JPS5853317B2 - Pulse compression radar method - Google Patents
Pulse compression radar methodInfo
- Publication number
- JPS5853317B2 JPS5853317B2 JP51158141A JP15814176A JPS5853317B2 JP S5853317 B2 JPS5853317 B2 JP S5853317B2 JP 51158141 A JP51158141 A JP 51158141A JP 15814176 A JP15814176 A JP 15814176A JP S5853317 B2 JPS5853317 B2 JP S5853317B2
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- pulse
- delay
- wave
- transmitted wave
- 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
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
- G01S13/02—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)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】 この発明はパルス圧縮レーダ装置に関するものである。[Detailed description of the invention] This invention relates to a pulse compression radar device.
第1図は従来の階段状周波数変調パルス圧縮レーダー装
置(周波数分割数5の場合)のブロック図を表わす。FIG. 1 shows a block diagram of a conventional stepped frequency modulation pulse compression radar device (in the case of 5 frequency divisions).
図に於いて、1は周波数f。の水晶発振器、2はf。In the figure, 1 is the frequency f. crystal oscillator, 2 is f.
の整数倍のCW波を発生する周波数逓倍器である。This is a frequency multiplier that generates a CW wave that is an integral multiple of .
3はパルス幅τのパルス発生器、4はこのパルス発生器
3から発生するパルス波にO9τ、2τ、3τ、4τの
遅延を与える遅延回路、5は切換回路、6〜10はゲー
ト回路でf、〜f5のCW波を幅τのパルスでゲートし
、幅5τの高周波パルス列を発生する。3 is a pulse generator with a pulse width τ, 4 is a delay circuit that gives delays of O9τ, 2τ, 3τ, and 4τ to the pulse wave generated from this pulse generator 3, 5 is a switching circuit, and 6 to 10 are gate circuits f , ~f5 is gated with a pulse of width τ to generate a high-frequency pulse train of width 5τ.
11はこれらのパルス列をマイクロ波に周波数変換して
送信する送信機、12は送受切換器、13はレーダアン
テナ、14は受信波を周波数変換しフィルターにより周
波数f1f2f3f、f5の5波に分離する受信機、1
5は切換回路5の切換に対応して切り換える切換回路、
16〜20は受信波が同時刻で合成されるよう各パルス
に夫々、O2τ、2τ。11 is a transmitter that converts the frequency of these pulse trains into microwaves and transmits them; 12 is a transmitter/receiver switch; 13 is a radar antenna; 14 is a receiver that converts the frequency of the received waves and separates them into five waves of frequencies f1f2f3f and f5 using a filter. Machine, 1
5 is a switching circuit that switches in response to switching of the switching circuit 5;
16 to 20 are O2τ and 2τ for each pulse, respectively, so that the received waves are combined at the same time.
3τ、4τの遅延を与える遅延回路、21は合成後の受
信波を検波する検波回路、22はブラウン管等の指示装
置である。Delay circuits providing delays of 3τ and 4τ, 21 a detection circuit for detecting the combined received wave, and 22 an indicating device such as a cathode ray tube.
ここで説明したパルス圧縮レーダ装置は距離分解能をそ
こなうことなく、最大探知距離を大きくすることができ
る。The pulse compression radar device described here can increase the maximum detection distance without impairing the distance resolution.
以上で述べた従来のパルス圧縮レーダ装置は送信時と受
信時において、遅延回路、ゲート回路をそれぞれ別個に
もたねばならない。The conventional pulse compression radar device described above must have separate delay circuits and gate circuits for transmission and reception.
また、それぞれ、CW波を発生するのに水晶発振器と周
波数逓倍器をもつ。Each of them also has a crystal oscillator and a frequency multiplier to generate CW waves.
パルス圧縮比を大きくして距離分解能を上げる為には周
波数の分割数を大きくする必要があるがその場合、送信
時と受信時に別々の回路を持たねばならないということ
は、コスト的に大きな障害となる。In order to increase the pulse compression ratio and increase the distance resolution, it is necessary to increase the number of frequency divisions, but in that case, the need to have separate circuits for transmitting and receiving is a major obstacle in terms of cost. Become.
そこで、この発明は送信波を発生するのに高周波インパ
ルスを用い、フィルター回路、遅延回路、ゲート回路を
送受共用することにより、レーダー装置の低コスト化を
目的とする。Therefore, the present invention aims to reduce the cost of a radar device by using a high frequency impulse to generate a transmission wave and by sharing a filter circuit, a delay circuit, and a gate circuit for transmission and reception.
以下に、この発明のパルス圧縮レーダ装置を詳細に説明
する。The pulse compression radar device of the present invention will be explained in detail below.
これまでのパルス圧縮レーダ装置が、送信パルス列を発
生するのに第1図のように水晶発振器、個々の階段状変
調周波数に対応した周波数逓倍器、個々のゲート回路を
使用するのに対して、この発明の装置ではインパルス、
現実的には非常に狭いパルス幅のマイクロ波矩形変調波
のスペクトルが広い地域にわたり平坦であることを利用
し、個々の階段状変調周波数に等しい中心周波数を持つ
帯域通過フィルターにより抽出し、遅延、合成すること
により送信波を発生するものである。Conventional pulse compression radar devices use a crystal oscillator, a frequency multiplier corresponding to each stepped modulation frequency, and individual gate circuits to generate a transmission pulse train, as shown in Figure 1. In the device of this invention, an impulse,
In reality, we take advantage of the fact that the spectrum of microwave rectangular modulation waves with extremely narrow pulse widths is flat over a wide area, and extract them using bandpass filters with center frequencies equal to the individual stepped modulation frequencies, delay them, A transmission wave is generated by combining them.
送信時、第2図のインパルス発生器23で発生された幅
の非常に狭いマイクロ波矩形変調波は送受切換器24を
通過し、各々帯域通過フィルター25〜33により抽出
され、フィルター出力として各々のフィルターの中心周
波数をキャリアとする振幅変調波が得られる。During transmission, the microwave rectangular modulated wave with a very narrow width generated by the impulse generator 23 in FIG. An amplitude modulated wave with the center frequency of the filter as a carrier is obtained.
第3図aは9個のフィルター25〜33によって抽出さ
れるマイクロ波矩形変調波の周波数スペクトル成分であ
り、第3図すは各々のフィルター25〜33で抽出され
る周波数スペクトル成分、第3図Cは各々のフィルター
25〜33の時間応答波形をあられす。Figure 3a shows the frequency spectrum components of the microwave rectangular modulated wave extracted by nine filters 25-33; C shows the time response waveforms of each of the filters 25 to 33.
各フィルター出力は各フィルター25〜33に対応して
固定時間τだけ異なった遅延時間をもつ第2図34〜4
2の遅延回路を通過し、43〜51のゲート回路により
固定時間τでゲートされ各々増幅器52〜60で増幅さ
れた後、合成器6により合成される。Each filter output has a delay time that differs by a fixed time τ corresponding to each filter 25 to 33 in FIG.
The signals pass through delay circuit No. 2, are gated at a fixed time τ by gate circuits 43 to 51, are amplified by amplifiers 52 to 60, and are then combined by combiner 6.
第3図dは遅延回路34〜42、ゲート回路43〜51
通過後の各々の出力の時間関係をあられし、第3図eは
合成器6の出力をあられす。FIG. 3d shows delay circuits 34 to 42 and gate circuits 43 to 51.
The time relationship of each output after passing through is shown, and FIG. 3e shows the output of the combiner 6.
送信する前にこれにリミットをかけると第4図a、bに
示すような階段状に周波数変調された送信波が得られる
。If a limit is applied to this before transmission, a stepped frequency modulated transmission wave as shown in FIGS. 4a and 4b is obtained.
インパルス発生器23より発生されるパルスの周波数成
分が完全に平坦でないことにより、完全な階段状変調波
とはならず、それぞれに若干の周波数の乱れが生ずるが
、これはパルス圧縮にはほとんど影響しない。Since the frequency components of the pulses generated by the impulse generator 23 are not completely flat, they do not become perfectly stepped modulated waves, and slight frequency disturbances occur in each wave, but this has little effect on pulse compression. do not.
第1図に示すように、今までの装置は受信時に送信時と
は別のフィルター、切換回路および遅延回路を使用して
パルス圧縮するが、この発明の装置では第2図に示され
るように受信パルスを送信時と同じフィルター25〜3
3、遅延回路34〜42を使用してパルス圧縮する。As shown in FIG. 1, conventional devices use different filters, switching circuits, and delay circuits for pulse compression during reception, but the device of the present invention compresses pulses as shown in FIG. The same filter 25 to 3 used when transmitting the received pulse
3. Pulse compression is performed using delay circuits 34-42.
リミッタ−を通った送信波は第4図a −cにあられさ
れる。The transmitted waves passing through the limiter are shown in Figures 4a-c.
第4図aは送信波の泣絡線、第4図すは送信波内の周波
数変調特性、第4図Cは送信波の周波数スペクトルを示
す。FIG. 4a shows the contact line of the transmitted wave, FIG. 4 shows the frequency modulation characteristics within the transmitted wave, and FIG. 4C shows the frequency spectrum of the transmitted wave.
fT(t)、その周波数スペクトルFT(f)を数式で
表わすと、まず、合成器61により合成される前のそれ
ぞれの波形fnr(t)、FnT(f)は次のようにな
る。When fT(t) and its frequency spectrum FT(f) are expressed mathematically, first, the respective waveforms fnr(t) and FnT(f) before being synthesized by the synthesizer 61 are as follows.
であり振幅Anパルス幅πのパルス波形を表わす。represents a pulse waveform with an amplitude An and a pulse width π.
したがって、送信波f r(t)およびその周波数スペ
クルFr(7’)は
となる。Therefore, the transmitted wave f r(t) and its frequency spectrum Fr(7') are as follows.
なお、An、Bnは定数、fn、tnは第4図a、b、
cに示すような関係にある。Note that An and Bn are constants, and fn and tn are as shown in Figure 4 a, b,
The relationship is as shown in c.
この送信波が標的により反射されてふたたび受信波とし
て第2図のレーダアンテナ63、送受切換器62を通り
、ミキサー64へはいる。This transmitted wave is reflected by the target and passes through the radar antenna 63 and transmission/reception switch 62 shown in FIG. 2 as a received wave again, and enters the mixer 64.
ここでミキサー64のローカル周波数を送信波の周波数
スペクトルFTCf)の中心周波数の2倍に選ぶことに
よって、第5図a、bに示すように、ミキサー64の出
力における受信波の周波数変調特性は合成器61の出力
における送信波の周波数変調特性(第4図b)と時間的
に対称になる。By selecting the local frequency of the mixer 64 to be twice the center frequency of the frequency spectrum FTCf) of the transmitted wave, the frequency modulation characteristics of the received wave at the output of the mixer 64 are synthesized, as shown in Fig. 5a and b. This is temporally symmetrical with the frequency modulation characteristic of the transmitted wave at the output of the transmitter 61 (FIG. 4b).
したがって、ミキサー64の出力における受信波の周波
数スペクトルは(3)式で表わされる。Therefore, the frequency spectrum of the received wave at the output of the mixer 64 is expressed by equation (3).
さらにこの受信波が、送信時と同じフィルター25〜3
3それに続く遅延線34〜42ゲ一ト回路43〜51、
増幅器52〜60を通るそれぞれの出力は合成器61で
同時刻に合成されることになりパルス圧縮が実現できる
。Furthermore, this received wave is filtered through the same filters 25 to 3 as at the time of transmission.
3 subsequent delay lines 34-42 gate circuits 43-51,
The respective outputs passing through the amplifiers 52 to 60 are combined at the same time by the combiner 61, so that pulse compression can be realized.
以上で述べたこの発明では、受信波を送信波の周波数ス
ペクトルの中心の2倍のローカル周波数でミキシングす
ることにより、送受共用のフィルター25〜33、遅延
線34〜42を用いてパルス圧縮しているため、低コス
ト化を実現することができる。In the invention described above, by mixing the received wave at a local frequency twice the center of the frequency spectrum of the transmitted wave, pulse compression is achieved using filters 25 to 33 and delay lines 34 to 42 for both transmission and reception. Therefore, cost reduction can be achieved.
第1図は従来のパルス圧縮レーダ装置を示す構成図、第
2図はこの発明の一実施例を示す構成図、第3図aは9
個のフィルタにより抽出されるマイクロ波矩形変調波の
周波数成分を示す特性図、第3図すは各々のフィルター
で抽出される周波数スペクトル成分を示す特性図、第3
図Cはフィルタの出力を示す波形図、第3図d及びeは
、遅延回路、ゲート回路及び合成画の出力を示す波形図
、第4図aは送信波を示す波形図、第4図すは送信波の
周波数変調特性を示す特性図、第4図Cは送信波の周波
数スペクトルを示す特性図、第5図aは受信パルスの波
形図、第5図すはミキサー64の出力における受信波の
周波数変調特性を示す特性図、第5図Cはミキサー64
出力における受信波の周波数スペクトルを示す特性図で
ある。
図中、23はインパルス発生回路、24は送受切換回路
、25〜23はフィルター、34〜42は遅延回路、4
3〜51はゲート回路、52〜60は増幅器、61は合
成器、62は送受切換器、63はレーダアンテナ、64
はミキサー 65は検波回路、66は指示器である。FIG. 1 is a block diagram showing a conventional pulse compression radar device, FIG. 2 is a block diagram showing an embodiment of the present invention, and FIG.
Figure 3 is a characteristic diagram showing the frequency components of microwave rectangular modulated waves extracted by each filter.
Figure C is a waveform diagram showing the output of the filter, Figures 3 d and e are waveform diagrams showing the output of the delay circuit, gate circuit, and composite image, Figure 4 a is a waveform diagram showing the transmitted wave, and Figure 4 4 is a characteristic diagram showing the frequency modulation characteristics of the transmitted wave, FIG. 4 C is a characteristic diagram showing the frequency spectrum of the transmitted wave, FIG. 5 a is a waveform diagram of the received pulse, and FIG. FIG. 5C is a characteristic diagram showing the frequency modulation characteristics of the mixer 64.
FIG. 3 is a characteristic diagram showing a frequency spectrum of a received wave at the output. In the figure, 23 is an impulse generation circuit, 24 is a transmission/reception switching circuit, 25 to 23 are filters, 34 to 42 are delay circuits, 4
3 to 51 are gate circuits, 52 to 60 are amplifiers, 61 is a combiner, 62 is a transmission/reception switch, 63 is a radar antenna, 64
is a mixer, 65 is a detection circuit, and 66 is an indicator.
Claims (1)
った中心周波数をもつ帯域フィルターを通し、さらに夫
々のフィルターの中心周波数に対応して、固定時間ずつ
遅延時間の異なる遅延線を通し各遅延線の遅延時間の差
に等しい時間でゲートし合成することにより所望の階段
状に周波数変調された伸長パルスを得、この伸長パルス
を送信波とし、目標物により反射されて到来する受信波
を送信波の周波数スペクトラムの中心の2倍のローカル
周波数でミキシングして、周波数変調特性を送信波のそ
れと時間的に対称にした後、上記フィルター及び遅延線
を通すことによりパルス圧縮するように構成して成るパ
ルス圧縮レーダ装置。1 Pass a narrow rectangular impulse through bandpass filters with center frequencies that differ by a predetermined frequency, and then pass them through delay lines with different delay times by a fixed amount of time corresponding to the center frequency of each filter.The delay of each delay line is By gated and synthesized at a time equal to the time difference, an expanded pulse frequency-modulated in a desired stepped manner is obtained, and this expanded pulse is used as a transmitted wave, and the received wave reflected by the target and arriving is set to the frequency of the transmitted wave. Pulse compression configured to mix at a local frequency twice the center of the spectrum to make the frequency modulation characteristics temporally symmetrical with that of the transmitted wave, and then compress the pulse by passing it through the above filter and delay line. radar equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51158141A JPS5853317B2 (en) | 1976-12-29 | 1976-12-29 | Pulse compression radar method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51158141A JPS5853317B2 (en) | 1976-12-29 | 1976-12-29 | Pulse compression radar method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5383595A JPS5383595A (en) | 1978-07-24 |
| JPS5853317B2 true JPS5853317B2 (en) | 1983-11-28 |
Family
ID=15665154
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51158141A Expired JPS5853317B2 (en) | 1976-12-29 | 1976-12-29 | Pulse compression radar method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5853317B2 (en) |
-
1976
- 1976-12-29 JP JP51158141A patent/JPS5853317B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5383595A (en) | 1978-07-24 |
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