JPH0257876B2 - - Google Patents
Info
- Publication number
- JPH0257876B2 JPH0257876B2 JP58128517A JP12851783A JPH0257876B2 JP H0257876 B2 JPH0257876 B2 JP H0257876B2 JP 58128517 A JP58128517 A JP 58128517A JP 12851783 A JP12851783 A JP 12851783A JP H0257876 B2 JPH0257876 B2 JP H0257876B2
- Authority
- JP
- Japan
- Prior art keywords
- pulse
- radar
- signal
- output
- switch
- 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.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S13/00—Systems 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
- G01S13/88—Radar or analogous systems specially adapted for specific applications
- G01S13/89—Radar or analogous systems specially adapted for specific applications for mapping or imaging
- G01S13/90—Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S13/00—Systems 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
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
- G01S13/06—Systems determining position data of a target
- G01S13/08—Systems for measuring distance only
- G01S13/10—Systems for measuring distance only using transmission of interrupted, pulse modulated waves
- G01S13/26—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave
- G01S13/28—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave with time compression of received pulses
Landscapes
- Engineering & Computer Science (AREA)
- Remote Sensing (AREA)
- Radar, Positioning & Navigation (AREA)
- Physics & Mathematics (AREA)
- Computer Networks & Wireless Communication (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】
この発明は航空機等の飛しよう体に搭載され地
上をマツピングする合成開口レーダに関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a synthetic aperture radar that is mounted on a flying object such as an aircraft and maps the ground.
まず、従来のこの種の合成開口レーダの構成と
原理について説明する。第1図は従来の合成開口
レーダの構成を示すブロツク図、第2図はレーダ
を搭載した航空機又は飛しよう体と目標との幾何
学的関係を表わす図、第3図は受信エコーのタイ
ミングを表わす図、第4図および第5図はレンジ
ウオーク補償を表わす図である。以下順を追つて
各図の説明をする。 First, the configuration and principle of a conventional synthetic aperture radar of this type will be explained. Figure 1 is a block diagram showing the configuration of a conventional synthetic aperture radar, Figure 2 is a diagram showing the geometric relationship between an aircraft or flying object equipped with the radar and a target, and Figure 3 shows the timing of received echoes. Figures 4 and 5 are diagrams representing range walk compensation. Each figure will be explained in order below.
さて、第1図に於いて、コヒーレント信号発生
器1より出力されたIF(Intermediate
Frequency)帯のCW信号はパルス伸長装置2に
入力されここで一定時間T内で時間と共に周波数
が変化するチヤープ信号(チヤープ帯域幅=B)
又は符号パルス系列が得られる。このとき、上記
チヤープ信号又は符号パルス系列はトリガ信号発
生器15からのトリガ信号に同期して発生される
ものとする。パルス伸長装置2の出力はミキサ3
で安定化局部発振器4からのRF(Radio
Frequency)信号と混合され高出力増輻器5で高
出力化された後、送受切換器6,アンテナ7を経
て電波となつて空間に放射される。目標で反射さ
れた電波は再びアンテナ7、送受切換器6を経て
ミキサ3に入力され、ここで安定化局部発振器4
からのRF信号と混合されてIF帯の信号となる。 Now, in Fig. 1, the IF (Intermediate
The CW signal in the Frequency) band is input to the pulse stretcher 2, where it receives a chirp signal (chirp bandwidth = B) whose frequency changes with time within a certain time T.
Or a coded pulse sequence can be obtained. At this time, it is assumed that the chirp signal or code pulse sequence is generated in synchronization with the trigger signal from the trigger signal generator 15. The output of the pulse stretcher 2 is the mixer 3.
RF (Radio) from local oscillator 4 stabilized by
After being mixed with a frequency (frequency) signal and increased in output by a high-output amplifier 5, it passes through a transmitter/receiver switch 6 and an antenna 7, and is radiated into space as a radio wave. The radio waves reflected by the target are inputted again to the mixer 3 via the antenna 7 and the transmitter/receiver switch 6, where they are input to the stabilized local oscillator 4.
It is mixed with the RF signal from the IF band and becomes an IF band signal.
上記IF帯の信号はIF増幅器8で増幅された後
パルス圧縮装置9でレンジ方向にチヤープ信号で
はほぼ1/Bに符号パルス系列の場合ではサブパ
ルスの幅τsに圧縮される。 The IF band signal is amplified by an IF amplifier 8, and then compressed in the range direction by a pulse compressor 9 to approximately 1/B in the case of a chirp signal and to a sub-pulse width τ s in the case of a code pulse sequence.
上記、圧縮された信号は位相検波器10aでコ
ヒーレント信号発生器1からの信号で位相検波さ
れれる。同時にコヒーレント信号発生器1からの
信号は90゜移相器11を経て位相検波器10bに
入力される。 The compressed signal is subjected to phase detection using the signal from the coherent signal generator 1 by the phase detector 10a. At the same time, the signal from the coherent signal generator 1 passes through a 90° phase shifter 11 and is input to the phase detector 10b.
位相検波器10bに入力された上記圧縮された
信号は90゜移相器からの出力により位相検波され
る。位相検波器10a及び10bの出力は各々ゲ
ート回路12a,12bに入力されてゲーテイン
グされた後アジマス圧縮装置13に入力される。
アジマス圧縮装置では種々のアジマス方向に存在
する目標からのレーダエコーのドツプラー周波数
が異なることを利用して目標をアジマス方向で分
離してアジマス分解能を向上させる。このように
して得られた信号を表示装置14に入力してレン
ジ方向及びアジマス方向共に高い分解能の画像を
得る。 The compressed signal inputted to the phase detector 10b is phase detected by the output from the 90° phase shifter. The outputs of the phase detectors 10a and 10b are input to gate circuits 12a and 12b, respectively, and after being gated, are input to the azimuth compression device 13.
The azimuth compression device uses the fact that the Doppler frequencies of radar echoes from targets existing in various azimuth directions are different to separate targets in the azimuth direction and improve azimuth resolution. The signals thus obtained are input to the display device 14 to obtain high resolution images in both the range direction and the azimuth direction.
第2図に示す慣性座標系xyzにおいてxy面内の
点目標(P(説明の便宜上xy面内に1個のみ存在
するものとするが特に一般性は失われない)が原
点からのrの距離、y軸からθの角度に存在し航
空機に搭載されたレーダ装置Rにより点目標Pを
観測するものとする。このとき航空機はy軸に平
行に一定の高度hで一定速度Vで飛行し、t=0
では座標(0,0,h)の位置に存在するものと
仮定する。第3図に示ようにt=0でレーダ装置
Rより送信された送信パルス(イ・a)に対しパ
ルス圧縮装置9の出力における点目標Pからの受
信エコー(ロ・a)は
τ0=2/c√2 2+2 2+2 (1)
で与えられる時間だけ遅延してレーダ装置Rで受
信される。ここにCは光速である。レーダ装置R
の送信パルスの繰返し周期をTとすればt=Tで
レーダ装置Rより送信された送信パルス(イ・
b)に対し、パルス圧縮装置9の出力における点
目標Pからの受信エコー(ロ・b)は
τ1=2/c√2 2+(−)2
+2(2)
で与えられる時間だけ遅延してレーダ装置Rで受
信される。同様にしてNTを合成開口時間とすれ
ばt=NTで送信された送信パルス(イ・d)で
は
τN=2/c√2 2+(−
)2+2(3)
で与えられる時間だけ遅延してパルス圧縮装置9
の出力における点目標Pからのエコー(ロ・d)
が受信される。このようにパルス圧縮装置9の出
力における点目標Pからのエコーをゲート回路1
2a及び12bによつて抽出するためには航空機
の移動に共なつてゲートの位置を動かす必要があ
る。例えば第4図および第5図はこの様子を表し
ており、100,1,100,2,…,100,
N+1はメモリ例えばシフトレジスタの如きもの
でT1,T2…,TLはレンジ方向に存在するL個の
目標からのパルス圧縮装置9の出力におけるエコ
ー信号を表わす。(この場合ではL個の複数目標
について説明する)
上記メモリは左から入力され右に順次移動するも
のと仮定する。 In the inertial coordinate system xyz shown in Figure 2, a point target (P (for convenience of explanation, it is assumed that only one object exists in the xy plane, but the generality is not lost) in the xy plane is at a distance of r from the origin. , a point target P exists at an angle θ from the y-axis and is observed by a radar device R mounted on the aircraft.At this time, the aircraft flies parallel to the y-axis at a constant altitude h and a constant speed V, t=0
Assume that it exists at the coordinates (0, 0, h). As shown in FIG. 3, for the transmitted pulse (a) transmitted from the radar device R at t=0, the received echo (b・a) from the point target P at the output of the pulse compression device 9 is τ 0 = 2/c√ 2 2 + 2 2 + 2 (1) The signal is received by the radar device R after being delayed by the time given by 2/c√ 2 2 + 2 2 + 2 (1). Here C is the speed of light. Radar device R
If the repetition period of the transmission pulse is T, then the transmission pulse (I) transmitted from the radar device R at t=T is
For b), the received echo (lo b) from the point target P at the output of the pulse compression device 9 is τ 1 = 2/c√ 2 2 + (-) 2
+ 2 (2) is received by the radar device R with a delay of the time given by (2). Similarly, if NT is the synthetic aperture time, then τ N =2/c√ 2 2 + (-
) 2 + 2 (3)
The echo from the point target P at the output of
is received. In this way, the echo from the point target P in the output of the pulse compression device 9 is transmitted to the gate circuit 1.
2a and 12b, it is necessary to move the gate position as the aircraft moves. For example, FIGS. 4 and 5 show this situation, and 100, 1, 100, 2, ..., 100,
N+1 is a memory such as a shift register, and T 1 , T 2 . . . , T L represent echo signals at the output of the pulse compressor 9 from L targets existing in the range direction. (In this case, L plural targets will be explained.) It is assumed that the above memory is inputted from the left and sequentially moved to the right.
第4図において、(a)はt=0で送信されたとき
のL個の目標からのエコー信号がメモリ100,
1に記憶されており、(b)はt=Tで送信されたと
きのL個の目標からのエコー信号がメモリ10
0,2に記憶されている様子を表わす。以下同様
にt=2Tで送信されたときのエコー信号はメモ
リ100,3に記憶され、t=NTではメモリ1
00,N+1に記憶されるものとする。第4図か
ら明らかなようにt=0からt=NTまでの間に
目標からのエコー信号は第2図に示すようにレー
ダ装置Rを搭載した航空機の前方に目標を捕え、
合成開口時間が短いものとすれば、これらの目標
とレーダ装置R迄の距離が短くなるにつれ徐々に
左に移動する。このため同一の目標からのエコー
信号に対しては第5図に示すように同一のレンジ
ビンに来るように上記メモリ内で転送する必要が
ある。これによりアジマス圧縮装置13では同一
目標の情報がメモリ100,1からメモリ10
0,N+1にわたつて同一のレンジビンに存在さ
せるようにできるので、(N+1)個の同一のヒ
ワジビンの各々の情報に所定の位相補償を施すこ
とにより、アジマス方向に圧縮することができ
る。 In FIG. 4, (a) shows that the echo signals from L targets when transmitted at t=0 are stored in the memory 100,
(b) shows that the echo signals from L targets when transmitted at t=T are stored in the memory 10.
0 and 2 are stored. Similarly, the echo signal transmitted at t=2T is stored in memories 100 and 3, and at t=NT, the echo signal is stored in memory 100 and 3.
00, N+1. As is clear from FIG. 4, the echo signal from the target from t=0 to t=NT captures the target in front of the aircraft equipped with radar device R, as shown in FIG.
Assuming that the synthetic aperture time is short, as the distances between these targets and the radar device R become shorter, they gradually move to the left. For this reason, it is necessary to transfer echo signals from the same target within the memory so that they come to the same range bin as shown in FIG. As a result, in the azimuth compression device 13, information for the same target is transferred from the memory 100,1 to the memory 10.
0 and N+1 can be made to exist in the same range bin, so by applying a predetermined phase compensation to the information of each of the (N+1) identical range bins, it is possible to compress the information in the azimuth direction.
この発明はこれらの欠点を改善するためパルス
圧縮装内にスイツチを設けたもので以下図面につ
いて詳細に説明する。 The present invention provides a switch within the pulse compression device in order to overcome these drawbacks, and will be described in detail below with reference to the drawings.
第6図はこの発明の実施例であつて21はタツ
プ付遅延線又はタツプ付シフトレジスタ,16は
移相器,17は各移相器からの出力の和を求める
もので例えば加算器などが考えられる。18は第
1図におけるIF増幅器8の出力,19は第1図
におけるパルス圧縮装置9の出力,20は各移相
器16の入力端をコモンとしてタツプ付遅延線又
はタツプ付シフトレジスタの各タツプ点を切換え
ることのできるもの例えばスイツチである。21
の各タツプはチヤープ信号ではチヤープ帯域幅B
の逆数、符号化パルス系列ではサブパルス幅τsに
対応する時間だけ遅延しているものとする。 FIG. 6 shows an embodiment of the present invention, in which 21 is a tapped delay line or a tapped shift register, 16 is a phase shifter, and 17 is a device for calculating the sum of outputs from each phase shifter, such as an adder. Conceivable. 18 is the output of the IF amplifier 8 in FIG. 1, 19 is the output of the pulse compression device 9 in FIG. An example of something that can change the point is a switch. 21
Each tap in the chirp signal has a chirp bandwidth B
It is assumed that the encoded pulse sequence is delayed by a time corresponding to the sub-pulse width τ s .
さて、第2図において航空機に搭載されたレー
ダ装置Rの移動に共なつて点目標Pからの受信エ
コーはt=nTで送信された送信パルスに対し
τo=2/c√2 2+(−
)2+2(4)
で与えられる時間だけ遅延してレーダ装置Rで受
信される。合成開口時間中に(N+1)個のパル
スが送信されるものとすればn=N/2+1のとき
の遅延時間τN/2+1を基準にして
NG=τo−τN/2+1/τ0 (5)
で与えられるゲート数のずれNGを求める。ここ
に〔 〕はガウス記号,τ0はチヤープ信号では
1/B、符号パルス系列ではτsである。 Now, in Fig. 2, as the radar device R mounted on the aircraft moves, the received echo from the point target P becomes τ o = 2/c√ 2 2 + ( −
) 2 + 2 (4) It is received by the radar device R with a delay of the time given by (4). If (N+1) pulses are transmitted during the synthetic aperture time, then based on the delay time τ N/2+ 1 when n=N/2+1, N G =τ o −τ N/2+ 1 /τ 0 (5) Find the deviation N G in the number of gates given by: Here, [ ] is a Gaussian symbol, τ 0 is 1/B for the chirp signal, and τ s for the code pulse sequence.
まずIF増幅器の出力18はタツプ付遅延線又
はタツプ付シフトレジスタ21に入力される。こ
のとき、式(5)のNGが最大のとき即ちn=0では
第6図に示すように各スイツチ20の接点はすべ
て左側に倒れており、NGの値が1減少するにつ
れて各スイツチ20の接点を現在の右隣側に移動
させる。これらのスイツチ20の出力を予めチヤ
ープ信号又は符号サブパルスの符号より設定され
る位相を有した移相器16を通して加算器17に
より和を求めれば航空機の移動にも拘わらず送信
パルスに対し一定の時間遅延した位置に圧縮した
パルスをつくることができる。この出力19は従
来の位相検波器10a,10bに入力として用い
られる。スイツチ20の切換えはすべて制御装置
22において式(4),式(5)を計算して得られる結果
に基ずいて発生さた制御信号に従つて制御され
る。 First, the output 18 of the IF amplifier is input to a tapped delay line or tapped shift register 21. At this time, when N G in equation (5) is maximum, that is, when n = 0, all the contacts of each switch 20 are tilted to the left as shown in FIG. 6, and as the value of N G decreases by 1, each switch Move the contact point 20 to the right side of the current location. If the outputs of these switches 20 are passed through a phase shifter 16 whose phase is set in advance by the sign of the chirp signal or code sub-pulse and the sum is calculated by an adder 17, a constant time period relative to the transmitted pulse can be obtained regardless of the movement of the aircraft. A compressed pulse can be created at a delayed position. This output 19 is used as an input to a conventional phase detector 10a, 10b. All switching of the switch 20 is controlled in accordance with a control signal generated by the control device 22 based on the results obtained by calculating equations (4) and (5).
以上のようにこの発明に係る合成開口レーダで
はパルス圧縮装置内のタツプ付遅延線又はタツプ
付遅延線における各タツプ出力にスイツチを設け
これを航空機に搭載されたレーダの移動につれて
スイツチで各タツプ出力を切換えることによつて
目標からのレーダエコーを同一レンジビンに位置
させることができ、アジマス圧縮の信号処理を容
易にする利点がある。 As described above, in the synthetic aperture radar according to the present invention, a switch is provided for each tap output in the tapped delay line or tapped delay line in the pulse compression device, and the switch is used to adjust each tap output as the radar mounted on the aircraft moves. By switching, the radar echoes from the target can be located in the same range bin, which has the advantage of facilitating signal processing for azimuth compression.
第1図は従来の合成開口レーダの構成を示すブ
ロツク図、第2図はレーダを搭載した航空機又は
飛しよう体と目標との幾何学的関係を表わす図、
第3図は受信エコーのタイミングを表わす図、第
4図および第5図はレンジウオーク補償を表わす
図、第6図は本発明によるパルス圧縮装置を示す
図である。
1はコヒーレント信号発生器、2はパルス伸長
装置、3はミキサ、4は安定化局部発振器、5は
高出力増幅器、6は送受切換器、7はアンテナ、
8はIF増幅器、9はパルス圧縮装置、10は位
相検波器、11は90゜移相器、12はゲート回路、
13はアジマス圧縮装置、14は表示装置、15
はトリガ信号発生器、16は移相器、17は加算
器、18はIF増幅器の出力、19は加算器出力、
20はスイツチ、21はタツプ付遅延線又はタツ
プ付シフトレジスタ、22は制御装置、Rはレー
ダ装置、Pは点目標、イ,a,イ,b,イ,c,
イ,dは送信パルス、ロ,a,ロ,b,ロ,c,
ロ,dは受信エコー、100,1〜100,N+
1はメモリである。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 showing the configuration of a conventional synthetic aperture radar, and FIG. 2 is a diagram showing the geometric relationship between an aircraft or flying object equipped with the radar and a target.
FIG. 3 is a diagram showing the timing of received echoes, FIGS. 4 and 5 are diagrams showing range walk compensation, and FIG. 6 is a diagram showing a pulse compression device according to the present invention. 1 is a coherent signal generator, 2 is a pulse stretcher, 3 is a mixer, 4 is a stabilizing local oscillator, 5 is a high output amplifier, 6 is a transmission/reception switch, 7 is an antenna,
8 is an IF amplifier, 9 is a pulse compression device, 10 is a phase detector, 11 is a 90° phase shifter, 12 is a gate circuit,
13 is an azimuth compression device, 14 is a display device, 15
is a trigger signal generator, 16 is a phase shifter, 17 is an adder, 18 is the output of the IF amplifier, 19 is the adder output,
20 is a switch, 21 is a delay line with taps or a shift register with taps, 22 is a control device, R is a radar device, P is a point target, a, a, b, b, a, c,
A, d are transmission pulses, b, a, b, b, b, c,
b, d is received echo, 100, 1 to 100, N+
1 is memory. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.
Claims (1)
装置を用いた合成開口レーダにおいて、パルス圧
縮装置としてタツプ付遅延線又はタツプ付シフト
レジスタと上記の各タツプの出力端に取り付けた
スイツチと、上記各スイツチの出力端に取り付け
た移相器と、上記移相器の出力端に加算器を設け
て、航空機又は飛しよう体に搭載されたレーダ装
置の移動につれて制御装置からの制御信号に従つ
て上記移相器と上記タツプとの接続が上記スイツ
チによつて切換えられることを特徴とする合成開
口レーダ。1. In a synthetic aperture radar that uses a pulse compression device to increase the resolution in the range direction, the pulse compression device includes a delay line with taps or a shift register with taps, a switch attached to the output end of each of the above taps, and each of the above switches. a phase shifter attached to the output end of the phase shifter, and an adder installed at the output end of the phase shifter to adjust the shift according to the control signal from the control device as the radar device mounted on the aircraft or flying object moves. A synthetic aperture radar characterized in that the connection between the phase converter and the tap is switched by the switch.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58128517A JPS6020167A (en) | 1983-07-14 | 1983-07-14 | Synthetic-aperture radar |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58128517A JPS6020167A (en) | 1983-07-14 | 1983-07-14 | Synthetic-aperture radar |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6020167A JPS6020167A (en) | 1985-02-01 |
| JPH0257876B2 true JPH0257876B2 (en) | 1990-12-06 |
Family
ID=14986692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58128517A Granted JPS6020167A (en) | 1983-07-14 | 1983-07-14 | Synthetic-aperture radar |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6020167A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08318495A (en) * | 1995-05-20 | 1996-12-03 | Koenig & Bauer Albert Ag | Cutting device |
-
1983
- 1983-07-14 JP JP58128517A patent/JPS6020167A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08318495A (en) * | 1995-05-20 | 1996-12-03 | Koenig & Bauer Albert Ag | Cutting device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6020167A (en) | 1985-02-01 |
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