JPS60140168A - Ultrasonic distance measuring apparatus - Google Patents

Ultrasonic distance measuring apparatus

Info

Publication number
JPS60140168A
JPS60140168A JP25063083A JP25063083A JPS60140168A JP S60140168 A JPS60140168 A JP S60140168A JP 25063083 A JP25063083 A JP 25063083A JP 25063083 A JP25063083 A JP 25063083A JP S60140168 A JPS60140168 A JP S60140168A
Authority
JP
Japan
Prior art keywords
pulse
circuit
ultrasonic
time
transmission
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
JP25063083A
Other languages
Japanese (ja)
Inventor
Masayuki Tone
利根 昌幸
Tsutomu Yano
屋野 勉
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP25063083A priority Critical patent/JPS60140168A/en
Publication of JPS60140168A publication Critical patent/JPS60140168A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO 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
    • G01S15/00Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems
    • G01S15/02Systems using the reflection or reradiation of acoustic waves, e.g. sonar systems using reflection of acoustic waves
    • G01S15/06Systems determining the position data of a target
    • G01S15/08Systems for measuring distance only
    • G01S15/10Systems for measuring distance only using transmission of interrupted, pulse-modulated waves
    • G01S15/101Particularities of the measurement of distance

Abstract

PURPOSE:To enable the measurement of distance in a wide range from the close to far range by controlling the number of waves of a transmission pulse corresponding to the distance to be measured with an output signal of a time measuring section for measuring time between respective pulses received and transmitted. CONSTITUTION:A transmission pulse is applied to an ultrasonic sensor 3 from a transmission circuit 2 and the pulse reflected from an object to be measured received with the ultrasonic sensor 3. Then, the pulse is amplified and detected with a receiving circuit 4 and compared with the reference voltage by a comparator circuit 5 to generate an output pulse according to being smaller or larger than the reference voltage. Then, a pulse is generated with a time measuring circuit 6 with the length corresponding to time between the transmitted pulse and the received pulse, namely, the proparation time between the transmission and reception of the ultrasonic pulse. Corresponding to the output of the circuit 6, a number of waves controlling circuit 10 regulates the gate pulse according to distance to be measured to control the number of waves of the transmission pulse.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は超音波距離測定装置に関するものであ従来例の
構成とその問題点 従来の超音波距離測定装置の構成を第1図に、図示する
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an ultrasonic distance measuring device.The configuration of a conventional example and its problemsThe configuration of a conventional ultrasonic distance measuring device is illustrated in FIG.

1は超音波センサ3に加える送信パルスの波数を制御す
るゲートパルスを発生し、またゲートパルスの発生に同
期して時間測定回路6の測定スタートパルスを発生する
ゲートパルス発生回路、2は送(Flパルスを超音波セ
ンサ3に印加する送信回路、4は被測定物(図示せず)
によって反射された超音波反射パルスを超音波センサ3
で受波したのち、その出力を増幅、検波する受信回路、
6は受信回路の出力電圧を基準電圧と比較し、出力電圧
と基準電圧との大小に応じて出力パルスを発生する比較
回路、6は送信パルスと受信パルスの間の時間即ち、超
音波パルス伝播時間を測定する時間測定回路でありゲー
トパルス発生回路1によって発生されたスタートパルス
から比較回路6の出力パルスま(の時間間隔を測定する
。7は時間−・距離変換回路であり、上述のようにして
測定された時間を一定の関係式によって距離に変換する
1 is a gate pulse generation circuit that generates a gate pulse that controls the wave number of the transmission pulse applied to the ultrasonic sensor 3, and also generates a measurement start pulse for the time measurement circuit 6 in synchronization with the generation of the gate pulse; 2 is a transmission ( A transmitting circuit that applies Fl pulses to the ultrasonic sensor 3, 4 is an object to be measured (not shown)
The ultrasonic pulse reflected by the ultrasonic sensor 3
A receiving circuit that amplifies and detects the output after receiving the wave at
6 is a comparison circuit that compares the output voltage of the receiving circuit with a reference voltage and generates an output pulse depending on the magnitude of the output voltage and the reference voltage. 6 is the time between the transmitted pulse and the received pulse, that is, the ultrasonic pulse propagation. This is a time measurement circuit that measures time, and measures the time interval from the start pulse generated by the gate pulse generation circuit 1 to the output pulse of the comparison circuit 6. 7 is a time/distance conversion circuit, as described above. Convert the measured time to distance using a certain relational expression.

以上のような構成の超音波距離測定装置における各部の
波形を第2図にろくず。第2図において、aはゲー]・
パルス発生回路1で発生され、送信パルスの波数を決め
るゲートパルス、bは超音波センサ3に印加される送信
パルス、Cは受信回路4において受信される受信波形で
あり、8は送信回路2から受信回路4への送信信号の漏
洩波形、9シL被測定物からの反射波形である。dは受
信回路4において上記漏洩波および反射波を検波整流し
/こ後の波形、eは比較回路6において検波・整流波形
dの振幅と基準電圧Es とを比較し、検波・整流波形
dの振幅が基準電圧EsJ:り大きいときに発生される
出力パルスであり送イ菖パルスbの1ン」り部分との時
間間隔Toが測定距離に対応する3゜従来、一般に使用
される超音波センサ3のパルス応答特性は不十分であっ
たので超音波センサ3の送信振幅を飽和振幅まで完全に
立上らせた状態で使用するためには、波数の多い送信パ
ルスによ−・て超音波センサ3を駆動することが必要で
あり、第2図Cに示す漏洩波8の継続1積間Tdを十分
短かくすることは困難であった。従って漏洩波8の継続
時間Tdの時間内に反射波9を受波するような近接距離
に被測定物が存在する場合は、第3図に示すように反射
波9と漏洩波8が時間軸上で重畳し、距離測定が困難に
なるという問題点を有していた。一方、近接距離測定を
可能とするため、反射波9と漏洩波8が時間軸上で重畳
しないように送信パルスの波数を少なくしたときは超音
波センサ3の過渡応答特性が不十分なために、超音波セ
ンサ3の送信振巾は、第4Naに示す送信パルスの波数
が十分多いときの飽和振rlJvsまで立上らず第4図
すに示すように飽和振巾Vsと比較して小さい振11]
VLか得られないので測定距離を大きく取ることが困難
になるという問題点を有していた。
Figure 2 shows the waveforms of each part of the ultrasonic distance measuring device configured as described above. In Figure 2, a is game]
The gate pulse generated by the pulse generation circuit 1 determines the wave number of the transmission pulse, b is the transmission pulse applied to the ultrasonic sensor 3, C is the reception waveform received by the reception circuit 4, and 8 is the reception waveform from the transmission circuit 2. These are the leakage waveform of the transmission signal to the receiving circuit 4 and the reflected waveform from the 9th L measured object. d is the waveform after detection and rectification of the leaky wave and reflected wave in the receiving circuit 4, and e is the waveform after the detected and rectified waveform d is detected and rectified in the comparator circuit 6. This is an output pulse that is generated when the amplitude is greater than the reference voltage EsJ, and the time interval To from the 1-input part of the sending pulse b is 3 degrees, which corresponds to the measurement distance. Since the pulse response characteristics of the ultrasonic sensor 3 were insufficient, in order to use the ultrasonic sensor 3 with the transmission amplitude completely raised to the saturation amplitude, it was necessary to It is necessary to drive the sensor 3, and it has been difficult to make the duration Td of the leakage wave 8 shown in FIG. 2C sufficiently short. Therefore, if the object to be measured exists at such a close distance that the reflected wave 9 is received within the duration time Td of the leaky wave 8, the reflected wave 9 and the leaked wave 8 are separated from each other on the time axis as shown in FIG. This has the problem that the distance measurement becomes difficult due to the overlapping of the two objects. On the other hand, when the wave number of the transmitted pulse is reduced so that the reflected wave 9 and the leaked wave 8 do not overlap on the time axis to enable close distance measurement, the transient response characteristics of the ultrasonic sensor 3 are insufficient. , the transmission amplitude of the ultrasonic sensor 3 does not rise to the saturation amplitude rlJvs when the wave number of the transmission pulse shown in No. 4 Na is sufficiently large, but becomes a small amplitude compared to the saturation amplitude Vs as shown in Fig. 4. 11]
This method has a problem in that it is difficult to obtain a large measurement distance because VL cannot be obtained.

発明の目的 本発明は以上のような従来の問題点を解決するためにな
されたもので超音波距離測定装置の距離測定を近接距離
から遠距離に至る広い範囲にわたって可能にすることを
目的とするものである。
Purpose of the Invention The present invention has been made to solve the above-mentioned conventional problems, and an object of the present invention is to enable distance measurement using an ultrasonic distance measuring device over a wide range from close distances to long distances. It is something.

発明の構成 本発明は上記目的を達成するもので、超音波センサと、
前記超音波センサに送信パルスを印加する送信部と、被
測定物からの超音波反射パルスを受信する受信部と、前
記受信部の出力電圧と基q一定電圧を比較する比較部上
、送信パルスと受信バルクの間の時間を測定する時間測
定部と、前記11i’1間測定部で測定された伝播時間
を距離に変換する時間−距離変換部と、前記時間測定部
の出力仏−弓により前記送信部の送信パルスの波数を制
御する波数制御部とを具備することを特徴とする超音波
距離測定装置を提供するものである。
Structure of the Invention The present invention achieves the above object, and includes an ultrasonic sensor,
a transmitter that applies a transmit pulse to the ultrasonic sensor; a receiver that receives the ultrasonic reflected pulse from the object to be measured; a comparator that compares the output voltage of the receiver with the base q constant voltage; and a time-distance conversion unit that converts the propagation time measured by the 11i'1 measurement unit into a distance, and the output of the time measurement unit The present invention provides an ultrasonic distance measuring device characterized by comprising a wave number control section that controls the wave number of the transmission pulse of the transmitting section.

実施例の説明 以下に本発明の実施例を図[nlを用いて説明する。Description of examples Examples of the present invention will be described below using FIG.

第6図は本発明の一実施例における超音波iI!1gj
 禽IFilll+定装置のブロック図を示す。
FIG. 6 shows ultrasonic iI! in one embodiment of the present invention! 1gj
FIG. 2 shows a block diagram of the poultry IFill+ stationary device.

図において、2は送信回路、3は超音波プロニブ、4は
受信回路、5は比較回路、6はh間測驚回路、7は時間
−距離変換回路であり10は時間測定回路6の出力に対
応した信号を用いて送信パルスの波数を制御するための
波数制御回路で、測定11.’11ii1が短かいとき
、即ち測定距離の短かいときは、ゲートパレスを短かく
して送信パルスの波数?少々くし、測定時間が長いとき
即ち測定距離の長いときはゲートパルスを長くして送信
パルスの波数を多くするように動作する。
In the figure, 2 is a transmitting circuit, 3 is an ultrasonic probe, 4 is a receiving circuit, 5 is a comparison circuit, 6 is an h-interval start-up circuit, 7 is a time-distance conversion circuit, and 10 is the output of the time measurement circuit 6. Measurement 11. with a wave number control circuit for controlling the wave number of the transmitted pulse using a corresponding signal. When '11ii1 is short, that is, when the measurement distance is short, shorten the gate palace and adjust the wave number of the transmitted pulse. When the measurement time is long, that is, the measurement distance is long, the gate pulse is lengthened to increase the wave number of the transmitted pulse.

波数制御回路10の一実施例を第6図に、各部の波形を
第7図に示す。6は送信パルスと受信パルス間の時間を
測定する(仏間測定回路であり第7図aに示すように超
音波パルスの送受仏間の伝播時間Toに対応した長さの
パルスを発生ずる。また波数制御回路10の積分回路、
ピークホールド回路11およびゲートパルス発生回路1
2から成っており時間測定回路6の出力パルス(第7図
a)を積分した後(第7図b)のピーク値をビークホル
ト回路11にホールドし、ホールドされた電圧値を用い
てゲートパルス発生回路12のパルス長ざを決定する定
数を制住1することにより、ゲートパルス長を変化させ
て、送信パルスの波数を開側1する。ここにゲー トパ
ルス長さを決定する定数は例えばコンデ/すCの容積、
であり、バリギャップを用いることによって電圧に応じ
た容u1変化が可能となり、従って超音波・4ノシ、ス
の伝播[Pl−間即ち測定距離に応じてゲーレ(ルス長
さを変化することが1]能となる。
An embodiment of the wave number control circuit 10 is shown in FIG. 6, and waveforms of various parts are shown in FIG. 6 measures the time between the transmitted pulse and the received pulse (it is a distance measuring circuit, which generates a pulse with a length corresponding to the propagation time To between the transmitting and receiving pulses of the ultrasonic pulse as shown in Fig. 7a). an integrating circuit of the control circuit 10;
Peak hold circuit 11 and gate pulse generation circuit 1
After integrating the output pulse of the time measuring circuit 6 (Fig. 7a), the peak value (Fig. 7b) is held in the peak hold circuit 11, and the gate pulse is generated using the held voltage value. By setting the constant that determines the pulse length of the circuit 12 to 1, the gate pulse length is changed and the wave number of the transmission pulse is set to 1 on the open side. Here, the constant that determines the gate pulse length is, for example, the volume of the capacitor/cell C,
By using a burr gap, it is possible to change the capacitance u1 according to the voltage, and therefore the propagation of ultrasonic waves [Pl-, that is, the Gehle length can be changed depending on the measurement distance]. 1] Become Noh.

波数制御回路10の第2の実施例乏′第8図に、各部の
波形を第9図に示す。
A second embodiment of the wave number control circuit 10 is shown in FIG. 8, and waveforms at various parts are shown in FIG. 9.

6は時間測定回路であり、第9図すに示すように超音波
パルスの送受仏間の伝播時間T(1に対応した長さのパ
ルスを発生する。寸だ波数制御回路10ハ積分回路、レ
ベルコンパレータ137坪安定マルチバイブレーク14
.送信タイミングノ(ルス発生回路16およびアンドゲ
ート16」:り成っている。時間測定回路6の出力・々
ルス(第9図b)の積分波形(第9図C)を人力とり、
、lrときのレベルコンパレータ13の出カッ(レス(
TB 9 図d ) (7)?&縁を用いて一定時間T
1なる長さの・ζノトスを発生する単安定マルチバイブ
レータ14を動作させる。
6 is a time measurement circuit, which generates a pulse having a length corresponding to the propagation time T (1) between the transmitter and receiver of the ultrasonic pulse as shown in Fig. 9. Comparator 137 tsubo stable multi-by break 14
.. The transmission timing signal consists of a pulse generation circuit 16 and an AND gate 16.The integrated waveform (Fig. 9C) of the output pulse of the time measurement circuit 6 (Fig. 9B) is manually obtained.
, the output of the level comparator 13 when lr (res()
TB 9 Figure d) (7)? & T for a certain period of time using the edges
A monostable multivibrator 14 that generates .zeta.notos with a length of 1 is operated.

単安定マルチバイブレータ14の出力ノ:ルス(第9図
6)の長さT1ばTs なる繰返しItd期をもったパ
ルス幅Tp7i1.る送信タイミングノくルア、(i9
図a)と時間的に1畳する部分をもつように設定さ■る
。上記送信タイミングパルス(第9図a)は第8図にお
いて送信タイミングパルス発生回路16によって発生さ
れる。
The output voltage of the monostable multivibrator 14 is a pulse width Tp7i1. with a repeating Itd period of length T1 (see FIG. 9, 6) and Ts. Lua, (i9
It is set so that it has a part that is 1 tatami in time with Figure a). The transmission timing pulse (FIG. 9a) is generated by the transmission timing pulse generation circuit 16 in FIG.

次に単安定マルチバイブレータ14の出力パルス(第9
図e)と送信タイミング・Z)レス(第9図a)をアン
トゲ−1・16に人力することにより、第9図fに示す
パルス幅T27zるパ/L・スが得られる。
Next, the output pulse of the monostable multivibrator 14 (9th
By manually inputting the transmission timing and transmission timing Z) (FIG. 9a) to the computer game 1.16, a pulse width T27z shown in FIG. 9F can be obtained.

このパルスを送信用ゲ−トパルスとして用いることによ
り送信パレスの波数を制御することが可能であり、測定
距離の大きい時は上記パルス幅T2が長くなり、測定距
離の小さい時はパルス幅T2は短かくすることができる
By using this pulse as a transmission gate pulse, it is possible to control the wave number of the transmission pulse. When the measurement distance is large, the pulse width T2 becomes long, and when the measurement distance is small, the pulse width T2 is short. It is possible to do this.

かかる実施例においては測定距離に応じて送イhパルス
の波数を制作1することにより近接距離から遠距離まで
の広範囲にわたって正確な距離測定が可能となる。
In this embodiment, by adjusting the wave number of the transmitted h pulse according to the measurement distance, it becomes possible to accurately measure distances over a wide range from close distances to long distances.

発明の効果 以上要するに本発明は超音波センサと、前記超音波セン
サに送信パルスを印加する送信部と、被測定物からの超
音波反射ノ:)レスを受イア)する受イア1部と、前記
受信部の出力電圧と基準電圧とを」シリ・交1−る比較
部と、送信パルスと受信バA/スの間の1lj1間を測
定する時間測定部と、前記時間測定部で測定された伝播
時間を距離に変換する時間−距離変換部と、前記時間測
定部の出力信号により前記送信部の送信パルスの波数を
制御する波数制省11部とを具備することを特徴とする
超音波距離測定装置を提供するもので、測定耐量1に対
応した出力(M”kj’ %用いて送信パルスの波数を
制御し、測定距離が小さくなるほど送イハパルスの波数
を少なく、4だ測定距離が大きくなるほど送信)々レス
の波数を多くすることが可能となるので、超音波距離測
定装置の測定範囲を近接距離から長いl[′1jllf
flに奎るーまて広い範囲に設定することができる。
Effects of the Invention In summary, the present invention includes an ultrasonic sensor, a transmitting section that applies a transmitting pulse to the ultrasonic sensor, a receiving ear section that receives ultrasonic waves reflected from an object to be measured; a comparison section that compares the output voltage of the receiving section and a reference voltage serially and crosswise; a time measuring section that measures the interval between the transmitting pulse and the receiving bus A/S; The ultrasonic wave is characterized by comprising: a time-distance conversion section that converts the propagation time into a distance; and a wave number control section 11 that controls the wave number of the transmission pulse of the transmitter based on the output signal of the time measurement section. This device provides a distance measuring device that controls the wave number of the transmitted pulse using the output (M"kj'%) corresponding to the measurement tolerance level 1. The smaller the measurement distance is, the lower the wave number of the transmitted pulse is. I see, since it is possible to increase the number of waves for each response (transmission), the measurement range of the ultrasonic distance measuring device can be extended from close distance to l['1jllf
It can be set in a wide range.

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

第1図は従来の超音波111j 11Jff測定装置の
1fJi成ブロツブロック2図は従来の超音波距離測定
装置における各部の波形を示すタイミングチャー1・、
第3図は送信パルスの漏洩波と反射、Cルスが中8畳し
A−ス応答特性の説明図、第6図は本発明の一実施例に
おける超音波距離測定装置の構成ブロック図、第6図は
本発明の要部である波数制御回路の第一実施例を示ずブ
o 、7り図、第7図は前記第一実施実施例を示すブロ
ック図、第9図は前記第二実施例における各部の波形を
示すタイミングチャー トである。 2−・・送信回路、3 ・・超音波センサ、4・・・受
信回路、6・ ・比較回路、6・一時間測定回路、7 
・・時間−距離変換回路、1o・・・−波数制御回路、
11−・ ・ピークホールド回路、12・・・・ゲート
パルス発生回路、13・ レベルコンパレータ、14・
・・単安定マルチバイブレータ、16 ・送信タイミン
グパルス発生回路、16・・−アントゲ−ト。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第 
1 図 集2図 第 3 (2) 第 4 図 第 5 図 4 5 6 7 第6図 第7図 第 8 図 1θ / 5 第9図 背 Tz
Figure 1 shows the 1fJi block diagram of a conventional ultrasonic distance measuring device.
FIG. 3 is an explanatory diagram of leakage waves and reflections of transmitted pulses, C las and A las response characteristics, FIG. 6 is a block diagram of the configuration of an ultrasonic distance measuring device according to an embodiment of the present invention, 6 is a block diagram showing the first embodiment of the wave number control circuit, which is the main part of the present invention. FIG. 7 is a block diagram showing the first embodiment, and FIG. 9 is a block diagram showing the second embodiment. 5 is a timing chart showing waveforms of various parts in an example. 2-...Transmission circuit, 3...Ultrasonic sensor, 4...Reception circuit, 6--Comparison circuit, 6-One hour measurement circuit, 7
...Time-distance conversion circuit, 1o...-wave number control circuit,
11-・Peak hold circuit, 12・・Gate pulse generation circuit, 13・Level comparator, 14・
・Monostable multivibrator, 16 ・Transmission timing pulse generation circuit, 16...-ant gate. Name of agent: Patent attorney Toshio Nakao and 1 other person
1 Figure 2 Figure 3 (2) Figure 4 Figure 5 Figure 4 5 6 7 Figure 6 Figure 7 Figure 8 Figure 1θ / 5 Figure 9 Back Tz

Claims (1)

【特許請求の範囲】 (1)超音波センサと、前記超音波センナに送信パルス
を印加する送信部と、被測定物からの超音波反射パルス
を受信する受信部と、前記受信部の出力電圧と基準電圧
とを比較する比較部と、送信パルスと受信パルスの間の
時間を測定する時間測定部と、前記時間測定部で測定さ
れた伝播時間を距離に変換する時間−距離変換部と、前
記時間測定部の出力信号によシ前記送信部の送信パルス
の波数を制御する波数制御部とを具備することを特徴と
する超音波距離測定装置。 (お 時間測定部で測定された超音波パルスの伝播時間
が長いほど、送信パルスの波数が多くなるように波数制
御部が制御されることを特徴とする特許請求の範囲第1
項記載の超音波距離測定装置。 およびゲートパルス発生回路からなり、グー1パルス発
生回路のパルス長ざは積分回路に接続されたピークホー
ルド回路の出力によって匍I ml+される如く構成さ
れていることを特徴とする特許請求の範囲第1項または
第2項記載の超音波距離測定装置。 (4)波数制御部が積分回路と、レベルコンパレータト
、前記レベルコンパレータの出力パルスによって発振タ
イミングを制御される単安定マルチバイブレークと、超
音波パルスの繰返し周期ヲ与えるパルスを発生する送信
タイミングパルス発生回路と一前記単安定マルチバイブ
レークの出力と前記送信タイミングパルス発生回路から
のパルスとの論理和をめるアントゲ−1・とからなるこ
とを特徴とする特r1−請求の範囲第1項記載の超音波
距離測定装置。
[Scope of Claims] (1) An ultrasonic sensor, a transmitter that applies a transmission pulse to the ultrasonic sensor, a receiver that receives an ultrasonic reflected pulse from an object to be measured, and an output voltage of the receiver. and a reference voltage; a time measurement unit that measures the time between the transmitted pulse and the received pulse; and a time-distance conversion unit that converts the propagation time measured by the time measurement unit into distance; An ultrasonic distance measuring device comprising: a wave number control section that controls a wave number of a transmission pulse of the transmitting section based on an output signal of the time measuring section. (The first claim is characterized in that the wave number control unit is controlled so that the longer the propagation time of the ultrasonic pulse measured by the time measurement unit, the greater the wave number of the transmitted pulse.
The ultrasonic distance measuring device described in . and a gate pulse generating circuit, and the pulse length of the first pulse generating circuit is configured to be equal to 1 ml+ by the output of the peak hold circuit connected to the integrating circuit. The ultrasonic distance measuring device according to item 1 or 2. (4) The wave number control unit includes an integrating circuit, a level comparator, a monostable multi-vibration whose oscillation timing is controlled by the output pulse of the level comparator, and a transmission timing pulse generator that generates a pulse that gives the repetition period of the ultrasonic pulse. 1. A circuit according to claim 1, comprising: a circuit; and an ant game 1 for calculating the logical sum of the output of the monostable multi-by-break and the pulse from the transmission timing pulse generation circuit. Ultrasonic distance measuring device.
JP25063083A 1983-12-27 1983-12-27 Ultrasonic distance measuring apparatus Pending JPS60140168A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25063083A JPS60140168A (en) 1983-12-27 1983-12-27 Ultrasonic distance measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25063083A JPS60140168A (en) 1983-12-27 1983-12-27 Ultrasonic distance measuring apparatus

Publications (1)

Publication Number Publication Date
JPS60140168A true JPS60140168A (en) 1985-07-25

Family

ID=17210708

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25063083A Pending JPS60140168A (en) 1983-12-27 1983-12-27 Ultrasonic distance measuring apparatus

Country Status (1)

Country Link
JP (1) JPS60140168A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS643582A (en) * 1987-06-26 1989-01-09 Kurita Water Ind Ltd Ultrasonic range finder
JPH01143991A (en) * 1987-11-30 1989-06-06 Tatsuta Electric Wire & Cable Co Ltd Ultrasonic distance measuring instrument
JP2004205232A (en) * 2002-12-24 2004-07-22 Tsutsui Denshi:Kk Ultrasonic wave length measuring apparatus
CN102707287A (en) * 2012-05-28 2012-10-03 四川华立德科技有限公司 Piezoelectric type ultrasonic distance measurement system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS643582A (en) * 1987-06-26 1989-01-09 Kurita Water Ind Ltd Ultrasonic range finder
JPH01143991A (en) * 1987-11-30 1989-06-06 Tatsuta Electric Wire & Cable Co Ltd Ultrasonic distance measuring instrument
JP2004205232A (en) * 2002-12-24 2004-07-22 Tsutsui Denshi:Kk Ultrasonic wave length measuring apparatus
CN102707287A (en) * 2012-05-28 2012-10-03 四川华立德科技有限公司 Piezoelectric type ultrasonic distance measurement system

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