JPS581125A - Spatial filter device - Google Patents

Spatial filter device

Info

Publication number
JPS581125A
JPS581125A JP9921781A JP9921781A JPS581125A JP S581125 A JPS581125 A JP S581125A JP 9921781 A JP9921781 A JP 9921781A JP 9921781 A JP9921781 A JP 9921781A JP S581125 A JPS581125 A JP S581125A
Authority
JP
Japan
Prior art keywords
filter device
spatial filter
optical
optical fibers
photodetection
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
JP9921781A
Other languages
Japanese (ja)
Inventor
Masakatsu Kurita
正勝 栗田
Naotake Nagao
長尾 尚武
Koji Morishita
森下 耕次
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.)
Omron Corp
Original Assignee
Tateisi Electronics Co
Omron Tateisi Electronics Co
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 Tateisi Electronics Co, Omron Tateisi Electronics Co filed Critical Tateisi Electronics Co
Priority to JP9921781A priority Critical patent/JPS581125A/en
Publication of JPS581125A publication Critical patent/JPS581125A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • G02B27/42Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect
    • G02B27/46Systems using spatial filters

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To permit a differential spatial filter device of simple structure, which measures a velocity, etc., by using the optical irregularity of a body to be measured, to perform stable velocity measurement without any restriction even under strong electromagnetic induction, in a liquid, and in an explosive atmosphere, by arraying the photodetection ends of optical fibers in a line, and leading alternate optical fibers to two photodetectors. CONSTITUTION:The photodetection ends 14 of optical fibers 19 are arrayed in a line and alternate fibers are put together as a fiber bundle 16 and a fiber bundle 17. Incident light from a moving body is guided from alternate photodetection ends 14 through the fiber bundles 16 and 17 and added together by a photodetector, respectively. Therefore, this spatial filter device is utilized for the measurement of the velocity of the moving body, etc. Since this filter device has the simple and durable constitution and also handles light signals, so there is no influence of electromagnetically induced noise and the stable velocity measurement is carried out even under strong electromagnetic induction, in a liquid, and in an explosive atmosphere.

Description

【発明の詳細な説明】 本発明に、被測定物の光学的むらを用いて遮1などを測
定する差動!空間フィルタ装置K11lするものである
DETAILED DESCRIPTION OF THE INVENTION In the present invention, there is a differential method that uses optical unevenness of the object to be measured to measure occlusions, etc.! This is a spatial filter device K11l.

従来の空間フィルタ装置1は11111に示すような櫛
状の受光素子11!Fiを用いて構成されている。
A conventional spatial filter device 1 includes a comb-shaped light receiving element 11 as shown in 11111! It is configured using Fi.

光学系により移動物体から放射1反射あるいは透過した
光によるtIIをこの受光素子1群の受光面に結ぶとと
Kよシ、移動物体が有している光学的むら0周波数(空
関周#1黴という)分有のうちある特電の空間周波数の
みが選択されて、出力端子2.sよシ信号を出力する。
When the optical system connects the tII of the light reflected or transmitted from the moving object to the light-receiving surface of the first group of light-receiving elements, the optical unevenness of the moving object becomes Only a certain special electric spatial frequency is selected from among the distributions (referred to as mold), and the output terminal 2. Outputs the s and shi signals.

これに対し、−の空間周波数成分は受光面上で中ヤンセ
ルされて、物体の移動に対して信号として出力されない
On the other hand, the negative spatial frequency component is canceled on the light receiving surface and is not output as a signal in response to the movement of the object.

さて、ここで選択された空間周波数を持つ像が受光面上
で機の崗きKli直の1崗に移動するとき、櫛のlビ、
チ(受光素子lO:本分)O移11に対し、出力端子2
.1にあられれる償号扛それぞれ1周期変化する。この
2つの出力を差動増幅するととによって光源O変動やS
動物体0[視的な明fO変化など直流的な変動によるノ
イズに無−係に信号をと〕出すことができる。
Now, when the image with the spatial frequency selected here moves to one point on the light-receiving surface, the comb's l bi,
Output terminal 2 for 11 (light receiving element lO: main purpose)
.. Each of the redemption names that appear in 1 changes by one period. When these two outputs are differentially amplified, light source O fluctuations and S
It is possible to output a signal regardless of the noise caused by direct current fluctuations such as changes in visual brightness of the moving object.

物体011動aft計鋼するs合に#1llN21AK
示すように構成する11波黴検知−6が差動増5aso
出力信号の中心周波数を検知するように′なっテ1/)
る・前述のようKs11Il物体90@0空閾フィルタ
装置4C)1ビ、チ*11hK対し出力信号F118M
変化するので、IIO移動移動色度力信号の中心周波数
O関に#i比例鞠係が成立し、物体9の速度をV、光学
系80倍率を1.空間フィルタのピッチをP・出力信号
の中心周液数をfとすると、 Vニー・Pf となる。
#1llN21AK when measuring object 011
The 11-wave mold detection-6 configured as shown is a differential increaser 5aso
Detect the center frequency of the output signal (1/)
-As mentioned above, Ks11Il object 90@0 empty threshold filter device 4C) Output signal F118M for 1 bit, chi*11hK
Therefore, the #i proportional relationship is established in the center frequency O of the IIO moving chromatic power signal, and the velocity of the object 9 is V and the magnification of the optical system 80 is 1. Assuming that the pitch of the spatial filter is P and the frequency around the center of the output signal is f, then V knee Pf is obtained.

Pと腫は定数であるから中心馬皺黴fK対し簡単な乗算
で物体O遮縦Vを演算回路マて求めることがてきる。
Since P and tumor are constants, the object O occlusion V can be determined by a simple multiplication of the center wrinkle fK using an arithmetic circuit.

を友、空間フィルタ装置の別の形■として第1図のよう
に鋸状O位@格子10によってフィルタ作用をさせるも
のが知られて−る。移動物体からの光18は位相格子l
Kよって2方向の光束11FK分離され、レンズ11に
よって2つの光束群蝶、意つO光検出−12に受光され
る。
Another type of spatial filter device is known, as shown in FIG. The light 18 from the moving object passes through the phase grating l
The light beams 11FK are separated in two directions by the light beam K, and are received by the lens 11 into two groups of light beams, ie, the O light detection -12.

この形の空間フィルタもSS物体の光を櫛状に1つおき
に分離加算するため、前述の受光素子群のように2りO
光検出lit 20出力を差動増幅することでjail
!を検出することができる。
This type of spatial filter also separates and adds the light from the SS object every other object in a comb-like manner, so like the light receiving element group mentioned above, there are two
Jail by differentially amplifying the light detection lit 20 outputs
! can be detected.

ところが受光素子群による空間フィルタ#tW/lては
、大蓋モータの近くでの連#−足をする揚台Oような強
電磁誘導下では、空間フィルタ装置の各出力中増@器出
力に電磁ノイズが乗)ヤすく、中心周波数fの検出が困
IlKなる仁と中、液体中、爆発性雰囲気中など本来電
気を使用するに不便である場所ての速fil定4困−で
ある。
However, the spatial filter #tW/l using a group of light-receiving elements is under strong electromagnetic induction, such as a lifting platform near a large lid motor, where each output of the spatial filter device is affected by the multiplier output. It is difficult to determine the center frequency f in places where it is inconvenient to use electricity, such as inside liquids, explosive atmospheres, etc., where it is difficult to detect the center frequency f due to electromagnetic noise.

また、位相格子による光束分−による空間フィル/装置
は、光検出器の位置に光学ファイバをIIILル付ける
仁とKよって上記のtiiieiさは緩和されるが、位
相格子、レンズ系、光学ファイバで構成する光学系が被
雑になる欠点がある。
In addition, the spatial filling/device using a phase grating for light flux can alleviate the above problem by attaching an optical fiber to the photodetector position, but the phase grating, lens system, and optical fiber can alleviate the above problem. This has the disadvantage that the optical system that constitutes it is complicated.

この発明は、強電磁誘導下や液体中、爆発性雰囲気中に
おいても全く制約なしに簡単な構造て安定に連f管計掬
することのてきる空間フィルタ装置を提供する仁とを目
的としている。
The object of the present invention is to provide a spatial filter device that has a simple structure and is capable of stably collecting continuous f-tubes without any restrictions, even under strong electromagnetic induction, in liquids, and in explosive atmospheres. .

以下、本@@〇一実施例について図面を参黒し1kから
説明する。第4図は一実施例O外観斜視図、第611t
j分解斜視図である。これら0図に示すように、多数O
光学ファイバ1−がガイPli20.21OVIIIで
tjさまれることKよって、各光学ファイバ19の受光
端が一列に整列されている。そして光学ファイバ19t
j1本おきにファイバ束16とファイ/ぐ東17とKま
とめられ、これらファイバ東1g、170端lIは光検
出WI1gに導かれる。具体的KulイP歇101!1
で光学7フイパ1@tはさんだamこのように構成した
空間フィルタ装置に第611に示すように%移動物体か
ら款射、jj射あるいは透過し友党28を入射させると
、入射:tU克学ファイバ受光端14の1)$Pきにフ
ァイバ束111.17によって導かれ、光検出器18で
加算される。したがって111wJ及び難8園の空87
4ルタ装置と岡Isの作用をし、移動物体O遵度針欄な
どに用いることができゐ・ 第7図社、%に回転体の回転速i[測定用として構成し
た空間フィルタ装置26で、ガイr板・20.21の半
円状Oe!J*に沿って光学7アイパ受光端14を配列
することによって、光学7フイi受光端14を円弧状に
整列させたものである〇 この空間フィルタ装@28Ujll!8図のようにモー
タ24の軸26の周fiK光学ファイバ受光端を配する
ことができるため、軸26などO回転体の速f掬定に適
している。第6図に示すようにファイバ束16.17に
よシ光が達<Kmて導かれるので、光検出器18をモー
タ24かも離れた位置に置くことができる。この光検出
器18の出力は差動増幅器22で差動増幅された優、周
波数検出e!x21に送られ出力信40中心周腋数が検
知され、演算処11回路28によ)回転速度に換算され
て、図示しないモータ制御回路に送られる・ この第8図に示すように1モータ24から電磁ノイズs
2が発生したとしても、光検出器18以降の電気信号系
を遠くに離しておけば、こO電離ノイズ82Fi光学フ
ィルタに’f1人することがないので、電磁ノイズ82
に全く影響されずに回転遍度鋼足を行なうことができる
Hereinafter, embodiments of the present invention will be described starting from 1k with reference to the drawings. FIG. 4 is an external perspective view of one embodiment O, No. 611t
j is an exploded perspective view. As shown in these 0 diagrams, many O
Since the optical fibers 1- are sandwiched by the guides Pli20, 21OVIII, the light receiving ends of each optical fiber 19 are aligned in a line. And optical fiber 19t
Every other fiber bundle 16 and optical fibers 17 and 17 are put together, and these fibers 1g and 170 end lI are guided to a photodetector WI1g. Specific Kul-i P-101!1
When the optical 7 filter 1 @ t is sandwiched in the spatial filter device constructed in this way and the friend 28 is incident on it from a moving object as shown in No. 611, the incident: tUkatsugaku 1) $P of the fiber light receiving end 14 is guided by the fiber bundle 111.17 and added by the photodetector 18. Therefore, 111wJ and Nan8en no Sora 87
4 router device and Oka Is, and can be used for moving objects O compliance needle column, etc. , Guy r plate 20.21 semicircular Oe! By arranging the optical 7-eye receiving ends 14 along J*, the optical 7-eye receiving ends 14 are arranged in an arc shape.〇This spatial filter device @28Ujll! Since the receiving end of the fiK optical fiber can be disposed around the shaft 26 of the motor 24 as shown in FIG. 8, it is suitable for scooping the speed f of an O-rotating body such as the shaft 26. As shown in FIG. 6, since the light reaches the fiber bundle 16, 17 and is guided at a distance of <Km, the photodetector 18 can be placed at a distance from the motor 24 as well. The output of this photodetector 18 is differentially amplified by a differential amplifier 22 and frequency detection e! The output signal 40 is sent to x21, and the center circumference number is detected, converted to rotational speed by the arithmetic processing circuit 28), and sent to the motor control circuit (not shown).As shown in FIG. Electromagnetic noise from
Even if 2 occurs, if the electrical signal system after the photodetector 18 is kept far away, there will be no ionization noise 82Fi optical filter, so electromagnetic noise 82
It is possible to perform rotational uniformity steel legs without being affected at all.

9上夾m例について説明したように1本発明によれば、
きわめて簡単でかつ畷牟な構成て空間フィルタIi*を
実現できるとともに、この空間フィルタ装置は電気信号
でなく光信号を扱うものであるから電1lIII導ノイ
ズに影響されず、強電磁114下、液体中、爆発性雰囲
気中でも安定した追腹、胞転遍縦の計−が可能である。
According to the present invention, as explained in the above 9 cases,
Spatial filter Ii* can be realized with an extremely simple and simple configuration, and since this spatial filter device handles optical signals rather than electrical signals, it is not affected by electrical conduction noise, and it is not affected by electromagnetic noise. Even in medium and explosive atmospheres, it is possible to perform stable retaliation and vertical rotation.

ζ SUO簡単′&説明 第1mlは従来例の千m1lli、第2図は従来の光学
フィルタを用いた速度計書を11−する7口。
ζ SUO Simple & Explanation The 1st ml is a conventional example of 1,000ml, and the 2nd figure is a 7-port 11-liter speedometer using a conventional optical filter.

り動、I18図#i働の従来例の斜視図、jlI4図は
本発明〇−実施飼O外m斜視図、亀す図社同夷1/1A
f4の分解斜視図、亀・図は岡実層側を用い九遭腹計橢
會説明するためのプロ、り図、97図は他O実論例の外
観斜視図、第8鈎は第7図の実施例管用いた1転達度一
定を脱−する7口。
Fig. I18 is a perspective view of a conventional example of operation, jlI4 is a perspective view of the present invention 〇-implemented feeding outside m, Kamesuzusha Doi 1/1A
An exploded perspective view of f4, the tortoise diagram is a professional diagram for explaining the nine-sea plan using the Oka real layer side, Figure 97 is an external perspective view of the other O example, and the 8th hook is the 7th hook. The example shown in the figure shows a 7-hole system that uses a tube with a constant degree of transfer.

り図である。This is a diagram.

1・・・受光素子、4.26・・・空間フィルタ装置、
9・−・移動物体、    10・・・位相格子、12
.18・・・光検出器、 14・−・光学ファイバ受光端、  16・・・*m。
1... Light receiving element, 4.26... Spatial filter device,
9... Moving object, 10... Phase grating, 12
.. 18...Photodetector, 14...Optical fiber light receiving end, 16...*m.

16.17・・・ファイバ束、19・・・光学ファイバ
、20 、21−・・ガイ+7,1m。
16.17...Fiber bundle, 19...Optical fiber, 20, 21-...Guy +7.1m.

出願人 立石電橡株式会社 箋5(支) 筈〃遡 3 )$−7目 ′IP9自 ノνApplicant: Tateishi Electric Co., Ltd. Note 5 (branch) Should be back 3 )$-7th 'IP9 self No ν

Claims (1)

【特許請求の範囲】 (I)  受光−を−列に整列した複数の光学ファイバ
【一本おきに2つの光検出器に導びいた構造を有するこ
と1*像とする空間フィルタ装置。 (2)を枚のIイド鈑で複数の光学ファイバをはさむと
とKよって、光学7アイパを整列したことを特徴とする
特許請求の範−纏1項記載の空間フィルタ装置。   
[Scope of Claims] (I) A spatial filter device that receives light from a plurality of optical fibers arranged in a row and has a structure in which every other fiber is guided to two photodetectors. 2. A spatial filter device according to claim 1, characterized in that seven optical eyers are aligned by sandwiching a plurality of optical fibers between two I-id plates.
JP9921781A 1981-06-26 1981-06-26 Spatial filter device Pending JPS581125A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9921781A JPS581125A (en) 1981-06-26 1981-06-26 Spatial filter device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9921781A JPS581125A (en) 1981-06-26 1981-06-26 Spatial filter device

Publications (1)

Publication Number Publication Date
JPS581125A true JPS581125A (en) 1983-01-06

Family

ID=14241487

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9921781A Pending JPS581125A (en) 1981-06-26 1981-06-26 Spatial filter device

Country Status (1)

Country Link
JP (1) JPS581125A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59176914U (en) * 1983-05-12 1984-11-27 電機計測株式会社 signal detector
JPS6023833U (en) * 1983-07-26 1985-02-18 株式会社島津製作所 spatial filter
US4653849A (en) * 1983-05-31 1987-03-31 Compagnie Industrielle Des Telecommunications Cit-Alcatel Optical space-division switching assembly
FR2824913A1 (en) * 2001-05-15 2002-11-22 Hamou Cyril Ben Optical velocity meter has a measurement head with a multiplicity of fiber optic cables for creating a light pattern of the surface of a moving object with electronics for carrying out spectral analysis of the reflected signal

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59176914U (en) * 1983-05-12 1984-11-27 電機計測株式会社 signal detector
US4653849A (en) * 1983-05-31 1987-03-31 Compagnie Industrielle Des Telecommunications Cit-Alcatel Optical space-division switching assembly
JPS6023833U (en) * 1983-07-26 1985-02-18 株式会社島津製作所 spatial filter
FR2824913A1 (en) * 2001-05-15 2002-11-22 Hamou Cyril Ben Optical velocity meter has a measurement head with a multiplicity of fiber optic cables for creating a light pattern of the surface of a moving object with electronics for carrying out spectral analysis of the reflected signal

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