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JPS6340883A - Disturbing wave suppressing system - Google Patents

Disturbing wave suppressing system

Info

Publication number
JPS6340883A
JPS6340883A JP61184443A JP18444386A JPS6340883A JP S6340883 A JPS6340883 A JP S6340883A JP 61184443 A JP61184443 A JP 61184443A JP 18444386 A JP18444386 A JP 18444386A JP S6340883 A JPS6340883 A JP S6340883A
Authority
JP
Japan
Prior art keywords
frequency
transmitted
pulse
linear
output
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.)
Pending
Application number
JP61184443A
Other languages
Japanese (ja)
Inventor
Haruo Akagi
赤木 治生
Shoji Matsuda
庄司 松田
Masaya Takase
雅也 高瀬
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61184443A priority Critical patent/JPS6340883A/en
Publication of JPS6340883A publication Critical patent/JPS6340883A/en
Pending legal-status Critical Current

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  • Radar Systems Or Details Thereof (AREA)

Abstract

PURPOSE:To suppress disturbing waves in a linear/nonlinear FM system pulse compression radar by changing over the sweep polarities of transmitted and received pulses. CONSTITUTION:The output of a modulated pulse generator 1 in an intermediate frequency (IF) band is transmitted via a local oscillator 3a or 3b and a frequency converter 2. Received signals are mixed with the output of the oscillator 3a or 3b to be converted to IF signals by a frequency converter 4 and inputted to a pulse compression filter 5. The frequency of the pulse generator 1 increases from f1 to f2 with time and the frequency band of transmitted pulses are assumed to range from fTL to fTH. The frequencies fL and fH of the oscillators 3a and 3b are selected so as to satisfy expressions fL=fTL-f1 and fH=fTH+f2, respectively. Thus, when a pulse-like FM disturbing frequency sweep polarity agrees with that of transmitted and received signals, the oscillators 3a and 3b are changed over to each other to invert frequency sweep polarities whereby the disturbance can be suppressed.

Description

【発明の詳細な説明】 [産業上の利用分野J この発明は、リニア又はノンリニアE’M方式のパルス
圧縮レーダの妨害波抑圧方式に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application J] The present invention relates to an interference wave suppression method for a linear or non-linear E'M type pulse compression radar.

〔従来の技術] 従来のリニア又はノンリニアFM方式のパルス圧縮レー
ダは、M、工、 5kolnik ’工ntroduc
tion t。
[Prior art] Conventional linear or non-linear FM type pulse compression radars are
tion t.

Radar Systems“(5econd Edi
tion) McGraw−Hllllnternat
ional Company P493〜497 に記
載されている構成となっている。
Radar Systems “(5econd Edi
tion) McGraw-Hllllnternat
ional Company P493-497.

第3図は、この方式の系統図であり、図において、(υ
はリニア又はノンリニアFMの変調パルス発生器であり
、(2)は送信系の周波#、変換器、(3)は局部発振
器、(4)は交信系の周波数変換器、(5)はパルス圧
縮フィルタである。
Figure 3 is a system diagram of this method, and in the figure (υ
is a linear or non-linear FM modulation pulse generator, (2) is a transmission system frequency converter, (3) is a local oscillator, (4) is a communication system frequency converter, and (5) is a pulse compression It's a filter.

次に動作について第4図の動作説明図を参照しつつ説明
する。変調パルス発生器(1)は、IP帯の変調パルス
を発生するものであり、その出力は第4図(a)に示す
ように、時間とともに周rL政が変化するものであり、
その変化を第4図(b)に示す。ここでは、周−i故が
時間とともに増加する場合(以下「アンプ・チャープ」
という)を示しているが、周波数が時間とともに減少す
る場合(以′F「ダウン・チャープ」という)について
も同様の動作をする。また、ここでは、周波数が時間に
対し直線的に変化するリニアFMの場合を例示している
が、周波数が時間(対し非直線的に増加又は減少するノ
ンリニアFMについても以下同様の動作をする。さて、
変調パルス発生器(1)の出力は、局部発振器(3)の
出力により、周波数変換器(2)でRF帯に同波数変換
されて送信される。RF帯の受信信Ji3は、周波政変
換器(4)により、局部発振器(3)の出力上混合され
て工F信J8に変換され、パルス圧縮フィルり(5ンに
より、パルス圧縮される。このパフレスフィックルク(
5)は、第4図(c)に示すように、送信パルスと逆の
周波数分散特性をもつため、受信パルスは、時間軸上で
振幅方間に槓み上がり、第4図(d)に示すようなパル
ス圧細反形が出力さnる。
Next, the operation will be explained with reference to the operation explanatory diagram of FIG. 4. The modulated pulse generator (1) generates modulated pulses in the IP band, and its output has a frequency that changes over time as shown in FIG. 4(a).
The change is shown in FIG. 4(b). Here, we will consider the case where the frequency -i increases with time (hereinafter referred to as "amp chirp").
However, the same operation occurs when the frequency decreases over time (hereinafter referred to as "down chirp"). Further, here, a case of linear FM where the frequency changes linearly with respect to time is illustrated, but the same operation will be performed below for non-linear FM where the frequency increases or decreases non-linearly with respect to time. Now,
The output of the modulated pulse generator (1) is converted into an RF band by the frequency converter (2) using the output of the local oscillator (3), and then transmitted. The received signal Ji3 in the RF band is mixed by the frequency converter (4) on the output of the local oscillator (3), converted into the industrial signal J8, and pulse-compressed by a pulse compression filter (5). This puffless fickle look (
5) has a frequency dispersion characteristic opposite to that of the transmitted pulse, as shown in Figure 4(c), so the received pulse rises in the amplitude direction on the time axis, and as shown in Figure 4(d). A pulse compression rectangle as shown is output.

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

従来のパルス圧縮レーダけ、以上のように構成されてい
るので、パルス状のFM妨害に対しては、その周波数掃
引極性が送受信パルスのそれと一致している場合には、
受信信うと同様にパルス圧縮され、妨害が強調されると
いう問題点があった。
Since the conventional pulse compression radar is configured as described above, for pulse-shaped FM interference, if the frequency sweep polarity matches that of the transmitted and received pulses,
There was a problem in that the pulses were compressed in the same way as in the case of reception and reception, and interference was emphasized.

この発明は、上記のような問題点を解消するためになさ
れたもので、パルス状のFM妨害の周波数掃引極性が、
送受信パルスのそれと一致した場合Pこは、送受信パル
スの周波数掃引極性を反転させ妨害を抑圧することを目
的とする。
This invention was made to solve the above problems, and the frequency sweep polarity of pulsed FM interference is
The purpose of this is to invert the frequency sweep polarity of the transmitted and received pulses when it matches that of the transmitted and received pulses, thereby suppressing interference.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る妨害波抑圧方式は、リニア又はノンリニ
アFMの送受信パルスを用いるパルス圧縮レーダにおい
て、送受信パルスの周波数掃引極性を切り換えるもので
ある。
The interference wave suppression method according to the present invention switches the frequency sweep polarity of the transmitted and received pulses in a pulse compression radar that uses linear or non-linear FM transmitted and received pulses.

〔作用J 上記のように、送受信パルスの周波数掃引極性を切り換
えることにより、パルス状のFM妨害の周波数掃引極性
と送受信パルスのそれとを逆の関係にすることができ、
妨害のみを抑圧することができる。
[Effect J As described above, by switching the frequency sweep polarity of the transmitted and received pulses, it is possible to reverse the relationship between the frequency sweep polarity of the pulsed FM disturbance and that of the transmitted and received pulses,
Only interference can be suppressed.

〔実施例J 以下、この発明の一英施例を図について説明する0 第1図は、局部発振器の周波数を切り換えることにより
送受信パルスの周波数掃引極性を反転させる例である。
[Embodiment J] Hereinafter, an embodiment of the present invention will be described with reference to the figures. FIG. 1 is an example in which the frequency sweep polarity of the transmitted and received pulses is reversed by switching the frequency of the local oscillator.

第1図において、(1)は工F帯の賀調パルス発生器で
あり、(2)は送信系の周波政変換器、(3a)、(3
b)は2種の局部発振器、(4)は受信系の周波政変換
器、(5)はパルス圧縮フィルタ、(6)は2種の局部
発振器の切換えスイッチである。
In Fig. 1, (1) is the frequency pulse generator for the F band, (2) is the frequency converter for the transmission system, (3a), (3
b) is two types of local oscillators, (4) is a receiving system frequency converter, (5) is a pulse compression filter, and (6) is a changeover switch for the two types of local oscillators.

以下、第2図に示す動作説明図を用いて実施例の動作を
説明する。
Hereinafter, the operation of the embodiment will be explained using the operation explanatory diagram shown in FIG.

第2図(a)は工F帯の変調パルス発生器(1)の出力
のJi”M特性を示したものでありここでは、周波数が
時間とともにflからf2まで増加するアンプ・チャー
プの場合を例示している。第2図(b)はこの出力のス
ベタトルを示す。今、送受信パルスの8波数帯域をfr
bからfTHまでとし、一方の8部発振器(3a)の周
波玖1°Lを fL=f7L−fl なる関係に選ぶと、第2図(0)、(dJに示すように
送信パルスの周波数は時間とともにfTLからfTHに
増加し、アップ・チャープとなる。また、他方の局部発
振器(3b)の周波&f■を fH=f’TH+fl なる関係に選ふと第2図(e八(f)に示すように送信
パルスの周波数は、時間ととも[fTHからfTLに減
少しダクン・チャープとなる。従ってスイッチ(6)に
より局部発振器(:la)、(3b)を切換えることに
より、送信パルスの絢波孜掃引極性を切換えることカニ
できる。
Figure 2 (a) shows the Ji'M characteristic of the output of the modulated pulse generator (1) in the F band. Here, we will consider the case of an amplifier chirp whose frequency increases from fl to f2 with time. Figure 2(b) shows the smoothness of this output.Now, the 8 wave number bands of the transmitted and received pulses are fr
b to fTH, and if the frequency 1°L of one of the 8-part oscillators (3a) is chosen as fL=f7L-fl, the frequency of the transmitted pulse is as shown in Figure 2 (0) and (dJ). As time passes, fTL increases to fTH, resulting in an up-chirp.If the frequency &f■ of the other local oscillator (3b) is chosen to have the relationship fH=f'TH+fl, the relationship shown in Figure 2 (e8(f)) The frequency of the transmitted pulse decreases from fTH to fTL with time, resulting in a dank chirp. Therefore, by switching the local oscillators (:la) and (3b) with the switch (6), the frequency of the transmitted pulse is It is possible to switch the sweep polarity.

なお、上記実施例では、変調パルス発生器の出力をアン
プ・チャープとしたが、ダクン・チャープの場合も全く
同様である。
In the above embodiment, the output of the modulation pulse generator is an amplifier chirp, but the same applies to the case of a dakun chirp.

また、上記実施例で4よ、局部発振器を切り換えで、送
信パルスの周波数掃引極性を切換えろ例を示したが、他
の方決として、変u、tパルス発生器及びパルス圧縮フ
ィルタをアップ・チャープ用とメ゛クン・チャープ用の
2式用意して、又は2通りの動作をさせて、それらを切
換えてもよい。
In addition, in the above embodiment 4, an example was shown in which the frequency sweep polarity of the transmitted pulse was changed by switching the local oscillator, but as another method, the variable U and T pulse generators and the pulse compression filter could be upgraded. It is also possible to prepare two sets, one for chirp and one for main chirp, or to operate in two ways and to switch between them.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、送信パルスのj−改
故掃引極性を刀り換えられるよう構成したので、パルス
状のElAfn書に対してもパルス圧縮♂ず、抑圧する
効果が得られる。
As described above, according to the present invention, since the j-modification sweep polarity of the transmitted pulse can be switched, the effect of suppressing the pulsed ElAfn writing without compressing it can be obtained. .

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

第1図はこの発明の1実施例による妨害波抑圧方式の系
統図、第2図はその動作説明図である。 第3図は従来のパルス圧縮レーダの系統図、第4図はそ
の前作説明図である。 また、図において、(1)は変調パルス発生器、(2)
は送信系の周e故変換器、(3)、(3&)、(3b)
は局部yΔ受器、(4)は受信系の同波政変換器、(5
)はパルス圧縮7 □(ルタ、(6)は局部発振器の切
換スイッチである。 7!1−21図中、同一符号は同−又は相当部分を示す
。 代 理 人  大  岩    増  雄(JqJ A     Q     も
FIG. 1 is a system diagram of an interference wave suppression system according to an embodiment of the present invention, and FIG. 2 is an explanatory diagram of its operation. FIG. 3 is a system diagram of a conventional pulse compression radar, and FIG. 4 is an explanatory diagram of its predecessor. In addition, in the figure, (1) is a modulated pulse generator, (2)
are transmission system frequency converters, (3), (3&), (3b)
is the local yΔ receiver, (4) is the same-wavelength converter in the receiving system, and (5
) is the pulse compression 7 □ (ruter), and (6) is the local oscillator selector switch. In Figure 7!1-21, the same reference numerals indicate the same or equivalent parts. Agent: Masuo Oiwa (JqJ A Q too

Claims (1)

【特許請求の範囲】[Claims] リニア又はノンリニアFM方式のパルス圧縮レーダーに
おいて、送受信パルス内の周波数掃引の極性を切り換え
ることにより、周波数掃引妨害波を抑圧することを特徴
とした妨害波抑圧方式。
An interference wave suppression method characterized by suppressing frequency sweep interference waves in a linear or non-linear FM type pulse compression radar by switching the polarity of the frequency sweep within the transmitted and received pulses.
JP61184443A 1986-08-05 1986-08-05 Disturbing wave suppressing system Pending JPS6340883A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61184443A JPS6340883A (en) 1986-08-05 1986-08-05 Disturbing wave suppressing system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61184443A JPS6340883A (en) 1986-08-05 1986-08-05 Disturbing wave suppressing system

Publications (1)

Publication Number Publication Date
JPS6340883A true JPS6340883A (en) 1988-02-22

Family

ID=16153236

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61184443A Pending JPS6340883A (en) 1986-08-05 1986-08-05 Disturbing wave suppressing system

Country Status (1)

Country Link
JP (1) JPS6340883A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06138215A (en) * 1992-10-26 1994-05-20 Nec Corp Radar signal processing method
JP2016024173A (en) * 2014-07-24 2016-02-08 東京計器株式会社 Radar system and radar signal processing method

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5550175A (en) * 1978-10-05 1980-04-11 Nec Corp Received signal processor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5550175A (en) * 1978-10-05 1980-04-11 Nec Corp Received signal processor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06138215A (en) * 1992-10-26 1994-05-20 Nec Corp Radar signal processing method
JP2016024173A (en) * 2014-07-24 2016-02-08 東京計器株式会社 Radar system and radar signal processing method

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