JPH1082855A - Object measuring device - Google Patents

Object measuring device

Info

Publication number
JPH1082855A
JPH1082855A JP25781196A JP25781196A JPH1082855A JP H1082855 A JPH1082855 A JP H1082855A JP 25781196 A JP25781196 A JP 25781196A JP 25781196 A JP25781196 A JP 25781196A JP H1082855 A JPH1082855 A JP H1082855A
Authority
JP
Japan
Prior art keywords
wave
received
waveform
received waveform
signal
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
JP25781196A
Other languages
Japanese (ja)
Inventor
Eiji Murao
英治 村尾
Naoyuki Hikita
尚之 疋田
Hideo Hosoya
英生 細谷
Satoshi Morioka
里志 森岡
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.)
Mazda Motor Corp
Original Assignee
Mazda Motor 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 Mazda Motor Corp filed Critical Mazda Motor Corp
Priority to JP25781196A priority Critical patent/JPH1082855A/en
Publication of JPH1082855A publication Critical patent/JPH1082855A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To accurately detect received waveform with an analogical simple circuit constitution even in the case where reflected wave (received waveform) is superposed on the first half part of transmitted waveform and reduce a wrong detection by the compression of a right slope part fluctuated relatively easily, by providing a means for compressing only the latter half part (right slope part) of received wavform, and comparing the received waveform, compressed by this means, with a prescribed threshold value to measure a parameter on a testee, and reduce dispersion caused by reverberation by compressing the right slope part (reverberating wave part) of a reverberation signal so as to be able to cope with the measurement with an inexpensive transmitting device. SOLUTION: In this object measuring device, wave motion is transmitted toward a prescribed detecting direction by a transmitting device 5, and the wave motion reflected by a subject 6 is received by a receiving device 7 to convent it into an electric signal so as to measure a parameter on the subject 6. In this case, a means 11 for compressing only the latter half part of received waveform is provided, and the received waveform compressed by the means 11 is compared with a prescribed threshold value to measure the above- mentioned parameter.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、例えば超音波な
どの波動を所定検知方向に向けて送波装置で送波し、障
害物などの被検物体で反射された波動を受波装置にて受
波して電気信号に変換し、被検物体に関するパラメータ
(例えば被検物体までの距離)を測定するような物体測
定装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for transmitting a wave such as an ultrasonic wave in a predetermined detection direction by a wave transmitting device, and a wave reflected by a test object such as an obstacle by a wave receiving device. The present invention relates to an object measuring apparatus that receives a wave, converts the signal into an electric signal, and measures a parameter (for example, a distance to the object) related to the object.

【0002】[0002]

【従来の技術】従来、上述例の物体測定装置において送
波された波動たとえば超音波が被検物体で反射されて、
この反射波を受波する時、信号処理の段階において反射
信号を検出する手段としては特開平5−87911号公
報に記載されたSTC(Sensitivity Time Control、感
度時間コントロール)法と、実開昭57−79782号
公報に記載されたTTC(Threshold Time Control時間
しきい値コントロール)法とがある。
2. Description of the Related Art Conventionally, a wave, for example, an ultrasonic wave transmitted by an object measuring apparatus of the above-described example is reflected by an object to be measured.
Means for detecting the reflected signal at the signal processing stage when receiving the reflected wave include the STC (Sensitivity Time Control) method described in Japanese Patent Application Laid-Open No. Hei 5-87911 and the method disclosed in There is a TTC (Threshold Time Control) method described in -79782.

【0003】前者のSTC法は近距離からの反射信号と
遠距離からの反射信号のレベルが同等になるように超音
波受波回路の増幅率を変更し、一定のしきい値にて反射
信号を検出する方法である。後者のTTC法は受信波形
のバックグランドレベルがフラットでない領域におい
て、時間に対応して比較器(コンパレータ)の基準にレ
ベルとしてのしきい値を変化させることで、反射信号を
検出する方法である。
In the former STC method, the amplification factor of the ultrasonic wave receiving circuit is changed so that the level of the reflected signal from a short distance becomes equal to the level of the reflected signal from a long distance, and the reflected signal is set at a certain threshold value. Is a method for detecting In the latter TTC method, in a region where the background level of the received waveform is not flat, a reflected signal is detected by changing a threshold value as a level with reference to a comparator in accordance with time. .

【0004】いま図5に示すように受信信号がない場合
の送信波の波形をaとし、この送信波の前半部(左側ス
ロープ部)に反射はbが上乗されるような場合、上述の
STC法により信号処理部の増幅器の増幅率を減衰させ
ると、反射波bを含む波形aの全体が圧縮され、本来検
出すべき反射波bまでもが同様に圧縮されるので、この
反射波b(つまり受波波形)を的確に検出することがで
きない問題点があった。
[0005] As shown in FIG. 5, the waveform of a transmission wave when there is no reception signal is denoted by a, and the reflection b is added to the first half (left slope) of the transmission wave. When the amplification factor of the amplifier in the signal processing unit is attenuated by the STC method, the entire waveform a including the reflected wave b is compressed, and even the reflected wave b to be detected is similarly compressed. (That is, the received waveform) cannot be accurately detected.

【0005】また上述のように送信波の前半部(左側ス
ロープ部)に反射波bが上乗された場合、TTC法によ
りしきい値(図5のカーブc参照)を時間に対応させて
変化させても左側のスロープ部に上乗された上述の反射
波b(つまり受波波形)を検出することは困難となる問
題点があった。
When the reflected wave b is added to the first half (left slope) of the transmitted wave as described above, the threshold value (see curve c in FIG. 5) is changed according to time by the TTC method. Even if this is done, there is a problem that it is difficult to detect the above-mentioned reflected wave b (that is, a received waveform) superimposed on the left slope portion.

【0006】[0006]

【発明が解決しようとする課題】この発明の請求項1記
載の発明は、受波波形の後半部(右側スロープ部)のみ
を圧縮する手段を設け、この手段で圧縮された受波波形
を所定のしきい値と比較して被検物体に関するパラメー
タを測定することで、送波波形の前半部に上述の如き反
射波(受波波形)が上乗されているような場合において
も、アナログ的な簡単な回路構成にて的確に受波波形の
検出を行なうことができ、しかも比較的変動しやすい右
側スロープ部の圧縮により誤検知を低減させることがで
き、さらには残響信号の右側スロープ部(残響波部)を
圧縮することにより、残響に起因するばらつきの低減を
図り、これにより安価な送波装置での対応が可能となる
物体測定装置の提供を目的とする。
According to the first aspect of the present invention, there is provided means for compressing only the latter half (right slope) of the received waveform, and the received waveform compressed by this means is subjected to a predetermined process. By measuring the parameter relating to the object to be measured in comparison with the threshold value, even if the reflected wave (received waveform) is added to the first half of the transmitted waveform as described above, the analog With the simple and simple circuit configuration, it is possible to accurately detect the received waveform, and to reduce the erroneous detection by compressing the relatively swayable right slope section. It is an object of the present invention to provide an object measurement device that reduces a variation caused by reverberation by compressing a reverberation wave portion, thereby enabling an inexpensive transmission device to cope with the problem.

【0007】この発明の請求項2記載の発明は、上記請
求項1記載の発明の目的と併せて、上述のしきい値を時
間と共にその値が低下すべく構成することで、受波は本
来時間と共に減衰するので、この受波の減衰としきい値
の変化とが対応して、より一層正確な受波検知を行うこ
とができる物体測定装置の提供を目的とする。
According to a second aspect of the present invention, in addition to the object of the first aspect of the present invention, the above-described threshold value is configured so that its value decreases with time. The object of the present invention is to provide an object measuring apparatus capable of performing more accurate detection of a received wave because the attenuation of the received wave and the change of the threshold value correspond to the attenuation of the received wave with time.

【0008】この発意の請求項3記載の発明は、上記請
求項1もしくは2記載の発明の目的と併せて、送波をパ
ルスに状に実行すると共に、送波と受波との時間差に基
づいて被検物体までの距離を測定すべく構成すること
で、物体検知のみならず被検物体までの距離を正確に測
定することができる物体測定装置の提供を目的とする。
[0008] The invention according to claim 3 of the invention combines the object of the invention described in claim 1 or 2 with transmitting a pulse in the form of a pulse and based on the time difference between the transmitted wave and the received wave. It is an object of the present invention to provide an object measuring device capable of accurately measuring not only the object detection but also the distance to the object by configuring the apparatus to measure the distance to the object.

【0009】この発明の請求項4記載の発明は、上記請
求項1,2もしくは3記載の発明の目的と併せて、波動
として超音波を用いることで、特に残響や送受波レベル
の変動等の影響が大きい超音波であっても正確な物体測
定ないし測距が達成できて、この超音波に好適な物体測
定装置の提供を目的とする。
According to a fourth aspect of the present invention, in addition to the object of the first, second, or third aspect of the present invention, the use of ultrasonic waves as waves makes it possible to reduce reverberation and fluctuations in transmission and reception levels. It is an object of the present invention to provide an object measuring apparatus which can achieve accurate object measurement or distance measurement even with an ultrasonic wave having a large influence, and is suitable for the ultrasonic wave.

【0010】[0010]

【課題を解決するための手段】この発明の請求項1記載
の発明は、波動を所定検知方向に向けて送波装置で送波
し、被検物体で反射された上記波動を受波装置にて受波
して電気信号に変換し、被検物体に関するパラメータを
測定する物体測定装置であって、受波波形の後半部のみ
を圧縮する手段を備え、上記手段で圧縮された受波波形
を所定のしきい値と比較して上記パラメータを測定する
物体測定装置であることを特徴とする。
According to a first aspect of the present invention, a wave is transmitted by a wave transmitting device in a predetermined detection direction, and the wave reflected by a test object is transmitted to a wave receiving device. An object measuring device that receives and converts the received signal into an electric signal, and measures parameters related to a test object, including a unit that compresses only the latter half of the received waveform. The object measuring device measures the parameter by comparing with a predetermined threshold value.

【0011】この発明の請求項2記載の発明は、上記請
求項1記載の発明の構成と併せて、上記しきい値は時間
と共にその値が低下する物体測定装置であることを特徴
とする。
According to a second aspect of the present invention, in addition to the configuration of the first aspect, the threshold value is an object measuring device whose value decreases with time.

【0012】この発明の請求項3記載の発明は、上記請
求項1もしくは2記載の発明の構成と併せて、上記送波
はパルス状に行なわれ、送波と受波との時間差に基づい
て被検物体までの距離を測定する物体測定装置であるこ
とを特徴とする。
According to a third aspect of the present invention, in addition to the configuration of the first or second aspect, the transmission is performed in a pulse form, and the transmission is performed based on a time difference between the transmission and the reception. It is an object measuring device for measuring a distance to a test object.

【0013】この発明の請求項4記載の発明は、上記請
求項1,2もしくは3記載の発明の構成と併せて、上記
波動が超音波に設定された物体測定装置であることを特
徴とする。
According to a fourth aspect of the present invention, in addition to the configuration of the first, second, or third aspect of the present invention, the object is an object measuring apparatus in which the wave is set to an ultrasonic wave. .

【0014】[0014]

【発明の作用及び効果】この発明の請求項1記載の発明
によれば、上述の送波装置は波動を所定検知方向(被検
物体の方向)に向けて送波し、受波装置は上述の送波が
被検物体で反射された波動(反射波)を受波して電気信
号に変換するが、上述の圧縮手段は受波波形の後半部
(右側スロープ部)のみを圧縮するので、送波波形の前
半部に反射波(受波波形)が上乗されているような場
合、この検出したい反射波の信号をスロープの右側まで
相対的に移動させ検出可能な状態と成すことができる。
According to the first aspect of the present invention, the above-described wave transmitting device transmits a wave in a predetermined detection direction (the direction of a test object), and the wave receiving device transmits the wave in the above-described direction. The transmitted wave of (1) receives the wave (reflected wave) reflected by the test object and converts it into an electric signal. However, since the above-described compression means compresses only the latter half (the right slope) of the received waveform, In the case where a reflected wave (received waveform) is superimposed on the first half of the transmitted waveform, the signal of the reflected wave to be detected is relatively moved to the right side of the slope to be in a detectable state. .

【0015】このため圧縮された受波波形を所定しきい
値と比較することで反射波(受波波形)を的確に検出す
ることができる効果がある。加えて、アナログ的な簡単
な回路構成にて受波検出ができ、しかも比較的変動しや
すい右側スロープ部の圧縮により誤検知を低減させるこ
とができる効果がある。さらに残響信号の右側スロープ
部(残響波部)を圧縮することで、残響に起因するばら
つきの低減を図って、これにより安価な送波装置での対
応が可能となる効果がある。
Therefore, there is an effect that the reflected wave (received waveform) can be accurately detected by comparing the compressed received waveform with a predetermined threshold value. In addition, there is an effect that reception can be detected with a simple analog circuit configuration, and erroneous detection can be reduced by compressing the relatively sloping right slope. Further, by compressing the right slope portion (reverberation wave portion) of the reverberation signal, variation caused by reverberation can be reduced, and thus, there is an effect that an inexpensive transmission device can be used.

【0016】この発明の請求項2記載の発明によれば、
上記請求項1記載の発明の効果と併せて、上述のしきい
値を時間と共にその値が低下すべく構成したので、受波
は本来時間と共に減衰するので、この受波の減衰としき
い値の変化とが対応して、より一層正確な受波検知を行
うことができる効果がある。
According to the invention described in claim 2 of the present invention,
In addition to the effect of the first aspect of the present invention, the above-mentioned threshold value is configured to decrease with time, so that the reception wave naturally attenuates with time. There is an effect that more accurate wave detection can be performed in response to the change.

【0017】この発意の請求項3記載の発明によれば、
上記請求項1もしくは2記載の発明の効果と併せて、送
波をパルスに状に実行すると共に、送波と受波との時間
差に基づいて被検物体までの距離を測定すべく構成した
ので、物体検知のみならず被検物体までの距離を正確に
測定することができる効果がある。
According to the invention described in claim 3 of the present invention,
In addition to the effect of the first or second aspect of the present invention, the transmission is performed in the form of a pulse, and the distance to the test object is measured based on the time difference between the transmission and the reception. In addition to the object detection, there is an effect that the distance to the test object can be accurately measured.

【0018】この発明の請求項4記載の発明によれば、
上記請求項1,2もしくは3記載の発明の効果と併せ
て、波動として超音波を用いたので、特に残響や送受波
レベルの変動等の影響が大きい超音波であっても正確な
物体測定ないし測距が達成できて、測距レンジが短い超
音波に好適となる効果がある。
According to the invention described in claim 4 of the present invention,
Since the ultrasonic wave is used as the wave in addition to the effect of the invention described in the above-mentioned claim 1, 2 or 3, it is possible to accurately measure the object even if the ultrasonic wave has a large influence such as a reverberation or a fluctuation of the transmission / reception level. The distance measurement can be achieved, and there is an effect that it is suitable for an ultrasonic wave having a short distance measurement range.

【0019】[0019]

【実施例】この発明の一実施例を以下図面に基づいて詳
述する。図面は物体測定装置を示し、図1において、こ
の物体測定装置1はシステム制御部2の次段に送信波形
を形成する送信部3を介して、超音波トランスジューサ
4の送波部5を接続している。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below in detail with reference to the drawings. The drawing shows an object measuring device. In FIG. 1, the object measuring device 1 is connected to a transmitting unit 5 of an ultrasonic transducer 4 via a transmitting unit 3 which forms a transmitting waveform at the next stage of a system control unit 2. ing.

【0020】上述の送波部5は波動すなわち超音波を被
検物体6の方向(所定検知方向)に向けてパルス状に送
波する送波装置であって、この被検物体6で反射された
波動は受波装置としての受波部7にて受波され、電気信
号に変換される。この実施例では上述の送波部5と受波
部7とは一体化されているが、図1にあっては説明の便
宜上、それぞれに分けて図示している。
The above-mentioned transmitting unit 5 is a transmitting device for transmitting a wave, that is, an ultrasonic wave, in a pulse shape toward the object 6 (predetermined detection direction). The wave is received by the wave receiving unit 7 as a wave receiving device, and is converted into an electric signal. In this embodiment, the above-described transmitting unit 5 and receiving unit 7 are integrated, but are separately illustrated in FIG. 1 for convenience of explanation.

【0021】上述の受波部7の次段には増幅器8、検波
器9、比較器10をこの順に接続する一方、前述のシス
テム制御部2の送信トリガを受けて作動するSTC信号
発生回路11とTTC信号発生回路12とを設け、さら
に上述のシステム制御部2および比較器10にスタート
・トリガライン13およびストップ・トリガライン14
を各別に介して距離計数部15を接続している。
An amplifier 8, a detector 9, and a comparator 10 are connected in this order to the next stage of the receiving unit 7, and an STC signal generating circuit 11 which operates upon receiving a transmission trigger from the system control unit 2. And a TTC signal generation circuit 12, and a start trigger line 13 and a stop trigger line 14 are provided in the system control unit 2 and the comparator 10.
Are connected to the distance counting unit 15 via each of them.

【0022】ここで、上述の増幅器8は電気信号に変換
後の受波信号を増幅する増幅率可変形の増幅手段(可変
増幅率端子に印加される電圧値によりその増幅率が変化
するもの)で、上述の検波器9は増幅後の受波信号の包
絡線を抽出するような検波処理を実行し、上述の比較器
9は検波後の信号としきい値とを比較して比較出力を形
成する。
Here, the above-mentioned amplifier 8 is a variable gain type amplifying means for amplifying a received signal after being converted into an electric signal (amplifier having a variable gain depending on a voltage value applied to a variable gain terminal). Then, the above-described detector 9 performs a detection process for extracting an envelope of the amplified received signal, and the above-described comparator 9 compares the detected signal with a threshold to form a comparison output. I do.

【0023】また上述の距離計数部15は送信トリガの
送信時に出力されるスタート・トリガにより計数を開始
し、比較器10の出力としてのストップ・トリガにより
計数を終了し、送波時刻と受波時刻との時間差に基づい
て被検物体6までの距離を測定する。つまり、この距離
計数部15は時間差と波の伝搬速度との積をとって距離
情報に変換するものである。
The above-described distance counting section 15 starts counting by a start trigger output at the time of transmission of a transmission trigger, ends counting by a stop trigger as an output of the comparator 10, and determines the transmission time and reception time. The distance to the test object 6 is measured based on the time difference from the time. That is, the distance counting section 15 converts the product of the time difference and the wave propagation velocity into distance information.

【0024】しかも、上述のSTC信号発生回路11は
増幅器8に対してSTC信号(時間に対応して増幅率を
低くする信号)を出力し、受波波形(図2に示す送波形
aに反射波bが上乗した波形)の後半部(右側スロープ
部)のみを圧縮し、同図に示す受波波形dを受波波形e
で示すように圧縮する。また上述のTTC信号発生回路
12は比較器10に対してTTC信号(時間と共にしき
い値が低下する信号)を出力し、図2に示すしきい値の
カーブcを同図に示すしきい値のカーブfのように変化
させる。
Further, the above-described STC signal generating circuit 11 outputs an STC signal (a signal for decreasing the amplification factor in accordance with time) to the amplifier 8 and reflects the received waveform (the transmission waveform a shown in FIG. 2). Only the latter half (right slope) of the waveform b) is compressed, and the received waveform d shown in FIG.
Compress as shown by. The above-described TTC signal generation circuit 12 outputs a TTC signal (a signal whose threshold value decreases with time) to the comparator 10, and changes the threshold curve c shown in FIG. As shown by the curve f.

【0025】図示実施例は上記の如く構成するものにし
て、以下作用を説明する。
The illustrated embodiment is configured as described above, and the operation will be described below.

【0026】システム制御部2からの送信トリガを受け
て送信部3は送信波形を形成し、送波部5は被検物体6
の方向に向けて超音波をパルス状に送波する。この被検
物体6で反射された超音波は受波部7により受波され、
電気信号に変換された後、次段の増幅器8で増幅される
が、この増幅器8に対してはSTC信号が印加されてお
り、時間と共に増幅率が低下するので、図2に示す受波
波形dはその後半部(右側スロープ部)のみが圧縮され
た受波波形eとなり、送波波形aの前半部に反射波(受
波波形)bが上乗されているような場合、この検出した
い反射波bの信号は相対的に右側へ移動させられた状態
となる。
Upon receiving a transmission trigger from the system controller 2, the transmitter 3 forms a transmission waveform, and the transmitter 5
The ultrasonic wave is transmitted in a pulse shape in the direction of. The ultrasonic wave reflected by the test object 6 is received by the wave receiving unit 7,
After being converted into an electric signal, the signal is amplified by an amplifier 8 at the next stage. Since the STC signal is applied to the amplifier 8 and the amplification factor decreases with time, the received waveform shown in FIG. d is a received waveform e in which only the latter part (right slope part) is compressed, and if the reflected wave (received waveform) b is added to the first half of the transmitted waveform a, this detection is desired. The signal of the reflected wave b is relatively shifted to the right.

【0027】また上述の比較器10に対してはTTC信
号が印加されており、時間と共にしきい値が低下するの
で、受波の減衰度合としきい値の変化(カーブcからカ
ーブfへの変化)度合とが略対応する。
Since the TTC signal is applied to the comparator 10 and the threshold value decreases with time, the degree of attenuation of the received wave and the change in the threshold value (change from the curve c to the curve f) ) The degree substantially corresponds to the degree.

【0028】したがって、上述のように送波波形aの前
半部(左側スロープ部)に反射波bが上乗しても、アナ
ログ的な簡単な回路構成により、的確に反射波(受波波
形)bの検出を行なうことができ、距離計数数15はス
タート・トリガの印加時点と、圧縮された状態下おける
反射波bがしきい値fに達した時に比較出力される比較
器10からのストップ・トリガの印加時点の差(送波と
受波との時間差)に基づいて被検物体6までの距離を測
定することができる。
Therefore, even if the reflected wave b is added to the first half (left slope portion) of the transmitted waveform a as described above, the reflected wave (received waveform) can be accurately obtained by a simple analog circuit configuration. b can be detected, and the distance count 15 is determined by the start trigger application time and the stop from the comparator 10 which is compared and output when the reflected wave b in the compressed state reaches the threshold value f. The distance to the test object 6 can be measured based on the difference between the application points of the trigger (the time difference between the transmitted wave and the received wave).

【0029】以上要するに、上述の送波装置(送波部5
参照)は波動(超音波参照)を所定検知方向に向けて送
波し、受波装置(受波部7参照)は上述の送波が被検物
体6で反射された波動(反射波)を受波して電気信号に
変換するが、上述の圧縮手段(STC信号発生回路11
参照)は受波波形の後半部(右側スロープ部)のみを圧
縮するので、送波波形aの前半部に反射波(受波波形)
bが上乗されているような場合、この検出したい反射波
bの信号をスロープの右側まで相対的に移動(波形e参
照)させることができる。
In short, the above-described wave transmitting device (wave transmitting unit 5)
) Transmits a wave (refer to an ultrasonic wave) in a predetermined detection direction, and a wave receiving device (refer to a wave receiving unit 7) transmits the wave (reflected wave) in which the above-described transmitted wave is reflected by the object 6. The received signal is converted into an electric signal.
) Compresses only the latter half (the right slope) of the received waveform, so that the reflected wave (received waveform) appears in the first half of the transmitted waveform a.
When b is added, the signal of the reflected wave b to be detected can be relatively moved to the right side of the slope (see waveform e).

【0030】このため圧縮された受波波形eを所定しき
い値(カーブf参照)と比較することで反射波(受波波
形)bを的確に検出することができる効果がある。加え
て、アナログ的な簡単な回路構成にて受波検出ができ、
しかも比較的変動しやすい右側スロープ部の圧縮により
誤検知を低減させることができる効果がある。さらに残
響信号の右側スロープ部(残響波部)を圧縮すること
で、残響に起因するばらつきの低減を図って、これによ
り安価な送波装置での対応が可能となる効果がある。
Therefore, there is an effect that the reflected wave (received waveform) b can be accurately detected by comparing the compressed received waveform e with a predetermined threshold (see curve f). In addition, the received wave can be detected with a simple analog circuit configuration.
In addition, there is an effect that erroneous detection can be reduced by compression of the right slope portion which is relatively easily changed. Further, by compressing the right slope portion (reverberation wave portion) of the reverberation signal, variation caused by reverberation can be reduced, and thus, there is an effect that an inexpensive transmission device can be used.

【0031】また、上述のしきい値をTTC信号発生回
路12により時間と共にその値が低下すべく構成したの
で、受波は時間と共に減衰し、この受波の減衰としきい
値の変化とが対応するため、より一層正確な受波検知を
行なうことができる効果がある。
Since the above threshold value is configured to decrease with time by the TTC signal generation circuit 12, the reception wave attenuates with time, and the attenuation of the reception wave corresponds to the change in the threshold value. Therefore, there is an effect that more accurate wave reception detection can be performed.

【0032】さらに、送波をパルスに状に実行すると共
に、送波と受波との時間差に基づいて上述の距離計数部
15が被検物体6までの距離を計測するので、物体検知
のみならず被検物体6までの距離を正確に測定すること
ができる効果がある。
Further, the transmission is executed in the form of a pulse, and the distance counting unit 15 measures the distance to the object 6 based on the time difference between the transmission and reception. This has the effect that the distance to the test object 6 can be accurately measured.

【0033】加えて、波動として超音波を用いたので、
特に残響や送受波レベルの変動等の影響が大きい超音波
であっても正確な物体測定ないし測距が達成できて、測
距レンジが短い超音波に好適となる効果がある。
In addition, since an ultrasonic wave was used as a wave,
In particular, accurate measurement or ranging of an object can be achieved even with an ultrasonic wave having a great influence of reverberation or fluctuation of a transmitted / received wave level, which is advantageous for an ultrasonic wave having a short ranging range.

【0034】図3は超音波センサヘッドの構成を示し、
この超音波センサヘッド16は電磁シールド効果(ノイ
ズ混入防止効果)を得る目的で、金属製の共振筺体17
と同様に金属製の裏板18とを用い、これら両者17,
18の内部に圧電振動子としての圧電セラミック素子1
9(図1の超音波トランスジューサ4に相当)と、受信
回路部20とを設置し、回路グランド(アース部)21
を共振筺体17に接続している。しかも共振筺体17の
内部を制振および防水を兼ねるシリコンゴム系の充填材
22で充填し、裏面を裏板18にてカバーし、この裏板
18も接地している。なお、図中23はケーブルであ
る。
FIG. 3 shows the configuration of the ultrasonic sensor head.
The ultrasonic sensor head 16 is provided with a metallic resonance housing 17 for the purpose of obtaining an electromagnetic shielding effect (effect of preventing noise mixing).
A metal back plate 18 is used in the same manner as
Piezoelectric ceramic element 1 as a piezoelectric vibrator inside 18
9 (corresponding to the ultrasonic transducer 4 in FIG. 1) and the receiving circuit unit 20, and a circuit ground (earth unit) 21.
Are connected to the resonance housing 17. Moreover, the inside of the resonance housing 17 is filled with a silicone rubber-based filler 22 that also functions as a vibration damper and a waterproofer, and the back surface is covered with the back plate 18, and the back plate 18 is also grounded. In the figure, reference numeral 23 denotes a cable.

【0035】圧電セラミック素子19の出力端子からラ
イン19a,19bを介して直接得た信号を受信回路部
20にて増幅し、信号レベルを充分高くして、さらにイ
ンピーダンスを充分低くして出力すべく構成している。
上述の出力端子から直接信号を得るのでノイズの混入が
少ないうえ、その段階で増幅器8(図1参照)により信
号レベルを充分高くすること並びに伝送系のインピーダ
ンスを低くすることにより、S/N比が大幅に改善さ
れ、高感度受信が可能となる。また極めて簡単な回路で
実現でき、かつ簡単な構造体に納まるため、低コスト
で、占有スペースおよび消費電力も小となる。また上述
の充填材22残響を抑止するダンパ効果をも確保するこ
とができる。
In order to amplify a signal directly obtained from the output terminal of the piezoelectric ceramic element 19 via the lines 19a and 19b in the receiving circuit section 20, to make the signal level sufficiently high, and further to make the impedance sufficiently low for output. Make up.
Since the signal is directly obtained from the output terminal described above, noise is less mixed, and at this stage, the signal level is sufficiently increased by the amplifier 8 (see FIG. 1) and the impedance of the transmission system is reduced, so that the S / N ratio is reduced. Is greatly improved, and high-sensitivity reception becomes possible. Further, since it can be realized with an extremely simple circuit and can be accommodated in a simple structure, the cost is low, the occupied space and the power consumption are small. In addition, a damper effect for suppressing the reverberation of the filler 22 can be secured.

【0036】図4は上述の物体測定装置の使用態様の一
例を示し、例えば図3に示す超音波センサヘッド16を
車両23のフロント側、リヤ側に複数配設して、複数検
知領域A〜Fを確保すべく構成し、この物体測定装置を
車載用のコーナセンサ、バックソナーとして用いるよう
に構成したものである。このように構成すると、車両2
3の駐車時その他必要時に車両23と被検物体6との間
の距離を計測することができるので至便である。
FIG. 4 shows an example of usage of the above-described object measuring apparatus. For example, a plurality of ultrasonic sensor heads 16 shown in FIG. F is ensured, and the object measuring device is configured to be used as a corner sensor and a back sonar for a vehicle. With this configuration, the vehicle 2
This is convenient because the distance between the vehicle 23 and the test object 6 can be measured when the vehicle 3 is parked or when necessary.

【0037】この発明の構成と、上述の実施例との対応
において、この発明の波動は、実施例の超音波に対応
し、以下同様に、送波装置は、送波部5に対応し、受波
装置は、受波部7に対応し、パラメータは、被検物体6
までの距離に対応し、圧縮する手段は、STC信号発生
回路11に対応し、しきい値を時間と共に低下させる手
段は、TTC信号発生回路12に対応するも、この発明
は、上述の実施例の構成のみに限定されるものではな
い。例えば、波動としては上述の超音波に代えて電磁波
やレーザ等の他の波動を用いてもよい。
In the correspondence between the configuration of the present invention and the above-described embodiment, the wave of the present invention corresponds to the ultrasonic wave of the embodiment, and similarly, the transmitting apparatus corresponds to the transmitting section 5, The wave receiving device corresponds to the wave receiving unit 7, and the parameter is
The means for compressing and corresponding to the distance up to corresponds to the STC signal generating circuit 11 and the means for lowering the threshold value with time corresponds to the TTC signal generating circuit 12. However, the present invention is not limited only to the above configuration. For example, another wave such as an electromagnetic wave or a laser may be used instead of the above-described ultrasonic wave.

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

【図1】 本発明の物体測定装置を示すブロック図。FIG. 1 is a block diagram showing an object measuring device according to the present invention.

【図2】 受波検出時の波形およびしきい値の説明図。FIG. 2 is an explanatory diagram of a waveform and a threshold value when a received wave is detected.

【図3】 超音波センサヘッドの断面図。FIG. 3 is a sectional view of an ultrasonic sensor head.

【図4】 本発明の物体測定装置の使用態様の一例を示
す概略平面図。
FIG. 4 is a schematic plan view showing an example of a usage mode of the object measuring device of the present invention.

【図5】 従来の問題点を示す説明図。FIG. 5 is an explanatory view showing a conventional problem.

【符号の説明】 5…送波部 6…被検物体 7…受波部 11…STC信号発生回路 12…TTC信号発生回路[Explanation of Symbols] 5 ... Transmission unit 6 ... Test object 7 ... Reception unit 11 ... STC signal generation circuit 12 ... TTC signal generation circuit

───────────────────────────────────────────────────── フロントページの続き (72)発明者 森岡 里志 広島県安芸郡府中町新地3番1号 マツダ 株式会社内 ────────────────────────────────────────────────── ─── Continued on the front page (72) Inventor Satoshi Morioka 3-1, Shinchi, Fuchu-cho, Aki-gun, Hiroshima Mazda Co., Ltd.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】波動を所定検知方向に向けて送波装置で送
波し、被検物体で反射された上記波動を受波装置にて受
波して電気信号に変換し、被検物体に関するパラメータ
を測定する物体測定装置であって、受波波形の後半部の
みを圧縮する手段を備え、上記手段で圧縮された受波波
形を所定のしきい値と比較して上記パラメータを測定す
る物体測定装置。
1. A wave transmitting device in which a wave is directed in a predetermined detection direction by a wave transmitting device, and the wave reflected by an object to be measured is received by a wave receiving device and converted into an electric signal. An object measuring device for measuring a parameter, comprising: means for compressing only the latter half of a received waveform, and comparing the received waveform compressed by the means with a predetermined threshold to measure the parameter. measuring device.
【請求項2】上記しきい値は時間と共にその値が低下す
る請求項1記載の物体測定装置。
2. An object measuring apparatus according to claim 1, wherein said threshold value decreases with time.
【請求項3】上記送波はパルス状に行なわれ、送波と受
波との時間差に基づいて被検物体までの距離を測定する
請求項1もしくは2記載の物体測定装置。
3. The object measuring apparatus according to claim 1, wherein the transmitting is performed in a pulse shape, and the distance to the object to be measured is measured based on a time difference between the transmitting and receiving waves.
【請求項4】上記波動が超音波に設定された請求項1,
2もしくは3記載の物体測定装置。
4. The method according to claim 1, wherein the wave is set to an ultrasonic wave.
4. The object measuring device according to 2 or 3.
JP25781196A 1996-09-05 1996-09-05 Object measuring device Pending JPH1082855A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25781196A JPH1082855A (en) 1996-09-05 1996-09-05 Object measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25781196A JPH1082855A (en) 1996-09-05 1996-09-05 Object measuring device

Publications (1)

Publication Number Publication Date
JPH1082855A true JPH1082855A (en) 1998-03-31

Family

ID=17311456

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25781196A Pending JPH1082855A (en) 1996-09-05 1996-09-05 Object measuring device

Country Status (1)

Country Link
JP (1) JPH1082855A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010256317A (en) * 2009-04-24 2010-11-11 Avermedia Information Inc Ultrasonic reception module, ultrasonic distance measuring system, ultrasonic distance measuring method, and overhead camera
JP2022155232A (en) * 2021-03-30 2022-10-13 パナソニックIpマネジメント株式会社 Ranging device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010256317A (en) * 2009-04-24 2010-11-11 Avermedia Information Inc Ultrasonic reception module, ultrasonic distance measuring system, ultrasonic distance measuring method, and overhead camera
JP2022155232A (en) * 2021-03-30 2022-10-13 パナソニックIpマネジメント株式会社 Ranging device

Similar Documents

Publication Publication Date Title
US6304179B1 (en) Ultrasonic occupant position sensing system
KR200492445Y1 (en) Circuit for acoustic distance time of flight compensation
US4315325A (en) Echo ranging pulse discrimination circuit
JP4377121B2 (en) Distance measurement and pressure measurement inside air spring
JPS6224747B2 (en)
US20210156995A1 (en) Time-varying template for improved short-distance performance in coded ultrasonic ranging
US6614719B1 (en) Ultrasonic doppler effect speed measurement
US4453238A (en) Apparatus and method for determining the phase sensitivity of hydrophones
EP0393828A3 (en) A method and apparatus for testing the response of a stress wave sensor
JPH1082855A (en) Object measuring device
JP3296804B2 (en) Obstacle judgment method
JP3047588B2 (en) Ultrasonic transducer for liquid concentration meter
JPS5826283A (en) Ultrasonic measuring device with self-diagnosing function
JP2818025B2 (en) Ultrasonic ranging device
US20230028853A1 (en) Variable resonance frequency acoustic wave emission and/or detection device
JP2803857B2 (en) Ultrasonic detector
KR0152725B1 (en) Distance measurement method and apparatus using ultrasonic wave
JPH04233487A (en) Ultrasonic distance measuring apparatus
KR20010056696A (en) Device and method for measuring distance using ultrasonic waves
JPH0454471Y2 (en)
KR100192637B1 (en) Apparatus and method for detecting the optimum driving frequency of ultrasonic sensor
JP3296985B2 (en) Ultrasonic snow gauge
KR0129845B1 (en) Distance measurement method and apparatus using ultrasonic wave
JPH03180794A (en) Method and instrument for ultrasonic distance measurement
JP2820315B2 (en) Ultrasonic ranging device