JP2582556B2 - MTI pulse radar device - Google Patents
MTI pulse radar deviceInfo
- Publication number
- JP2582556B2 JP2582556B2 JP61196869A JP19686986A JP2582556B2 JP 2582556 B2 JP2582556 B2 JP 2582556B2 JP 61196869 A JP61196869 A JP 61196869A JP 19686986 A JP19686986 A JP 19686986A JP 2582556 B2 JP2582556 B2 JP 2582556B2
- Authority
- JP
- Japan
- Prior art keywords
- phase
- signal
- pulse
- mti
- transmission pulse
- 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 - Fee Related
Links
Landscapes
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は,航空機等の移動目標のみを検出するMTIレ
ーダ装置に関するものである。Description: TECHNICAL FIELD The present invention relates to an MTI radar device that detects only a moving target such as an aircraft.
(従来の技術) 従来のMTIレーダ装置は,第2図に示すような回路構
成を用いている。すなわち,マグネトロン1から出た高
周波のパルス信号は,方向性結合器2を介して送信信号
の一部を取り出され,安定化局部発振器7の出力と6の
混合器1で混合され,送信信号の位相情報を持った位相
引き込み信号が得られる。この信号を使って送信信号に
コヒーレントな基準信号をコヒーレント発振器10で作
る。アンテナ4からの受信信号はサーキュレータ3を通
り安定化局部発振器7の出力と8の混合器2で混合さ
れ,IF増幅器9で増幅された後,二分された位相検波器1
1および12に入る。コヒーレント発振器10で得られた基
準信号も二分され,一方は位相検波器11に入力され,他
方は90°ハイブリッド13で90°だけ位相をずらされて位
相検波器12に入り,受信信号は位相検波される。位相検
波器11,12の出力をI(In-phase)チャンネルビデオ,
およびQ(Quadrature)チャンネルビデオと呼び,消去
器14で固定物体からの反射信号が消去され,移動物体だ
けが取り出されたMTIビデオ15が得られる。(Prior Art) A conventional MTI radar device uses a circuit configuration as shown in FIG. That is, a high-frequency pulse signal output from the magnetron 1 is partially extracted from the transmission signal via the directional coupler 2 and mixed with the output of the stabilized local oscillator 7 by the mixer 1 of 6 to obtain the transmission signal. A phase pull-in signal having phase information is obtained. Using this signal, a coherent oscillator 10 creates a reference signal that is coherent to the transmission signal. The received signal from the antenna 4 passes through the circulator 3 and is mixed with the output of the stabilized local oscillator 7 by the mixer 2 of 8 and amplified by the IF amplifier 9 and then divided into two by the phase detector 1
Enter 1 and 12. The reference signal obtained by the coherent oscillator 10 is also bisected, one is input to the phase detector 11, and the other is shifted in phase by 90 ° by the 90 ° hybrid 13 and enters the phase detector 12, and the received signal is subjected to phase detection. Is done. Outputs of the phase detectors 11 and 12 are I (In-phase) channel video,
And Q (Quadrature) channel video, the reflected signal from the stationary object is eliminated by the erasure unit 14, and the MTI video 15 from which only the moving object is extracted is obtained.
(発明が解決しようとする問題点) 従来のこの種のMTIレーダ受信機では,十分に周波数
の安定なコヒーレント発振器が得られないこと,特に,
送信パルス幅が短くなるとコヒーレントな発振が非常に
難しくなること,および精度を要求されるレーダでは増
幅型送信機を使い,非常に高価になるという欠点があっ
た。(Problems to be solved by the invention) With this type of conventional MTI radar receiver, a coherent oscillator with sufficiently stable frequency cannot be obtained.
Shorter transmission pulse widths make coherent oscillation very difficult, and radars that require precision use amplifier-type transmitters and are very expensive.
(問題点を解決するための手段) 本発明の目的は,前述従来技術の欠点を解消するため
になされたものであって,高安定な発振器を基準信号発
生源とし,送信パルスと受信パルスとのコヒーレンスを
送信パルスの位相検波出力と受信信号の位相検波出力と
の間で複素乗算を行い,両者の位相差を取り出すことに
よって,マグネトロンを使用しながらも高安定で且つ高
精度のMTIパルスレーダ装置を提供することにある。(Means for Solving the Problems) An object of the present invention is to solve the above-mentioned drawbacks of the prior art, in which a highly stable oscillator is used as a reference signal source, and a transmission pulse and a reception pulse are used. Complex multiplication between the phase detection output of the transmission pulse and the phase detection output of the received signal to obtain the phase difference between the two, thereby obtaining a highly stable and accurate MTI pulse radar using a magnetron. It is to provide a device.
(実施例) 以下第1図に示す本発明の一実施例につき詳説する。Embodiment An embodiment of the present invention shown in FIG. 1 will be described in detail below.
図において,1はマグネトロン,2は方向性結合器,3はサ
ーキュレータ,4はアンテナ,5は変調器,6は送信パルスを
中間周波数に変換する混合器1,7は安定化局部発振器,8
は受信パルスを中間周波数に変換する混合器2,9はIF増
幅器,101は水晶発振器,102,103,11,12は位相検波器1〜
4,13は信号の位相を90°ずらす90°ハイブリッド,104〜
107はAD変換器1〜4,108は複素乗算器,14は消去器,15は
MTIビデオ出力端子である。In the figure, 1 is a magnetron, 2 is a directional coupler, 3 is a circulator, 4 is an antenna, 5 is a modulator, 6 is a mixer that converts transmission pulses to an intermediate frequency, 1 is a stabilized local oscillator, and 8 is
Are mixers 2 and 9 for converting received pulses to an intermediate frequency, IF amplifiers 101, crystal oscillators 101, 102, 103, 11, 12 are phase detectors 1 to
4,13 are 90 ° hybrids that shift the signal phase by 90 °, 104 ~
107 is an AD converter 1-4, 108 is a complex multiplier, 14 is an erasure device, 15 is
MTI video output terminal.
マグネトロン1からの送信パルスは方向性結合器2を
介して送信信号の一部が取り出され,安定化局部発振器
7の出力と6の混合器1で混合され,中間周波数に変換
される。アンテナ4からの受信信号はサーキュレータ3
を通り安定化局部発振器7の出力と8の混合器2で混合
され,中間周波数に変換され,IF増幅器9で十分に増幅
される。中間周波数に変換された送信パルスと受信信号
は二分され,それぞれ102,103および11,12で示される位
相検波器に入る。水晶発振器101を使った基準信号は十
分に安定で中間周波数と同じ発振周波数を使用する。基
準信号は二分され他方は90°ハイブリッド13で位相を90
°ずらされ,位相検波器103,12に入力する。送信パルス
を位相検波後104,105のAD変換器1,2でAD変換された信号
をそれぞれIt,Qt,受信パルスを位相検波後106,107のA
D変換器3,4でAD変換された信号をIr,Qrとし,複素信号
と考えればZr=Ir+JQr,Zt=It+JQtとなる。なおIt,
Qtについては送信ごとに1回だけ送信パルスをAD変換す
る。A part of the transmission pulse from the magnetron 1 is taken out through the directional coupler 2 and mixed with the output of the stabilized local oscillator 7 in the mixer 1 and converted into an intermediate frequency. The received signal from the antenna 4 is transmitted to the circulator 3
, And is mixed with the output of the stabilized local oscillator 7 by the mixer 2 of 8, converted to an intermediate frequency, and sufficiently amplified by the IF amplifier 9. The transmission pulse and the reception signal converted to the intermediate frequency are bisected and enter the phase detectors indicated by 102, 103 and 11, 12, respectively. The reference signal using the crystal oscillator 101 is sufficiently stable and uses the same oscillation frequency as the intermediate frequency. The reference signal is bisected and the other is 90 ° hybrid 13 with phase 90
And is input to the phase detectors 103 and 12. After the transmission pulse is phase-detected, the signals AD-converted by the AD converters 1 and 2 at 104 and 105 are respectively I t and Q t , and the reception pulse is subjected to phase detection at A and 106 at 107.
The signals AD-converted by the D converters 3 and 4 are I r and Q r , and if they are considered to be complex signals, Z r = I r + JQ r and Z t = I t + JQ t . Note that I t ,
For Q t is only once transmitted pulse AD conversion for each transmission.
高周波での送信パルスと受信パルスとのコヒーレンス
は取れているが,中間周波数では位相のそろっていない
基準信号で位相検波するためにZr,Ztは送信ごとに位相
がランダムになる。しかしながら,Zr,とZtの角度差は
Zrが固定物体からの受信信号であれば一定となる。また
移動物体であれば受信信号はドプラ効果により周波数が
変化し,ZrとZtの角度差はドプラの周期で変化する。MT
Iレーダで欲しい情報はZrとZtの角度差であり,それはZ
rとZtの複素共役なZr *との積により得られる。このこ
とは,Zr=r1eJQ1,Zt=r2eJQ2とすればZrZt *=r1r2e
J(θ1−θ2)となりZrとZtの角度差が求まることが
わかる。送信パルスの振幅 は通常一定であるが,マグネトロンの出力が電源変動等
で振幅が変わってもr2 2で除算しておけばマグネトロン
の出力変動の補正が可能である。While coherence between the transmission pulses at a high frequency and the received pulse are taken, Z r, Z t the phase for each transmission is randomly to phase detection by the reference signal without phase alignment at an intermediate frequency. However, the angular difference of Z r, and Z t is
If Zr is a received signal from a fixed object, it is constant. The received signal if the moving object is the frequency changes by the Doppler effect, the angle difference between the Z r and Z t varies with a period of Doppler. MT
I want information I radar is the angle difference between the Z r and Z t, it Z
a complex conjugate of r and Z t obtained by the product of the Z r *. This means that, if Z r = r 1 e JQ1, Z t = r 2 e JQ2 Z r Z t * = r 1 r 2 e
J (θ 1 -θ 2) it can be seen that the angular difference between the next Z r and Z t are obtained. Transmit pulse amplitude Is usually constant, the output power fluctuation of the magnetron can be corrected division to Oke if magnetron output varies r 2 2 be varied in amplitude.
複素乗算器108で得られるIチャンネルビデオおよび
Qチャンネルビデオは,I=IrIt+QrQt,Q=ItQr-IrQtと
なり,この信号を使って消去器14を通せば固定物体から
の反射信号が消去され,移動物体からの反射信号だけが
検出されたMTIビデオが得られる。I channel video and Q channel video obtained by the complex multiplier 108, I = I r I t + Q r Q t, Q = I t Q r -I r Q t , and the passed, canceller 14 uses this signal For example, an MTI video in which the reflection signal from the fixed object is eliminated and only the reflection signal from the moving object is detected is obtained.
以上述べた実施例においては高周波パルス発振源とし
てマグネトロンの場合で説明してあるが,ガン発振器等
を用いたパルス発振源を使用するMTIレーダ装置にも適
用できる。In the above-described embodiment, the case where the magnetron is used as the high-frequency pulse oscillation source has been described.
(発明の効果) 以上説明したようにマグネトロンを使ったパルスレー
ダで高安定,高精度の位相検波出力が得られることか
ら,航空管制用レーダ,気象用ドプラレーダ等コヒーレ
ントビデオを使用するレーダでクライストロンのように
高価な増幅型送信機を使用しなくてもよいことから,低
価格化に寄与できるという利点があり,さらに舶用レー
ダのように普及されている分野にも適用され,MTIのよう
な高度な処理が可能になる。(Effects of the Invention) As described above, a highly stable and highly accurate phase detection output can be obtained with a pulse radar using a magnetron. This eliminates the need for expensive amplifier-type transmitters, thus contributing to lower prices. It is also applied to fields that are widely used, such as marine radars. Processing can be performed.
第1図は本発明の一実施例を示すブロック回路図,及び
第2図は従来のMTIパルスレーダ装置を示すブロック回
路図である。 1……マグネトロン,2……方向性結合器,3……サーキュ
レータ,4……アンテナ,5……変調器,6……混合器1,7…
…安定化局部発振器,8……混合器2,9……IF増幅器,10…
…コヒーレント発振器,11〜12……位相検波器1,2,13…
…90°ハイブリッド,14……消去器,15……MTIビデオ出
力,101……水晶発振器,102,103……位相検波器3,4,104
〜107……AD変換器1〜4,108……複素乗算器。FIG. 1 is a block circuit diagram showing one embodiment of the present invention, and FIG. 2 is a block circuit diagram showing a conventional MTI pulse radar device. 1 ... magnetron, 2 ... directional coupler, 3 ... circulator, 4 ... antenna, 5 ... modulator, 6 ... mixer 1,7 ...
... stabilized local oscillator, 8 ... mixer 2,9 ... IF amplifier, 10 ...
… Coherent oscillators, 11-12 …… Phase detectors 1, 2, 13…
... 90 ° hybrid, 14 ... Eraser, 15 ... MTI video output, 101 ... Crystal oscillator, 102,103 ... Phase detector 3,4,104
... 107 AD converters 1-4,108 ... Complex multipliers.
Claims (1)
レントな基準信号により位相検波し、抽出した位相情報
により固定物体からの反射信号を消去して移動物体から
の反射信号のみを取り出すよう構成されたMTIパルスレ
ーダ装置において、位相検波器の基準信号を得るために
送信パルスと位相のそろっていない連続信号を出力する
高安定な発振器と、該発振器の出力信号を使用して前記
送信パルスの直交位相検波を行う第1の直交位相検波器
と、前記反射信号の直交位相検波を行う第2の直交位相
検波器と、それぞれの位相検波器の出力の複素乗算を行
う複素乗算器とを備えて、前記送信パルスとコヒーレン
トな反射信号の位相情報のみを取り出すことを特徴とす
るMTIパルスレーダ装置。The present invention is characterized in that a reflected signal from an object is phase-detected by a coherent reference signal to a transmission pulse, a reflected signal from a fixed object is erased based on the extracted phase information, and only a reflected signal from a moving object is extracted. In the MTI pulse radar device, a highly stable oscillator that outputs a continuous signal that is not in phase with a transmission pulse to obtain a reference signal of a phase detector, and a quadrature of the transmission pulse using the output signal of the oscillator. A first quadrature phase detector for performing phase detection, a second quadrature phase detector for performing quadrature phase detection of the reflection signal, and a complex multiplier for performing complex multiplication of outputs of the respective phase detectors An MTI pulse radar apparatus, which extracts only phase information of a coherent reflected signal from the transmission pulse.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61196869A JP2582556B2 (en) | 1986-08-22 | 1986-08-22 | MTI pulse radar device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61196869A JP2582556B2 (en) | 1986-08-22 | 1986-08-22 | MTI pulse radar device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6352080A JPS6352080A (en) | 1988-03-05 |
JP2582556B2 true JP2582556B2 (en) | 1997-02-19 |
Family
ID=16364999
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61196869A Expired - Fee Related JP2582556B2 (en) | 1986-08-22 | 1986-08-22 | MTI pulse radar device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2582556B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2847390B2 (en) | 1989-07-24 | 1999-01-20 | 日本無線株式会社 | MTI radar device |
-
1986
- 1986-08-22 JP JP61196869A patent/JP2582556B2/en not_active Expired - Fee Related
Non-Patent Citations (1)
Title |
---|
吉田孝監修"レーダ技術"電子通信学会 P.65〜P.97 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2847390B2 (en) | 1989-07-24 | 1999-01-20 | 日本無線株式会社 | MTI radar device |
Also Published As
Publication number | Publication date |
---|---|
JPS6352080A (en) | 1988-03-05 |
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