JPS5855812A - Laser distance measuring device - Google Patents
Laser distance measuring deviceInfo
- Publication number
- JPS5855812A JPS5855812A JP15512181A JP15512181A JPS5855812A JP S5855812 A JPS5855812 A JP S5855812A JP 15512181 A JP15512181 A JP 15512181A JP 15512181 A JP15512181 A JP 15512181A JP S5855812 A JPS5855812 A JP S5855812A
- Authority
- JP
- Japan
- Prior art keywords
- laser
- light
- beam splitting
- polarization
- splitting polarizer
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
- G01S7/499—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00 using polarisation effects
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Measurement Of Optical Distance (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、ジャイアントパルス発振をするQスイッチ
レーザ装置管送信部として有するレーザ測距装置に関す
る0
従来のレーザ測距装置の系統図の一例を第1図に示す。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a laser range finder having a Q-switched laser device tube transmitter that emits giant pulse oscillations. An example of a system diagram of a conventional laser range finder is shown in FIG.
このレーザ測距装置において、qスイッチレーザ装置1
から出力されたレーザ光は、コリメータ2を通してビー
ムひろがりt小さくされて目標へ照射される0このとき
、目標の照準はあらかじめパララックス調整され友しン
ズBa=Set有する照準眼鏡Jt−用いて行われる。In this laser distance measuring device, a q-switch laser device 1
The laser beam output from the collimator 2 spreads the beam to a smaller size and irradiates it to the target. At this time, aiming at the target is performed using sighting glasses Jt- which have been parallax adjusted in advance and have friends Ba=Set. .
目標からの反射光は、受信光学系3で受信される。The reflected light from the target is received by the receiving optical system 3.
レーザパルス出力時に、Qスイッチレーザ装置1から出
力されるパルス(パルス1)と反射光受信時Kjt、検
出1ijbから出力されるパルス(パルス2)が測距信
号処理および表示回路4に入力される0測距信号処理お
よび表示回路4は、Qスイッチレーザ装置1から出力さ
れるノくルスの時間おくれを計測して、目標までの距離
會計算し、これを表示する0以上が第1図に示すレーザ
測距装置の動作である0
一般に、レーザ測距装置で、レーザ出力を変えずに測距
距離を長くするためには、受光径(すなわち、受信光学
系30対物レンズja)を大きくする必要がある。ま几
同時に目標にできるだけ多くのレーザ光が集中するよう
に、コリメータ2のコリメート比を大きく、すなわち、
対物レンズJai大きくする必要がある。その結果、第
1図に示すような構成のレーザ測距装置は大きく重くな
ってしまう欠点があった。When outputting a laser pulse, the pulse (pulse 1) output from the Q-switch laser device 1 and the pulse (pulse 2) output from the detection 1ijb when receiving reflected light are input to the ranging signal processing and display circuit 4. The 0 distance measurement signal processing and display circuit 4 measures the time delay of the Norms output from the Q-switched laser device 1, calculates the distance to the target, and displays the distance from 0 to the target as shown in FIG. 0 Generally, in a laser range finder, in order to increase the distance measured without changing the laser output, the light receiving diameter (i.e., the receiving optical system 30 objective lens ja) must be increased. There is a need. In order to simultaneously concentrate as much laser light as possible on the target, the collimation ratio of collimator 2 is increased, that is,
It is necessary to increase the objective lens Jai. As a result, the laser distance measuring device having the configuration shown in FIG. 1 has the drawback of being large and heavy.
この発明は、上記従来の欠点を除去するためになされた
もので、測距目標からの反射光を光検出器に導入するた
めにレーザコリメータとして使用される光学系と、偏光
変換手段と、ビーム分割偏光器とを共用することにエリ
、小形でかつ軽量にできるレーザ測距装置を提供するこ
と金目的とする。This invention was made to eliminate the above-mentioned conventional drawbacks, and includes an optical system used as a laser collimator to introduce reflected light from a distance measurement target into a photodetector, a polarization conversion means, and a beam beam. It is an object of the present invention to provide a laser distance measuring device that can be made compact and lightweight since it can be used in common with a split polarizer.
以下、この発明のレーザ測距装置の実施例について図面
に基づき説明する0第2図はその一実施例の構成を示す
図である0この第2図において、11はルーフプリズム
であり、このルーフプリズム11、直角プリズム12、
ビーム分割偏光器13、プリズム14とによる光共振器
内にレーザ媒質15、ポッケルスセル15が配置されて
、レーザ光パルス発振装置としてOQスイッチレーザ装
置が構成されている。Hereinafter, an embodiment of the laser distance measuring device of the present invention will be explained based on the drawings.0 Fig. 2 is a diagram showing the configuration of one embodiment.0 In this Fig. 2, numeral 11 is a roof prism; Prism 11, right angle prism 12,
A laser medium 15 and a Pockels cell 15 are arranged in an optical resonator formed by a beam splitting polarizer 13 and a prism 14, and an OQ switch laser device is configured as a laser light pulse oscillation device.
ここでプリズム14はルーフプリズム1ノおよびこのル
ーフプリズム11の稜線に直交する光路折り曲げ平面を
有する直角プリズムを一体に組み合わせ次形状管有する
とともに入射光と反射光との偏光面が一致するように選
択され次屈折率を有するプリズムである。このプリズム
14は幾何光学的には、ルーフプリズム11と同様の性
能を有し、偏光的には平行平面鏡と同じ性質1有してい
る。Here, the prism 14 is selected so that the roof prism 1 and the rectangular prism having an optical path bending plane perpendicular to the ridgeline of the roof prism 11 are combined together to have a tube with the following shape, and the planes of polarization of the incident light and the reflected light are the same. It is a prism with a refractive index of This prism 14 has the same performance as the roof prism 11 in terms of geometrical optics, and has the same properties 1 as a parallel plane mirror in terms of polarization.
プリズム14、ポッケルスセル16、ビーム分割偏光器
13、集光レンズ11、光検出器18は同一軸上に配置
されているOlた、1#は照準用光学系であり、その前
方にはグイクロイックミラー20.対物レンズ22が同
一軸上に配置されている。The prism 14, Pockels cell 16, beam splitting polarizer 13, condensing lens 11, and photodetector 18 are arranged on the same axis. Loic Miller 20. Objective lenses 22 are arranged on the same axis.
マタ、直角プリズム21に対向して直角プリズム23が
配置されており、この直角プリズム23と凹レンズ24
お1びグイクロイックミラー20は同一軸上に配設され
ている。A right-angle prism 23 is arranged opposite to the right-angle prism 21, and this right-angle prism 23 and a concave lens 24
The mirror 1 and the microchroic mirror 20 are arranged on the same axis.
Qスイッチレーザ装置からのレーザ出力光は偏光変換手
段としての直角プリズム21および直角プリズム23に
より、直線偏光から円偏光に変換される。この円偏光化
は直角プリズム21.23の全反射における位相ずれ全
利用して行われる。このため、ビーム分割偏光器13の
偏光面と、直角プリズム21、直角プリズム23の光路
折り曲げ平面は、45°の角度で交わる↓うに配置され
ており、直角プリズム23お工び直角プリズム21の全
反射面へのレーザ光の入射角は45°になる工うに配置
されているO
1友、直角プリズム23お工び直角プリズム2ノは、屈
折率が1゜554±0.010の範囲の値を持つ材質で
造られている。このように偏光変換手段は2つの直角プ
リズム21.21で構成できるが、2つの直角プリズム
が一体化されたプリズム食用いても工い。Laser output light from the Q-switched laser device is converted from linearly polarized light to circularly polarized light by a right angle prism 21 and a right angle prism 23 as polarization conversion means. This circular polarization is performed by making full use of the phase shift in the total reflection of the right angle prisms 21 and 23. Therefore, the polarization plane of the beam splitting polarizer 13 and the optical path bending planes of the right-angle prism 21 and the right-angle prism 23 are arranged so that they intersect at an angle of 45 degrees. The angle of incidence of the laser beam on the reflective surface is 45°.The right-angle prism 23 and the right-angle prism 2, which are arranged in such a way, have a refractive index in the range of 1°554±0.010. It is made of material that has. In this way, the polarization conversion means can be constituted by two right-angle prisms 21, 21, but it can also be constructed by using a prism plate in which two right-angle prisms are integrated.
なお、第2図には示されていないが、光検出器18の出
力は第1図の場合と同様にして、測距信号処理および表
示回路に送られ、そこで目標までの距離を計測して表示
するようになっている。Although not shown in FIG. 2, the output of the photodetector 18 is sent to the ranging signal processing and display circuit in the same manner as in FIG. 1, where the distance to the target is measured. It is designed to be displayed.
次に以上のように構成されたこの発明のレーザ測距装置
の動作について説明する。レーザ光はほとんど完全な円
偏光として、対物レンズ22から出力される。そして物
体(図示せず)に照射されたレーザ光は、通常の場合、
偏光面はほとんど変化せずに反射される。すなわち、偏
光に関しては平行平面鏡に近い性質を有していると考え
てよい。このレーザ光の反射光はレーザコリメータとし
ての対物レンズ22、グイクロイックミラー201凹レ
ンズ24、直角プリズム21.直角プリズム21、ビー
ム分割偏光器is、集光レンズ12t−経て、光検出器
1#に導入される0
ビーム分割偏光器13から直角プリズム21ヘ出力され
たレーザ光は反射光として再びビーム分割偏光器13に
入力されるまでに4回全反射を受けるので再び直線偏光
になるがその偏光面はビーム分割偏光器11の偏光面と
直角になるので、すべて集光レンズ1rへ反射される。Next, the operation of the laser distance measuring device of the present invention configured as described above will be explained. The laser beam is output from the objective lens 22 as almost completely circularly polarized light. In normal cases, the laser beam irradiated onto an object (not shown) is
The plane of polarization is reflected almost unchanged. In other words, it can be considered to have properties similar to a parallel plane mirror in terms of polarization. The reflected light of this laser beam is transmitted through an objective lens 22 as a laser collimator, a guichroic mirror 201, a concave lens 24, a right-angle prism 21. The laser beam outputted from the beam splitting polarizer 13 to the right angle prism 21 is beam split and polarized again as reflected light. Since the light undergoes total reflection four times before being input to the device 13, it becomes linearly polarized light again, but since its plane of polarization is perpendicular to the plane of polarization of the beam splitting polarizer 11, it is all reflected to the condenser lens 1r.
すなわち、偏光的なpスはほとんど受けずに光検出器1
Bへ反射光を導入することができる。In other words, the photodetector 1 receives almost no polarized ps.
Reflected light can be introduced into B.
なお、対物レンズ22、照準用光学系11は照準眼鏡を
構成している。そしてレーザコリメータの対物レンズ2
2は測距目標照準のための照準眼鏡あるいはTVカメラ
の対物レンズとして利用することもできる。Note that the objective lens 22 and the aiming optical system 11 constitute aiming glasses. And the objective lens 2 of the laser collimator
2 can also be used as sighting glasses for aiming at a distance measuring target or as an objective lens for a TV camera.
以上述べ友ようにこの発明のレーザ測距装置にLれば、
レーザコリメータおLび偏光変換手段、ビーム分割偏光
器とを目標からの反射光を光検出器へ導入する受信用光
学系として共用する1うにしたので、小形でかつ軽量と
することができる。As mentioned above, if the laser distance measuring device of this invention is used,
Since the laser collimator L, the polarization conversion means, and the beam splitting polarizer are used together as a receiving optical system that introduces the reflected light from the target to the photodetector, it can be made small and lightweight.
第1図は従来のレーザ測距装置の構成図、第21PQは
この発明のレーザ測距装置の一実施例の構成を示す図で
−ある0FIG. 1 is a configuration diagram of a conventional laser distance measurement device, and 21PQ is a diagram showing the configuration of an embodiment of the laser distance measurement device of the present invention.
Claims (1)
るレーザ光パルス発振装置と、このレーザ光パルス発振
装置からの直線偏光したレーザ光を円偏光にする偏光変
換手段と、この偏光変換手段で円偏光されたレーザ光t
コリメートして目標体に照射する光学系と、前記目標体
からの反射光を検出する光検出器と、この光検出器の出
力信号が供給され前記目標体までの距離を算出して表示
する手段と金具備し、前記光学系及び前記偏光変換手段
及び前記ビーム分割偏光器を経由して前記目標体からの
反射光を前記光検出器に導くようにしたことを特徴とす
るレーザ測距装置。A laser light pulse oscillation device that outputs linearly polarized laser light from a beam splitting polarizer, a polarization conversion means that converts the linearly polarized laser light from the laser light pulse oscillation device into circular polarization, and the polarization conversion means. circularly polarized laser beam t
An optical system that collimates and irradiates the target object, a photodetector that detects reflected light from the target object, and a means that is supplied with an output signal of the photodetector and calculates and displays the distance to the target object. and a metal fitting, and the reflected light from the target object is guided to the photodetector via the optical system, the polarization conversion means, and the beam splitting polarizer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15512181A JPS5855812A (en) | 1981-09-30 | 1981-09-30 | Laser distance measuring device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15512181A JPS5855812A (en) | 1981-09-30 | 1981-09-30 | Laser distance measuring device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5855812A true JPS5855812A (en) | 1983-04-02 |
Family
ID=15599021
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15512181A Pending JPS5855812A (en) | 1981-09-30 | 1981-09-30 | Laser distance measuring device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5855812A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0283222A2 (en) * | 1987-03-20 | 1988-09-21 | Digital Optronics Corporation | 3-Dimensional vision system utilizing coherent optical detection |
-
1981
- 1981-09-30 JP JP15512181A patent/JPS5855812A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0283222A2 (en) * | 1987-03-20 | 1988-09-21 | Digital Optronics Corporation | 3-Dimensional vision system utilizing coherent optical detection |
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