΔ0/cosΔ0+Γ〕 (10)
但しΓ=γ−1/γ+1(γは最大、最小の比)
最大、最小の比γは
γ=S1+S2/S1−S2
従つて
Γ=γ−1/γ+1=S1+S2/S1−S2−1/S1+S2/
S1−S2+1=S2/S1
となり、(10)式は
X=tan-1sinΔ0/cosΔ0+S2/S1 (11)
となる。 Solving the simultaneous equations from equations (6) and (8), k=Γ/(1+ΓcosΔ 0 +Γ 2 ) 1/2 (9) X=tan -1 [sinΔ 0 /cosΔ 0 +Γ] (10) However, Γ= γ-1/γ+1 (γ is the ratio of maximum and minimum) The maximum and minimum ratio γ is γ=S 1 +S 2 /S 1 -S 2Therefore , Γ=γ-1/γ+1=S 1 +S 2 /S 1 −S 2 −1/S 1 +S 2 /
S 1 −S 2 +1=S 2 /S 1 , and equation (10) becomes X=tan −1 sinΔ 0 /cosΔ 0 +S 2 /S 1 (11).
[発明の効果]
以上のように、この発明によれば、位相受信機
を用いるかわりに、複数個の振幅受信機の出力レ
ベルの変化のデータから、到来電波の相対位相を
演算により求めている為、瞬探機能を保持しつつ
相対位相を精度よく求められ、確度の高い方探装
置を得ることができる効果がある。[Effects of the Invention] As described above, according to the present invention, instead of using a phase receiver, the relative phase of an incoming radio wave is calculated from data on changes in the output level of a plurality of amplitude receivers. Therefore, the relative phase can be determined with high accuracy while maintaining the instantaneous search function, and a highly accurate direction finding device can be obtained.
第1図は本発明のブロツク図、第2図は複数の
受信チヤンネルの各合成ベクトルの関係を説明す
る図、第3図は従来の方探装置のブロツク図であ
る。図中1,2は素子アンテナ、3は位相検波受
信機、4はコンソール、5,6は信号ケーブル、
7,8は電力分配器、9a,9b,9cは結合
器、10a,10b,10cは振幅受信機、11
a,11b,11cは半固定又は固定位相器、1
2,13,14はT1、T2、T3受信チヤンネルで
ある。なお、図中同一あるいは相当部分には同一
符号を付して示してある。
FIG. 1 is a block diagram of the present invention, FIG. 2 is a diagram illustrating the relationship between composite vectors of a plurality of receiving channels, and FIG. 3 is a block diagram of a conventional direction finding device. In the figure, 1 and 2 are element antennas, 3 is a phase detection receiver, 4 is a console, 5 and 6 are signal cables,
7, 8 are power dividers, 9a, 9b, 9c are combiners, 10a, 10b, 10c are amplitude receivers, 11
a, 11b, 11c are semi-fixed or fixed phase shifters, 1
2, 13, and 14 are T 1 , T 2 , and T 3 receiving channels. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.
Claims (1)
テナと、上記第1及び第2の素子アンテナで受信
した信号の相対位相を検出する回路を有し、上記
相対位相から電波の到来方向を演算するコンソー
ルとからなる方探装置において、上記第1の素子
アンテナで受信した信号を分配する第1の電力分
配器と、上記第2の素子アンテナで受信した信号
を分配する第2の電力分配器と、上記第2の電力
分配器により分配された複数の信号のそれぞれ位
相を異ならしめる複数の半固定又は固定位相器
と、上記複数の半固定又は固定位相器によりそれ
ぞれ異なつた位相偏位を受けたそれぞれの出力信
号と上記第1の電力分配器により分配されたそれ
ぞれの信号をベクトル合成する複数の結合器と、
上記複数の結合器から出たレベルの異なる複数の
信号を受信する複数の振幅受信機とそれぞれ異な
る受信レベルの差から第1及び第2の素子アンテ
ナに到来する信号の相対位相及び到来方向を演算
するコンソールを有することを特徴とする方探装
置。1 It has first and second element antennas that receive incoming radio waves, and a circuit that detects the relative phase of the signals received by the first and second element antennas, and calculates the direction of arrival of the radio waves from the relative phase. A direction finding device comprising a console that distributes signals received by the first element antenna, and a second power divider that distributes signals received by the second element antenna. , a plurality of semi-fixed or fixed phase shifters that make the phases of the plurality of signals distributed by the second power divider different, and a plurality of semi-fixed or fixed phase shifters that receive different phase deviations, respectively. a plurality of combiners that vector-combine the respective output signals and the respective signals distributed by the first power divider;
A plurality of amplitude receivers receive a plurality of signals with different levels output from the plurality of couplers, and the relative phase and direction of arrival of the signals arriving at the first and second element antennas are calculated from the difference between the respective different reception levels. A direction finding device characterized by having a console for.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8343886A JPS62239074A (en) | 1986-04-11 | 1986-04-11 | Direction finder |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8343886A JPS62239074A (en) | 1986-04-11 | 1986-04-11 | Direction finder |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62239074A JPS62239074A (en) | 1987-10-19 |
| JPH0549070B2 true JPH0549070B2 (en) | 1993-07-23 |
Family
ID=13802433
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8343886A Granted JPS62239074A (en) | 1986-04-11 | 1986-04-11 | Direction finder |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62239074A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62240880A (en) * | 1986-04-14 | 1987-10-21 | Mitsubishi Electric Corp | Direction finder |
-
1986
- 1986-04-11 JP JP8343886A patent/JPS62239074A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62239074A (en) | 1987-10-19 |
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