Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0785007B2 - Length measuring instrument - Google Patents
[go: Go Back, main page]

JPH0785007B2 - Length measuring instrument - Google Patents

Length measuring instrument

Info

Publication number
JPH0785007B2
JPH0785007B2 JP63041219A JP4121988A JPH0785007B2 JP H0785007 B2 JPH0785007 B2 JP H0785007B2 JP 63041219 A JP63041219 A JP 63041219A JP 4121988 A JP4121988 A JP 4121988A JP H0785007 B2 JPH0785007 B2 JP H0785007B2
Authority
JP
Japan
Prior art keywords
phase difference
phase
length measuring
photodetector
light
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
JP63041219A
Other languages
Japanese (ja)
Other versions
JPH01216202A (en
Inventor
敏嗣 植田
正博 渡
克巳 磯崎
康弘 坂巻
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Electric 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 Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP63041219A priority Critical patent/JPH0785007B2/en
Publication of JPH01216202A publication Critical patent/JPH01216202A/en
Publication of JPH0785007B2 publication Critical patent/JPH0785007B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Instruments For Measurement Of Length By Optical Means (AREA)

Description

【発明の詳細な説明】 <産業上の利用分野> 本発明はレーザ光の干渉を利用して,波長を単位とした
高精度,高分解能の測長を行うことが出来るとともに,
アブソリュートな測長出力を得ることの出来る波長器に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention makes it possible to perform length measurement with high accuracy and high resolution in units of wavelength by utilizing interference of laser light.
The present invention relates to a wavelength device that can obtain an absolute measurement output.

<従来の技術> はじめに本発明を適用するアブソリュートな測長器の一
例として,本出願人が先に提案した特願昭60−277380に
ついて第4図を用いて簡単に説明する。この提案はマイ
ケルソンの干渉光学系を利用した波長器において,2つ以
上の波長の異なる光を切り換えて,測定対象までの距離
に応じた光の位相遅れ量を順次測定すると共に,これら
の波長と位相遅れ量との関係から測定対象までの距離を
求めるようにしたものである。図において1は波長の異
なる複数のコヒーレントな光(λ〜λ)を選択的に
発生するレーザ光源,HMRはハーフミラー,PD1はフォトデ
イテクタ,CC1,CC2はキューブコーナである。キューブコ
ーナCC1は波長動作に応じて移動する波長側のキューブ
コーナ,キューブコーナCC2は一定の距離に固定された
基準側のキューブコーナである。AOMは光の位相遅れ量
をヘテロダイン検出するために基準測の光を変調する音
響光学変調器(以下,AO変調器という),6はAO変調器を
一定周波数fbで駆動する変調信号源,4はフォトディテク
タPD1の出力に含まれる位相遅れ量を検出する位相検出
器である。このように構成された測長器は,レーザのマ
イケルソン干渉を利用したものである。
<Prior Art> First, as an example of an absolute length measuring instrument to which the present invention is applied, Japanese Patent Application No. 60-277380 previously proposed by the present applicant will be briefly described with reference to FIG. In this proposal, a wavelength device using Michelson's interference optical system switches two or more lights with different wavelengths and sequentially measures the phase delay of the light according to the distance to the measurement target. The distance to the measurement target is obtained from the relationship between the phase delay amount and the phase delay amount. In the figure, 1 is a laser light source that selectively generates a plurality of coherent light beams (λ 1 to λ 4 ) having different wavelengths, HMR is a half mirror, PD1 is a photodetector, and CC1 and CC2 are cube corners. Cube corner CC1 is a cube corner on the wavelength side that moves according to wavelength operation, and cube corner CC2 is a cube corner on the reference side that is fixed at a fixed distance. AOM is an acousto-optic modulator (hereinafter referred to as AO modulator) that modulates the reference measurement light to detect the amount of optical phase delay, 6 is a modulation signal source that drives the AO modulator at a constant frequency fb, 4 Is a phase detector that detects the amount of phase delay included in the output of the photodetector PD1. The length measuring device configured in this way utilizes Michelson interference of a laser.

レーザ光源1は例えば一定波長の光源とその波長を任意
の量だけシフトさせる波長シフタ(図示せず)により構
成され,任意の波長の光を順次発生する。演算回路5は
測定に使用された光の波長とそのときの位相遅れ量との
関係から,キューブコーナCC1間での距離を求めるもの
である。
The laser light source 1 is composed of, for example, a light source having a constant wavelength and a wavelength shifter (not shown) that shifts the wavelength by an arbitrary amount, and sequentially generates light having an arbitrary wavelength. The arithmetic circuit 5 determines the distance between the cube corners CC1 from the relationship between the wavelength of the light used for measurement and the amount of phase delay at that time.

このように構成された測長器において,光の角周波数を
ω,AO変調器AOMにおける変調角周波数をωb(=2πf
b)とし,レーザ光源1から出射される光の振幅Voを Vo=sinωt (1) とすると,AO変調器AOM1により変調された光の振幅V1は V1=sin(ωt+ωb)t (2) キューブコーナCC1を介して戻って来た光の振幅V2は V2=sin(ωt+φ) (3) となる。なお,φは基準側および測長側の各光路におけ
る光路長の差に対応して発生する位相遅れ量である。
In the length measuring device configured in this way, the angular frequency of light is ω, and the modulation angular frequency of the AO modulator AOM is ωb (= 2πf
b) and the amplitude Vo of the light emitted from the laser light source 1 is Vo = sinωt (1), the amplitude V1 of the light modulated by the AO modulator AOM1 is V1 = sin (ωt + ωb) t (2) Cube corner The amplitude V2 of the light returning via CC1 is V2 = sin (ωt + φ) (3). Note that φ is a phase delay amount that occurs corresponding to the difference in optical path length between the reference side optical path and the length measuring side optical path.

フォトディテクタPD1上では,上記の(2),(3)式
に示されるような2つの光のが重畳されるので,入射す
る光の振幅は V1+V2=sin(ω+ωb)t+sin(ωt+φ) =2sin(ω+ωbt/2+φ)cos{(ωbt −φ)/2} (4) のように,V1,V2の和となる。ここで,フォトディテクタ
PD1の出力は入射する光の振幅の2乗に比例するので,
理論的には (V1+V2) =4sin{(ω+ωb/2)t+φ}・cos{(ωbt −φ)/2} (5) となるが,フォトディテクタPD1は光の周波数には応答
出来ず,平均値を示すようになるので,その出力Vpは Vp=2+2cos(ωbt−φ) (6) となる。
On the photodetector PD1, the two lights as shown in the above equations (2) and (3) are superposed, so that the amplitude of the incident light is V1 + V2 = sin (ω + ωb) t + sin (ωt + φ) = 2sin (ω + ωbt / 2 + φ) cos {(ωbt −φ) / 2} (4) is the sum of V1 and V2. Where the photo detector
Since the output of PD1 is proportional to the square of the amplitude of the incident light,
Theoretically, (V1 + V2) 2 = 4sin {(ω + ωb / 2) t + φ} ・ cos {(ωbt −φ) / 2} (5), but the photodetector PD1 cannot respond to the optical frequency and the average value is The output Vp is Vp = 2 + 2cos (ωbt−φ) (6).

したがって,AO変調器AOM1における変調角周波数ωbが
わかっていれば,フォトディテクタPD1の出力Vpの値か
ら位相遅れ量を算出することが出来る。
Therefore, if the modulation angular frequency ωb in the AO modulator AOM1 is known, the phase delay amount can be calculated from the value of the output Vp of the photodetector PD1.

同様にこの位相遅れ量を異った波長に対応して順次測定
し,これらの測定結果を連立方程式として解くことによ
り測定対象までの距離を求めることができる。
Similarly, the distance to the measurement target can be obtained by sequentially measuring the amount of phase delay corresponding to different wavelengths and solving these measurement results as simultaneous equations.

<発明が解決しようとする問題点> ところで,上記のような測長器においては波長器の外部
環境(例えば,温度や振動など)が変化すると合成され
たレーザの位相差分布に傾きが生じ,フォトディテクタ
PD1の出力が変化する。その結果,基準としてのAO変調
器AOM1からの信号の位相との差に誤差が発生する。
<Problems to be Solved by the Invention> By the way, in the above-described length measuring instrument, when the external environment (for example, temperature or vibration) of the wavelength instrument changes, the phase difference distribution of the synthesized laser is inclined, Photo detector
PD1 output changes. As a result, an error occurs in the difference from the phase of the signal from the AO modulator AOM1 as the reference.

第5図(イ),(ロ),(ハ)は,基準としてAOM1のド
ライブ信号の位相A(これは電気信号が直接位相差検出
器に入力されるので空間的な位相分布は持たない)とフ
ォトディテクタPD1に入射する光の位相差の傾きBおよ
びAとBの位相差Cの関係を示す模式図である。図にお
いて, (イ)は測長距離が零で,かつ,前記Bの位相に傾きが
ない状態を示している。この場合,Cに示すそれぞれの波
長a,bの位相差は零(a,bが重畳している)である。
5 (a), (b), and (c) show the phase A of the drive signal of AOM1 as a reference (this has no spatial phase distribution because the electric signal is directly input to the phase difference detector). 3A and 3B are schematic diagrams showing the relationship between the slope B of the phase difference of the light incident on the photodetector PD1 and the phase difference C of A and B. In the figure, (a) shows a state in which the measurement distance is zero and the phase of B is not inclined. In this case, the phase difference between the wavelengths a and b shown in C is zero (a and b are superposed).

(ロ)は測長側のキューブコーナCC1を任意の距離だけ
移動させた時の状態を示すもので,CC1側に前記ずれや空
気の揺ぎがまったく発生しなかった場合であり,測長距
離に相当する位相差φを検出することが出来る。
(B) shows the condition when the cube corner CC1 on the length measuring side is moved by an arbitrary distance, and it shows the case where the above-mentioned displacement or air sway did not occur on the CC1 side. The phase difference φ corresponding to can be detected.

(ハ)は空気の揺ぎなどによりPD1に入射する合成波の
位相差に傾きθが発生した場合であり,この傾きにより
位相差の回転中心がずれてPD1の出力がΔφの分だけ変
化し,本来φであるべき位相差がφとなる。この様な
空気の揺ぎ等による位相差の傾きは測定値の誤差となる
という問題があった。
(C) is the case where the phase difference of the composite wave incident on PD1 has a slope θ due to air turbulence, etc. This slope causes the center of rotation of the phase difference to shift, and the output of PD1 changes by Δφ. , The phase difference that should be φ is φ 1 . There is a problem in that the inclination of the phase difference due to such air fluctuations causes an error in the measured value.

本発明は上記従来技術の問題点に鑑みて成されたもの
で,演算装置に位相差の傾きと測長誤差の関係から補正
値を算出するテーブルを設けておき,複数個のフォトデ
ィテクタの出力から位相差の傾きを演算し,補正するこ
とにより正確な測定を行うことを目的とする。
The present invention has been made in view of the above-mentioned problems of the prior art, and a table for calculating a correction value from the relationship between the inclination of the phase difference and the measurement error is provided in the arithmetic device, and the output of a plurality of photodetectors is used. The purpose is to perform accurate measurement by calculating and correcting the slope of the phase difference.

<問題点を解決するための手段> 上記問題点を解決するための本発明の構成は,少なくと
も2つ以上の波長の異なるレーザ光を切り換えて,測定
対象までの距離に応じた光の位相遅れ量をフォトディテ
クタおよび位相差検出装置を用いて順次測定すると共
に,これらの波長と位相遅れ量との関係から前期測定対
象までの距離を演算装置を用いて求めるようにしたマイ
ケルソンの干渉光学系を用いた測長器において,前記フ
ォトディテクタはその受光面を複数個に分割するととも
に,前記位相差検出装置は前記複数のフォトディテクタ
の出力信号に基づいて前記フォトディテクタに入射する
前記レーザ光の位相差分布の傾きを検出し,前記演算器
は前記位相差分布の傾きに応じて波長値を補正するよう
に構成したことを特徴とするものである。
<Means for Solving the Problems> The configuration of the present invention for solving the above problems is such that at least two or more laser lights having different wavelengths are switched and the phase delay of the light according to the distance to the object to be measured. The Michelson interference optics system is used to measure the quantity sequentially using a photodetector and a phase difference detector, and to calculate the distance to the measurement target in the previous period from the relationship between these wavelengths and the amount of phase delay using an arithmetic unit. In the length measuring instrument used, the photodetector divides its light-receiving surface into a plurality of light receiving surfaces, and the phase difference detector detects the phase difference distribution of the laser light incident on the photodetector based on the output signals of the plurality of photodetectors. It is characterized in that the calculator detects the inclination and corrects the wavelength value according to the inclination of the phase difference distribution.

<実施例> 第1図は本発明の測長器の一実施例を示す構成図であ
る。第1図において第4図と同様のものには同様の符号
を付して説明は省略するが,本発明においては演算装置
51には例えば第2図に示すような位相差分布の傾きと位
相ドリフトの関係から補正値を算出するテーブルがあら
かじめ設けられている。また,フォトディテクタPD1の
形状を図に示すようにE,F,G,Hの4つに分割して独立し
たものとし,それぞれを対向して配置する。
<Embodiment> FIG. 1 is a block diagram showing an embodiment of the length measuring device of the present invention. In FIG. 1, the same components as those in FIG. 4 are designated by the same reference numerals and the description thereof will be omitted.
In 51, for example, a table for calculating a correction value from the relationship between the slope of the phase difference distribution and the phase drift as shown in FIG. 2 is provided in advance. Further, as shown in the figure, the shape of the photodetector PD1 is divided into four E, F, G, and H to be independent, and they are arranged facing each other.

上記構成において,それぞれのフォトディテクタ(E〜
H)の信号は位相差検出装置41に出力され,その出力の
総和が演算されるとともにそれらの信号から例えばE−
F,G−Hの演算を行い,位相差の傾きψ1を演算す
る。
In the above configuration, each photo detector (E to
The signal H) is output to the phase difference detection device 41, the sum of the outputs is calculated, and from these signals, for example, E-
The F, G-H calculations are performed to calculate the slopes ψ 1 , ψ 2 of the phase difference.

これらの演算結果は演算装置51に送出され,前記総和の
信号とAOM1からの信号に基づいて測長すべき距離を演算
するが,その前にフォトディテクタ(E〜H)を用いて
演算された位相差の傾きψ1から前記補正テーブル
を用いて前記総和の信号の補正を行う。
These calculation results are sent to the calculation device 51, and the distance to be measured is calculated based on the signal of the sum and the signal from AOM1, but before that, the distance calculated using the photo detectors (E to H) is calculated. The signal of the total sum is corrected from the inclinations ψ 1 and ψ 2 of the phase difference using the correction table.

なお,本実施例においては4分割したフォトディテクタ
を1個用いた例について説明したが,例えば本出願人が
特願昭62−184270としてすでに出願している第3図に示
すような構成の測長器にも適用することが出来る。この
ような構成によれば2つのレーザから出射した波長の異
なる光をCC1,CC2を互いに逆向きに通過するようにして
一方の信号の位相差信号を基準側(例えばPD1),他方
の位相差信号を測長側(PD2)で受光し,それらの位相
差信号の位相差から距離を求めるようにしたものである
が,この様な場合も空気の揺ぎなどによるドリフトはま
ぬがれない。
In the present embodiment, an example in which one photodetector divided into four parts is used has been described. For example, the length measurement having the configuration shown in FIG. 3 which the applicant of the present invention has already filed as Japanese Patent Application No. 62-184270. It can also be applied to vessels. According to such a configuration, the light having different wavelengths emitted from the two lasers passes through CC1 and CC2 in opposite directions, and the phase difference of one signal is applied to the reference side (for example, PD1) and the phase difference of the other. The signal is received on the length measurement side (PD2), and the distance is calculated from the phase difference of those phase difference signals, but in such a case, drift due to air sway, etc., cannot be avoided.

従ってこの様な場合も演算器の中に位相分布の傾きと位
相ドリフト量の補正テーブルを設けておき,それぞれの
フォトディテクタを複数個(図では4個)に分割し,そ
の4つの信号からPD1,PD2に入射する合成波の位相分布
の傾きを求め,その傾きの相対的な差に基づいて位相差
を補正することにより,誤差のない測長器を実現するこ
とができる。
Therefore, even in such a case, a correction table for the gradient of the phase distribution and the amount of phase drift is provided in the arithmetic unit, and each photodetector is divided into a plurality (four in the figure), and PD1, PD1, By obtaining the slope of the phase distribution of the composite wave incident on PD2 and compensating for the phase difference based on the relative difference in the slope, it is possible to realize a length-measuring device without error.

なお,測長器は上記実施例の構成のものに限ることなく
マイケルソンの干渉光学系を利用し,その合成波の位相
差をフォトディテクタで受光するものであれば本実施例
に示したもの以外にも適用可能である。
Note that the length measuring device is not limited to that of the above-described embodiment, and a Michelson interference optical system is used, and other than that shown in this embodiment as long as the photodetector receives the phase difference of the composite wave. It is also applicable to.

また,フォトディテクタは4分割した例を示したが原理
的には2分割でも良く,さらに6分割,8分割であっても
よい。そのような場合はより精度高く傾きを測定するこ
とが出来る。
Further, the photodetector is divided into four, but in principle it may be divided into two, and may be divided into six and eight. In such a case, the inclination can be measured with higher accuracy.

<発明の効果> 以上,実施例とともに具体的に説明したように本発明に
よれば,複数のフォトディテクタにより位相差分布の傾
きの求め,あらかじめ求めて置いた位相差分布の傾きと
ドリフト量の関係から測長値を補正するようにしたので
温度や振動による出力ドリフトを補正した測長器を実現
することが出来る。
<Effects of the Invention> According to the present invention as specifically described above with reference to the embodiments, the inclination of the phase difference distribution is obtained by a plurality of photodetectors, and the relationship between the inclination of the phase difference distribution and the drift amount obtained in advance is obtained. Since the length measurement value is corrected according to, it is possible to realize a length measuring device in which output drift due to temperature and vibration is corrected.

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

第1図は本発明の測長器の一実施例を示す構成図,第2
図は位相差分布の傾きとドリフト量の関係を示す図,第
3図は本発明を他の測長器に適用した例を示す構成図,
第4図は従来例を示す図,第5図は波面の傾きとドリフ
トの関係を説明する為の模式図である。 1,2……レーザ光源,41……位相差検出装置,51……演算
装置,AOM……音響光学変調器,CC1,CC2……キューブコー
ナ,HMR……ハーフミラー,PD1,PD2……フォトディテク
タ。
FIG. 1 is a block diagram showing an embodiment of the length measuring device of the present invention, and FIG.
FIG. 3 is a diagram showing the relationship between the slope of the phase difference distribution and the amount of drift, and FIG. 3 is a configuration diagram showing an example in which the present invention is applied to another length measuring device.
FIG. 4 is a diagram showing a conventional example, and FIG. 5 is a schematic diagram for explaining the relationship between the inclination of the wavefront and the drift. 1,2 …… Laser light source, 41 …… Phase difference detector, 51 …… Computer, AOM …… Acousto-optic modulator, CC1, CC2 …… Cube corner, HMR …… Half mirror, PD1, PD2 …… Photo detector .

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】少なくとも2つ以上の波長の異なるレーザ
光を切り換えて,測定対象までの距離に応じた光の位相
遅れ量をフォトディテクタおよび位相差検出装置を用い
て順次測定すると共に,これらの波長と位相遅れ量との
関係から前記測定対象までの距離を演算装置を用いて求
めるようにしたマイケルソンの干渉光学系を用いた測長
器において,前記フォトディテクタはその受光面を複数
個に分割するとともに,前記位相差検出装置は前記複数
のフォトディテクタの出力信号に基づいて前記フォトデ
ィテクタに入射する前記レーザ光の位相差分布の傾きを
検出し,前記演算器は前記位相差分布の傾きに応じて測
長値を補正するように構成したことを特徴とする測長
器。
1. At least two or more laser beams having different wavelengths are switched to sequentially measure a phase delay amount of light according to a distance to a measurement target by using a photodetector and a phase difference detection device, and these wavelengths are also measured. In the length measuring device using Michelson's interference optical system, the distance to the measurement object is calculated from the relationship between the phase delay amount and the phase delay amount, and the photodetector divides its light-receiving surface into a plurality of parts. At the same time, the phase difference detection device detects the slope of the phase difference distribution of the laser light incident on the photodetectors based on the output signals of the plurality of photodetectors, and the arithmetic unit measures the slope according to the slopes of the phase difference distribution. A length measuring instrument characterized by being configured to correct a long value.
JP63041219A 1988-02-24 1988-02-24 Length measuring instrument Expired - Lifetime JPH0785007B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63041219A JPH0785007B2 (en) 1988-02-24 1988-02-24 Length measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63041219A JPH0785007B2 (en) 1988-02-24 1988-02-24 Length measuring instrument

Publications (2)

Publication Number Publication Date
JPH01216202A JPH01216202A (en) 1989-08-30
JPH0785007B2 true JPH0785007B2 (en) 1995-09-13

Family

ID=12602282

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63041219A Expired - Lifetime JPH0785007B2 (en) 1988-02-24 1988-02-24 Length measuring instrument

Country Status (1)

Country Link
JP (1) JPH0785007B2 (en)

Also Published As

Publication number Publication date
JPH01216202A (en) 1989-08-30

Similar Documents

Publication Publication Date Title
EP0646767B1 (en) Interferometric distance measuring apparatus
US4776701A (en) Displacement measuring apparatus and method
EP0193742B1 (en) Wavelength scanning interferometry and interferometer employing laser diode
US5485274A (en) Fiber optic interferometer with wavelength-stabilized light source
US5146293A (en) Phase-stepping fiber-optic projected fringe system for surface topography measurements
JP2755757B2 (en) Measuring method of displacement and angle
EP0342016B1 (en) Optical position measurement
EP0199137B1 (en) Method of and apparatus for optically measuring displacement
GB2071905A (en) Angular velocity sensor based on a ring laser
JPH06174844A (en) Laser distance measuring apparatus
JPH0785007B2 (en) Length measuring instrument
JPS62135703A (en) End measuring machine
GB2178162A (en) Fibre optic gyroscope
JPH0214588A (en) Ring laser gyroscope
JPH06117810A (en) Absolute length measuring instrument with disturbance correction function
SU1215004A1 (en) Arrangement for measuring displacements
CN113899322B (en) System and method for measuring rotational displacement and angular velocity
JPH02189412A (en) Optical fiber gyroscope
JP2656624B2 (en) Interferometer tilt control method
JPH0575241B2 (en)
JPH0695003B2 (en) Length measuring instrument
JPH0695004B2 (en) Three-dimensional shape measuring device
JPH064247Y2 (en) Moving distance measuring device
SU1186942A1 (en) Arrangement for contactless measurement of polished surface profile
SU1730533A1 (en) Device for measuring angular position of an object