JPS63236936A - Optical temperature measuring instrument - Google Patents

Optical temperature measuring instrument

Info

Publication number
JPS63236936A
JPS63236936A JP62070836A JP7083687A JPS63236936A JP S63236936 A JPS63236936 A JP S63236936A JP 62070836 A JP62070836 A JP 62070836A JP 7083687 A JP7083687 A JP 7083687A JP S63236936 A JPS63236936 A JP S63236936A
Authority
JP
Japan
Prior art keywords
temperature
light
interference film
image sensor
optical fiber
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
JP62070836A
Other languages
Japanese (ja)
Inventor
Isao Hishikari
功 菱刈
Toshihiko Ide
敏彦 井手
Mitsuo Ishige
石毛 光雄
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.)
Chino Corp
Original Assignee
Chino 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 Chino Corp filed Critical Chino Corp
Priority to JP62070836A priority Critical patent/JPS63236936A/en
Publication of JPS63236936A publication Critical patent/JPS63236936A/en
Pending legal-status Critical Current

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  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To perform stable temperature measurement with high sensitivity by using an interference film filter as a temperature sensing part and an image sensor for a photodetection part and measuring temperature from variation in the quantity of photodetection. CONSTITUTION:Light from a light source 1 is projected by an optical fiber 21 on the interference film filter 3 as the temperature sending part which varies in transmissivity or reflection factor with temperature and light from an optical fiber 22 is diffracted spectrally by a spectral means 4 such as a diffraction grating and photodetected by the image sensor 5 such as a CCD. The interference film filter 3 shifts in transmission wavelength characteristics to the long- wavelength side as the temperature rises, so the peak value wavelength and temperature are found previously. Further, picture elements of the sensor 5 and wavelength are made to correspond to each other and then the temperature is measured stably with high accuracy from the picture element position of the peak value or bottom value among respective picture element outputs without being affected by variation in the light quantity and the optical path.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、光ファイバを利用した光学式濃度測定装置
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to an optical concentration measuring device using an optical fiber.

[従来の技術] 従来、温度により透過率等が変化する半導体等を感温部
とし、これにファイバにより光を投光、受光し、検出器
の受光量の変化から温度を測定するものである。
[Prior art] Conventionally, a semiconductor or the like whose transmittance changes depending on temperature is used as a temperature sensing part, light is emitted to and received by a fiber, and the temperature is measured from the change in the amount of light received by a detector. .

〔この発明が解決しようとする問題点]しかしながら、
これらの方法では、光源の強度変化、光ファイバの曲げ
や周囲温度変化その他の環境の変化による光量変化等に
より安定した測定が困難であった。また、光ファイバの
長さによる光損失の変化や光コネクタの接合損失のバラ
ツキ等により、測定条件の変更や互換性を取るのは困難
であった。
[Problems to be solved by this invention] However,
With these methods, stable measurement is difficult due to changes in the intensity of the light source, changes in light amount due to bending of the optical fiber, changes in ambient temperature, and other environmental changes. In addition, it has been difficult to change measurement conditions and ensure compatibility due to changes in optical loss depending on the length of the optical fiber and variations in splicing loss of optical connectors.

この発明の目的は、以上の点に鑑み、感湿部として干渉
膜フィルタを用い、高感度の温度測定を可能とした光学
式測定装置を提供づることである。
In view of the above points, an object of the present invention is to provide an optical measuring device that uses an interference film filter as a humidity sensing section and is capable of highly sensitive temperature measurement.

E問題点を解決するための手段] この発明は、温度により透過率または反射率が変化する
感温部としての干渉膜フィルタに光ファイバを介して光
源からの光を投受光し、光ファイバからの光を分光手段
で分光してイメージセンサで検出し、このイメージセン
サの各画素出力のうちピーク値またはボトム値の画素位
置から測定手段で温度を測定するようにした光学式温度
測定装置である。
Means for Solving Problem E] This invention projects and receives light from a light source via an optical fiber to an interference film filter as a temperature-sensitive part whose transmittance or reflectance changes depending on temperature, and from the optical fiber. This is an optical temperature measuring device in which the light is separated by a spectroscopic means and detected by an image sensor, and the temperature is measured by a measuring means from the pixel position of the peak value or bottom value of each pixel output of this image sensor. .

[実施例] 第1図は、この発明の一実施例を示す構成説明図である
[Embodiment] FIG. 1 is a configuration explanatory diagram showing an embodiment of the present invention.

図において、白熱電球、ハロゲンランプ、LED等の光
源1の光は、光ファイバ21により感温部としての多層
の干渉膜フィルタ3に投光され、この半値幅の狭いバン
ドパスフィルタのような干渉膜フィルタ3を透過した光
は光ファイバ22により取り出される。この光ファイバ
22からの光は回折格子、プリズム等の分光手段4で分
光され、COD等のイメージセンサ5の各画素で受光さ
れ、このイメージセンサ5の出力から測定手段6で温度
の測定が行われる。
In the figure, light from a light source 1 such as an incandescent bulb, a halogen lamp, or an LED is projected through an optical fiber 21 to a multilayer interference film filter 3 as a temperature sensing section, and the interference filter 3, such as a band-pass filter with a narrow half-width, is transmitted through an optical fiber 21. The light transmitted through the membrane filter 3 is extracted by an optical fiber 22. The light from this optical fiber 22 is separated by a spectroscopic means 4 such as a diffraction grating or a prism, and is received by each pixel of an image sensor 5 such as a COD, and the temperature is measured by a measuring means 6 from the output of this image sensor 5. be exposed.

つまり、干渉膜フィルタ3は温度Tが上昇すると、第2
図AからA′というように透過波長特性が長波長側にシ
フトし、ピーク値の波長λと温度Tとの関係を、あらか
じめ実験、計W等で求めておけば、測定手段6によりピ
ーク値波長から温度Tが求まる。
In other words, when the temperature T rises, the interference film filter 3
If the transmission wavelength characteristic shifts to the long wavelength side as shown from A to A' in the diagram, and the relationship between the wavelength λ of the peak value and the temperature T is determined in advance by experiment, measurement W, etc., the peak value can be measured by the measuring means 6. Temperature T can be found from the wavelength.

一方、イメージセンサ5は、分光手段4で分光された光
を受光するため、第2図の横軸をイメージセンサ5の画
素位置(番号)とすると、イメージセンサ5の出力は第
2図と類似の出力波長が得られる。従って、予めイメー
ジセンサ5の画素と波長との対応を取っておけば、出力
波形の画素位置からtm 11 Tを求めることができ
る。
On the other hand, since the image sensor 5 receives the light separated by the spectrometer 4, if the horizontal axis in FIG. 2 is the pixel position (number) of the image sensor 5, the output of the image sensor 5 is similar to that in FIG. output wavelength is obtained. Therefore, if the correspondence between the pixels of the image sensor 5 and the wavelength is established in advance, tm 11 T can be determined from the pixel position of the output waveform.

このように、この発明では、ピーク値の位置のみが必要
であって、ピーク位置の検出に必要な光量さえあれば、
光量の変化は測定値に本質的な影響を及ぼさない。この
ため、光源のドリフ1へ、光ファイバの曲げの変化や長
さの変化、光コネクタ等による光損失の変化の影響を受
けることなく、安定した測定が可能である。また、出力
はイメージセンサ5の画素位置のため、デジタル化も容
易である。
In this way, in this invention, only the position of the peak value is required, and as long as there is the amount of light necessary to detect the peak position,
Changes in the amount of light have no essential effect on the measured values. Therefore, stable measurement is possible without being affected by the drift 1 of the light source, changes in bending or length of the optical fiber, changes in optical loss due to optical connectors, etc. Furthermore, since the output is based on the pixel position of the image sensor 5, it is easy to digitize it.

なお、干渉膜フィルタ3としては、高屈折率膜にSiま
たはGe1低屈折率膜にSiO等を用い、蒸着等により
多m膜を形成し、温度範囲、感度に応じた所望の透過波
長特性をもつフィルタとする。
The interference film filter 3 is made of Si or Ge for the high refractive index film, SiO, etc. for the low refractive index film, and is formed into a multi-m film by vapor deposition or the like, and has the desired transmission wavelength characteristics according to the temperature range and sensitivity. A filter with

このように多層の干渉膜フィルタの層数、膜構成を変え
ることにより必要とするバンドパス特性をもつフィルタ
が1りられ、また、3i 、Qeの屈折率の温度係数は
約1.5X10−’//’Cと十分大きく、感温部どし
て十分使用できる。
In this way, by changing the number of layers and film configuration of the multilayer interference film filter, one filter with the required bandpass characteristics can be obtained, and the temperature coefficient of the refractive index of 3i and Qe is approximately 1.5X10-'//'C is large enough to be used as a temperature sensing part.

第3図は、この発明の他の一実施例を示す構成説明図で
、第1図と同一符号は同等の構成要素を示す。
FIG. 3 is a configuration explanatory diagram showing another embodiment of the present invention, in which the same reference numerals as in FIG. 1 indicate equivalent components.

図において、光源1からの光は、ハーフミラ−7を介し
て光ファイバ2により感温部としての干渉膜フィルタ3
に投光される。光ファイバ2の先端に蒸着その他で設け
られた半値幅の狭いバンドパスフィルタのような干渉膜
フィルタ3を反射した光は再び光ファイバ2を介して取
り出され、ハーフミラ−7で反射される。このハーフミ
ラ−7で反射した光は分光手段4で分光されイメージセ
ンサ5で受光され、このイメージセンサ5の出力から測
定手段6で温度が測定される。
In the figure, light from a light source 1 is transmitted via a half mirror 7 to an optical fiber 2 through an interference film filter 3 as a temperature sensing section.
is illuminated. The light reflected by an interference film filter 3 such as a bandpass filter with a narrow half-width provided at the tip of the optical fiber 2 by vapor deposition or other means is extracted again through the optical fiber 2 and reflected by a half mirror 7. The light reflected by the half mirror 7 is separated by the spectroscopic means 4 and received by the image sensor 5, and the temperature is measured by the measuring means 6 from the output of the image sensor 5.

つまり、干渉膜フィルタ3は、温度Tが上昇すると、第
4図△からA−へというように反射波長特性が長波長側
にシフトする。従って、第1図と同様の原理でイメージ
センサ5のボトム値の画素位置から温度Tを求めること
ができる。
In other words, when the temperature T of the interference film filter 3 rises, the reflection wavelength characteristic shifts to the long wavelength side from Δ to A- in FIG. 4. Therefore, the temperature T can be determined from the bottom value pixel position of the image sensor 5 using the same principle as in FIG.

また、第5図で示すように、光ファイバ20の端面に干
渉膜フィルタ3を蒸着等で形成することにより(たとえ
ば多数の光ファイバの端面に同時に干渉膜フィルタを形
成することにより)、均一なS湿部が、安価、人聞に生
産でき、互換性も有し、また、光コネクタ20aにより
光ファイバ2に蒸着可能とすることにより、取り扱い、
保守等が容易なものとなる。つまり、このような光コネ
クタ20aを用いたとしても、光量変動は外乱とならな
い方式であるので、光コネクタ20aを交換しても、そ
の結合損失のバラツキ等の影響は受けることがない。
Furthermore, as shown in FIG. 5, by forming an interference film filter 3 on the end face of the optical fiber 20 by vapor deposition or the like (for example, by forming interference film filters on the end faces of many optical fibers at the same time), uniform The S wet part can be produced inexpensively and easily, has compatibility, and can be deposited on the optical fiber 2 using the optical connector 20a, making it easy to handle,
Maintenance, etc. becomes easier. In other words, even if such an optical connector 20a is used, variations in the amount of light do not cause a disturbance, so even if the optical connector 20a is replaced, it will not be affected by variations in coupling loss.

[発明の効果コ 以上述べたように、この発明は、感温部として干渉膜フ
ィルタを用い、分光手段からの光を光ファイバを利用し
てイメージセンサに入射させ、各画素位置から温度を測
定するようにしているので、売場変化の影響を受けるこ
とがなく、光路の影響等を受けることがなく、高精度に
安定した1ll11温が可能となる。
[Effects of the Invention] As described above, the present invention uses an interference film filter as the temperature sensing section, makes light from the spectroscopic means enter the image sensor using an optical fiber, and measures the temperature from each pixel position. Therefore, it is not affected by changes in the sales floor, it is not affected by the optical path, etc., and it is possible to maintain a stable temperature with high accuracy.

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

第1図、第3図、第5図は、この発明の一実施例を示す
構成説明図、第2図、第4図は、波長特性説明図である
。 1・・・光源、2.20.21.22・・・光ファイバ
、3・・・干渉膜フィルタ、4・・・分光手段、5・・
・イメージセンサ、6・・・測定手段、7・・・ハーフ
ミラ−120a・・・光コネクタ
FIGS. 1, 3, and 5 are configuration explanatory diagrams showing one embodiment of the present invention, and FIGS. 2 and 4 are wavelength characteristic diagrams. DESCRIPTION OF SYMBOLS 1...Light source, 2.20.21.22...Optical fiber, 3...Interference film filter, 4...Spectroscopy means, 5...
・Image sensor, 6... Measuring means, 7... Half mirror 120a... Optical connector

Claims (1)

【特許請求の範囲】[Claims] 1、温度により透過率または反射率が変化する感温部と
しての2個の干渉膜フィルタと、この干渉膜フィルタに
光源からの光を投光し干渉膜フィルタを透過または反射
した光を取り出す光ファイバと、この光ファイバからの
光を分光する分光手段と、この分光手段で分光された光
を受光するイメージセンサと、このイメージセンサの各
画素出力のうちピーク値またはボトム値から温度を測定
する測定手段とを備えたことを特徴とする光学式温度測
定装置。
1. Two interference film filters as temperature-sensitive parts whose transmittance or reflectance changes depending on temperature, and a light that projects light from a light source onto these interference film filters and extracts the light that is transmitted or reflected by the interference film filters. A fiber, a spectroscopic means for separating the light from the optical fiber, an image sensor for receiving the light separated by the spectroscopic means, and a temperature is measured from the peak value or bottom value of each pixel output of the image sensor. An optical temperature measuring device characterized by comprising: a measuring means.
JP62070836A 1987-03-25 1987-03-25 Optical temperature measuring instrument Pending JPS63236936A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62070836A JPS63236936A (en) 1987-03-25 1987-03-25 Optical temperature measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62070836A JPS63236936A (en) 1987-03-25 1987-03-25 Optical temperature measuring instrument

Publications (1)

Publication Number Publication Date
JPS63236936A true JPS63236936A (en) 1988-10-03

Family

ID=13443049

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62070836A Pending JPS63236936A (en) 1987-03-25 1987-03-25 Optical temperature measuring instrument

Country Status (1)

Country Link
JP (1) JPS63236936A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54158954A (en) * 1978-06-02 1979-12-15 Asea Ab Device for measuring fiber optical
JPS5641223B2 (en) * 1973-01-13 1981-09-26
JPS6144334A (en) * 1984-08-08 1986-03-04 Mitsubishi Electric Corp Temperature measuring device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5641223B2 (en) * 1973-01-13 1981-09-26
JPS54158954A (en) * 1978-06-02 1979-12-15 Asea Ab Device for measuring fiber optical
JPS6144334A (en) * 1984-08-08 1986-03-04 Mitsubishi Electric Corp Temperature measuring device

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