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JPS6355481A - Device for generating line object rotary laser beam in plane position detecting device using laser - Google Patents

Device for generating line object rotary laser beam in plane position detecting device using laser

Info

Publication number
JPS6355481A
JPS6355481A JP19909686A JP19909686A JPS6355481A JP S6355481 A JPS6355481 A JP S6355481A JP 19909686 A JP19909686 A JP 19909686A JP 19909686 A JP19909686 A JP 19909686A JP S6355481 A JPS6355481 A JP S6355481A
Authority
JP
Japan
Prior art keywords
laser beam
prism
laser
mirror
motor
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.)
Granted
Application number
JP19909686A
Other languages
Japanese (ja)
Other versions
JPH0476634B2 (en
Inventor
Tatsuyuki Ochi
越智 達之
Nobuo Tanaka
信男 田中
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.)
Kajima Corp
Original Assignee
Kajima Corp
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 Kajima Corp filed Critical Kajima Corp
Priority to JP19909686A priority Critical patent/JPS6355481A/en
Priority to US07/066,423 priority patent/US4874238A/en
Priority to GB8714988A priority patent/GB2195852B/en
Priority to DE8718134U priority patent/DE8718134U1/en
Priority to DE19873722429 priority patent/DE3722429A1/en
Priority to FR878709868A priority patent/FR2603376B1/en
Priority to CH3301/87A priority patent/CH676504A5/de
Publication of JPS6355481A publication Critical patent/JPS6355481A/en
Publication of JPH0476634B2 publication Critical patent/JPH0476634B2/ja
Granted legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To obtain a line object rotary laser beam having high accuracy by constituting the titled device so that a laser beam is reflected two times in a prism and a mirror. CONSTITUTION:A pentagonal prism 5 is installed in the center of a rotary base 3 which is rotated on a horizontal plane by a motor 2, and a laser oscillator 4 is provided on a revolving shaft 2a of the motor 2. Also, on the rotary base 3, a composite prism 6 is installed in the optical axis direction of the prism 5, and a right-angle mirror 7 is provided on a fixed part. In this state, when the motor 2 rotates, the rotary base 3 rotates clockwise, and the prisms 5, 6 rotate at a prescribed speed. A laser beam from the oscillator 4 is curved by 90 deg. by the prism 5, divided into two by the prism 6, and one of them is emitted as one of line object beams, namely, a counterclockwise laser beam CCW, and the other is made incident on the mirror 7. The laser beam which has been made incident on the mirror 7 is reflected by the mirror 7, and emitted as the other of the line object beams, namely, a clockwise laser beam CW. In this way, a line object rotary laser beam is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、三角測量の原理によって!!f[地点の座標
を求めるに際し、レーザーを用いて平面位置を検出する
装置において線対象回転レーザー、光線を作る装置に関
する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is based on the principle of triangulation! ! f [Relates to a device that creates a line-symmetric rotating laser and a light beam in a device that uses a laser to detect a plane position when determining the coordinates of a point.

[従来の技術及びその問題点] 三角測量によって平面位置を求める従来の方法は、トラ
ンシットを用いて行うのが普通であり、トランシットに
よる場合は、トランシットを操作する測量±1名とポー
ルをもつ作業員の少なくとも2名の人員を必要とし、ま
た熟練を要すと共に作業時間もかかるものであった。
[Prior art and its problems] The conventional method of determining a plane position by triangulation is usually carried out using a transit, and when using a transit, it requires ±1 surveyor to operate the transit and work with a pole. This method requires at least two people to work together, requires skill, and is time-consuming.

そこで本出願人はレーザーを用いて測mを行う方法につ
いて先に特許出願を行った(特願昭60−267481
号)。この方法は三角測量の原理によって計測地点の座
標を求めるに際し、2箇所の基準点に線対象な2光線を
むらのない旋回速度で旋回照射するレーザー燈台を設け
、その対象軸を各々他方の基準点の方向に合せ、一方、
計測地点にはレーザー光を検知するセンサーおよび正確
な時開測定装置を設けて、レーザー燈台により照射され
る線対象な2光線を検知する時間間隙を計測しこれを演
算装置に入力して計測点とレーザー光線の線対象軸との
なす角度に変換し、その角度と予め計測されている基準
点の距離とから計測地点の座標を停出する方法であるが
、この方法において問題になるのは、レーザー燈台すな
わち線対象回転レーザー光線を作る装置を構成するプリ
ズムやミラー等の取付をきわめて高精度で行わねばなら
ない点である。
Therefore, the present applicant previously filed a patent application for a method of measuring meters using a laser (Patent application No. 60-267481).
issue). In this method, when determining the coordinates of a measurement point using the principle of triangulation, a laser lighthouse is installed at two reference points that irradiates two line-symmetrical beams at an even rotational speed, and each axis of interest is set as the reference point of the other. Align with the direction of the point, while
A sensor that detects laser light and an accurate time measurement device are installed at the measurement point to measure the time gap between detecting two symmetrical beams emitted by the laser lighthouse, and input this to a calculation device to determine the measurement point. The method is to convert the coordinates of the measurement point into an angle between the symmetrical axis of the laser beam and the symmetrical axis of the laser beam, and then determine the coordinates of the measurement point from that angle and the distance of the reference point that has been measured in advance.The problem with this method is that The point is that the installation of the prisms, mirrors, etc. that make up the laser lighthouse, that is, the device that creates the line-symmetric rotating laser beam, must be done with extremely high precision.

本発明は、プリズムやミラーの中でレーザー光を2回反
射させる構成とすることによりプリズムやミラー等の取
付誤差を相殺し、きわめて高精度の線対象回転レーザー
光線を作ることができる装置を提供すべくなされたもの
である。
The present invention provides a device that can create a line-symmetric rotating laser beam with extremely high precision by canceling installation errors of the prism or mirror by reflecting the laser beam twice in the prism or mirror. This is something that has been done as much as possible.

[問題点を解決するための手段] 第1図および第2図において、鉛直軸を回転軸としてむ
らのない回転速度で回転するモータ2により水平面上で
回転させられる回転台3の中心にペンタプリズム5を設
置し、レーザー発振器4をモータ2の回転軸2a上に設
ける。さらに回転台3上に、ペンタプリズム5の光軸方
向に複合プリズム6を設置し、複合プリズム6はビーム
スプリッタ−及び2個の直角反射面を持つものである。
[Means for Solving the Problems] In FIGS. 1 and 2, a pentaprism is mounted at the center of a rotary table 3 that is rotated on a horizontal plane by a motor 2 that rotates at an even speed with a vertical axis as the rotation axis. 5 is installed, and a laser oscillator 4 is installed on the rotating shaft 2a of the motor 2. Furthermore, a compound prism 6 is installed on the rotary table 3 in the optical axis direction of the pentaprism 5, and the compound prism 6 has a beam splitter and two right-angled reflecting surfaces.

固定部に直角ミラー7を、ミラーの交差部「1をモータ
2の回転軸2aと直角に、かつ交わるように設置する。
A right-angle mirror 7 is installed on the fixed part so that the intersection part "1" of the mirror is perpendicular to and intersects with the rotation axis 2a of the motor 2.

[発明の作用] 第1図および第2図において、モータ2が回転すること
により回転台3が矢印で示す時計方向に回転し、それに
伴いペンタプリズム5及び複合プリズム6が所定の回転
速度でむらなく回転する。
[Operation of the invention] In FIGS. 1 and 2, as the motor 2 rotates, the rotary table 3 rotates in the clockwise direction indicated by the arrow, and the pentaprism 5 and the compound prism 6 rotate unevenly at a predetermined rotational speed. It rotates without any problem.

レーザー発振器4からのレーザー光はペンタプリズム5
によって90度曲げられる。ペンタプリズム5からのレ
ーザー光は複合プリズム6によって2分され、一方は線
対象レーザー光線の一方、すなわち反時計回りレーザー
光線CCWとして外側に出し、他方は高さを変えて回転
中心に戻す。回転中心に戻されたレーザー光は直角ミラ
ー7により線対象ビーム光線の他方、すなわち時計回り
のレーザー光線CWとして反射される。これにより線対
象な回転レーザー光線を得ることができる。
The laser beam from the laser oscillator 4 passes through the pentaprism 5
can be bent 90 degrees by The laser beam from the pentaprism 5 is divided into two by a compound prism 6, one of which is emitted to the outside as one of the line-symmetrical laser beams, that is, a counterclockwise laser beam CCW, and the other is returned to the center of rotation after changing its height. The laser beam returned to the center of rotation is reflected by the right-angle mirror 7 as the other line-symmetrical beam, that is, the clockwise laser beam CW. This makes it possible to obtain a line-symmetric rotating laser beam.

[発明の効果] プリズム、ミラーでレーザー光を90度、180度な曲
げているが、プリズム、ミラーの中で2回反射させてい
るので曲げ方向のプリズム、ミラー取付誤差を相殺して
入射角を90度、180度にま曲げることができる。第
3図(ハ)にペンタプリズムにおいて取付誤差αを相殺
する態様を示す。また当然モータの軸振れも相殺するこ
とができる。
[Effects of the invention] The laser beam is bent by 90 degrees and 180 degrees by the prism and mirror, but since it is reflected twice in the prism and mirror, the angle of incidence is adjusted by canceling out the prism and mirror mounting errors in the bending direction. Can be bent 90 degrees or 180 degrees. FIG. 3(c) shows a mode of canceling out the mounting error α in the pentaprism. Naturally, the shaft vibration of the motor can also be offset.

[実施例] 以下、図面を参照して本発明の実施例につき説明する。[Example] Embodiments of the present invention will be described below with reference to the drawings.

側面視でほぼ口字状を呈する取付架台1を備えており、
該架台1の下方水平部1a上には鉛直軸を回転軸として
むらのない回転速度で回転するモータ2により回転され
る回転台3が設けられている。また架台1にはモータ2
の回転軸2a上にレーザー発振器4が取付けられている
It is equipped with a mounting frame 1 that has an almost mouth-like shape when viewed from the side.
A rotary table 3 is provided on the lower horizontal portion 1a of the pedestal 1 and is rotated by a motor 2 that rotates at an even rotational speed about a vertical axis. Also, the mount 1 has a motor 2.
A laser oscillator 4 is mounted on the rotating shaft 2a.

回転台3上には回転台3の中心にペンタプリズム5が設
置されており、さらに回転台3上にはペンタプリズム5
の光軸方向に複合プリズム6が設置されている。また取
付架台1(固定部)の上方水平部1bには直角ミラー7
がミラーの交差部nをモータの回転軸(レーザー光軸)
2aと直角にかつ交わるようにして取付けられている。
A pentaprism 5 is installed on the rotary table 3 at the center of the rotary table 3, and a pentaprism 5 is installed on the rotary table 3.
A composite prism 6 is installed in the optical axis direction. In addition, a right-angle mirror 7 is mounted on the upper horizontal part 1b of the mounting frame 1 (fixed part).
The intersection point n of the mirror is the rotation axis of the motor (laser optical axis)
It is attached so as to be perpendicular to and intersect with 2a.

第3図ないし第5図にペンタプリズム5、複合プリズム
6、及び直角ミラー7を示す。ペンタプリズム5は第3
図(イ)、(ロ)に示すように2面のなす角が45痕の
反射面りを持つものである。
A pentaprism 5, a compound prism 6, and a right-angle mirror 7 are shown in FIGS. 3 to 5. Pentaprism 5 is the third
As shown in Figures (a) and (b), the angle formed by the two surfaces has 45 reflective surfaces.

複合プリズム6は第4図(イ)、)(ロ)に示すように
2面のなす角が90度の反射面りを持ち、かつ1面がビ
ームスプリッタ−6aとなっている。
As shown in FIGS. 4(a) and 4(b), the composite prism 6 has two reflecting surfaces with an angle of 90 degrees, and one surface serves as a beam splitter 6a.

直角ミラー7は2面のなす角が90邸の反則面りを持つ
The right-angle mirror 7 has an angle of 90 angles between its two sides.

モータ2が回転することにより回転台3が矢印で示す時
計方向に回転し、それに伴いペンタプリズム5及び複合
プリズム6が所定の回転速痕でむらなく回転する。レー
ザー発振器4からのレーザー光はペンタプリズム5によ
って90麿曲げられる。ペンタプリズム5からのレーザ
ー光は複合プリズム6によって2分され、一方は線対象
ビーム光線の一方、すなわち反時計回りレーザー光線C
CWとして外側に出し、他方は高さを変えて回転中心に
戻す。回転中心に戻されたレーザー光は直角ミラー7に
にり線対象ビーム光線の他方、すなわち時計回りのレー
ザー光sicwとして反射される。これにより線対象な
回転レーザー光線を得ることができる。第2図において
mは線対象軸である。
As the motor 2 rotates, the rotary table 3 rotates in the clockwise direction indicated by the arrow, and accordingly, the pentaprism 5 and the composite prism 6 rotate evenly at a predetermined rotation speed. The laser beam from the laser oscillator 4 is bent by 90 degrees by the pentaprism 5. The laser beam from the pentaprism 5 is split into two by a compound prism 6, one of which is one of the symmetrical beams, i.e. the counterclockwise laser beam C.
Take it outside as CW, and change the height of the other one and return it to the center of rotation. The laser beam returned to the center of rotation is reflected by the right-angle mirror 7 as the other side of the diagonal target beam, that is, the clockwise laser beam sicw. This makes it possible to obtain a line-symmetric rotating laser beam. In FIG. 2, m is the line symmetry axis.

第6図ないし第8図に直角ミラ一部での反射によるレー
ザー光の反転(線対象軸に対して)状況を示す。第6図
においてミラーに対しレーザー光は451mの入射角を
持つ。第7図においてレーザー光は光路平面A、B、C
内を通る。A//B、A十〇、B土Cである。B平面内
で線対象軸mに角度θを持って入射したレーザー光はA
平面内でmに対して角度θを持つ。第8図においてミラ
ーを上部から見るとミラー光線n上の点を反射点とした
ごと(レーザー光は線対象に反射される。
FIGS. 6 to 8 show how the laser beam is reversed (with respect to the symmetrical axis) due to reflection on a part of the right-angled mirror. In FIG. 6, the laser beam has an incident angle of 451 m with respect to the mirror. In Figure 7, the laser beam is on optical path planes A, B, and C.
pass inside. A//B, A10, B Sat C. The laser beam incident on the line symmetry axis m at an angle θ in the B plane is A
It has an angle θ with respect to m in the plane. In FIG. 8, when the mirror is viewed from above, a point on the mirror beam n is taken as a reflection point (the laser beam is reflected line-symmetrically).

プリズム5.6、ミラー7でレーザー光は90度、18
0度に曲げているが、プリズム5.6、ミラー7の中で
2回反射されているので曲げ方向のプリズム、ミラー取
付誤差を相殺して入射角を90度、180度に曲げるこ
とができる。第3図(ハ)はペンタプリズム5において
取付誤差αを相殺する態様を示す。また当然モータ2の
軸振れも相殺することができる。
The laser beam is 90 degrees with prism 5.6 and mirror 7, 18
Although it is bent at 0 degrees, it is reflected twice in prism 5.6 and mirror 7, so the angle of incidence can be bent to 90 degrees and 180 degrees by canceling out the prism and mirror installation errors in the bending direction. . FIG. 3(C) shows a mode in which the installation error α is canceled out in the pentaprism 5. Naturally, the axial vibration of the motor 2 can also be offset.

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

図面は本発明の実施例を示し、第1図および第2図は線
対象回転レーザー光線を作る装置を示し、第1図は立面
図、第2図は平面図、第3図ないし第5図はペンタプリ
ズム、複合プリズム、直角ミラーを示し、第3図(イ)
はペンタプリズムの側面図、第3図(ロ)は正面図、第
3図(ハ)は取付誤差の相殺を示す側面図、第4図(イ
)は複合プリズムの側面図、第4図(ロ)は正面図、第
5図(イ)は直角ミラーの側面図、第5図(ロ)は正面
図、第6図ないし第8図は直角ミラ一部での反射による
レーザー光の反転を示し、第6図は側面図、第7図は鳥
観図、第8図は上面図である。 1・・・取付架台  2・・・モータ  3・・・回転
台 4・・・レーザー発振器  5・・・ペンタプリズ
ム  6・・・複合プリズム7・・・直角ミラー
The drawings show an embodiment of the invention, and FIGS. 1 and 2 show an apparatus for producing a line-symmetric rotating laser beam, FIG. 1 being an elevational view, FIG. 2 being a plan view, and FIGS. 3 to 5. Figure 3 (a) shows a pentaprism, a compound prism, and a right-angle mirror.
is a side view of the pentaprism, FIG. 3(B) is a front view, FIG. 3(C) is a side view showing cancellation of installation errors, FIG. Figure 5 (b) is a front view, Figure 5 (a) is a side view of the right-angle mirror, Figure 5 (b) is a front view, and Figures 6 to 8 show the inversion of the laser beam due to reflection on a part of the right-angle mirror. 6 is a side view, FIG. 7 is a bird's-eye view, and FIG. 8 is a top view. 1...Mounting frame 2...Motor 3...Rotary table 4...Laser oscillator 5...Penta prism 6...Complex prism 7...Right angle mirror

Claims (1)

【特許請求の範囲】[Claims] むらのない回転速度で回転するモータにより平面上で回
転させられる回転台の中心にペンタプリズムを設置し、
レーザー発振器をモータの回転軸上に設けて、該レーザ
ー発振器からのレーザー光をペンタプリズムによつて9
0度曲げ、回転台に、ペンタプリズムの光軸方向に複合
プリズムを設置し、該複合プリズムはビームスプリッタ
ー及び2個の直角反射面を持っており、ペンタプリズム
からのレーザー光を2分して一方は線対象レーザー光線
の一方として外側に出し、他方は高さを変えて回転中心
に戻し、固定部に直角ミラーを、ミラーの交差部をモー
タの回転軸と直角に、かつ交わるように設置し、複合プ
リズムで回転中心に戻されたレーザー光を線対象ビーム
光線の他方として反射させ、これにより線対象な回転レ
ーザー光線を得ることを特徴とするレーザーを用いた平
面位置検出装置において線対象回転レーザー光線を作る
装置。
A pentaprism is installed at the center of a rotating table that is rotated on a flat surface by a motor that rotates at an even speed.
A laser oscillator is installed on the rotating shaft of the motor, and the laser beam from the laser oscillator is transmitted through a pentaprism.
A compound prism is placed in the direction of the optical axis of the pentaprism on a rotating table with a 0 degree bend, and the compound prism has a beam splitter and two right-angled reflective surfaces, which splits the laser beam from the pentaprism into two. One side is sent out as one of the line-symmetric laser beams, and the other is returned to the center of rotation by changing the height. A right-angle mirror is installed on the fixed part so that the intersection of the mirrors is perpendicular to and intersects with the rotation axis of the motor. In a planar position detection device using a laser, the laser beam returned to the rotation center by a compound prism is reflected as the other side of the line-symmetric rotating laser beam, thereby obtaining a line-symmetric rotating laser beam. equipment for making.
JP19909686A 1986-08-27 1986-08-27 Device for generating line object rotary laser beam in plane position detecting device using laser Granted JPS6355481A (en)

Priority Applications (7)

Application Number Priority Date Filing Date Title
JP19909686A JPS6355481A (en) 1986-08-27 1986-08-27 Device for generating line object rotary laser beam in plane position detecting device using laser
US07/066,423 US4874238A (en) 1986-08-27 1987-06-25 Method and device for measurement with laser beam
GB8714988A GB2195852B (en) 1986-08-27 1987-06-26 Method and apparatus for obtaining surveying measurements using laser beam
DE8718134U DE8718134U1 (en) 1986-08-27 1987-07-07 Angle measuring device using a laser
DE19873722429 DE3722429A1 (en) 1986-08-27 1987-07-07 ANGLE MEASURING METHOD AND DEVICE USING A LASER
FR878709868A FR2603376B1 (en) 1986-08-27 1987-07-10 LASER BEAM MEASURING METHOD AND DEVICE, PARTICULARLY FOR DETERMINING THE COORDINATES OF A POINT
CH3301/87A CH676504A5 (en) 1986-08-27 1987-08-27

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19909686A JPS6355481A (en) 1986-08-27 1986-08-27 Device for generating line object rotary laser beam in plane position detecting device using laser

Publications (2)

Publication Number Publication Date
JPS6355481A true JPS6355481A (en) 1988-03-09
JPH0476634B2 JPH0476634B2 (en) 1992-12-04

Family

ID=16402052

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19909686A Granted JPS6355481A (en) 1986-08-27 1986-08-27 Device for generating line object rotary laser beam in plane position detecting device using laser

Country Status (1)

Country Link
JP (1) JPS6355481A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2016522201A (en) * 2013-05-23 2016-07-28 シンジェンタ パーティシペーションズ アーゲー Tank mix formulation

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2016522201A (en) * 2013-05-23 2016-07-28 シンジェンタ パーティシペーションズ アーゲー Tank mix formulation

Also Published As

Publication number Publication date
JPH0476634B2 (en) 1992-12-04

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