JPS6383686A - Laser distance measuring instrument - Google Patents

Laser distance measuring instrument

Info

Publication number
JPS6383686A
JPS6383686A JP23031086A JP23031086A JPS6383686A JP S6383686 A JPS6383686 A JP S6383686A JP 23031086 A JP23031086 A JP 23031086A JP 23031086 A JP23031086 A JP 23031086A JP S6383686 A JPS6383686 A JP S6383686A
Authority
JP
Japan
Prior art keywords
frequency
laser
measured
light
reflected
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
JP23031086A
Other languages
Japanese (ja)
Inventor
Hidemi Takahashi
秀実 高橋
Minoru Kimura
実 木村
Hiroyuki Naito
宏之 内藤
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 JP23031086A priority Critical patent/JPS6383686A/en
Publication of JPS6383686A publication Critical patent/JPS6383686A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the accuracy of distance measurement, by obtaining a laser beam frequency-modulated by an electro-optical light modulator, radiating a part of it on an object to be measured after taking it out as a reference beam, and detecting a frequency difference between a reflected beam of light and the reference beam. CONSTITUTION:The electro-optical light modulator 11 is arranged in the resonator of a laser 1, and when a modulating power source 4 is changed, the length of the resonator is changed based on the change of reflectance due to an electro-optical effect, therefore, the frequency of an oscillating light of the laser 1 is modulated. A part of a frequency-modulated laser beam which being taken out by a beam splitter 5 as the reference beam, then being induced to a detector 9, is projected on the object 7 to be measured. The reflected light from the object 7 to be measured is reflected on a partial reflecting mirror 6, and induced to the detector 9. The detected signals of the reflected rays of light and the reference beam detected by the detector 9 are sent to a frequency analyzer 10, and the frequency of a beat signal is measured, and distance to the object 7 to be measured is calculated. In such a manner it is possible to increase the modulation quantity of a frequency and the number of repeat of modulation, and to perform a linear frequency modulation for an impressed voltage, thereby, it is possible to heighten the accuracy of the distance measurement.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は、レーザー光を用いて対象物までの距離を測
定するレーザー測距装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a laser distance measuring device that measures the distance to an object using laser light.

従来の技術 対象物までの給体距離をレーザーを用いて測定すること
はロボットの遠隔操作のための視覚情報源として最近注
目されている。このようなレーザー測距装置のなかにF
M  CWレーザーレーダと呼ばれる方式がある。この
方式に関しては例えばアイイーイーイー・ジャーナル・
オブ・クウオ/タム・エレクトロニクスQE−8巻 9
1〜92頁1972年(IEEE  JQuantum
EIectronics、 vol。
BACKGROUND ART Measuring the feed distance to an object using a laser has recently attracted attention as a visual information source for remote control of robots. Among such laser distance measuring devices, F
There is a method called MCW laser radar. Regarding this method, for example, IEE Journal
Ob Kuo/Tam Electronics QE-8 Volume 9
1-92, 1972 (IEEE JQuantum
EI electronics, vol.

QE−8,PP91〜92. 1972)に記載されて
いる。以下、第3図を参照して、従来のFM−CWレー
ザーレーダについて説明する。
QE-8, PP91-92. 1972). Hereinafter, a conventional FM-CW laser radar will be explained with reference to FIG.

第3図においてレーザー1の共振器を構成する全反射鏡
2をピエゾ素子3によって保持する。ピエゾ素子3にか
かる電圧を変調用電源4によって変化させると、共振器
長の変化のためにレーザー光の発振周波数は変調される
。この様子を第4図に示す。変調用電源4に三角波電圧
を印加すると、第4図(a)に示したようにレーザー光
の発振周波数はflからf2に直線的に変化する0図中
実線は送信波、破線は反射波を示し、送信後反射波を受
信するまでの時間△tは△t=共で表わされる。こC のように変調されたレーザー光を第3図に示したようと
対象物7に照射する。対象物からの散乱光を部分反射鏡
6によって受光し、検出器9に導く。
In FIG. 3, a total reflection mirror 2 constituting a resonator of a laser 1 is held by a piezo element 3. When the voltage applied to the piezo element 3 is changed by the modulation power source 4, the oscillation frequency of the laser beam is modulated due to the change in the resonator length. This situation is shown in FIG. When a triangular wave voltage is applied to the modulation power source 4, the oscillation frequency of the laser beam changes linearly from fl to f2 as shown in Figure 4(a). In the figure, the solid line represents the transmitted wave, and the broken line represents the reflected wave. The time Δt from transmission until receiving the reflected wave is expressed as Δt=. A laser beam modulated as shown in FIG. 3 is irradiated onto the object 7 as shown in FIG. Scattered light from the object is received by a partial reflecting mirror 6 and guided to a detector 9.

他方、レーザー光の一部を参照光としてビームスプリッ
タ−5によって取り出し、検出器9に導く。
On the other hand, a part of the laser beam is extracted as a reference beam by a beam splitter 5 and guided to a detector 9.

レンズ8はレーザー光の集光のために用いている。Lens 8 is used to condense laser light.

検出されたビート信号の周波数は第4図(b)のように
なシ、その周波数は対象物までの距離に比例する0すな
わち、周波数変調量△f=f2−f、、変調のくシ返し
周波数を畑、ビート信号の周波数をfb対象物までの距
離をLとすると という関係が成り立つ。ここでCは光の速度である。従
って、周波数分析器1oによってビート信号の周波数を
測定すれば対象物までの距離が求まるわけである・。
The frequency of the detected beat signal is as shown in Fig. 4(b), and the frequency is 0, which is proportional to the distance to the target object. The relationship holds that the frequency is field, the frequency of the beat signal is fb, and the distance to the object is L. Here C is the speed of light. Therefore, by measuring the frequency of the beat signal using the frequency analyzer 1o, the distance to the object can be determined.

発明が解決しようとする問題点 以上のような構成において全反射鏡2により共振器長を
変化させ、レーザー光の周波数を変調させる方式ではピ
エゾ素子の時間応答性の点から高速なくシ返しが不可能
であり、変調のくり返し周波数fmはI KH2以下と
なり、測距精度は制限を受ける。また、ピエゾ素子が印
加電圧に対して直線的に変化しないといった問題も測距
精度を低下させている。本発明は以上のような問題点を
解決するものであシ、精度のよいレーザー測距装置を提
供するものである。
Problems to be Solved by the Invention In the above-mentioned configuration, the method of changing the resonator length using the total reflection mirror 2 and modulating the frequency of the laser beam is not fast and does not cause reciprocation due to the time response of the piezo element. It is possible, but the repetition frequency fm of modulation will be less than IKH2, and the distance measurement accuracy will be limited. Further, the problem that the piezo element does not change linearly with the applied voltage also reduces distance measurement accuracy. The present invention solves the above-mentioned problems and provides a highly accurate laser distance measuring device.

問題点を解決するための手段 本発明はレーザ共振器の内部に電気光学光変調器を設置
して周波数変調されたレーザー光を取り出し、レーザー
光の一部を参照光としてとり出すとともに被測定物に照
射し、反射光と参照光との周波数差を検出するようにし
だものである。
Means for Solving the Problems The present invention installs an electro-optic optical modulator inside a laser resonator to take out a frequency-modulated laser beam, and takes out a part of the laser beam as a reference beam. The device irradiates the reflected light and detects the frequency difference between the reflected light and the reference light.

作用 本発明は上記構成によシミ気光学光変調器によって周波
数変調を行なうため、周波数変調量、変調くシ返し数を
大きくとることができるとともに、印加電圧に対して直
線的な周波数変調が行なえるために、精度よい測距を行
なうことができる〇実施例 以下、本発明の一実施例を第1図にもとづいて説明する
。第3図と同じ部位には同一番号を付しである。
Function: Since the present invention performs frequency modulation using the optical light modulator having the above-mentioned configuration, the amount of frequency modulation and the number of modulation cycles can be increased, and the frequency modulation can be performed linearly with respect to the applied voltage. Embodiment Hereinafter, one embodiment of the present invention will be described based on FIG. 1. The same parts as in FIG. 3 are given the same numbers.

レーザー1の共振器内部に電気光学光変調器11を設置
し、変調用電源4の電圧を変化させると電気光学効果に
よる屈折率変化から共振器長が変化するため、レーザー
1の発振光の周波数は変調される。電気光学光変調器1
1に対して変調用電源4により三角波電圧を印加すれば
、第4図に示したのと同様の周波数変調が行なえ、以下
、対象物7に周波数変調されたレーザー光を照射し、反
射光とのビート信号を測定し、対象物7までの距離を求
める構成は第4図の従来例と同様である。CO2レーザ
ーの場合には、繰シ返し周波数fmが500MH2、周
波数変調量△fがI MHz/ 100 V程度と1m
1△fが大きい値が得られる。距離分解能△Lは、周波
数測定精度をΔfbとすると(1)式からCΔfb ΔL = −(2) 4△ffm となるので、△Lfmは大きいほど距離測定精度はよい
値となる。また、本構成によれば印加電圧に対して直線
的な周波数変調が行なえ、距離測定精度は向上する。以
上のように本発明によれば精度のよに距離測定を行なう
ことができる。
When an electro-optic optical modulator 11 is installed inside the resonator of the laser 1 and the voltage of the modulation power source 4 is changed, the resonator length changes due to the change in refractive index due to the electro-optic effect, so the frequency of the oscillated light of the laser 1 changes. is modulated. Electro-optic light modulator 1
If a triangular wave voltage is applied to 1 by the modulation power source 4, frequency modulation similar to that shown in FIG. 4 can be performed. The configuration for measuring the beat signal of and determining the distance to the object 7 is the same as the conventional example shown in FIG. In the case of a CO2 laser, the repetition frequency fm is 500 MH2, and the frequency modulation amount △f is about I MHz/100 V, which is 1 m.
A large value of 1Δf is obtained. The distance resolution ΔL is CΔfb ΔL = −(2) 4Δffm from equation (1), where Δfb is the frequency measurement accuracy. Therefore, the larger ΔLfm is, the better the distance measurement accuracy is. Further, according to this configuration, linear frequency modulation can be performed on the applied voltage, and distance measurement accuracy is improved. As described above, according to the present invention, distance measurement can be performed with high accuracy.

第2図には本発明の別の実施例を示す。本実施例が第1
図と異なるのは、スキャナー12によって周波数変調さ
れたレーザー光の走査を行ない、同じスキャナー12を
通して対象物7の反射光を検出している点である。本構
成によれば距離画像として三次元情報を得ることができ
る。このような距離画像はロボットの三次元視覚などに
有効である。
FIG. 2 shows another embodiment of the invention. This example is the first
The difference from the figure is that a scanner 12 scans with frequency-modulated laser light, and the reflected light from the object 7 is detected through the same scanner 12. According to this configuration, three-dimensional information can be obtained as a distance image. Such distance images are effective for three-dimensional vision of robots.

発明の効果 以上述べたように本発明はレーザー共振器の内部に設置
した電気光学光変調器によって周波数変調されたレーザ
ー光を得、対照物に照射し、反射光の周波数を検出する
ことによって距離を測定する精度よいレーザー測距装置
を提供するものである。
Effects of the Invention As described above, the present invention obtains frequency-modulated laser light using an electro-optic light modulator installed inside a laser resonator, irradiates it onto a target object, and detects the frequency of the reflected light to determine the distance. The purpose of the present invention is to provide a laser distance measuring device with high accuracy for measuring.

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

第1図は本発明の一実施例におけるレーザー測距装置の
概略図、第2図は本発明の他の実施例のレーザー測距装
置の概略図、第3図は従来のレーザー測距装置の概略図
、第4図は周波数変調方式レーザー測距装置の原理図で
ある。 1・・・レーザー、2・・・全反射鏡、3・・・ビエソ
、4・・・変調用電源、5・・・ビームスプリンター、
6・・・部分反射鏡、7・・・対象物、8・・・レンズ
、9・・・検出器、10・・・周波数分析器、11・・
・電気光学光変調器、12・・・スキャナー。 代理人の氏名 弁理士 中 尾 敏 男  ほか1名輪 算 〆 妃 セ1 巨         紀 −智
FIG. 1 is a schematic diagram of a laser distance measuring device according to an embodiment of the present invention, FIG. 2 is a schematic diagram of a laser ranging device according to another embodiment of the present invention, and FIG. 3 is a schematic diagram of a conventional laser ranging device. The schematic diagram, FIG. 4, is a principle diagram of a frequency modulation type laser distance measuring device. 1... Laser, 2... Total reflection mirror, 3... Vieso, 4... Modulation power supply, 5... Beam splinter,
6... Partially reflecting mirror, 7... Target, 8... Lens, 9... Detector, 10... Frequency analyzer, 11...
- Electro-optic light modulator, 12...scanner. Name of agent: Patent attorney Toshio Nakao and one other person

Claims (2)

【特許請求の範囲】[Claims] (1)レーザー発振器の内部に電気光学光変調器を設け
たレーザー光源と、前記レーザー光源からのレーザー光
の一部を参照光として取り出すとともに、被測定物に照
射する手段と、前記参照光と被測定物からの反射光との
周波数差を検出する手段とを具備したことを特徴とする
レーザー測距装置。
(1) A laser light source including an electro-optic light modulator provided inside a laser oscillator, a means for extracting a part of the laser light from the laser light source as a reference light and irradiating it onto an object to be measured, 1. A laser distance measuring device comprising means for detecting a frequency difference between light reflected from an object to be measured.
(2)レーザー光を被測定物に照射する手段がスキャナ
を備えている特許請求の範囲第1項記載のレーザー測距
装置。
(2) The laser distance measuring device according to claim 1, wherein the means for irradiating the object to be measured with laser light includes a scanner.
JP23031086A 1986-09-29 1986-09-29 Laser distance measuring instrument Pending JPS6383686A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23031086A JPS6383686A (en) 1986-09-29 1986-09-29 Laser distance measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23031086A JPS6383686A (en) 1986-09-29 1986-09-29 Laser distance measuring instrument

Publications (1)

Publication Number Publication Date
JPS6383686A true JPS6383686A (en) 1988-04-14

Family

ID=16905828

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23031086A Pending JPS6383686A (en) 1986-09-29 1986-09-29 Laser distance measuring instrument

Country Status (1)

Country Link
JP (1) JPS6383686A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03135782A (en) * 1989-10-20 1991-06-10 Tokyo Koku Keiki Kk Triangular wave modulated semiconductor laser device with linearlized frequency variation of output light
JP2008157827A (en) * 2006-12-25 2008-07-10 Seiko Epson Corp Dial plate for timepiece, and the timepiece
JP2014522979A (en) * 2011-07-15 2014-09-08 ソフトキネティック センサー エヌブイ Method for providing distance information and time of flight camera

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03135782A (en) * 1989-10-20 1991-06-10 Tokyo Koku Keiki Kk Triangular wave modulated semiconductor laser device with linearlized frequency variation of output light
JP2008157827A (en) * 2006-12-25 2008-07-10 Seiko Epson Corp Dial plate for timepiece, and the timepiece
JP2014522979A (en) * 2011-07-15 2014-09-08 ソフトキネティック センサー エヌブイ Method for providing distance information and time of flight camera

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