JPS59196411A - Level utilizing laser light - Google Patents

Level utilizing laser light

Info

Publication number
JPS59196411A
JPS59196411A JP7174683A JP7174683A JPS59196411A JP S59196411 A JPS59196411 A JP S59196411A JP 7174683 A JP7174683 A JP 7174683A JP 7174683 A JP7174683 A JP 7174683A JP S59196411 A JPS59196411 A JP S59196411A
Authority
JP
Japan
Prior art keywords
laser beam
mirror
optical axis
mirrors
lens
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
JP7174683A
Other languages
Japanese (ja)
Inventor
Yasuto Ozaki
尾崎 康人
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP7174683A priority Critical patent/JPS59196411A/en
Priority to US06/524,036 priority patent/US4693567A/en
Priority to EP83304767A priority patent/EP0102221B1/en
Priority to DE8383304767T priority patent/DE3378381D1/en
Priority to AT83304767T priority patent/ATE38437T1/en
Priority to CA000434743A priority patent/CA1245487A/en
Publication of JPS59196411A publication Critical patent/JPS59196411A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C15/00Surveying instruments or accessories not provided for in groups G01C1/00 - G01C13/00
    • G01C15/002Active optical surveying means
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0911Anamorphotic systems

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To obtain a projected light beam having a wide angle range, by reflecting a laser beam having a specified diameter by a plurality of cylindrical reflecting surfaces, thereby obtaining the fan shaped luminous flux. CONSTITUTION:Laser light from laser oscillator 1 is reflected by first twin mirrors comprising a Y-axis adjusting mirror 2 and an X-axis adjusting mirror 3. Then, the laser light is reflected by second twin mirrors 4 and guided to a lens system comprising a concave lens 5 and convex lens 6. The laser light inputted to an optical axis 7 is made to be luminous flux having a specified diameter (d) and inputted to a reflector 8. The reflector 8 has three cylindrical reflecting surfaces, whose reflecting angles increase as the optical axis 7 is approached. The luminous flux having the diameter (d) on the optical axis 7 is reflected on a horizontal plane and a vertical plane as fan shaped luminous fluxes, which diffused at a wide angle, respectively.

Description

【発明の詳細な説明】 く技術分野〉 本発明はレーザ光により、被測量物上に直接水平線等を
映し出す水準儀に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a leveling instrument that projects a horizon directly onto an object to be surveyed using a laser beam.

〈従来技術〉 従来のこの種の水準儀として、レーザビームをシリンド
リカルレンズで屈折させる方式、あるいは多角柱状の回
転ミラーで反射させる方式のものがある。前者は屈折後
のビームの開き角が小さく、後者は回転機構を要する為
装置が複雑になり、しかもスポットが走るだけであるか
ら、連続した投光線を映し出すことができない欠点があ
る。
<Prior Art> As a conventional leveling instrument of this type, there is a method in which a laser beam is refracted by a cylindrical lens, or a method in which a laser beam is reflected by a rotating polygonal mirror. The former has the disadvantage that the aperture angle of the beam after refraction is small, and the latter requires a rotation mechanism, making the device complex, and since the spot only runs, it is not possible to project a continuous light beam.

〈発明の目的〉 本発明の目的は、広角度に亘って連続した投光線を映し
出すことができ、しかも、構造が簡単で、かつ、容易に
組立調整し得るレーザ光を用いた水準儀を提出すること
にある。
<Object of the Invention> The object of the present invention is to provide a leveling instrument using a laser beam that can project a continuous light beam over a wide angle, has a simple structure, and can be easily assembled and adjusted. There is a particular thing.

〈発明の構成〉 レーザ光発生源と、そのレーザ光を拡散させる凹レンズ
と、その凹レンズの後方に配設された凸レンズと、その
凸レンズの後方に配設されたシリンドリカル反射面と、
上記レーザ光発生源と上記凹レンズの間に配設された少
くとも2個の互に直交する反射体を有し、それら2個の
反射体のうちの一方のものにX方向調整機構を設け、他
方のものにY方向調整機構を設けたことを特徴としてい
〈実施例〉 第1図に本発明実施例の構成図を示す。
<Configuration of the Invention> A laser beam generation source, a concave lens that diffuses the laser beam, a convex lens disposed behind the concave lens, a cylindrical reflective surface disposed behind the convex lens,
at least two mutually orthogonal reflectors disposed between the laser light generation source and the concave lens, and one of the two reflectors is provided with an X-direction adjustment mechanism; Another feature is that a Y-direction adjustment mechanism is provided. Embodiment FIG. 1 shows a configuration diagram of an embodiment of the present invention.

レーザ発振器1はHe−Neレーザ管であって、赤色の
可視レーザ光を出力する。このレーザ光は、Y@調整鏡
2およびX軸調整鏡3からなる第1の二枚鏡で反射され
た後、交角が90°に固定された第2の二枚鏡4で反射
され、凹レンズ5および凸レンズ6からなるレンズ系に
誘導される。このレンズ系は、光軸7上に入射されたレ
ーザ光を光軸7上の所定の口径dを有する光線束となし
、その光軸7上に設けられた反射体8に入射させる。
The laser oscillator 1 is a He-Ne laser tube, and outputs a red visible laser beam. This laser beam is reflected by a first two-piece mirror consisting of a Y@adjustment mirror 2 and an X-axis adjustment mirror 3, then reflected by a second two-piece mirror 4 whose intersection angle is fixed at 90°, and is then reflected by a concave lens. 5 and a convex lens 6. This lens system converts laser light incident on the optical axis 7 into a beam of light having a predetermined diameter d on the optical axis 7, and makes the laser beam incident on the reflector 8 provided on the optical axis 7.

反射体8は、第2図(a)にその平面図、 (b)に正
面図を示す如(、光軸7に近づくほど反射角が増大する
シリンドリカル状の反射面を3個有し、光軸7上の口径
dなる光線束を、第3図に示す如く、水平面上および鉛
直面上にそれぞれ広角度拡散する扇形光線束として反射
させ、受光体上に水平投光線および鉛直投光線が映し出
されるよう構成されている。この受光体上における水平
投光線および鉛直投光線の幅は、レンズ系の凹レンズ5
をその光軸7上で摺動変位自在とし、レンズ系からの光
線束の合焦点を変化させることによって調節することが
でき、任意の距離に置かれた受光体近傍に合焦させるよ
うにすれば、極めて鋭い直線を映し出すことができる。
The reflector 8 has three cylindrical reflecting surfaces in which the angle of reflection increases as it approaches the optical axis 7, and as shown in FIG. As shown in Fig. 3, a beam of light having an aperture of d on the axis 7 is reflected as a fan-shaped beam of light that is diffused at a wide angle on the horizontal and vertical planes, respectively, and a horizontal and vertical beam is projected onto the photoreceptor. The width of the horizontal light emitting line and the vertical light emitting line on this photoreceptor is determined by the concave lens 5 of the lens system.
is slidably displaceable on its optical axis 7, and can be adjusted by changing the focusing point of the light beam from the lens system, so that it can be focused near the photoreceptor placed at an arbitrary distance. It is possible to project extremely sharp straight lines.

さて、上述の如き直線を得るには、レンズ系の光軸7上
に正しくレーザ光を誘導しなければならないが、本発明
では以下に説明する如き機構によって、容易にその誘導
を可能としている。
Now, in order to obtain the above-mentioned straight line, it is necessary to correctly guide the laser beam onto the optical axis 7 of the lens system, but in the present invention, this guidance is easily made possible by the mechanism described below.

第4図はレーザ発振器1からのレーザ光を、レンズ系の
光軸7上に誘導する第1および第2の二枚鏡の拡大図で
ある。第1の二枚鏡のY!II+調整鏡2は、紙面に直
交する軸上に回動自在の円柱21に取り付けられ、X@
tll整鏡3は上鏡3柱21と直交する軸上に回動自在
の円柱31に取り付けられている。従って、円柱21を
回動させると第1の二枚鏡の交角θが変化し、円柱31
を回動させると第1の二枚鏡の交線10が傾斜する。ま
た、第2の二枚鏡4は、その交角を90°に固定され、
それぞれ円柱31と平行な軸上を摺動かつ回動自在の円
柱41に取り付けられている。今、レーザ発振器1から
のレーザ光がaの如く、光軸7に対して第4図紙面上に
おいて平行でない場合、Y軸調整鏡2を回動して第1の
二枚鏡の交角θを調節することによって平行となすこと
ができる。また、第2の二枚鏡4に入射される光がbの
如くで、その結果第2の二枚鏡4からの反射光がCの如
(、第4図紙面上光軸7に対して平行にずれている場合
、第2の二枚鏡4を上方に摺動調節することによって反
射光を平行移動せしめて光軸7上に載せることができる
。また、第5図に第4図の要部平面図に示す如(、光が
dの如く光軸7に対して第5図紙面上において平行でな
い場合、X!Il+調整鏡3を回動調節することにより
平行となすことができる。更に、第6図に同様に第4図
の要部平面図を示す如く、光がeの如く光軸7に対して
平行にずれている場合、X軸調整鏡3および第2の二枚
鏡4を図の如く回動調節することによって反射光を平行
移動せしめて光軸7上に載せることができる。
FIG. 4 is an enlarged view of the first and second two mirrors that guide the laser beam from the laser oscillator 1 onto the optical axis 7 of the lens system. The first double mirror Y! The II+ adjustment mirror 2 is attached to a cylinder 21 that is rotatable on an axis perpendicular to the plane of the paper, and
The tll adjustment mirror 3 is attached to a cylindrical column 31 that is rotatable on an axis perpendicular to the upper mirror 3 column 21. Therefore, when the cylinder 21 is rotated, the intersection angle θ of the first two mirrors changes, and the cylinder 31
When rotated, the intersection line 10 of the first two mirrors is inclined. Further, the second two-piece mirror 4 has its intersection angle fixed at 90°,
Each is attached to a cylinder 41 that is slidable and rotatable on an axis parallel to the cylinder 31. Now, if the laser beam from the laser oscillator 1 is not parallel to the optical axis 7 on the paper surface of FIG. It can be made parallel by adjusting. Also, the light incident on the second two-piece mirror 4 is as shown in b, and as a result, the reflected light from the second two-piece mirror 4 is as shown in C (with respect to the optical axis 7 on the paper in Figure 4). If the two mirrors 4 are deviated in parallel, the reflected light can be moved in parallel and placed on the optical axis 7 by adjusting the second two-piece mirror 4 upward. If the light is not parallel to the optical axis 7 on the plane of FIG. 5 as shown in the plan view of the main part (d), it can be made parallel by rotating the X!Il+ adjusting mirror 3. Furthermore, as shown in FIG. 6, which is also a plan view of the main part of FIG. 4, when the light is deviated parallel to the optical axis 7 as shown in e, By adjusting the rotation of 4 as shown in the figure, the reflected light can be moved in parallel and placed on the optical axis 7.

第7図に本発明の他の実施例を示す。この実施例が第1
図のものと相違する点は、レーザ発振器lと、凹レンズ
50間に2枚の反射鏡2A、3Aが設けられており、そ
の一方のもの2AがY軸調整機構を備え、他方のもの3
AがX軸調整機構を備えていることである。この実施例
においても、レーザ光発光源1は光学系の下方に配設す
ることができ、反射鏡2Δ、3Aの位置と角度の調節に
より反射体8に入射するレーザビームの中心軸の位置及
び傾き角を調整することができる。
FIG. 7 shows another embodiment of the present invention. This example is the first
The difference from the one in the figure is that two reflective mirrors 2A and 3A are provided between the laser oscillator l and the concave lens 50, one of which 2A is equipped with a Y-axis adjustment mechanism, and the other mirror 3A is provided with a Y-axis adjustment mechanism.
A is equipped with an X-axis adjustment mechanism. In this embodiment as well, the laser beam source 1 can be disposed below the optical system, and the position and angle of the central axis of the laser beam incident on the reflector 8 can be adjusted by adjusting the positions and angles of the reflectors 2Δ and 3A. Tilt angle can be adjusted.

〈効果) 以上説明したように、本発明によれば、所定口径を有す
るレーザビームを複数のシリンドリカル状反射面によっ
て反射させて扇形光線束を得ている為、従来のビームの
屈折による方式に比して極めて広角度の投光線を得るこ
とができる。また、反射面を静止させた状態で扇形光線
束を得ている為、投光線は連続的なものとなる。更に、
レーザ発振器からのレーザビームを、第1および第2の
二枚鏡の合鏡の反射を経てレンズ系の光軸上に導びき、
合鏡を所定方向に調節自在としているので、レーザ光発
光器と光学系の間の位置関係を厳格に製作しなくても、
第1および第2の反射鏡の調節のみにより反射体8に入
射するレーザビームの位置及び方向を調節することがで
きるので、製作が容易になり、また、レーザ光発光器と
光学系等を直列に配設せず立体的に配設することができ
るので、装置全体の全長が短縮される。
<Effects> As explained above, according to the present invention, a laser beam having a predetermined diameter is reflected by a plurality of cylindrical reflecting surfaces to obtain a fan-shaped ray bundle. As a result, an extremely wide-angle projection beam can be obtained. Furthermore, since the fan-shaped ray bundle is obtained with the reflecting surface stationary, the projected light rays are continuous. Furthermore,
A laser beam from a laser oscillator is guided onto the optical axis of a lens system through reflection from a combination of first and second mirrors,
Since the mirror can be adjusted in a predetermined direction, there is no need to create a strict positional relationship between the laser beam emitter and the optical system.
Since the position and direction of the laser beam incident on the reflector 8 can be adjusted only by adjusting the first and second reflecting mirrors, manufacturing is facilitated, and the laser beam emitter and the optical system are connected in series. Since the device can be arranged three-dimensionally without having to be placed in the middle, the overall length of the entire device can be shortened.

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

第1図は本発明実施例の構成図、第2図(a)。 (b)はそれぞれ本発明実施例の反射体の平面図および
正面図、第3図はその反射体の作用説明図、第4図は本
発明実施例の第1および第2の二枚鏡の拡大図、第5図
および第6図はその作用を説明する為の要部平面図であ
る。第7図は本発明の他の実施例を示す構成図である。 1−レーザ発振器、    2.2A−Y@調整鏡3.
3A−X@調整鏡、  4−第2の二枚鏡5−凹レンズ
、     6−凸レンズ7−レンズ系の光軸、  8
−反射体 10−第1の二枚鏡の交線。 θ−第1の二枚鏡の交角 特許出願人       尾 崎 康 人代理人 弁理
士西1)新
FIG. 1 is a configuration diagram of an embodiment of the present invention, and FIG. 2(a). (b) is a plan view and a front view of a reflector according to an embodiment of the present invention, FIG. 3 is an explanatory diagram of the function of the reflector, and FIG. The enlarged view, FIG. 5, and FIG. 6 are plan views of essential parts for explaining the operation. FIG. 7 is a configuration diagram showing another embodiment of the present invention. 1-Laser oscillator, 2.2A-Y@adjustment mirror3.
3A-X@adjustment mirror, 4-second double mirror 5-concave lens, 6-convex lens 7-optical axis of lens system, 8
- Reflector 10 - Intersection line of the first two mirrors. θ - Intersection angle of the first two mirrors Patent applicant Yasushi Ozaki Representative Patent attorney Nishi 1) Arata

Claims (2)

【特許請求の範囲】[Claims] (1)レーザ光発生源と、そのレーザ光を拡散させる凹
レンズと、その凹レンズの後方に配設された凸レンズと
、その凸レンズの後方に配設されたシリンドリカル反射
面と、上記レーザ光発生源と上記凹レンズの間に配設さ
れた少くとも2個の互に直交する反射体を有し、それら
2個の反射体のうちの一方のものにX方向調整機構を設
け、他方のものにY方向調節機構を設けたことを特徴と
するレーザ光を用いた水準儀。
(1) A laser beam generation source, a concave lens that diffuses the laser beam, a convex lens disposed behind the concave lens, a cylindrical reflective surface disposed behind the convex lens, and the laser beam generation source. It has at least two mutually orthogonal reflectors disposed between the concave lenses, one of the two reflectors is provided with an X-direction adjustment mechanism, and the other is provided with a Y-direction adjustment mechanism. A leveling instrument that uses laser light and is characterized by being equipped with an adjustment mechanism.
(2)レーザ光発生源と、そのレーザ光を反射させる二
枚鏡であって、一方の鏡が当該二枚鏡の交角を変化させ
る方向に、他方の鏡が当該二枚鏡の交線を傾斜させる方
向に、それぞれ回動調節自在に設けられて成る第1の二
枚鏡と、その第1の二枚鏡を反射したレーザ光を反射さ
せる二枚鏡であって、交角が直角に固定された状態で当
該二枚鏡の主平面上の所定方向に摺動調節自在で、かつ
、上記所定方向上の軸を中心として回動調節自在の第2
の二枚鏡と、光軸上に入射された光を光軸上所定の口径
を有する光線束となすレンズ系と、そのレンズ系の光軸
上に設けられ、中心に近づくほど反射角が増大する複数
のシリンドリカル状曲面によって形成された反射面とを
備え、上記第1および第2の二枚鏡の各鏡の調節により
上記レーザ光発生源からのレーザ光を上記レンズ系の光
軸上に誘導し、上記反射面から少なくとも水平面上で拡
開する扇形光線束を反射して、受光体上に水平の投光線
が映し出されるよう構成したことを特徴とする特許請求
の範囲第1項記載のレーザ光を用いた水準ずM 。
(2) A laser beam generation source and two mirrors that reflect the laser beam, one mirror changing the intersection angle of the two mirrors, and the other mirror changing the intersection line of the two mirrors. a first two-piece mirror that is rotatably adjustable in the direction of inclination; and a two-piece mirror that reflects a laser beam reflected from the first two-piece mirror, the intersecting angle of which is fixed at a right angle. a second mirror that can be slidably adjusted in a predetermined direction on the main plane of the two-panel mirror in a state where
A two-piece mirror, a lens system that converts the light incident on the optical axis into a bundle of rays with a predetermined diameter on the optical axis, and a lens system that is installed on the optical axis of the lens system, and the angle of reflection increases as it approaches the center. and a reflecting surface formed by a plurality of cylindrical curved surfaces, and the laser beam from the laser beam generation source is directed onto the optical axis of the lens system by adjusting each of the first and second two mirrors. According to claim 1, the fan-shaped ray bundle is guided and reflected from the reflecting surface to spread out at least on a horizontal plane, so that a horizontal projected light ray is projected onto the photoreceptor. Levelless M using laser light.
JP7174683A 1982-08-21 1983-04-22 Level utilizing laser light Pending JPS59196411A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP7174683A JPS59196411A (en) 1983-04-22 1983-04-22 Level utilizing laser light
US06/524,036 US4693567A (en) 1982-08-21 1983-08-17 Apparatus for projecting luminous lines on an object by a laser beam
EP83304767A EP0102221B1 (en) 1982-08-21 1983-08-17 An apparatus for projecting luminous lines on an object by a laser beam
DE8383304767T DE3378381D1 (en) 1982-08-21 1983-08-17 An apparatus for projecting luminous lines on an object by a laser beam
AT83304767T ATE38437T1 (en) 1982-08-21 1983-08-17 DEVICE FOR PROJECTING LUMINOUS TRAILS ONTO AN OBJECT BY MEANS OF A LASER BEAM.
CA000434743A CA1245487A (en) 1982-08-21 1983-08-17 Apparatus of projecting luminous lines on an object by a laser beam

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7174683A JPS59196411A (en) 1983-04-22 1983-04-22 Level utilizing laser light

Publications (1)

Publication Number Publication Date
JPS59196411A true JPS59196411A (en) 1984-11-07

Family

ID=13469394

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7174683A Pending JPS59196411A (en) 1982-08-21 1983-04-22 Level utilizing laser light

Country Status (1)

Country Link
JP (1) JPS59196411A (en)

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