JP2639675B2 - Theodolite with laser - Google Patents

Theodolite with laser

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Publication number
JP2639675B2
JP2639675B2 JP63032666A JP3266688A JP2639675B2 JP 2639675 B2 JP2639675 B2 JP 2639675B2 JP 63032666 A JP63032666 A JP 63032666A JP 3266688 A JP3266688 A JP 3266688A JP 2639675 B2 JP2639675 B2 JP 2639675B2
Authority
JP
Japan
Prior art keywords
laser
optical system
theodolite
linearly polarized
beam splitter
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.)
Expired - Lifetime
Application number
JP63032666A
Other languages
Japanese (ja)
Other versions
JPH01209314A (en
Inventor
亮 西村
晴夫 谷
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.)
SOKIA KK
Original Assignee
SOKIA KK
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 SOKIA KK filed Critical SOKIA KK
Priority to JP63032666A priority Critical patent/JP2639675B2/en
Publication of JPH01209314A publication Critical patent/JPH01209314A/en
Application granted granted Critical
Publication of JP2639675B2 publication Critical patent/JP2639675B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、レーザ備え、レーザ光で基準位置から所定
の方向を設定でき、特にトンネル内や暗渠内での暗闇の
中でレーザ光を照射し所定の方向を決定できるセオドラ
イトに関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial application field) The present invention is provided with a laser and can set a predetermined direction from a reference position with a laser beam, and irradiates the laser beam particularly in the darkness in a tunnel or a culvert. And a theodolite capable of determining a predetermined direction.

(従来の技術) 従来のレーザを備えるセオドライトは、第5図示のよ
うに、接眼レンズa、焦点鏡b、ダハプリズムc、合焦
レンズe及び対物レンズfから成る眼視光学系と、レー
ザg、プリズムh、集光レンズm、プリズムi、合焦レ
ンズj、プリズムk、l及び対物レンズfから成るレー
ザ光学系とで構成されており、眼視光学系によって目標
物を視準すると共にレーザ光学系によって目標物にレー
ザ光を出射できるようになっている。
(Prior Art) As shown in FIG. 5, a conventional theodolite equipped with a laser includes a visual optical system including an eyepiece a, a focusing mirror b, a roof prism c, a focusing lens e, and an objective lens f, and a laser g, The laser optical system includes a prism h, a condenser lens m, a prism i, a focusing lens j, a prism k, l, and an objective lens f. A laser beam can be emitted to a target by a system.

このセオドライトによれば、例えば暗いトンネル内等
において、レーザ光の照射方向に合わせて掘削作業を進
めるといった使い方ができる。
According to the theodolite, it is possible to use it, for example, in a dark tunnel or the like, to perform excavation work in accordance with the irradiation direction of the laser beam.

(発明が解決しようとする課題) しかし、上記した従来のセオドライトは、対物レンズ
を両光学系で共用しているため次のような欠点がある。
(Problems to be Solved by the Invention) However, the conventional theodolite described above has the following disadvantages because the objective lens is shared by both optical systems.

レーザの倍率(対物レンズfから出射するレーザ光の
口径Dとレーザgから出射されるレーザ光の口径dとの
比)を上げると、対物レンズfから出射するレーザ光の
広がり角(発散角)が小さくなるため、遠方にまでレー
ザ光のスポットを小さくして使用することができるが、
第6図示のようにプリズムlが大きくなるため、眼視光
学系に有効に使用される対物レンズfの面積(斜線部
分)が小さくなり、視野が暗い。
When the magnification of the laser (the ratio of the diameter D of the laser light emitted from the objective lens f to the diameter d of the laser light emitted from the laser g) is increased, the spread angle (divergence angle) of the laser light emitted from the objective lens f is increased. Is small, so that the laser beam spot can be used at a small distance.
As shown in FIG. 6, since the prism 1 is large, the area (shaded area) of the objective lens f effectively used in the visual optical system is small, and the visual field is dark.

また、対物レンズfの中央部をレーザ光学系に使用す
るので、眼視光学系はそれ以外の領域しか使えず、分解
能が悪い。また、レーザ光が僅かではあるが対物レンズ
fで反射等して眼視望遠鏡へ入射するため、トンネル内
等の暗視野での使用が困難である。
Further, since the central portion of the objective lens f is used for the laser optical system, the visual optical system can use only the other area, and the resolution is poor. Further, although a small amount of the laser light is reflected by the objective lens f and enters the visual telescope, it is difficult to use the laser light in a dark field such as in a tunnel.

本発明は、従来のこのような欠点のないセオドライト
を提供することをその目的とするものである。
An object of the present invention is to provide a conventional theodolite free of such disadvantages.

(課題を解決するための手段) 本発明は、上記の目的を達成するために、レーザを備
え、そのレーザ光を眼視光学系の光軸に沿って出射する
ようにしたセオドライトにおいて、直線偏光レーザと、
前記眼視光学系とは別個のレーザ光学系と、前記眼視光
学系の対物レンズの前方に配設した偏光ビームスプリッ
タとを備え、前記直線偏光レーザから出射し前記レーザ
光学系を経た直線偏光レーザ光を前記偏光ビームスプリ
ッタで反射させ、前記眼視光学系の光軸に沿って出射す
るようにしたことを特徴とする。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides a theodolite having a laser, which emits the laser light along the optical axis of a visual optical system. A laser,
A laser optical system separate from the visual optical system, and a polarizing beam splitter disposed in front of an objective lens of the visual optical system, and linearly polarized light emitted from the linearly polarized laser and passing through the laser optical system. The laser beam is reflected by the polarization beam splitter and emitted along the optical axis of the visual optical system.

(作用) 直線偏光レーザから出射する直線偏光レーザは、レー
ザ光学系によって偏光ビームスプリッタに導かれ、ここ
で反射されて眼視光学系の光軸に沿って出射される。該
偏光ビームスプリッタは眼視光学系の光を透過させるの
で、レーザ光学系によってレーザ光を高倍率にしても眼
視光学系の視準機能が妨げられない。またレーザ光は偏
光ビームスプリッタで妨げられて眼視望遠鏡へ入射する
ことがない。
(Function) The linearly polarized laser beam emitted from the linearly polarized laser beam is guided to the polarization beam splitter by the laser optical system, reflected there, and emitted along the optical axis of the visual optical system. Since the polarizing beam splitter transmits light of the visual optical system, the collimating function of the visual optical system is not hindered even if the laser light is increased in magnification by the laser optical system. Further, the laser light is not hindered by the polarizing beam splitter and does not enter the visual telescope.

(実施例) 以下本発明の実施例を図面につき説明する。Embodiment An embodiment of the present invention will be described below with reference to the drawings.

第1図において、1は直線偏光レーザで、該レーザ1
から出射したレーザ光は、レーザ光学系の反射プリズム
2、焦光レンズ3、プリズム4、合焦レンズ5、対物レ
ンズ6及び反射鏡7を経て偏光ビームスプリッタ8で反
射されて補整板9を通過し、接眼レンズ10、焦点鏡11、
ダハプリズム12、合焦レンズ13、対物レンズ14、偏光ビ
ームスプリッタ8及び補整板9から成るレーザ光学系と
同軸に投光されるようになっており、また、該レーザ1
は、偏光ビームスプリッタ8に直線偏光レーザ光のS成
分が入射するように支持されている。
In FIG. 1, reference numeral 1 denotes a linearly polarized laser,
Is emitted from the laser beam, is reflected by a polarizing beam splitter 8 through a reflecting prism 2, a focusing lens 3, a prism 4, a focusing lens 5, an objective lens 6, and a reflecting mirror 7 of the laser optical system, and passes through a compensating plate 9. And eyepiece 10, focusing mirror 11,
The laser beam is projected coaxially with a laser optical system including a roof prism 12, a focusing lens 13, an objective lens 14, a polarizing beam splitter 8, and a compensating plate 9.
Are supported such that the S component of the linearly polarized laser light enters the polarization beam splitter 8.

該偏光ビームスプリッタ8は、直線偏光レーザ光のS
成分及びP成分について、例えば、第4図のS及びPで
示すような反射率特性を有し、例えば632.8nmの直線偏
光レーザ光のS成分を反射し、632.8nmの直線偏光レー
ザ光のP成分を透過し、632.8nmより短波長のS、P成
分とも透過するものである。
The polarization beam splitter 8 outputs the linearly polarized laser light S
The component and the P component have, for example, reflectance characteristics as shown by S and P in FIG. 4, and reflect the S component of the linearly polarized laser light of 632.8 nm, for example, and reflect the P component of the linearly polarized laser light of 632.8 nm. Component, and also transmits S and P components having a wavelength shorter than 632.8 nm.

前記補整板9は偏光ビームスプリッタ8による偏移分
を補正するもので、防塵ガラスの役目もする。
The compensating plate 9 corrects the shift caused by the polarizing beam splitter 8, and also functions as a dustproof glass.

尚、前記レーザ光学系は、レーザ1から出射したレー
ザ光Lがプリズム2及び集光レンズ3を経て、第1図及
び第2図に示すように、ダハプリズム12の占める空間に
集光するようになっているので、該レーザ光学系及び眼
視光学系を収納する筐体15を小さくすることができる。
Incidentally, the laser optical system is designed so that the laser beam L emitted from the laser 1 passes through the prism 2 and the condenser lens 3 and is condensed in the space occupied by the roof prism 12, as shown in FIGS. Therefore, the size of the housing 15 that houses the laser optical system and the visual optical system can be reduced.

以上のように偏光ビームスプリッタ8は、632.8nmの
偏光レーザのP成分及び632.8nmより短波長のP、S成
分の光が透過するので、眼視望遠鏡は、目標物に当り、
偏光成分がなく散乱しているレーザ光を確認できる。
As described above, the polarizing beam splitter 8 transmits the P component of the polarized laser having a wavelength of 632.8 nm and the P and S components having a wavelength shorter than 632.8 nm, so that the visual telescope hits a target object.
The laser light scattered without the polarization component can be confirmed.

前記ダハプリズム12に代えて第3図示のようにポロプ
リズム12Aを用いてもよく、これにより眼視用光学系を
短くすることができ、セオドライトをコンパクトなもの
にできる。
As shown in FIG. 3, a Porro prism 12A may be used instead of the roof prism 12, whereby the optical system for visual observation can be shortened and the theodolite can be made compact.

(発明の効果) 本発明は、上述のとおり構成されているので、レーザ
から出射されるレーザ光を高倍率化することができ、そ
れによってレーザ光の広がり角を小さくできるから、レ
ーザ光のスポットを遠方まで小さくして使用することが
でき、しかも眼視望遠鏡の分解能を測量機専用の望遠鏡
と同等にすることができる。また、レーザ光の眼視望遠
鏡への迷光がないから、トンネル等内の暗視野での使用
が容易になる等の効果がある。
(Effects of the Invention) Since the present invention is configured as described above, it is possible to increase the magnification of the laser light emitted from the laser and thereby reduce the spread angle of the laser light. Can be used at a distance, and the resolution of the optical telescope can be made equivalent to that of a telescope dedicated to surveying instruments. In addition, since there is no stray light of the laser light to the visual telescope, there is an effect that use in a dark field in a tunnel or the like becomes easy.

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

第1図は本発明の一実施例の要部の線図、第2図はその
ダハプリズムの断面図、第3図は本発明の他の実施例の
要部の線図、第4図は偏光ビームスプリッタの特性図、
第5図は従来のセオドライトの要部の線図、第6図はそ
の作動説明図である。 1…直線偏光レーザ、6…対物レンズ 8…偏光ビームスプリッタ、14…対物レンズ
FIG. 1 is a diagram of a main part of one embodiment of the present invention, FIG. 2 is a cross-sectional view of the roof prism, FIG. 3 is a diagram of a main part of another embodiment of the present invention, and FIG. Characteristic diagram of the beam splitter,
FIG. 5 is a diagram of a main part of a conventional theodolite, and FIG. 6 is an explanatory diagram of its operation. DESCRIPTION OF SYMBOLS 1 ... Linearly polarized laser, 6 ... Objective lens 8 ... Polarization beam splitter, 14 ... Objective lens

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】レーザを備え、そのレーザ光を眼視光学系
の光軸に沿って出射するようにしたセオドライトにおい
て、直線偏光レーザと、前記眼視光学系とは別個のレー
ザ光学系と、前記眼視光学系の対物レンズの前方に配設
した偏光ビームスプリッタとを備え、前記直線偏光レー
ザから出射し前記レーザ光学系を経た直線偏光レーザ光
を前記偏光ビームスプリッタで反射させ、前記眼視光学
系の光軸に沿って出射するようにしたことを特徴とする
レーザを有するセオドライト。
1. A theodolite comprising a laser and emitting the laser light along an optical axis of an eye optical system, a linearly polarized laser, a laser optical system separate from the eye optical system, A polarizing beam splitter disposed in front of the objective lens of the visual optical system, and reflecting the linearly polarized laser light emitted from the linearly polarized laser beam and passing through the laser optical system with the polarized beam splitter, A theodolite having a laser, which is emitted along an optical axis of an optical system.
JP63032666A 1988-02-17 1988-02-17 Theodolite with laser Expired - Lifetime JP2639675B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63032666A JP2639675B2 (en) 1988-02-17 1988-02-17 Theodolite with laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63032666A JP2639675B2 (en) 1988-02-17 1988-02-17 Theodolite with laser

Publications (2)

Publication Number Publication Date
JPH01209314A JPH01209314A (en) 1989-08-23
JP2639675B2 true JP2639675B2 (en) 1997-08-13

Family

ID=12365192

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63032666A Expired - Lifetime JP2639675B2 (en) 1988-02-17 1988-02-17 Theodolite with laser

Country Status (1)

Country Link
JP (1) JP2639675B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109520525A (en) * 2018-11-29 2019-03-26 中国科学院长春光学精密机械与物理研究所 The theodolite light axis consistency method of inspection, device, equipment and readable storage medium storing program for executing

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5748723A (en) * 1980-09-08 1982-03-20 Sanpack:Kk Method for selecting quantity of emitted light
JPS59100805A (en) * 1982-12-01 1984-06-11 Canon Inc Device for observing object
JPS6031614U (en) * 1983-08-09 1985-03-04 株式会社 測機舎 laser theodolite

Also Published As

Publication number Publication date
JPH01209314A (en) 1989-08-23

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