JPS62187272A - Pulse radar - Google Patents

Pulse radar

Info

Publication number
JPS62187272A
JPS62187272A JP61028882A JP2888286A JPS62187272A JP S62187272 A JPS62187272 A JP S62187272A JP 61028882 A JP61028882 A JP 61028882A JP 2888286 A JP2888286 A JP 2888286A JP S62187272 A JPS62187272 A JP S62187272A
Authority
JP
Japan
Prior art keywords
signal
received
noise
envelope
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.)
Pending
Application number
JP61028882A
Other languages
Japanese (ja)
Inventor
Toru Kumasaka
徹 熊坂
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.)
NEC Home Electronics Ltd
NEC Corp
Original Assignee
NEC Home Electronics Ltd
Nippon Electric Co Ltd
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 NEC Home Electronics Ltd, Nippon Electric Co Ltd filed Critical NEC Home Electronics Ltd
Priority to JP61028882A priority Critical patent/JPS62187272A/en
Publication of JPS62187272A publication Critical patent/JPS62187272A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To measure correct time even if there is a noise by slicing a signal obtained by detecting the envelope of a received signal above a constant amplitude value, and differentiating the slice signal and finding a zero-cross point. CONSTITUTION:Reflected light which is radiated from a transmission part 10 through an antenna 13 and received by an object of measurement is received by an antenna 1. This received signal is amplified 3, detected by an envelope detector 4, and then sliced above the constant amplitude value by a comparator 5 and an analog switch 6. Consequently, a slice signal 106 existing after the noise is removed is differentiated by a differentiating circuit 7 to obtain a signal 107 whose middle point crosses zero. The signal is waveform-shaped 8 into a pulse signal 108, which is inputted to a counter 9, so that a time interval between the middle point of the transmitted wave envelope and the zero- cross point is counted in the form of the number of input clocks from a clock oscillator 11. Then, the distance of the body to be measured is computed by an arithmetic display part 12 from the counted number of clocks and displayed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、パルス波により距離計測を行なうパルスレー
ダに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a pulse radar that measures distance using pulse waves.

〔従来の技術〕[Conventional technology]

パルスレーダによる計測は、方形状の包路線を有するパ
ルス変調波を放射し、対象物体の反射波を受信するまで
の受信時間から距離を測っていた。
Measurements using pulse radar emit a pulse modulated wave with a rectangular envelope, and measure the distance from the reception time until the reflected wave from the target object is received.

なお、パルスレーダとしては、電波のみならず超音波の
場合もあるが原理的には同一である。
Note that the pulse radar may use not only radio waves but also ultrasonic waves, but the principles are the same.

〔発明が解決しようとする手段〕[Means to be solved by the invention]

パルスレーダでは、送信波が第3図に示すように、一定
振幅の波が数波含まれた波形を繰返し放射する。受信波
は対象物体との距離の2倍を伝播する時間だけ遅れて受
信される。このときの波形は図示のように包路線は方形
でなく、立上がり、立下がりがなだらかな山形の波形に
なる。
In a pulse radar, a transmitted wave repeatedly emits a waveform including several waves of constant amplitude, as shown in FIG. The received wave is received with a delay of the time it takes to propagate twice the distance to the target object. The waveform at this time does not have a rectangular envelope line as shown in the figure, but a mountain-shaped waveform with gentle rises and falls.

従来、距離測定にあたり送信波の立上がり時間t0と、
受信波の立上がりとの時間差をとっているが、受信波を
雑音と区別するため、一定のしきい値のレベルmを超え
たときに受信波が到来したものとして、この時間差tを
求めていた。しかし受信波の立上がりがなだらかなため
レベルm以下の波形は無視され、△Lだけの誤差が生ず
る。レベルmを低下すれば誤差は少なくなるが、雑音を
信号と誤認するおそれが生ずる。
Conventionally, when measuring distance, the rise time t0 of the transmitted wave,
The time difference between the rise and the rise of the received wave is taken, but in order to distinguish the received wave from noise, this time difference t was determined by assuming that the received wave arrived when it exceeded a certain threshold level m. . However, since the rise of the received wave is gentle, waveforms below level m are ignored, resulting in an error of ΔL. If the level m is lowered, the error will be reduced, but there is a risk that noise will be mistaken for a signal.

本発明の目的は、上記の欠点を除去し、雑音がある場合
でも、正しい時間計測ができるパルスレーダを提供する
ことにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a pulse radar that eliminates the above-mentioned drawbacks and can accurately measure time even in the presence of noise.

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

本発明のパルスレーダは、受信波を包路線検波した信号
を一定振幅値以上でスライスする手段と。
The pulse radar of the present invention includes means for slicing a signal obtained by envelope detection of a received wave at a predetermined amplitude value or more.

前記スライス信号を微分して零交差点を求める手段と、
送信波包絡波形の中点と前記零交差点との時間間隔を求
める手段とを有するようにしたものである。
means for differentiating the slice signal to find a zero crossing point;
The apparatus includes means for determining the time interval between the midpoint of the transmitted wave envelope waveform and the zero crossing point.

〔作用〕[Effect]

本発明では、時間測定点として送信波・受信波ともに中
点としている。受信波をノイズから充分に区別できるレ
ベル以上の波形にスライスして、その中点をスライス波
形を微分し零交差点を求めることによってきめる。受信
波の波形から微分零交差点が中点を示す。ノイズは除去
されるので、ノイズが微分されることはない。
In the present invention, the time measurement point is the midpoint of both the transmitted wave and the received wave. The received wave is sliced into a waveform with a level higher than that which can be sufficiently distinguished from noise, and the midpoint is determined by differentiating the sliced waveform and finding the zero crossing point. From the waveform of the received wave, the differential zero crossing point indicates the midpoint. Since the noise is removed, the noise is not differentiated.

送信波は、立上がりでも正しく時間を定めることができ
るが、受信波の関係からその中点を基準時点とすれば、
受信波の時間差を正しく測定することになる。
The time can be determined correctly even at the rising edge of the transmitted wave, but from the relationship of the received wave, if the midpoint is used as the reference point,
This will accurately measure the time difference between received waves.

〔実施例〕〔Example〕

以下、図面を参照して本発明の一実施例につき説明する
。第1図は、電波によるパルスレーダの概略構成ブロッ
ク図を示したものである。第2図に各部の波形を示す。
Hereinafter, one embodiment of the present invention will be described with reference to the drawings. FIG. 1 shows a schematic block diagram of a pulse radar using radio waves. Figure 2 shows the waveforms of each part.

送信部10からアンテナ13を介して電波を放射し、測
定対象物体からの反射波をアンテナ1で受信する。アン
テナ1,13は共通のアンテナでもよい。アンテナlの
受信信号101は、ノイズを含むが、タンク回路2によ
って電波の周波数から離れたノイズPは除去される。た
だし電波の周波数あるいは近傍の周波数のノイズQはそ
のまま混入する。次に増幅器3で増幅した信号103を
包路線検波器4で検波した後、振幅レベルE以上の波形
をスライスする。このスライスは比較器5゜アナログス
イッチ6によって行なわれる。検波された信号104に
は信号Sの包路線のみならず、図示のように振幅が小さ
いが、ノイズQを含んでいる。そこで、比較器5で、レ
ベルE以上の信号のときのみ、アナログスイッチ6にゲ
ート信号105を送り、信号を導通させる。これによっ
てノイズQが除去された信号106を得る。
Radio waves are emitted from the transmitter 10 via the antenna 13, and the antenna 1 receives reflected waves from the object to be measured. The antennas 1 and 13 may be a common antenna. Although the received signal 101 of the antenna l contains noise, the noise P away from the radio wave frequency is removed by the tank circuit 2. However, noise Q at the frequency of the radio wave or a nearby frequency is mixed in as is. Next, the signal 103 amplified by the amplifier 3 is detected by the envelope line detector 4, and then the waveform having the amplitude level E or higher is sliced. This slicing is performed by a comparator 5° analog switch 6. The detected signal 104 includes not only the envelope of the signal S but also noise Q, although the amplitude is small as shown. Therefore, the comparator 5 sends a gate signal 105 to the analog switch 6 to make the signal conductive only when the signal is at level E or higher. As a result, a signal 106 from which noise Q has been removed is obtained.

信号106は、ちょうど受信信号Sの中点において最大
値になるから次の微分回路7で微分すると、信号107
のように、前記中点が零交差をする。次に波形整形回路
8により、中点が立下がるようなパルス信号108に整
形する。波形整形はたとえば演算増幅器で、入力信号が
正のとき、“1”を出力するようにすればよい。前記信
号108はカウンタ9のリセット端子に入力し、立下が
りでリセットするようにする。
Since the signal 106 reaches its maximum value exactly at the midpoint of the received signal S, when it is differentiated by the next differentiating circuit 7, the signal 107
As in, the midpoint crosses zero. Next, the waveform shaping circuit 8 shapes the pulse signal 108 so that the midpoint falls. The waveform shaping may be performed using, for example, an operational amplifier that outputs "1" when the input signal is positive. The signal 108 is input to the reset terminal of the counter 9, and is reset at the falling edge.

ロガカウンタ9には、送信部10の波形の中点で立下が
るパルス信号109がセント端子に入力して、送信波発
生時に、送信波の中点において、カウンタ9をセットし
、受信波による信号108によりリセットされるまでの
時間をクロンク発振器11からの大力クロック数で計数
する。計数されたクロック数から、測定対象物体までの
距離を演算表示部12が演算して、距離表示をする。
A pulse signal 109 that falls at the midpoint of the waveform of the transmitter 10 is input to the log counter 9 at the cent terminal, and when a transmission wave is generated, the counter 9 is set at the midpoint of the transmission wave, and the signal 109 due to the reception wave is set. The time until the clock is reset is counted by the number of high-power clocks from the Cronk oscillator 11. The calculation/display unit 12 calculates the distance to the object to be measured from the counted number of clocks and displays the distance.

前記送信波の中点は、周波数が低い場合は、方形状のパ
ルス列のパルス数が既知であるから、そのパルス数が1
/2になったことをカウントして求めることができる。
If the frequency is low, the midpoint of the transmitted wave is determined when the number of pulses in the rectangular pulse train is known, so the number of pulses is 1.
/2 can be calculated by counting.

周波数が高い場合には変調波の中点から求めてもよい。If the frequency is high, it may be determined from the midpoint of the modulated wave.

上記の説明において、スライスするレベルEの選定条件
は厳しくない。従来の方法ではレベルEになる時点を時
刻の基準にしたが、本発明では単にノイズ除去のためで
ある。
In the above description, the conditions for selecting level E for slicing are not strict. In the conventional method, the time point when level E is reached is used as the time reference, but in the present invention, this is simply for noise removal.

上記実施例は、電波を用いた場合であるが、超音波の場
合には、アンテナの代わりに共振振動子を用いれば同様
の回路構成でよい。
The above embodiment is a case where radio waves are used, but in the case of ultrasonic waves, a similar circuit configuration may be used if a resonant vibrator is used instead of the antenna.

〔発明の効果〕〔Effect of the invention〕

以上、詳しく説明したように、本発明では受信波の包絡
線検波された信号に含まれるノイズは、一定のレベルを
設定してスライスすることで除去される。そして送信波
は包絡線が方形な一定振幅のパルス列であっても、受信
波は伝播特性により包絡線の中央が山形になるので、微
分して零交差点を求めれば、零交差点が中点を示すよう
になる。
As described in detail above, in the present invention, noise contained in a signal obtained by envelope detection of a received wave is removed by setting a certain level and slicing the signal. Even if the transmitted wave is a pulse train of constant amplitude with a rectangular envelope, the received wave's envelope will have a mountain-shaped center at the center due to the propagation characteristics, so if you differentiate and find the zero crossing point, the zero crossing point will be the midpoint. It becomes like this.

この中点の決定は、受信波の立上がり状態に関係なく求
まるので正確であり、送信波の中点との時開蓋から誤差
なく距離を求めることができる。
This determination of the midpoint is accurate because it is determined regardless of the rising state of the received wave, and the distance between the midpoint of the transmitted wave and the lid can be determined without error.

上記のように、本発明のパルスレーダは、受信信号に含
まれるノイズおよび波形の立上がり状態により、測定値
に誤差を生じない距離測定をなすことができる。
As described above, the pulse radar of the present invention can perform distance measurement without causing errors in measurement values due to noise contained in the received signal and the rising state of the waveform.

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

第1図は、本発明の一実施例の概略構成ブロック図、第
2図は上記ブロック図の各部の信号波形図、第3図は従
来の距離測定を説明するための図である。 1.13・−アンテナ、 4−包絡線検波器、5・−比
較器、 6−アナログスイッチ、7−微分回路、 8−
  波形整形回路、9−・カウンタ、 1〇−送信部。
FIG. 1 is a schematic block diagram of an embodiment of the present invention, FIG. 2 is a signal waveform diagram of each part of the block diagram, and FIG. 3 is a diagram for explaining conventional distance measurement. 1.13 - antenna, 4 - envelope detector, 5 - comparator, 6 - analog switch, 7 - differentiator circuit, 8 -
Waveform shaping circuit, 9--counter, 10- transmitter.

Claims (1)

【特許請求の範囲】 反射波の受信時間により距離計測を行なうパルスレーダ
において、 受信波を包絡線検波した信号を一定振幅値以上でスライ
スする手段と、前記スライス信号を微分して零交差点を
求める手段と、送信波包絡波形の中点と前記零交差点と
の時間間隔を求める手段とを有することを特徴とするパ
ルスレーダ。
[Scope of Claims] A pulse radar that measures distance based on the reception time of reflected waves includes means for slicing a signal obtained by envelope detection of a received wave at a constant amplitude value or more, and differentiating the slice signal to find a zero crossing point. and means for determining the time interval between the midpoint of the transmitted wave envelope waveform and the zero crossing point.
JP61028882A 1986-02-14 1986-02-14 Pulse radar Pending JPS62187272A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61028882A JPS62187272A (en) 1986-02-14 1986-02-14 Pulse radar

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61028882A JPS62187272A (en) 1986-02-14 1986-02-14 Pulse radar

Publications (1)

Publication Number Publication Date
JPS62187272A true JPS62187272A (en) 1987-08-15

Family

ID=12260767

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61028882A Pending JPS62187272A (en) 1986-02-14 1986-02-14 Pulse radar

Country Status (1)

Country Link
JP (1) JPS62187272A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008232830A (en) * 2007-03-20 2008-10-02 Denso Corp Interference determination method and fmcw radar

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5233761A (en) * 1975-09-09 1977-03-15 Emu Rio Jiyuniaa Eriseo Short range measuring apparatus employing pulse laser diode
JPS5837576A (en) * 1981-08-31 1983-03-04 Nagoya Denki Kogyo Kk Pulse reflecting type range finder

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5233761A (en) * 1975-09-09 1977-03-15 Emu Rio Jiyuniaa Eriseo Short range measuring apparatus employing pulse laser diode
JPS5837576A (en) * 1981-08-31 1983-03-04 Nagoya Denki Kogyo Kk Pulse reflecting type range finder

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008232830A (en) * 2007-03-20 2008-10-02 Denso Corp Interference determination method and fmcw radar
US7728762B2 (en) 2007-03-20 2010-06-01 Denso Corporation Method for detecting interference in radar system and radar using the same
JP4492628B2 (en) * 2007-03-20 2010-06-30 株式会社デンソー Interference judgment method, FMCW radar

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