JPS5918472A - Distance measuring apparatus - Google Patents

Distance measuring apparatus

Info

Publication number
JPS5918472A
JPS5918472A JP57128729A JP12872982A JPS5918472A JP S5918472 A JPS5918472 A JP S5918472A JP 57128729 A JP57128729 A JP 57128729A JP 12872982 A JP12872982 A JP 12872982A JP S5918472 A JPS5918472 A JP S5918472A
Authority
JP
Japan
Prior art keywords
range gate
target
range
gate
distance
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
JP57128729A
Other languages
Japanese (ja)
Inventor
Hiroshi Higuchi
博 樋口
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 JP57128729A priority Critical patent/JPS5918472A/en
Publication of JPS5918472A publication Critical patent/JPS5918472A/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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/483Details of pulse systems
    • G01S7/486Receivers
    • G01S7/487Extracting wanted echo signals, e.g. pulse detection
    • G01S7/4873Extracting wanted echo signals, e.g. pulse detection by deriving and controlling a threshold value

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Abstract

PURPOSE:To achieve a higher stability in the short range measurement of distance and a higher capacity of max. distance measurement by always measuring the target at a fixed error alarming probability with a gate arranged in front of a range gate for capturing a target to detect noise such as back scattered light so that the threshold level for detecting the target is set measuring noise frequency. CONSTITUTION:A range gate 29 is set at the position containing a target reflected light as shown by the drawings (a) and (b) and a range gate generator 28 always generates a range gate 30 at the positon earier by the time tp than the range gate 29 as shown by the drawing (c). The time ranges of the range gates 29 and 30 are equal, tw. The range gate 30 moves in linkage with the range gate 29 for capturing targets and thus, the target can be detected at a fixed error alarming probability as always captured with the range gate 29 to measure the distance.

Description

【発明の詳細な説明】 この発明は、常に一定の誤警報確率で目標距離を測距す
ることのできる測距装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a distance measuring device that can always measure a target distance with a constant false alarm probability.

パルスレーザ光を送信して、伝搬遅延時間から目標用R
w測距する場合、大気1等による後方散乱や、他物体に
よる誤測距を少なくするため、従来次のような手段が用
いられていた。
Send a pulsed laser beam and determine the target R from the propagation delay time.
When performing distance measurement, the following methods have conventionally been used to reduce backscattering from the atmosphere and erroneous distance measurements caused by other objects.

第1図は従来のこの種装置の構成例を示す図であって、
(1)はパルスレーザ装置、 (2+はパルスレーザ光
、(3)は受信光学系、(4)は光電変換素子、(5)
は増巾器、(6)はパルス信号、(7)は電圧比較器、
(8)は固定聞直電圧発生回路、(9)は固定閾値電圧
、 (11はストップ信号、(Ioはスタート信号、 
(12はカウンタ。
FIG. 1 is a diagram showing an example of the configuration of a conventional device of this type,
(1) is a pulsed laser device, (2+ is a pulsed laser beam, (3) is a receiving optical system, (4) is a photoelectric conversion element, (5)
is an amplifier, (6) is a pulse signal, (7) is a voltage comparator,
(8) is a fixed direct voltage generation circuit, (9) is a fixed threshold voltage, (11 is a stop signal, (Io is a start signal,
(12 is a counter.

03は距離データである。03 is distance data.

パルスレーザ装置(1)で発生されるパルスレーザ光(
2;は目標にむけて送信され、目標からの反射光が受信
光学系(3)で受光されて、光電変換素子(4)で光電
変換される。光電変換された微弱な信号は増巾器(5)
で増巾されて十分な振巾な有するパルス信号(6)とな
り、電圧比較器(7)の一方の入力に印加される3、電
、圧比較器(7)の他方の入力には、固定電圧発生回路
(8)から固定閾値電圧(9)が印加され、パルス信号
(6)の振巾が固定閾値電圧(9)を越える場合にスト
ップ信号θ〔が電圧比較器(7)から出力される。
Pulsed laser light (
2; is transmitted toward the target, and the reflected light from the target is received by the receiving optical system (3) and photoelectrically converted by the photoelectric conversion element (4). The photoelectrically converted weak signal is sent to an amplifier (5)
The pulse signal (6) with sufficient amplitude is amplified by 3, and is applied to one input of the voltage comparator (7). A fixed threshold voltage (9) is applied from the voltage generation circuit (8), and when the amplitude of the pulse signal (6) exceeds the fixed threshold voltage (9), a stop signal θ is output from the voltage comparator (7). Ru.

ストップ信号01 far、 、パルスレーザ光送信時
にパルスレーザ装置fl)から出力されるスタート信号
α0とどもにカウンタ021に入力され9両者の時間間
隔から目柳距離が求めらJlで、距離データ0粉が出力
されろ。
The stop signal 01 far, is input to the counter 021 along with the start signal α0 output from the pulse laser device fl) when transmitting the pulsed laser beam, and the Meyanagi distance is calculated from the time interval between the two. will be output.

第2図は、後方散乱光および目標反射光によるパルス信
号(6)と固定量(直電圧(9)との関係4・示す図で
、横lIl+は距離、縦軸は振tl〕を示す。固定閾値
電圧(9)は通常の天候状態において、測距範囲内の後
方散乱光によるパルス信号が固定閾値電圧より小とl、
rる。なるべく低い111(に設定されており、この固
定閾値電圧をJjνえる11標反射光が検出されるよう
になっている。
FIG. 2 is a diagram showing the relationship 4 between the pulse signal (6) caused by the backscattered light and the target reflected light and the fixed amount (direct voltage (9), where the horizontal axis II1+ indicates the distance and the vertical axis indicates the amplitude t1). The fixed threshold voltage (9) is such that under normal weather conditions, if the pulse signal due to backscattered light within the ranging range is smaller than the fixed threshold voltage,
ru. The threshold voltage is set to 111 (as low as possible), so that 11-point reflected light that exceeds this fixed threshold voltage by Jjν is detected.

ところが、大気の視界か劣化し、後方散乱光が異常に増
大すると9図中、破線で示1−ように、近(3) 距離において後方散乱光によるパルス信号が固定間wi
電圧(9)ヲ越えるようになり、後方散乱による誤測距
が生じるようになる。あるいは、このような場合におい
ても誤測距がおこりにくいように。
However, when the visibility of the atmosphere deteriorates and the backscattered light increases abnormally, the pulse signal due to the backscattered light at a short (3) distance increases between fixed distances, as shown by the broken line in Figure 9.
The voltage (9) will be exceeded, and erroneous distance measurement will occur due to backscattering. Or to make it less likely that erroneous distance measurements will occur even in such cases.

固定閾値電圧(9)ヲすこし高めに設定しておくと。If you set the fixed threshold voltage (9) a little higher.

遠距離にある目標からのパルス信号が検出できなくなり
、従って最大側距離が低下する結果となる。
Pulse signals from distant targets will no longer be detected, resulting in a reduced maximum range.

このように、従来のこの種装置においては、外界の状態
により、誤測距がおこる確率、すなわち誤警報確率が変
化し、安定した測距が得られない欠点があった。
As described above, conventional devices of this type have the disadvantage that the probability of erroneous distance measurement, that is, the probability of false alarm, changes depending on the state of the outside world, making it impossible to obtain stable distance measurement.

この発明は、この欠点を除去するための手段を提供する
ものであって、以下1図を用いて詳細に説明する。
The present invention provides means for eliminating this drawback, and will be explained in detail below using FIG. 1.

第3図は、この発明による1実施例を示す図で。FIG. 3 is a diagram showing one embodiment according to the present invention.

パルスレーザ光を送信し7反射光を受光、光電変換、お
よび増i〕してパルス信号(6)ヲ得る過程は従来の装
置と同様なので、説明を省略1゛る。第3図において、
 (14+、 aeは電圧比較器、Ql19.αηはゲ
ート回路、0旧まカウンタ、 (liは基準パルス数設
定回路。
The process of transmitting a pulsed laser beam and receiving, photoelectrically converting, and amplifying the reflected light (7) to obtain a pulsed signal (6) is the same as that of the conventional device, so a description thereof will be omitted. In Figure 3,
(14+, ae is a voltage comparator, Ql19.αη is a gate circuit, 0 is a counter, (li is a reference pulse number setting circuit.

(4) (1)は判定回路、 011は加算回路、Q汎まデジタ
ル・アナログ(D/A)変換器、(至)、Q4)は抵抗
器、f!9は切換器、(2!は手動ゲート位置発生器、
@、(ハ)はレンジゲ−1・発生器、翰、(至)はレン
ジゲー)、(31)(62)は参照電圧である。
(4) (1) is a judgment circuit, 011 is an adder circuit, Q general digital/analog (D/A) converter, (to), Q4) is a resistor, f! 9 is a switch, (2! is a manual gate position generator,
@, (c) is the range game 1 generator, 翰, (to) is the range game), (31) and (62) are the reference voltages.

初期において、切換器(ハ)は接点すに接続されており
9手動レンジゲート・位置発生器(至)を手動操作する
ことにより、レンジゲート発生器(財)が出力するレン
ジゲー1−(2)は、第4図(a)および(1)lに示
すように、目標反射光を含む位置に設定される。レンジ
ゲート発生器(ハ)は常に、第4図(C)に示すように
In the initial stage, the switch (c) is connected to the contact point 1, and by manually operating the 9 manual range gate/position generator (to), the range gate generator outputs the range gate 1-(2). is set at a position that includes the target reflected light, as shown in FIGS. 4(a) and (1)l. The range gate generator (c) is always as shown in FIG. 4(c).

レンジゲートChiより時間tpだけ早い位置でレンジ
ゲートclf)Y生成するように構成されており、レン
ジゲーIll、CIの時間幅は等しく towである。
It is configured to generate the range gate clf)Y at a position earlier than the range gate Chi by a time tp, and the time widths of the range gates Ill and CI are equal tow.

初期において、加算回路00の出力には低い値の初期値
が設定されるように、加算回路011は構成されている
At the beginning, the adder circuit 011 is configured such that the output of the adder circuit 00 is set to a low initial value.

この直は、D/A変換器Q3で低い値のアナログ信号に
変換され、抵抗器e(、■で分圧されて電圧比較器Q場
の参照電圧入力に入力され、参照電圧(62)となる。
This direct signal is converted into a low-value analog signal by the D/A converter Q3, divided by the resistor e (, ■, and input to the reference voltage input of the voltage comparator Q field, and the reference voltage (62) Become.

電圧比較器αつの信号入力にはパルス信号(6)が入力
され、初期においては参照電圧(32)は、低い値であ
るので、この唾ヲ越えるパルス信号は数多くある。電圧
比較器09は、参照電圧(32)を越えるパルス信号(
6) ’k 、パルス整形して出力し。
A pulse signal (6) is input to the signal input of the voltage comparator α, and since the reference voltage (32) is initially at a low value, there are many pulse signals that exceed this value. Voltage comparator 09 detects a pulse signal (
6) 'k, pulse shaped and output.

これはゲート回路α力に入力されるので、参照電圧(3
2)を越える。レンジゲート(至)内の後方散乱9等に
よるパルス数が、カウンタttnでカウントされること
になる。カウンタα樽の出力であるパルスカウント数m
は4判定回路翰の一方の入力に入力され。
This is input to the gate circuit α power, so the reference voltage (3
Exceed 2). The number of pulses due to backscatter 9 etc. within the range gate (to) is counted by the counter ttn. Pulse count number m which is the output of counter α barrel
is input to one input of the 4 judgment circuit.

他方の入力には、基準パルス数設定回路α→の出力であ
る基準パルス数Mが入力されて9次の判定アルゴリズム
に従い、KY自然数として鎮りが判定回路(至)から出
力される。
The reference pulse number M, which is the output of the reference pulse number setting circuit α→, is input to the other input, and according to the 9th-order determination algorithm, the determination circuit (to) outputs calmness as a KY natural number.

この[Dは、加算回路Qυで前回の値に加算される結果
、後方散乱9等によるパルスカウント数mが基準量Mよ
り多ければ9次の参照電圧(32)は高くなり、少なけ
れば9次の参照電圧(62)は低くなるので、常に一定
の確率でレンジゲート(至)内の後方散乱、#によるパ
ルス信号が検出されることになる。
This [D is added to the previous value in the adder circuit Qυ. As a result, if the number m of pulse counts due to backscatter 9, etc. is greater than the reference amount M, the 9th reference voltage (32) becomes higher; if it is less, the 9th reference voltage (32) becomes higher. Since the reference voltage (62) becomes low, a pulse signal due to backscatter # within the range gate (to) will always be detected with a constant probability.

一方、ストップパルスχ検出するための電圧比較器a4
の参照電圧入力には、D/A変換器嬶の直接の出力(6
1)が参照電圧として入力され、これは前述の参照電圧
(32)より大であるので、抵抗器(ハ)。
On the other hand, voltage comparator a4 for detecting stop pulse χ
The reference voltage input is the direct output of the D/A converter (6
1) is input as the reference voltage, which is greater than the reference voltage (32) mentioned above, so resistor (c).

Q4の抵抗比、および基準パルス数M”l適切に設定す
ること罠より、常にレンジゲート端内においては、目標
反射光によるパルス信号のみが検出され。
By appropriately setting the resistance ratio of Q4 and the reference pulse number M''l, only the pulse signal due to the target reflected light is always detected within the range gate end.

同レンジゲート内の後方散乱光1等による誤警報確率を
許容できる一定σ刈+Hに保つことができる。
The false alarm probability due to backscattered light 1, etc. within the same range gate can be maintained at an acceptable constant σ+H.

なお、レンジゲート(至)が目標を捕捉し、距離データ
α謙が連続して得られるようになれば、切替器(ハ)は
接点aK接続され、毎回の距離データを用いてレンジゲ
−IJ1.<31が、自動的に設定されるので、目標は
常にレンジゲート(ハ)で捕捉された状態で、かつ前述
のように一定の誤警報確率で検出。
Note that when the range gate (to) captures the target and the distance data α range can be obtained continuously, the switch (c) is connected to the contact aK, and the range gate IJ1. <31 is automatically set, so the target is always captured by the range gate (c) and detected with a constant false alarm probability as described above.

測距されることになる。The distance will be measured.

(T) なお、上述の説明においては、レンジゲート(至)は目
標Y捕捉するレンジゲート翰と連動して動くようになっ
ているが、装置の構成を簡略にするため、レンジゲート
(至)を近距離の一定の位置に固定的に設定する構成ヶ
用いることもできる。
(T) In the above explanation, the range gate (to) is designed to move in conjunction with the range gate to capture the target Y, but in order to simplify the configuration of the device, the range gate (to) It is also possible to use a configuration in which the target is fixedly set at a fixed position at a short distance.

このように、この発明によれば、目標を捕捉するレンジ
ゲートの前に、後方散乱光1等による雑音を検出するゲ
ートヲ設け、このゲート内での雑音頻度を計測しながら
、目標検出のための閾値レベルヶ設定するので、常に一
定の誤警報確率で目標を測距することができ、近距離に
おける測距の安定性と、最大側距離の向上に著しく寄与
するこ第1図は従来の測距装置の構成の1例を示す図。
As described above, according to the present invention, a gate for detecting noise caused by backscattered light 1, etc. is provided before the range gate for capturing a target, and while measuring the frequency of noise within this gate, the range gate for target detection is Since the threshold level is set, it is possible to always measure the target with a constant false alarm probability, which significantly contributes to the stability of distance measurement at short distances and the improvement of the maximum distance.Figure 1 shows the conventional distance measurement method. The figure which shows one example of the structure of a device.

第2図はパルス信号を固定開鎖電圧との関係を示す図、
第3図はこの発明による装置の1実施例を示す図、第4
図はこの発明による目標とレンジゲートの関係ヲ示す図
であって、(1)はパルスレーザ装置、(2;はパルス
レーザ光、(3)は受信光学系、(4)(8) は光電変換素子、(6)はパルス信号、 (1(Iはス
タート信号、0υはストップ信号、a旧まカウンタ、α
漕は距離データ、α→、 01は電圧比較器、 as、
 (lηはゲート回路、08はカウンタ、 Qlは基準
パルス数設定回路。
Figure 2 is a diagram showing the relationship between the pulse signal and the fixed open chain voltage.
FIG. 3 is a diagram showing one embodiment of the device according to the present invention, and FIG.
The figure shows the relationship between the target and the range gate according to the present invention, in which (1) is a pulse laser device, (2) is a pulse laser beam, (3) is a receiving optical system, and (4) and (8) are photoelectronic devices. Conversion element, (6) is a pulse signal, (1 (I is a start signal, 0υ is a stop signal, a old counter, α
row is distance data, α→, 01 is voltage comparator, as,
(lη is a gate circuit, 08 is a counter, and Ql is a reference pulse number setting circuit.

(1)は判定回路、0υは加算回路、@、(ハ)はレン
ジゲート発生器、翰、(至)はレンジゲートI  (3
1)、(32)は参照電圧である。
(1) is the judgment circuit, 0υ is the adder circuit, @, (c) is the range gate generator, 翰, (to) is the range gate I (3
1) and (32) are reference voltages.

なお9図中、同一あるいは相当部分には同一符号を付し
て示しである。
In FIG. 9, the same or corresponding parts are designated by the same reference numerals.

代理人  葛 野 信 − 第1図Agent Nobu Kuzuno - Figure 1

Claims (1)

【特許請求の範囲】[Claims] ハルスレーザ光ヲ送信して、パルスレーザ光の伝搬遅延
時間から目標までの距離を求める測距装置において1反
射光を光電変換してパルス信号を生成する手段と、目標
距離に相当する時間位置に第1のレンジゲートヲ設定す
る手段と、第1のレンジゲートより早い時間位置に第2
のレンジゲートヲ設定する手段と、第1のレンジゲート
内において第1の閾値電圧を越えるパルス信号を検出す
る手段と、第2のレンジゲート内において第2の閾fl
fY越えるパルス信号を検出し、このパルス数をカウン
トする手段と、前記パルス数が定められたパルス数より
多い場合に出力電圧を増し、少ない場合に出力電圧を減
する電圧発生手段と、前記電圧発生手段の出力電圧を第
1の閾値電圧として設定する手段と、第1の閾値電圧を
分圧して第2の閾値@1圧として設定する手段とを備え
たことを特徴とする測距装置。
In a distance measuring device that transmits a Hals laser beam and determines the distance to the target from the propagation delay time of the pulsed laser beam, there is a means for photoelectrically converting one reflected beam to generate a pulse signal, and a means for generating a pulse signal at a time position corresponding to the target distance. means for setting a first range gate; and means for setting a second range gate at an earlier time position than the first range gate.
means for detecting a pulse signal exceeding a first threshold voltage within the first range gate; and means for detecting a pulse signal exceeding a first threshold voltage within the first range gate;
means for detecting a pulse signal exceeding fY and counting the number of pulses; voltage generating means for increasing an output voltage when the number of pulses exceeds a predetermined number of pulses; and decreasing the output voltage when the number of pulses is less than a predetermined number; A distance measuring device comprising: means for setting the output voltage of the generating means as a first threshold voltage; and means for dividing the first threshold voltage and setting it as a second threshold @1 voltage.
JP57128729A 1982-07-23 1982-07-23 Distance measuring apparatus Pending JPS5918472A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57128729A JPS5918472A (en) 1982-07-23 1982-07-23 Distance measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57128729A JPS5918472A (en) 1982-07-23 1982-07-23 Distance measuring apparatus

Publications (1)

Publication Number Publication Date
JPS5918472A true JPS5918472A (en) 1984-01-30

Family

ID=14992000

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57128729A Pending JPS5918472A (en) 1982-07-23 1982-07-23 Distance measuring apparatus

Country Status (1)

Country Link
JP (1) JPS5918472A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
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WO2002088772A1 (en) * 2001-04-25 2002-11-07 Nikon Corporation Range finder, range finding method, and photoelectric tranducing circuit
JP2002328167A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328166A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328169A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328168A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2008180593A (en) * 2007-01-24 2008-08-07 Matsushita Electric Works Ltd Distance change observation device
JP2011505545A (en) * 2007-09-27 2011-02-24 オムロン サイエンティフィック テクノロジーズ, インコーポレイテッド Clutter removal in an active object detection system.

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002088772A1 (en) * 2001-04-25 2002-11-07 Nikon Corporation Range finder, range finding method, and photoelectric tranducing circuit
JP2002328167A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328166A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328169A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2002328168A (en) * 2001-05-01 2002-11-15 Nikon Corp Ranging device and method
JP2008180593A (en) * 2007-01-24 2008-08-07 Matsushita Electric Works Ltd Distance change observation device
JP2011505545A (en) * 2007-09-27 2011-02-24 オムロン サイエンティフィック テクノロジーズ, インコーポレイテッド Clutter removal in an active object detection system.

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