JPH01101506A - Optical axis matching device - Google Patents
Optical axis matching deviceInfo
- Publication number
- JPH01101506A JPH01101506A JP25874687A JP25874687A JPH01101506A JP H01101506 A JPH01101506 A JP H01101506A JP 25874687 A JP25874687 A JP 25874687A JP 25874687 A JP25874687 A JP 25874687A JP H01101506 A JPH01101506 A JP H01101506A
- Authority
- JP
- Japan
- Prior art keywords
- reticle
- image
- optical axis
- laser
- optical system
- 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
-
- C—CHEMISTRY; METALLURGY
- C08—ORGANIC MACROMOLECULAR COMPOUNDS; THEIR PREPARATION OR CHEMICAL WORKING-UP; COMPOSITIONS BASED THEREON
- C08F—MACROMOLECULAR COMPOUNDS OBTAINED BY REACTIONS ONLY INVOLVING CARBON-TO-CARBON UNSATURATED BONDS
- C08F2/00—Processes of polymerisation
- C08F2/12—Polymerisation in non-solvents
- C08F2/16—Aqueous medium
- C08F2/22—Emulsion polymerisation
Landscapes
- Chemical & Material Sciences (AREA)
- Health & Medical Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Medicinal Chemistry (AREA)
- Polymers & Plastics (AREA)
- Organic Chemistry (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Mounting And Adjusting Of Optical Elements (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
との発明はレーザ測距装置のレーザ送信軸と規準光学系
光軸との整合を容易ならしめる光軸整合装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The invention relates to an optical axis alignment device that facilitates alignment of a laser transmission axis of a laser distance measuring device and an optical axis of a reference optical system.
第3図は、レーザ測距装置のレーザ光軸と規準軸との整
合を行う従来の方法を説明する図であって、(1)はレ
ーザ測距装置、(2)は送信光学系、(3)は規準光学
系、 (4)H接眼レンズ。FIG. 3 is a diagram illustrating a conventional method of aligning the laser optical axis of a laser range finder with a reference axis, in which (1) shows the laser range finder, (2) shows the transmission optical system, and ( 3) is the standard optical system, and (4) H eyepiece.
(5)ハレーザロッド端面からのコリメート光。(5) Collimated light from the end of the halasor rod.
(6)はコリメータ光、(7)はコリメータ、(8)は
コリメータ接眼部である。(6) is a collimator light, (7) is a collimator, and (8) is a collimator eyepiece.
第3図において、コリメータ(7)は最初9図の破線で
示す位置に設置される。送信光学系(211ft通して
観測されるレーザロッド端面からのコリメート光(5)
ヲコリメータ(7)で受光し。In FIG. 3, the collimator (7) is initially installed at the position indicated by the dashed line in FIG. Transmission optical system (collimated light from the end face of the laser rod observed through 211ft (5)
The light is received by the wokolimator (7).
接眼レンズ(8)を通して目視されるレーザロッド端面
像の中心が、コリメータ(7)の光軸中心にくるように
、コリメータ(7)に対するレーザ測距装置(1)の相
対位置・角度がまず調整される。First, the relative position and angle of the laser distance measuring device (1) with respect to the collimator (7) are adjusted so that the center of the laser rod end face image visually observed through the eyepiece (8) is aligned with the optical axis center of the collimator (7). be done.
上述の操作の後、コリメータ(7)ハ図の実線の位置に
、コリメータ(7)に付属の平行おくり機構を用いて平
行移動される。この位置において、今後はコリメータ(
7)から、コリメータ(7)の光軸に中心をおくレチク
ルのコリメータ光+6)がレーザ測距装置i! +11
の規準光学系(3)に入力される。したがって、接眼レ
ンズ+41からのぞくとレーザ測距装置(1)の規準視
野内に、前記レクチル像を認めることができる。After the above-described operation, the collimator (7) is translated in parallel to the position indicated by the solid line in the figure using the parallel moving mechanism attached to the collimator (7). At this position, the collimator (
7), the collimator light +6) of the reticle centered on the optical axis of the collimator (7) is the laser distance measuring device i! +11
is input to the reference optical system (3). Therefore, when looking through the eyepiece lens +41, the reticle image can be seen within the standard field of view of the laser distance measuring device (1).
第4図は、上述の規準視野内の儂の見え方を示す図であ
って、 +91&’!コリメータ())のレチクル像、
11(It!レーザ測距装置(11の規準光学系(3
)内の規準レチクル像である。FIG. 4 is a diagram showing how I look within the above-mentioned standard field of view, and shows +91&'! Collimator ()) reticle image,
11 (It! Laser distance measuring device (11 standard optical system (3)
) is the reference reticle image.
第4図において、前述までの説明で明らかなように、コ
リメータ(7)のレチクル像TIlの交点は、送信光学
系(2)の光軸位1!を表わしており、したがって、こ
の図においては、送信光軸は、規準レチクル(9)の白
抜き中心で表わされる規準光軸と9図に示す1だけずれ
ていることになる。よりて、従来の光軸整合操作におい
ては、接眼レンズを通して上述のレチクル像を見ながら
、レーザ測距装置m1 filの規準レチクル位置を調
節し、規準レチクル像α1がコリメータ(7)のレチク
ル像α〔に重なるようにしていた。In FIG. 4, as is clear from the above explanation, the intersection of the reticle image TIl of the collimator (7) is located at the optical axis position 1! of the transmission optical system (2). Therefore, in this figure, the transmission optical axis is shifted by 1 shown in FIG. 9 from the reference optical axis represented by the white center of the reference reticle (9). Therefore, in the conventional optical axis alignment operation, the reference reticle position of the laser range finder m1 fil is adjusted while viewing the above-mentioned reticle image through the eyepiece, so that the reference reticle image α1 becomes the reticle image α of the collimator (7). I made it overlap with [.
このように、従来においては、まずコリメータ(7)ヲ
通して送信光学系(2)内部のレーザロッド端面な見る
必要がめるが、端面が可視光で、無限遠に見えるように
するために、送信光学系(2)の色収差を可視光波長と
レーザ光波長(通常、1.06μm)の2つの波長帯で
除去する必要が生じる。したがって、一般に、レーザ測
距装置(1)が高価格となる問題がある。In this way, conventionally, it is necessary to first see the end face of the laser rod inside the transmitting optical system (2) through the collimator (7), but in order to make the end face visible to infinity with visible light, the transmitter It becomes necessary to remove the chromatic aberration of the optical system (2) in two wavelength bands: visible light wavelength and laser light wavelength (usually 1.06 μm). Therefore, there is generally a problem that the laser distance measuring device (1) is expensive.
さらに前述の操作の説明で明らかなように、整合ごとに
コリメータ(7)を平行移動をさせる必要がるり、光軸
整合に要する時間が大となって、レーザ測距装置の整備
性上も問題となる。Furthermore, as is clear from the explanation of the operation above, it is necessary to move the collimator (7) in parallel for each alignment, and the time required for optical axis alignment becomes long, which poses problems in terms of maintainability of the laser range finder. becomes.
この発Fi4rz前述のコリメータ操作をすることなく
光軸整合が可能な光軸整合装置を実現することを目的と
する。The purpose of this Fi4rz is to realize an optical axis alignment device capable of optical axis alignment without the above-mentioned collimator operation.
この発明の光軸整合装置は、送信レーザ光の中心を1f
flI像検出し、これを画面にレチクル表示する手段と
、このレチクルが規準光学系(3)で規準可能なように
、コリメータレンズとを用いたものでめる。The optical axis alignment device of this invention aligns the center of the transmitted laser beam by 1f.
It uses a means for detecting the flI image and displaying it on a reticle on a screen, and a collimator lens so that the reticle can be referenced by a reference optical system (3).
第1図はこの発明による装置の構成の1実施例と、レー
ザ測距装置との位置関係を示す図でろって、αυは受光
レンズ、abはコリメータレンズ、 (1mは半透跳、
aaは撮1M素子、aSd増巾器、L1iはA/D変
換器、鰭は2値化回路、 (Illは重心点@算回路、
asは位置データ、■はレチクル発生回路、 121は
表示回路、raば表示装置、@は発熱量センサ、@は表
示器でるる。FIG. 1 is a diagram showing an embodiment of the configuration of the device according to the present invention and the positional relationship with the laser distance measuring device, in which αυ is a light receiving lens, ab is a collimator lens, (1 m is a semi-transparent jump,
aa is the 1M camera element, aSd amplifier, L1i is the A/D converter, fin is the binarization circuit, (Ill is the center of gravity @ calculation circuit,
as is the position data, ■ is the reticle generation circuit, 121 is the display circuit, RA is the display device, @ is the calorific value sensor, and @ is the display.
@1図に2いて、最初、初期操作によってレチクル発生
回路ωは、撮像素子Q4の視野中心に対応する原点に中
心をもつレチクル信号を生成し1表示回路Qυによりブ
ラウン管等表°示装FIt、口に表示される。この像ハ
、コリメータレンズazにより平行光束に変換されて、
レーザ測距装置口)の規準光学系(3)に入射し、規準
視野内に像として認めることかできる。@1 As shown in Figure 2, initially, the reticle generation circuit ω generates a reticle signal centered at the origin corresponding to the center of the field of view of the image sensor Q4 by the initial operation, and the display circuit Qυ generates a reticle signal that is transmitted to the display device FIt, such as a cathode ray tube, etc. Appears in the mouth. This image is converted into a parallel beam by the collimator lens az,
It enters the reference optical system (3) of the laser range finder (exit) and can be recognized as an image within the reference field of view.
第2図(a)は上述の規準視野内の儂を示す図でおって
、@ニ上述のレチクル像であり、これと規準レチクル像
(9)とが図のように一致するように、レーザ光波長f
c[Tl)の位It、角度がまず調整される。FIG. 2(a) is a diagram showing me in the above-mentioned reference field of view, and is the above-mentioned reticle image. light wavelength f
The angle of the order of c[Tl) is first adjusted.
次において、レーザ測距装置(1)からレーザ光が単発
、送信されると、レーザ光は、半透鏡a3によりパワー
が分割、減衰されて受信レンズallにより、撮gI素
子I上に結像される。Next, when a single laser beam is transmitted from the laser range finder (1), the power of the laser beam is divided and attenuated by the semi-transparent mirror a3, and the image is formed on the gI element I by the receiving lens all. Ru.
撮像素子Q4の出力は増巾器a5で増巾され、A/D変
換器1111でディジタルビデオに変換されたあと雑音
除去のため、定められたしまい値を用いて、2値化回路
顛で2値化される。2値化された信号ぼ、蔦心点演算回
路r1・に入力されて9重心点が求められることにより
、レーザ光の像中心、すなわちレーザ光軸が検出される
。この位置データα9はレチクル発生回路■に入力され
、今度は、上記表示装置@上の位置データa9に応じた
位置に、レチクルが表示される。The output of the image sensor Q4 is amplified by an amplifier a5, converted to digital video by an A/D converter 1111, and then converted into a digital video by a binarization circuit using a predetermined end value to remove noise. Valued. The binarized signal is input to the center point arithmetic circuit r1 to obtain nine centroid points, thereby detecting the image center of the laser beam, that is, the laser optical axis. This position data α9 is input to the reticle generating circuit (3), and the reticle is then displayed on the display device @ at a position corresponding to the position data a9.
第2図(b)uこのときのレチクル像(2)と規準レチ
クル信任9との関係を示しており、説明上レーザ送信軸
と規準軸とがEだけずれた場合について示している。な
お1図でレチクル像(2)の交点(至)は検出されたレ
ーザ光位置を表わしており1表示位置@では表示されな
い。FIG. 2(b) shows the relationship between the reticle image (2) and the reference reticle confidence 9 at this time, and for the sake of explanation, the case is shown in which the laser transmission axis and the reference axis are deviated by E. Note that in FIG. 1, the intersection (to) of the reticle image (2) represents the detected laser beam position and is not displayed at the 1 display position @.
したがって、操作者は規準視野を見ながら規準レチクル
を調整し、規準レチクル像19)を表示装置(至)で表
示されているレチクル像(至)に一致させることにより
、レーザ送信軸と規準軸とを容易に整合させることがで
きる。Therefore, the operator adjusts the reference reticle while looking at the reference field of view and aligns the reference reticle image 19) with the reticle image (to) displayed on the display device (to), thereby aligning the laser transmission axis and the reference axis. can be easily matched.
また、第1図に示すように、半透鏡a3の反射光を発熱
センサ@でうけ、これの発熱量を計測することにより、
レーザ光パワーを表示器@に同時に表示することもでき
るので、レーザ送信パワーの確認も合わせて行うことが
でき、整備性の向上に、大きく寄与することができる。In addition, as shown in Fig. 1, by receiving the reflected light from the semi-transparent mirror a3 with a heat generation sensor @ and measuring the amount of heat generated by this,
Since the laser light power can be displayed on the display at the same time, the laser transmission power can also be confirmed, which can greatly contribute to improving maintainability.
このように、この発明によれば、レーザ光を受光し、そ
の位vIItを画像計測の後、規準光学系視野内に表示
することができるので、容易にレーザ送信軸と視野軸と
のずれ量を知ることができ、きわめて迅速、かつ容易に
軸整合がとれるばかりでなく、送信光学系(2)はレー
ザ光波長に対してのみ、収査が除去されておればよく、
レーザ測距装置のコスト低減に大きく寄与することがで
きる。As described above, according to the present invention, it is possible to receive the laser beam and display the corresponding value vIIt within the field of view of the reference optical system after image measurement. Not only can axis alignment be achieved very quickly and easily, but the transmission optical system (2) only needs to eliminate convergence for the laser light wavelength.
This can greatly contribute to cost reduction of laser distance measuring devices.
第1図はこの発明の一実施例を示す図、第2図はこの発
明における規準視野内の像を示す図、第3図は従来の光
軸整合の方法を示す図、第4図は従来の方法における規
準視野内の像を示す図でろって、 anrz受光レンズ
、αaHコリメータレンズ、 +141は撮像素子、a
sは増幅器、(1・はA/D変換器、 anは2値化回
路、Qlltl!重心点演算回路、(至)はレチクル発
生回路、Qυは表示回路。
lZ3は表示装置である。
なお図中、同一おるいは相当する部分には同一符号を付
して示しである。FIG. 1 is a diagram showing an embodiment of the present invention, FIG. 2 is a diagram showing an image within a standard field of view in this invention, FIG. 3 is a diagram showing a conventional optical axis alignment method, and FIG. 4 is a diagram showing a conventional optical axis alignment method. This is a diagram showing the image within the standard field of view in the method of
s is an amplifier, (1. is an A/D converter, an is a binarization circuit, Qlltl! center of gravity calculation circuit, (to) is a reticle generation circuit, Qυ is a display circuit. lZ3 is a display device. Inside, the same or corresponding parts are denoted by the same reference numerals.
Claims (1)
系と、前記第1の光学系の像面に設置される撮像素子と
、前記撮像素子の出力を増巾する増巾器と、前記増巾器
の出力をアナログディジタル変換するA/D変換器と、
前記A/D変換器が出力するディジタルビデオ信号を2
値化する2値化手段と、前記2値化手段が出力するバイ
ナリビデオ信号をうけて、重心点位置データを演算出力
する重心点演算回路と、前記重心点演算回路の出力をう
けて、レチクルを発生し、これを画面表示する手段と、
前記画面表示手段の表示画像から発する光束をユリメー
ト光に変換する第2の光学系とを備えたことを特徴とす
る光軸整合装置。a first optical system that receives a transmitted laser beam of a laser ranging device; an image sensor installed on an image plane of the first optical system; an amplification device that amplifies the output of the image sensor; an A/D converter that converts the output of the amplifier into analog and digital;
The digital video signal output from the A/D converter is
A binarization means for converting into a value, a barycenter point calculation circuit for calculating and outputting barycenter point position data in response to the binary video signal outputted by the binarization unit, and a barycenter point calculation circuit for calculating and outputting barycenter point position data in response to the output of the barycenter point calculation circuit. A means of generating and displaying this on the screen,
An optical axis alignment device comprising: a second optical system that converts a luminous flux emitted from the display image of the screen display means into a urimate light.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25874687A JPH01101506A (en) | 1987-10-14 | 1987-10-14 | Optical axis matching device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25874687A JPH01101506A (en) | 1987-10-14 | 1987-10-14 | Optical axis matching device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01101506A true JPH01101506A (en) | 1989-04-19 |
Family
ID=17324507
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP25874687A Pending JPH01101506A (en) | 1987-10-14 | 1987-10-14 | Optical axis matching device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01101506A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002162470A (en) * | 2000-11-28 | 2002-06-07 | Nhk Spring Co Ltd | Object detection apparatus and its reference axis setting method |
| KR102694876B1 (en) * | 2023-05-24 | 2024-08-14 | 샹하이 인스티튜트 오브 메저먼트 앤드 테스팅 테크놀로지 | Adjustment method and adjustment apparatus for mutual parallelism of two back-to-back gratings |
-
1987
- 1987-10-14 JP JP25874687A patent/JPH01101506A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002162470A (en) * | 2000-11-28 | 2002-06-07 | Nhk Spring Co Ltd | Object detection apparatus and its reference axis setting method |
| KR102694876B1 (en) * | 2023-05-24 | 2024-08-14 | 샹하이 인스티튜트 오브 메저먼트 앤드 테스팅 테크놀로지 | Adjustment method and adjustment apparatus for mutual parallelism of two back-to-back gratings |
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