JPH0519098B2 - - Google Patents
Info
- Publication number
- JPH0519098B2 JPH0519098B2 JP14437087A JP14437087A JPH0519098B2 JP H0519098 B2 JPH0519098 B2 JP H0519098B2 JP 14437087 A JP14437087 A JP 14437087A JP 14437087 A JP14437087 A JP 14437087A JP H0519098 B2 JPH0519098 B2 JP H0519098B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- waveguide
- reference light
- measurement
- gas
- 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
Links
- 238000005259 measurement Methods 0.000 claims description 36
- 230000003287 optical effect Effects 0.000 claims description 23
- 239000013307 optical fiber Substances 0.000 claims description 8
- 238000005253 cladding Methods 0.000 claims description 4
- 239000000758 substrate Substances 0.000 claims description 4
- 239000007789 gas Substances 0.000 description 45
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 25
- 239000004065 semiconductor Substances 0.000 description 4
- 230000000087 stabilizing effect Effects 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000003487 electrochemical reaction Methods 0.000 description 2
- 239000008151 electrolyte solution Substances 0.000 description 2
- 229910044991 metal oxide Inorganic materials 0.000 description 2
- 150000004706 metal oxides Chemical class 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000001902 propagating effect Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 239000010408 film Substances 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 230000007257 malfunction Effects 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/39—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using tunable lasers
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Analytical Chemistry (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Optics & Photonics (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Light Guides In General And Applications Therefor (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、ガスの濃度等を光学的に検出させる
ための電池内蔵の超小型に形成されたガスセンサ
に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an ultra-compact gas sensor with a built-in battery for optically detecting gas concentration and the like.
(従来の技術)
従来、ガスの濃度を測定するためのガスセンサ
として、例えば電解液中に設けられた電極間に電
圧を印加し、ガスを陽極酸化させて、このとき流
れる電流を測定することによつてガスの濃度を検
出させる電気化学反応方式のガスセンサや、金属
酸化物の半導体に還元性ガスを吸着させたとき、
その電気伝導度が増加する現象を利用した半導体
方式のガスセンサなどがあつた。(Prior Art) Conventionally, as a gas sensor for measuring the concentration of gas, for example, a voltage is applied between electrodes provided in an electrolytic solution, the gas is anodized, and the current flowing at this time is measured. Therefore, when a reducing gas is adsorbed on an electrochemical reaction type gas sensor that detects the concentration of gas, or on a metal oxide semiconductor,
There have been semiconductor-based gas sensors that take advantage of this phenomenon of increased electrical conductivity.
(発明が解決しようとする問題点)
しかしながら上記従来のガスセンサのうち、電
気化学反応方式のガスセンサは電解液を用いてい
るため寿命が短く、かつ外形寸法が大きく高価で
あるという問題があつた。また、半導体方式のガ
スセンサの場合は、金属酸化物半導体の焼結体、
焼結膜、あるいは薄膜などからなる感応体部と、
これを加熱するヒータ、及び防爆用のネツトなど
で構成されているため、外形寸法を小さくするこ
とに限界があつた。そのため、狭小な場所に直接
ガスセンサを取付けたりすることが極めて困難で
あるという問題と、ガスセンサが屋内の天井等に
取付けられた場合に目立ち過ぎてインテリア性を
失うなどという問題があつた。(Problems to be Solved by the Invention) However, among the above-mentioned conventional gas sensors, the electrochemical reaction type gas sensor uses an electrolytic solution, so it has short lifespan, large external dimensions, and is expensive. In addition, in the case of semiconductor-based gas sensors, sintered bodies of metal oxide semiconductors,
A sensitive body part made of a sintered film or a thin film,
Since it consists of a heater to heat it and an explosion-proof net, there is a limit to how small the external dimensions can be made. Therefore, there were problems in that it was extremely difficult to directly install the gas sensor in a narrow space, and that when the gas sensor was installed on the ceiling indoors, it was too conspicuous and lost its interior design.
さらに、従来のガスセンサは一般に電源として
交流100Vを必要とするため、交流100V電源が容
易に供給できる場合に取付けることが必要条件と
なり、もし、交流100V電源が無い場所にガスセ
ンサを取付ける場合は、電源として電池を用いて
いたが、常時電源を供給していなければならない
ため、電池の消耗が早く、実用的ではないという
問題があつた。さらにアルコール等の雑ガスによ
り誤動作をすることがあるという問題があつた。 Furthermore, since conventional gas sensors generally require 100V AC as a power source, it is necessary to install the gas sensor in a place where 100V AC power can be easily supplied.If the gas sensor is installed in a place without 100V AC power, However, since power had to be constantly supplied, the battery ran out quickly, making it impractical. Furthermore, there was a problem in that malfunctions could occur due to miscellaneous gases such as alcohol.
そこで本発明においては、上記従来の問題点を
解決するためLSI(ラージスケールインテグレー
テツドサーキツト)等微細加工用写真技術などを
利用することにより、光フアイバの特性を有する
光導波路を超小型に形成し、さらに光導波路に接
続される光電部、演算部、電源部等をワンチツプ
状に一体化することによりガスセンサ全体を超小
型にするとともに、特定のガスに対してのみ吸収
される波長の光を測定光として用い、同ガスの吸
収されない波長の光を基準光として用いることに
より他のガスの影響を受けずに濃度等を検出さ
せ、また、電源として電池を用い、かつ上記測定
光、基準光の発光においては時間間隔を明けたパ
ルス光とすることにより電池の消耗を少なくして
電池の寿命を長くすることを技術的課題とするも
のである。 Therefore, in the present invention, in order to solve the above-mentioned conventional problems, an optical waveguide having the characteristics of an optical fiber is formed in an ultra-small size by using photographic technology for microfabrication such as LSI (large scale integrated circuit). Furthermore, by integrating the photoelectric section, arithmetic section, power supply section, etc. connected to the optical waveguide into a single chip, the entire gas sensor can be made ultra-compact, and the light of a wavelength that is absorbed only by a specific gas can be emitted. By using the wavelength of light that is not absorbed by the same gas as the reference light, the concentration, etc. can be detected without being affected by other gases.Also, by using a battery as the power source, the above measurement light and the reference light can be used as the measurement light. In light emission, the technical problem is to reduce the consumption of the battery and extend the life of the battery by using pulsed light with separated time intervals.
(問題点を解決するための手段)
上記課題解決のための技術的手段は、ガスの濃
度等を光学的に検出させるための超小型ガスセン
サを、光フアイバのクラツドに対応した特性を有
する薄板状の小さな基盤と光フアイバのコアに対
応した特性を有して前記基盤にうず巻き状に形成
された導波路とから成る光導波路と、前記ガスに
より吸収される波長の測定光を発光する測定光発
光手段と、前記ガスにより吸収されない波長の基
準光を発光する基準光発光手段と、前記測定光発
光手段と前記基準光発光手段それぞれに対して前
記測定光と前記基準光とをそれぞれパルス状に、
かつ一定時間毎に間欠的に発光させるための発光
信号を出力する発光制御手段と、前記測定光発光
手段から発光された前記パルス状の測定光と前記
基準光発光手段から発光された前記パルス状の基
準光とを合波と、合波した光を前記光導波路に伝
送する光合波手段と、前記光合波手段からの前記
合波光が前記導波路中を伝搬したあと、同導波路
から出光した前記測定光と基準光とを受光したう
え測定光の受光量と基準光の受光量それぞれに対
応した電気信号を出力する受光手段と、前記受光
手段から出力された前記測定光の受光量対応の電
気信号と前記基準光の受光量対応の電気信号とを
入力して前記ガスの濃度等を演算する演算手段と
のそれぞれを一体的に集合形成することである。(Means for solving the problem) The technical means for solving the above problem is to install an ultra-small gas sensor for optically detecting the concentration of gas, etc. into a thin plate-shaped sensor with characteristics compatible with the cladding of an optical fiber. an optical waveguide consisting of a small base and a waveguide formed in a spiral shape on the base with characteristics corresponding to the core of the optical fiber; and a measurement light emitting device that emits measurement light at a wavelength that is absorbed by the gas. a reference light emitting means for emitting reference light having a wavelength that is not absorbed by the gas; and pulses of the measuring light and the reference light to each of the measuring light emitting means and the reference light emitting means, respectively;
and a light emission control means for outputting a light emission signal for causing light emission intermittently at regular intervals; and a light emission control means for outputting a light emission signal for causing light emission intermittently at fixed time intervals; an optical multiplexing means for transmitting the multiplexed light to the optical waveguide; and an optical multiplexing means for transmitting the multiplexed light to the optical waveguide; and after the multiplexed light from the optical multiplexing means propagates through the waveguide, it is emitted from the waveguide. a light receiving means that receives the measurement light and the reference light and outputs an electric signal corresponding to the amount of the measurement light received and the amount of the reference light received, respectively; The method is to integrally form a calculation means for calculating the concentration of the gas by inputting an electric signal and an electric signal corresponding to the received amount of the reference light.
(作 用)
上記構成の超小型ガスセンサに依れば、発光制
御手段は測定光発光手段と基準光発光手段とに対
し、一定時間毎に前記測定光と前記基準光とをそ
れぞれパルス状に、かつ一定の出力で発光させる
ための発光信号を出力する。測定光発光手段から
発光されたパルス状の測定光と、基準光発光手段
から発光されたパルス状の基準光は光合波手段に
より合波され、直列光となつてうず巻き状に形成
された導波路を伝搬する。導波路中を測定光が伝
搬する過程で、導波路外に発生する測定光のエバ
ネツセント波が被検出ガスにより吸収される一
方、基準光は被検出ガスにより吸収されない状態
で、導波路から出光した測定光と基準光は受光手
段で受光され、受光手段から測定光の受光量と基
準光の受光量それぞれに対応した電気信号を演算
手段に出力する。演算手段は上記測定光の受光量
対応の電気信号をV、基準光の受光量対応の電気
信号をVoとし、ガス濃度Pを次式に基づいて演
算する。(Function) According to the ultra-compact gas sensor configured as described above, the light emission control means pulses the measurement light and the reference light to the measurement light emission means and the reference light emission means at fixed time intervals, respectively. It also outputs a light emission signal for emitting light at a constant output. The pulsed measurement light emitted from the measurement light emitting means and the pulsed reference light emitted from the reference light emitting means are combined by the optical multiplexing means to form serial light into a spiral waveguide. propagate. During the process of the measurement light propagating through the waveguide, the evanescent wave of the measurement light generated outside the waveguide is absorbed by the gas to be detected, while the reference light is not absorbed by the gas to be detected and is emitted from the waveguide. The measuring light and the reference light are received by the light receiving means, and the light receiving means outputs electrical signals corresponding to the received amounts of the measuring light and the reference light to the calculating means. The calculation means calculates the gas concentration P based on the following equation, with V representing the electric signal corresponding to the amount of received measurement light and Vo representing the electric signal corresponding to the amount of received reference light.
V/Vo=e×p(−αpl) …(1)
p=−1/αllogV/Vo …(2)
ただし、αは光吸収率、lは導波路長である。
上記式(1)から明らかなように導波路長lの長さが
長いほどV/Voが小さくなり、いわゆるガス濃
度検出感度を上げるものである。 V/Vo=e×p(−αpl) (1) p=−1/αllogV/Vo (2) where α is the optical absorption rate and l is the waveguide length.
As is clear from the above equation (1), the longer the waveguide length l, the smaller V/Vo becomes, which increases the so-called gas concentration detection sensitivity.
(実施例) 次に本発明の実施例を図面に従つて説明する。(Example) Next, embodiments of the present invention will be described with reference to the drawings.
第1図は、超小型ガスセンサの全体系統を示し
たブロツク図であり、第2図は、光導波路の断面
図である。第1図に示した光導波路1は、第2図
の断面図に示すように、光フアイバのクラツドに
相当する極めて薄い導波路基盤2に、LSI等の製
造等に用いられる写真技術、即ち微細加工技術を
用いることにより、光フアイバのコアに相当する
導波路3をうず巻き状に形成したものである。例
えば直径1cmの上記導波路基盤2に直径が例えば
50μmの導波路3をうず巻き状に形成する場合、
導波路3の1巻当りの長さは約3.14cmとなるた
め、延100cmの長さのうず巻き状の導波路3を形
成する場合のターン数は
100cm/3.14cm=31.8となるため約32本のうず
巻きを作れば良いことになる。 FIG. 1 is a block diagram showing the entire system of the ultra-small gas sensor, and FIG. 2 is a sectional view of the optical waveguide. As shown in the cross-sectional view of FIG. 2, the optical waveguide 1 shown in FIG. The waveguide 3, which corresponds to the core of the optical fiber, is formed into a spiral shape by using processing technology. For example, the waveguide substrate 2 with a diameter of 1 cm has a diameter of, for example,
When forming the 50 μm waveguide 3 in a spiral shape,
The length of each turn of the waveguide 3 is approximately 3.14 cm, so when forming a spiral waveguide 3 with a total length of 100 cm, the number of turns is 100 cm/3.14 cm = 31.8, so approximately 32 turns. It would be a good idea to make a spiral.
上記光導波路1に形成された導波路3の一方の
開口端は、レーザ発光部4に接合される入光口3
Aとなる一方、導波路3の他方の開口端は、後述
の測定光及び基準光を受光するフオトダイオード
5に接合される出光口3Bとなる。 One open end of the waveguide 3 formed in the optical waveguide 1 is a light entrance 3 that is joined to the laser emitting part 4.
A, while the other open end of the waveguide 3 becomes a light exit 3B that is connected to a photodiode 5 that receives measurement light and reference light, which will be described later.
レーザ発光部4は、被検出ガスを例えばメタン
CH4として、メタンにより吸収される波長の測
定光を発光させるレーザダイオード4Aと、メタ
ンにより吸収されない波長の基準光を発光させる
レーザダイオード4Bと、上記測定光と基準光と
を合波したうえ両光を直列光にして前記入光口3
Aに入光させる光合波器4Cとを内蔵している。 The laser emitting unit 4 converts the gas to be detected into, for example, methane.
CH4 includes a laser diode 4A that emits a measurement light with a wavelength that is absorbed by methane, a laser diode 4B that emits a reference light with a wavelength that is not absorbed by methane, and a laser diode 4B that combines the measurement light and the reference light and then generates both lights. into the light input port 3 as a series light.
It has a built-in optical multiplexer 4C that allows light to enter A.
レーザ発光部4はマイクロコンピユータ6と接
続されており、マイクロコンピユータ6から前記
レーザダイオード4Aと4Bとに対して発光信号
を出力する。マイクロコンピユータ6から出力さ
れる発光信号は、第4図に示すように例えば測定
光を10ミリ秒、基準光を10ミリ秒それぞれ続けて
同じ発光レベルで発光させ、10秒の間隔を置いて
再び測定光、基準光をそれぞれ10ミリ秒間づつ発
光させるという間欠発光をさせるためのものであ
る。一方、前記フオトダイオード5は上記マイク
ロコンピユータ6と接続されており、前記導波路
3の出光口3Bから出光した測定光及び基準光そ
れぞれの受光量対応の電気信号をマイクロコンピ
ユータ6に出力する。マイクロコンピユータ6
は、フオトダイオード5から出力された上記電気
信号を入力したうえ後述の作用によりメタンの濃
度を演算する。電池7は本実施例の超小型ガスセ
ンサの電源として設けられ、電池7の出力電圧は
安定化電源8により所定の電圧に安定化されたあ
と、レーザ発光部4、フオトダイオード5、マイ
クロコンピユータ6等に供給される。電池7、安
定化電源8は、例えばICカードのようにチツプ
状にして組込むことにより全体の形状を超小型に
形成するものである。 The laser emitting section 4 is connected to a microcomputer 6, and the microcomputer 6 outputs a light emission signal to the laser diodes 4A and 4B. The light emission signal output from the microcomputer 6 is, as shown in Fig. 4, for example, by emitting the measurement light for 10 milliseconds and the reference light for 10 milliseconds at the same light emission level, and then emitting it again at an interval of 10 seconds. This is for intermittent light emission in which the measurement light and reference light are emitted for 10 milliseconds each. On the other hand, the photodiode 5 is connected to the microcomputer 6, and outputs to the microcomputer 6 an electric signal corresponding to the amount of received measurement light and reference light emitted from the light exit 3B of the waveguide 3. microcomputer 6
inputs the electric signal outputted from the photodiode 5 and calculates the concentration of methane by the action described later. A battery 7 is provided as a power source for the ultra-small gas sensor of this embodiment, and after the output voltage of the battery 7 is stabilized to a predetermined voltage by a stabilizing power source 8, the output voltage of the battery 7 is stabilized to a predetermined voltage by a stabilizing power source 8, and then the output voltage of the battery 7 is stabilized to a predetermined voltage by a stabilizing power source 8. is supplied to The battery 7 and the stabilized power source 8 are formed into a chip shape and incorporated into the device, such as in an IC card, so that the overall shape is made extremely small.
次に、上記構成による実施例の作用を説明す
る。上記超小型ガスセンサが例えばメタン発生場
所に設置された状態で、マイクロコンピユータ6
はレーザダイオード4Aに対して測定光発光用の
発光信号を出力し、レーザダイオード4Aからメ
タンにより吸収される波長例えば1.3μm帯の測定
光を所定の光量で10ミリ秒間発光させ、続いてメ
タンにより吸収されない波長の基準光を測定光と
同一の光量で10ミリ秒間レーザダイオード4Bか
ら発光させる。レーザダイオード4Aから発光さ
れた測定光及びレーザダイオード4Bから発光さ
れた基準光は光合波器4Cで合波され、直列状の
光にされて光導波路1の入光口3Aから導波路3
に入光し、うず巻き状に形成された導波路3を伝
搬する。測定光が導波路3を伝搬する過程で、第
3図に示すように導波路基板2の外側に測定光の
エバネツセント波10が発生し、メタンと接触し
たとき、エバネツセント波10がメタンにより吸
収される。そのため、測定光は導波路3を伝搬す
る途中で減衰し、導波路3の出光口3Bから出光
してフオトダイオード5で受光される時点での測
定光はメタンガスの濃度に対応した吸収を受けた
あとの光量となる。 Next, the operation of the embodiment with the above configuration will be explained. With the ultra-compact gas sensor installed at a methane generation location, the microcomputer
outputs a light emitting signal for emitting measurement light to the laser diode 4A, causes the laser diode 4A to emit measurement light at a predetermined light intensity for 10 milliseconds at a wavelength that is absorbed by methane, for example, in the 1.3 μm band, and then A reference light having a wavelength that is not absorbed is emitted from the laser diode 4B for 10 milliseconds at the same light intensity as the measurement light. The measurement light emitted from the laser diode 4A and the reference light emitted from the laser diode 4B are multiplexed by an optical multiplexer 4C and made into series light, which is transmitted from the light entrance 3A of the optical waveguide 1 to the waveguide 3.
The light enters and propagates through the waveguide 3 formed in a spiral shape. As the measurement light propagates through the waveguide 3, an evanescent wave 10 of the measurement light is generated outside the waveguide substrate 2 as shown in FIG. 3, and when it comes into contact with methane, the evanescent wave 10 is absorbed by the methane. Ru. Therefore, the measurement light is attenuated while propagating through the waveguide 3, and the measurement light at the time it is emitted from the light exit 3B of the waveguide 3 and received by the photodiode 5 is absorbed in accordance with the concentration of methane gas. This will be the amount of light.
一方、基準光はロタンによつて吸収されないた
め、ほとんど減衰することなくフオトダイオード
5で受光される。フオトダイオード5により受光
された測定光光量対応の出力信号をV、フオトダ
イオード5により受光された基準光光量対応の出
力信号をVoとし、さらに、メタンの光吸収率を
α(0.054atm-1・cm-1)、導波路3の長さlを
(cm)、ガス濃度をp(ppm)とすると、メタンに
よる吸収式は
V/Vo=exp(−αpl) …(3)
となり、式(3)から、ガス濃度pを求める式(4)
p=−1/αllogV/Vo …(4)
が導かれる。上記式(4)により今、導波路長l=
100cm、α=0.054atm-1・cm-1V/Vo=0.984であ
る場合、ガス濃度pは5000ppmとなる。 On the other hand, since the reference light is not absorbed by the rotane, it is received by the photodiode 5 with almost no attenuation. The output signal corresponding to the amount of measurement light received by the photodiode 5 is V, the output signal corresponding to the amount of reference light received by the photodiode 5 is Vo, and the light absorption rate of methane is α (0.054 atm -1・cm -1 ), the length l of the waveguide 3 is (cm), and the gas concentration is p (ppm), then the absorption formula by methane is V/Vo=exp(-αpl)...(3), and the equation (3) ), formula (4) for determining the gas concentration p is derived: p=-1/αllogV/Vo (4). From the above equation (4), now the waveguide length l=
When 100 cm and α=0.054 atm −1 ·cm −1 V/Vo=0.984, the gas concentration p is 5000 ppm.
なお、メタンのガス濃度pを5000ppmとして導
波路3の長さlを1000cmにした場合には、式(3)か
らV/Vo=0.85となるため、ガス濃度の検出感
度を向上させることができる。またマイクロコン
ピユータ6に表示器及び圧電ブザー等を接続する
ことによつてガス濃度を表示させることができ
る。 Note that when the methane gas concentration p is 5000 ppm and the length l of the waveguide 3 is 1000 cm, V/Vo = 0.85 from equation (3), so the detection sensitivity of the gas concentration can be improved. . Furthermore, by connecting a display, a piezoelectric buzzer, etc. to the microcomputer 6, the gas concentration can be displayed.
(発明の効果)
以上のように本発明に依れば、光フアイバのコ
アに相当する導波路を、光フアイバのクラツドに
相当する薄板状の基盤にうず巻き状に形成するこ
とによつて所要の導波路長を確保し、さらに測定
光発光手段、基準光発光手段、受光手段、演算手
段及び電池等を一体的に、かつコンパクトに形成
することによつてガスセンサを超小型に構成でき
るため、ガスセンサの設定場所を限定することな
く、かつ室内等のインテリア性を失うことがない
ように設置することができ、また、測定光、基準
光の発光を間欠的に行うために、電池の寿命を長
くすることができるという効果がある。(Effects of the Invention) As described above, according to the present invention, the waveguide corresponding to the core of the optical fiber is formed in a spiral shape on the thin plate-like base corresponding to the cladding of the optical fiber. The gas sensor can be constructed in an ultra-compact size by ensuring the waveguide length and further forming the measuring light emitting means, the reference light emitting means, the light receiving means, the calculating means, the battery, etc. in an integrated and compact manner. It can be installed without limiting the setting location and without losing the interior design of the room, etc. Also, since the measurement light and reference light are emitted intermittently, the battery life is extended. The effect is that it can be done.
図面は実施例に係り、第1図は超小型ガスセン
サの全体系統図、第2図は光導波路の部分断面
図、第3図及び第4図は作用説明図である。
1…光導波路、2…導波路基板、3…導波路、
4…レーザ発光部、4A…レーザダイオード、4
B…レーザダイオード、4C…光合波器、5…フ
オトダイオード、6…マイクロコンピユータ、7
…電池、8…安定化電源。
The drawings relate to embodiments, and FIG. 1 is an overall system diagram of an ultra-small gas sensor, FIG. 2 is a partial sectional view of an optical waveguide, and FIGS. 3 and 4 are explanatory views of the operation. 1... Optical waveguide, 2... Waveguide substrate, 3... Waveguide,
4... Laser emitting section, 4A... Laser diode, 4
B...Laser diode, 4C...Optical multiplexer, 5...Photodiode, 6...Microcomputer, 7
...Battery, 8...Stabilized power supply.
Claims (1)
に検出させるための超小型に形成されたガスセン
サであつて、光フアイバのクラツドに対応した特
性を有する薄板状の小さな基盤と光フアイバのコ
アに対応した特性を有して前記基盤にうず巻き状
に形成された導波路とから成る光導波路と、前記
ガスにより吸収される波長の測定光を発光する測
定光発光手段と、前記ガスにより吸収されない波
長の基準光を発光する基準光発光手段と、前記測
定光発光手段と前記基準光発光手段それぞれに対
して前記測定光と前記基準光とをそれぞれパルス
状に、かつ一定時間毎に間欠的に発光させるため
の発光信号を出力する発光制御手段と、前記測定
光発光手段から発光された前記パルス状の測定光
と前記基準光発光手段から発光された前記パルス
状の基準光とを合波と、合波した光を前記光導波
路に伝送する光合波手段と、前記光合波手段から
の前記合波光が前記導波路中を伝搬したあと、同
導波路から出光した前記測定光と基準光とを受光
したうえ測定光の受光量と基準光の受光量それぞ
れに対応した電気信号を出力する受光手段と、前
記受光手段から出力された前記測定光の受光量対
応の電気信号と前記基準光の受光量対応の電気信
号とを入力して前記ガスの濃度等を演算する演算
手段とのそれぞれを一体的に集合形成したことを
特徴とする超小型ガスセンサ。1. An ultra-compact gas sensor for optically detecting gas concentration, etc. using a battery as a power source, which consists of a small thin plate-like base with characteristics compatible with optical fiber cladding and optical fiber cladding. an optical waveguide formed in a spiral shape on the substrate and having characteristics corresponding to the core; a measurement light emitting means for emitting measurement light having a wavelength that is absorbed by the gas; a reference light emitting means for emitting a reference light of a wavelength that is not detected; and the measuring light and the reference light are applied to each of the measuring light emitting means and the reference light emitting means in a pulsed manner and intermittently at regular intervals. a light emission control means for outputting a light emission signal for causing light to be emitted; and a light emission control means for combining the pulsed measurement light emitted from the measurement light emission means and the pulsed reference light emitted from the reference light emission means. , an optical multiplexer for transmitting the multiplexed light to the optical waveguide, and after the multiplexed light from the optical multiplexer propagates through the waveguide, the measurement light and the reference light output from the waveguide. a light-receiving means that receives the light and outputs an electric signal corresponding to the received amount of the measurement light and the received amount of the reference light, and an electric signal corresponding to the received amount of the measurement light output from the light-receiving means and the reference light An ultra-compact gas sensor characterized in that an electric signal corresponding to the amount of received light is input, and a calculation means for calculating the concentration of the gas and the like are integrally formed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62144370A JPS63308539A (en) | 1987-06-10 | 1987-06-10 | Super-mini gas sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62144370A JPS63308539A (en) | 1987-06-10 | 1987-06-10 | Super-mini gas sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63308539A JPS63308539A (en) | 1988-12-15 |
| JPH0519098B2 true JPH0519098B2 (en) | 1993-03-15 |
Family
ID=15360536
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62144370A Granted JPS63308539A (en) | 1987-06-10 | 1987-06-10 | Super-mini gas sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63308539A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP1291642A1 (en) * | 2001-09-05 | 2003-03-12 | Linde Medical Sensors AG | Sensor system comprising an integrated optical waveguide for the detection of chemical substances |
| JP2006220625A (en) * | 2005-02-14 | 2006-08-24 | Denso Corp | Infrared gas detector |
| WO2011062034A1 (en) * | 2009-11-17 | 2011-05-26 | 日本電気株式会社 | Gas detection device |
| CN108169158A (en) * | 2017-11-29 | 2018-06-15 | 全球能源互联网研究院有限公司 | A kind of gas detecting system based on gas sensor |
| JP6895480B2 (en) * | 2018-07-06 | 2021-06-30 | 旭化成エレクトロニクス株式会社 | Gas detector |
-
1987
- 1987-06-10 JP JP62144370A patent/JPS63308539A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63308539A (en) | 1988-12-15 |
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