JPH09257582A - Optical measuring method and optical measuring aid - Google Patents

Optical measuring method and optical measuring aid

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Publication number
JPH09257582A
JPH09257582A JP8063982A JP6398296A JPH09257582A JP H09257582 A JPH09257582 A JP H09257582A JP 8063982 A JP8063982 A JP 8063982A JP 6398296 A JP6398296 A JP 6398296A JP H09257582 A JPH09257582 A JP H09257582A
Authority
JP
Japan
Prior art keywords
light
detection target
subject
wavelength
optical measurement
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
JP8063982A
Other languages
Japanese (ja)
Inventor
Masahide Tsujishita
正秀 辻下
Hikari Hirano
光 平野
Masashi Nishigaki
雅司 西垣
Hideki Okamoto
秀樹 岡本
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.)
Osaka Gas Co Ltd
Original Assignee
Osaka Gas Co Ltd
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 Osaka Gas Co Ltd filed Critical Osaka Gas Co Ltd
Priority to JP8063982A priority Critical patent/JPH09257582A/en
Publication of JPH09257582A publication Critical patent/JPH09257582A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide a method for measuring the light in the condition that S/N ratio is high and that the influence of the heat to a light detecting unit is small. SOLUTION: In this method for measuring the light, the light to be detected, which is generated from a subject 2 to be checked in the high temperature condition side of a combustion chamber and which has a specified detecting wave length, is led to a light detecting unit 3 for measurement through a wave lenght selecting unit 10 for selectively transmitting the light. In this case, a selective reflecting mirror 7 for reflecting the light to be detected, which is generated from the subject 2 to be checked, to as wave length selecting unit side is deranged on an optical path extended from the subject 2 to be checked to the wave length selecting unit 10, and the light to be detected is led to the light detecting unit 3 for measurement.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、燃焼室内の高温状
態にある被検体から発生される特定検出波長の検出対象
光を、この検出対象光を選択的に透過する波長選択器を
介して光検出器に導いて計測する光計測方法に関するも
のであり、このような光計測法に使用できる光計測補助
具に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method in which light to be detected having a specific detection wavelength, which is generated from an object in a combustion chamber at a high temperature, is transmitted through a wavelength selector which selectively transmits the light to be detected. The present invention relates to an optical measurement method that guides to a detector to perform measurement, and relates to an optical measurement auxiliary tool that can be used in such an optical measurement method.

【0002】[0002]

【従来の技術】このような計測方法の従来の技術を、高
温炉内の火炎観察を例に取って、以下説明する。高温炉
内から選択的に固有の波長(この波長を特定検出波長と
呼ぶ)の光を検出する場合、この検出対象光に対して炉
内の高温体から発っせられる輻射がノイズの原因とな
る。このため、従来、光検出器の前方に波長選択器とし
ての選択透過フィルター等を配置して、光計測を行って
いた。光計測には、火炎からの自然発光において、その
特定波長成分を計測しようとするもの、火炎にレーザー
光を照射して、火炎から発生してくる蛍光を計測しよう
とするもの、様々なものが知られている。ここで、自然
発光を捉えようとする場合は、紫外、可視、赤外領域に
於ける輻射光が、ノイズ成分となるのであり、レーザー
光照射に伴う散乱光を捉えようとする場合は、先の自然
発光自体がノイズとなる。従って、計測にあたっては、
このようなノイズ除去を良好におこなう必要がある。
2. Description of the Related Art A conventional technique of such a measuring method will be described below by taking a flame observation in a high temperature furnace as an example. When light with a specific wavelength (this wavelength is called a specific detection wavelength) is selectively detected from inside the high-temperature furnace, the radiation emitted from the high-temperature body inside the furnace causes the noise for this detection target light. . Therefore, conventionally, a selective transmission filter or the like as a wavelength selector is arranged in front of the photodetector to perform optical measurement. There are various types of light measurement, such as those that try to measure the specific wavelength component of spontaneous emission from the flame, those that measure the fluorescence emitted from the flame by irradiating the flame with laser light. Are known. Here, when trying to capture spontaneous emission, radiant light in the ultraviolet, visible, and infrared regions becomes a noise component, and when trying to capture scattered light accompanying laser light irradiation, The natural light emission of becomes noise. Therefore, when measuring
It is necessary to satisfactorily remove such noise.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、従来の
方法で採用されてきた選択透過フィルター等にあって
は、そのノイズ成分に対する遮蔽特性が往々にして完全
でないため、ノイズとしての自然発光、高温赤熱状態に
ある炉内からの輻射などの影響が大きい場合には、S
(検出対象光の信号強度)/N(前記検出対象光以外の
成分の信号強度)が低下し、検出感度が低下するという
問題が存在した。また、光検出器に耐熱処理が施されて
いない場合は、検出器が炉内の高温体からの輻射熱の影
響を受けて故障しやすくなるという問題があった。
However, in the selective transmission filter or the like which has been adopted in the conventional method, the shielding property against the noise component is often not perfect, so that spontaneous emission as noise, high temperature red heat is generated. If the influence of radiation from the furnace in the state is large, S
There has been a problem that (signal intensity of light to be detected) / N (signal intensity of components other than the light to be detected) is lowered, and detection sensitivity is lowered. Further, when the photodetector is not heat-resistant, there is a problem that the detector is susceptible to radiant heat from the high temperature body in the furnace and is likely to fail.

【0004】従って、本願発明の目的は、S/N比が高
く、光検出器への熱の影響が少ない状態で光計測を行え
る光計測方法を得るとともに、このような手法に使用す
ることができる光計測補助具を得ることにある。
Therefore, an object of the present invention is to obtain an optical measurement method capable of performing optical measurement in a state where the S / N ratio is high and the influence of heat on the photodetector is small, and it is possible to use it in such a method. To get a light measurement auxiliary tool.

【課題を解決するための手段】[Means for Solving the Problems]

〔構成〕上記の目的を達成するための本発明による燃焼
室内の高温状態にある被検体から発生される特定検出波
長の検出対象光を、この検出対象光を選択的に透過する
波長選択器を介して光検出器に導いて計測する光計測方
法の特徴手段は、以下の通りである。即ち、被検体から
の検出対象光を波長選択器側に反射する選択反射ミラー
を被検体から波長選択器に到る光路上に配設し、検出対
象光を光検出器に導いて計測をおこなうのである。 〔作用〕この構成にあっては、被検体から発生される光
は選択反射ミラーに送られ、このミラーにより特定検出
波長の検出対象光が波長選択器側に反射される。一方、
ノイズ成分である特定検出波長以外の光は、選択反射ミ
ラーを透過し、波長選択器側へ向かうことはない。そし
て、波長選択器においては、その波長選択特性により、
計測に必要な検出対象光が選択されて、光検出器に送ら
れる。従って、従来のように透過型の波長選択器を備え
た構成に比べて、S/N比を格段に向上した状態で光計
測をおこなうことができる。さらに、光検出器に於ける
加熱要因となる輻射線(例えば赤熱状態にある燃焼室を
構成する炉壁からの輻射線)は、これをノイズ成分とし
て、選択反射ミラーの透過下手側に送れるため、光検出
器が加熱されて故障を起こす等の不都合を発生すること
もない。さて、このような構成との対比にあっては、選
択反射ミラー、波長選択器の組み合わせの代わりに、波
長選択器を複数枚備えることも考えられるが、この場
合、検出対象光の減衰が大きくなりすぎる。例えば、選
択反射ミラーにあっては、検出対象光を99%程度まで
反射し、減衰することなく波長選択器まで送れるが、波
長選択器の場合は、この減衰度が比較的大きい。従っ
て、本願の構成が格段に優位である。 〔構成〕さて、上記の方法を採るに、前記被検体が、高
温炉内に形成される火炎であることが好ましい。 〔作用〕高温炉内にあっては、一般に炉内壁が高温赤熱
状態にあり、当然この壁からの輻射も多く発生してい
る。しかしながら、炉内に於ける火炎の状態を良好に把
握しようとする要請は大きい。このような場合に、例え
ば、波長308nm近傍の検出対象光を、輻射光等と区
別して捉えると、炉内に於ける火炎の状態が良好に捉え
られる。そして、計測にあたり、先に説明した本願の特
徴手段を採用すると、炉内の火炎の状態をS/N比の高
い状態で、光検出器に大きな加熱負荷を加えることな
く、計測をおこなうことができる。 〔構成〕さらに、上記の方法を採るに、前記特定検出波
長の検出対象光が、前記被検体にレーザー光を照射する
ことにより、前記被検体から発する光であることが好ま
しい。 〔作用〕レーザー光を火炎等の被検体に照射し、この被
検体から発生される誘起蛍光等を検出して、火炎内に於
ける特定成分の分布を見たり、温度分布に推定を行った
りする場合に、S/N比を高めることは、必須の要件で
はあるが、火炎、火炎の周囲環境状況等によっては、従
来なかなか実現できないたぐいのものであった。しかし
ながら、本願にあっては、選択反射ミラーの計測系への
挿入という簡単な操作で、非常に有用なレーザー計測法
を、さらに使用勝手の良好なものとすることができた。 〔構成〕上記の目的を達成するための、光計測補助具の
特徴構成は以下の通りである。即ち、これは、光が導入
される入光部と、特定検出波長の検出対象光が導出され
る出光部とを備え、前記入光部と前記出光部との間の前
記検出対象光光路上に、前記入光部側から、前記入光部
からの前記検出対象光を前記出光部側に反射する選択反
射ミラーと前記検出対象光を選択的に透過する波長選択
器とを、記載順に備えて構成されている。 〔作用〕この光計測補助具は、検出対象光の光路に、入
光側から、入光部、選択反射ミラー、波長選択器、出光
部を、記載順に備えて構成されている。そして、使用に
あたっては、光検出器の検出光導入部位に出光部を対向
させて、さらに、発光している被検出体に入光部を対向
されて、配設して使用される。入光部から入光した光は
選択反射ミラーで、検出対象光とその他の光(ノイズ成
分)とに分けられ、検出対象光が波長選択器、出光部に
導かれて、光検出器に導入されて、光計測に利用され
る。従って、上記方法の説明にあたって説明したと同様
の作用・効果を発揮することができる。さらに、この光
計測補助具にあっては、これが一体に構成されるため、
良好な光学的性能を維持できるとともに、使用勝手のよ
い状態で、これを使用することができる。
[Structure] Detection target light of a specific detection wavelength generated from a subject in a high temperature state in the combustion chamber according to the present invention for achieving the above object, a wavelength selector that selectively transmits the detection target light. The characteristic means of the light measurement method of guiding the light to the photodetector via the light detector is as follows. That is, a selective reflection mirror that reflects the detection target light from the subject to the wavelength selector side is arranged on the optical path from the subject to the wavelength selector, and the detection target light is guided to the photodetector to perform measurement. Of. [Operation] In this configuration, the light generated from the subject is sent to the selective reflection mirror, and the detection target light of the specific detection wavelength is reflected to the wavelength selector side by this mirror. on the other hand,
Light other than the specific detection wavelength, which is a noise component, passes through the selective reflection mirror and does not go to the wavelength selector side. And in the wavelength selector, due to its wavelength selection characteristics,
The detection target light required for measurement is selected and sent to the photodetector. Therefore, the optical measurement can be performed in a state in which the S / N ratio is remarkably improved as compared with the conventional configuration including the transmission type wavelength selector. Furthermore, the radiation that causes heating in the photodetector (for example, the radiation from the furnace wall that constitutes the combustion chamber in the red heat state) can be sent as a noise component to the transmission lower side of the selective reflection mirror. Also, the inconvenience such as the photodetector being heated and causing a failure does not occur. Now, in contrast to such a configuration, it is possible to provide a plurality of wavelength selectors instead of the combination of the selective reflection mirror and the wavelength selector, but in this case, the attenuation of the detection target light is large. Too much. For example, in the selective reflection mirror, the light to be detected is reflected up to about 99% and can be sent to the wavelength selector without being attenuated, but in the case of the wavelength selector, this attenuation degree is relatively large. Therefore, the configuration of the present application is significantly superior. [Structure] In the above method, it is preferable that the subject is a flame formed in a high temperature furnace. [Operation] In a high-temperature furnace, the inner wall of the furnace is generally in a high-temperature, red-hot state, and a large amount of radiation is naturally generated from this wall. However, there is a great demand to satisfactorily understand the flame condition in the furnace. In such a case, for example, if the detection target light near the wavelength of 308 nm is captured separately from the radiant light, the state of the flame in the furnace can be captured well. When the characteristic means of the present application described above is adopted for the measurement, the flame state in the furnace can be measured with a high S / N ratio without applying a large heating load to the photodetector. it can. [Configuration] Furthermore, in the above method, it is preferable that the detection target light of the specific detection wavelength is light emitted from the subject by irradiating the subject with laser light. [Function] Irradiating a subject such as a flame with a laser beam and detecting the induced fluorescence generated from the subject to see the distribution of a specific component in the flame and estimate the temperature distribution. In this case, increasing the S / N ratio is an essential requirement, but depending on the flame, the surrounding environment of the flame, etc., it has been difficult to realize in the past. However, in the present application, a very useful laser measurement method can be made more convenient by a simple operation of inserting the selective reflection mirror into the measurement system. [Structure] The characteristic structure of the optical measurement auxiliary tool for achieving the above object is as follows. That is, this is provided with a light entrance portion into which light is introduced and a light exit portion from which detection target light of a specific detection wavelength is led out, and on the detection target light optical path between the light entrance portion and the light exit portion. In the, from the light incident portion side, a selective reflection mirror that reflects the detection target light from the light incident portion to the light output portion side, and a wavelength selector that selectively transmits the detection target light, comprising in order of description. Is configured. [Operation] This optical measurement auxiliary tool is configured to include, from the light entrance side, a light entrance part, a selective reflection mirror, a wavelength selector, and a light exit part in the optical path of the light to be detected. In use, the light exit portion is opposed to the detection light introduction portion of the photodetector, and the light entrance portion is opposed to the light-emitting detection object, and is used. The light incident from the light incident part is separated into detection target light and other light (noise component) by the selective reflection mirror, and the detection target light is guided to the wavelength selector and the light output part and introduced to the photodetector. And is used for optical measurement. Therefore, the same action and effect as described in the description of the above method can be exhibited. Furthermore, in this optical measurement auxiliary tool, since it is integrally configured,
It is possible to maintain good optical performance and to use it in a convenient state.

【0005】[0005]

【発明の実施の形態】本願の実施の形態を以下、図面を
参照しながら説明する。説明にあたっては、被検体であ
る加熱炉1内に形成される火炎2の状態を、光検出器で
あるスペクトル分析器3で観察し、その炉内火炎スペク
トルを計測する場合の例について説明する。この場合、
加熱炉内の空間が燃焼室内の空間に対応している。図1
は、本願の光計測方法を使用して、観測をおこなってい
る状態の装置構成を示しており、図5は、これを対比で
きる従来の装置構成を示している。バーナー4を備えた
加熱炉1内には、このバーナー4によって火炎2が形成
されている。同図において、模式的に火炎2を破線で示
しているが、実際には、高温状態にある加熱炉1内にあ
っては、内壁面5に於ける赤熱等との関係から火炎2を
目視(識別)することは、殆ど不可能である。さて、前
記加熱炉1には観測用の観測窓6が設けられており、こ
の窓6から、光が出てくる。そして、本願の方法を採る
場合は、この観測窓6に対して、これにほぼ45度で交
わる姿勢で選択反射ミラー7を配設する。即ち、観測窓
6から図1左側に直進する光8に対して、これに斜行す
る状態で選択反射ミラー7を配設し、選択反射ミラー7
による反射経路9は、前記光8の経路とは直交する図1
上下方向を向くものとされている。一方、このミラー7
を透過する光はミラー7を抜けて直進する。即ち、透過
光の光路と反射光の光路は異なるものとされるととも
に、選択反射ミラー7に対する入射光の光路と反射光の
光路も異なるものとされている。さて、反射経路9の下
手側には、波長選択器としての選択透過フィルター1
0、スペクトル分析器3が記載順に備えられている。従
って、選択反射ミラー7によって反射される、検出対象
となる特定検出波長の検出対象光が光検出器に導入され
る。
BEST MODE FOR CARRYING OUT THE INVENTION Embodiments of the present invention will be described below with reference to the drawings. In the description, an example will be described in which the state of the flame 2 formed in the heating furnace 1 which is the subject is observed by the spectrum analyzer 3 which is a photodetector, and the flame spectrum in the furnace is measured. in this case,
The space inside the heating furnace corresponds to the space inside the combustion chamber. FIG.
Shows a device configuration in a state in which observation is performed using the optical measurement method of the present application, and FIG. 5 shows a conventional device configuration with which this can be compared. In the heating furnace 1 equipped with the burner 4, the flame 2 is formed by the burner 4. In the figure, the flame 2 is schematically shown by a broken line, but actually, in the heating furnace 1 in a high temperature state, the flame 2 is visually observed due to the relationship with the red heat and the like on the inner wall surface 5. It is almost impossible to (identify). Now, the heating furnace 1 is provided with an observation window 6 for observation, and light is emitted from this window 6. Then, when the method of the present application is adopted, the selective reflection mirror 7 is arranged in such a manner that it intersects the observation window 6 at an angle of about 45 degrees. That is, the selective reflection mirror 7 is arranged so as to be oblique to the light 8 traveling straight from the observation window 6 to the left side in FIG.
1 is orthogonal to the path of the light 8 in FIG.
It is supposed to face up and down. On the other hand, this mirror 7
The light passing through passes through the mirror 7 and goes straight. That is, the optical path of transmitted light is different from the optical path of reflected light, and the optical path of incident light and the optical path of reflected light to the selective reflection mirror 7 are also different. On the lower side of the reflection path 9, a selective transmission filter 1 as a wavelength selector is provided.
0 and the spectrum analyzer 3 are provided in the order described. Therefore, the detection target light of the specific detection wavelength, which is the detection target and is reflected by the selective reflection mirror 7, is introduced into the photodetector.

【0006】以下さらに、具体的に使用した各機器の特
性について説明する。選択反射ミラー7としては、中心
波長308nm、半値幅20nm、反射率99%のもの
を使用し、選択透過フィルター10としては、中心波長
308nm、半値幅10nmのものを使用して、火炎の
炉内火炎スペクトルを求めた。従って、この場合は、波
長が308nm近傍のスペクトル情報を主に得たい場合
に対応しており、この波長近傍の情報は、炉壁からの輻
射、太陽光、室内蛍光管の蛍光等を避けたものとなり、
火炎に関する情報を良く代表できるものである。結果を
図2に示した。図2は横軸が波長であり、縦軸が各波長
に於ける光信号強度を示している。結果、中心波長30
8nm近傍の信号のみが良好に検出されていることがわ
かる。
The characteristics of each of the concretely used devices will be described below. The selective reflection mirror 7 has a center wavelength of 308 nm, a half width of 20 nm, and a reflectance of 99%. The selective transmission filter 10 has a center wavelength of 308 nm and a half width of 10 nm. The flame spectrum was determined. Therefore, this case corresponds mainly to the case where it is desired to obtain spectral information near the wavelength of 308 nm, and the information near this wavelength avoids radiation from the furnace wall, sunlight, fluorescence of indoor fluorescent tubes, and the like. Become a thing,
It can well represent information about flames. The results are shown in FIG. In FIG. 2, the horizontal axis represents wavelength and the vertical axis represents optical signal intensity at each wavelength. As a result, center wavelength 30
It can be seen that only the signal in the vicinity of 8 nm is satisfactorily detected.

【0007】以上が、本願の方法を使用した光計測の結
果であるが、上記の結果との比較のために、従来手法に
おいても、光計測をおこなった。この例の場合の装置系
を図5に、得られた信号スペクトルを図6に示した。図
5において対応する機器を図1と同一の図番で示してい
る。この場合は、当然、観測窓6から直交する方向に、
選択透過フィルター10、スペクトル分析器3が配設さ
れる。図2との比較において、図6の結果をみると、従
来手法にあっては、検出対象の308nm付近の信号は
良好に捉えられているものの、350nm以上の信号成
分が比較的多く含まれている。従って、図2の結果と図
6の結果を比較すると、前者の方が格段に優れている。
The above is the result of the optical measurement using the method of the present invention. For comparison with the above result, the optical measurement was also performed in the conventional method. The apparatus system in this example is shown in FIG. 5, and the obtained signal spectrum is shown in FIG. Corresponding devices are shown in FIG. 5 by the same drawing numbers as in FIG. In this case, of course, in the direction orthogonal to the observation window 6,
A selective transmission filter 10 and a spectrum analyzer 3 are provided. In comparison with FIG. 2, the result of FIG. 6 shows that the conventional method satisfactorily captures the signal in the vicinity of 308 nm to be detected, but contains a relatively large amount of signal components of 350 nm or more. There is. Therefore, comparing the result of FIG. 2 with the result of FIG. 6, the former is remarkably superior.

【0008】以上が、本願の実施の形態であるが、この
ような形態で光計測をおこなう場合にあっては、図3に
示すような光計測補助具50を使用することが好まし
い。この光計測補助具50は、光が導入される入光部5
1と、特定検出波長の検出対象光が導出される出光部5
2とを備え、入光部51と出光部52との間の検出対象
光光路53上に、入光部側から、入光部51からの検出
対象光を出光部側に反射する選択反射ミラー55と検出
対象光を選択的に透過する波長選択器56とを、記載順
に備えて構成されている。従って、入光部51を前記観
測窓6に向けて、出光部52を光検出器に向けて、簡便
に使用できる。この場合もまた、選択反射ミラー55に
対する入射光の光路と、このミラー55を透過した光の
光路及びミラー55によって反射される検出対象光の光
路とは異なっている。
The above is the embodiment of the present application, but in the case of performing the optical measurement in such a form, it is preferable to use the optical measurement auxiliary tool 50 as shown in FIG. The light measurement assisting tool 50 includes a light entering section 5 into which light is introduced.
1 and the light output part 5 from which the detection target light of the specific detection wavelength is derived.
2 and a selective reflection mirror for reflecting the detection target light from the light incident portion 51 to the light emission portion side on the detection target light optical path 53 between the light incident portion 51 and the light emission portion 52. 55 and a wavelength selector 56 that selectively transmits light to be detected are provided in the order described. Therefore, it is possible to easily use the light incident section 51 toward the observation window 6 and the light emitting section 52 toward the photodetector. Also in this case, the optical path of the incident light to the selective reflection mirror 55 is different from the optical path of the light transmitted through the mirror 55 and the optical path of the detection target light reflected by the mirror 55.

【0009】〔別実施の形態〕本願の別実施の形態につ
いて以下説明する。 (イ)上記の実施の形態にあっては、光検出器としては
スペクトル分析器を使用する例を示したが、これは、光
を検出対象として検出するものであればよく、これは、
上記のものの他、CCDカメラ、半導体光センサ、光電
管等であってもよい。 (ロ)上記の実施の形態にあっては、炉内の火炎を対象
とする場合を示したが、被検体としては、ボイラ、ター
ビン燃焼器、エンジン内等の閉空間内にある火炎であっ
てもよい。即ち、所謂、壁面等に覆われた閉空間である
燃焼室内に形成される火炎を光計測手法により計測する
場合に、本願の手法は好適に適応できる。 (ハ)上記の実施の形態にあっては、被検体として炉内
の火炎をそのまま観測したが、検出対象光の発生形態を
問うものではない。従って、自然発光の観測の他、LI
F、CARS、Raman散乱、Rayleigh散
乱、PIV法等を使用して、光計測をおこなう場合にあ
っても、本願の手法は好適に採用できる。 (ニ)上記の実施の形態にあっては、選択反射ミラー7
を単一、検出対象光の光路上に備えたが、図4に示すよ
うに、これを複数個備えて本願を適応することも好まし
い。尚、特許請求の範囲の項に図面との対照を便利にす
るために符号を記すが、該記入により本発明は添付図面
の構成に限定されるものではない。
Another Embodiment Another embodiment of the present application will be described below. (A) In the above embodiment, an example in which a spectrum analyzer is used as the photodetector has been shown, but this may be any as long as it detects light as a detection target.
Other than the above, a CCD camera, a semiconductor photosensor, a photoelectric tube, or the like may be used. (B) In the above embodiment, the case where the flame in the furnace is targeted was shown, but the subject is a flame in a closed space such as a boiler, a turbine combustor, or an engine. May be. That is, the method of the present application can be suitably applied to the case where the flame formed in the combustion chamber, which is a so-called closed space covered by the wall surface or the like, is measured by the optical measurement method. (C) In the above-described embodiment, the flame in the furnace was observed as it was as the subject, but it does not matter how the detection target light is generated. Therefore, in addition to observation of spontaneous emission,
Even when optical measurement is performed using F, CARS, Raman scattering, Rayleigh scattering, PIV method, or the like, the method of the present application can be preferably adopted. (D) In the above embodiment, the selective reflection mirror 7
However, as shown in FIG. 4, it is also preferable to provide a plurality of them on the optical path of the detection target light to apply the present invention. In the claims, reference numerals are provided for convenience of comparison with the drawings, but the present invention is not limited to the configuration shown in the attached drawings.

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

【図1】本願光計測方法を使用して火炎スペクトルを計
測している状態を示す図
FIG. 1 is a diagram showing a state in which a flame spectrum is measured using the optical measurement method of the present application.

【図2】本願方法によって得られる火炎スペクトルを示
す図
FIG. 2 is a diagram showing a flame spectrum obtained by the method of the present application.

【図3】本願の光計測補助具の構成を示す図FIG. 3 is a diagram showing a configuration of an optical measurement auxiliary tool of the present application.

【図4】本願の別実施の形態を示す図FIG. 4 is a diagram showing another embodiment of the present invention.

【図5】従来光計測方法を使用して火炎スペクトルを計
測している状態を示す図
FIG. 5 is a diagram showing a state in which a flame spectrum is measured using a conventional optical measurement method.

【図6】従来方法によって得られる火炎スペクトルを示
す図
FIG. 6 is a diagram showing a flame spectrum obtained by a conventional method.

【符号の説明】[Explanation of symbols]

2 被検体 3 光検出器 7 選択反射ミラー 10 波長選択器 51 入光部 52 出光部 55 選択反射ミラー 56 波長選択器 2 subject 3 photodetector 7 selective reflection mirror 10 wavelength selector 51 light input part 52 light output part 55 selective reflection mirror 56 wavelength selector

───────────────────────────────────────────────────── フロントページの続き (72)発明者 岡本 秀樹 大阪府大阪市中央区平野町四丁目1番2号 大阪瓦斯株式会社内 ──────────────────────────────────────────────────の Continued on the front page (72) Inventor Hideki Okamoto Osaka Gas Co., Ltd. 4-1-2, Hirano-cho, Chuo-ku, Osaka

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 燃焼室内の高温状態にある被検体(2)
から発生される特定検出波長の検出対象光を、前記検出
対象光を選択的に透過する波長選択器(10)を介して
光検出器(3)に導いて計測する光計測方法であって、
前記被検体(2)からの前記検出対象光を前記波長選択
器側に反射する選択反射ミラー(7)を前記被検体
(2)から前記波長選択器(10)に到る光路上に配設
し、前記検出対象光を前記光検出器(3)に導いて計測
する光計測方法。
1. A subject (2) in a combustion chamber in a high temperature state
An optical measurement method of guiding the detection target light of a specific detection wavelength generated from the photodetector (3) through a wavelength selector (10) that selectively transmits the detection target light, and measuring the light.
A selective reflection mirror (7) that reflects the detection target light from the subject (2) to the wavelength selector side is arranged on the optical path from the subject (2) to the wavelength selector (10). Then, the optical measurement method of guiding the detection target light to the photodetector (3) and measuring the same.
【請求項2】 前記被検体が、炉内に形成される火炎で
ある請求項1記載の光計測方法。
2. The optical measurement method according to claim 1, wherein the subject is a flame formed in a furnace.
【請求項3】 前記特定検出波長の検出対象光が、前記
被検体(2)にレーザー光を照射することにより、前記
被検体(2)から発する光である請求項1または2記載
の光計測方法。
3. The optical measurement according to claim 1, wherein the detection target light of the specific detection wavelength is light emitted from the subject (2) by irradiating the subject (2) with a laser beam. Method.
【請求項4】 光が導入される入光部(51)と、特定
検出波長の検出対象光が導出される出光部(52)とを
備え、前記入光部(51)と前記出光部(52)との間
の前記検出対象光光路上に、前記入光部側から、前記入
光部(51)からの前記検出対象光を前記出光部側に反
射する選択反射ミラー(55)と前記検出対象光を選択
的に透過する波長選択器(56)とを、記載順に備えた
光計測補助具。
4. A light entrance part (51) into which light is introduced and a light exit part (52) from which detection target light of a specific detection wavelength is led out, and the light entrance part (51) and the light exit part (52). 52) and a selective reflection mirror (55) that reflects the detection target light from the light incident part (51) from the light incident part side to the light output part side on the detection target light optical path between the light reflection part and the light reflection part. An optical measurement assisting tool, comprising: a wavelength selector (56) that selectively transmits light to be detected.
JP8063982A 1996-03-21 1996-03-21 Optical measuring method and optical measuring aid Pending JPH09257582A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8063982A JPH09257582A (en) 1996-03-21 1996-03-21 Optical measuring method and optical measuring aid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8063982A JPH09257582A (en) 1996-03-21 1996-03-21 Optical measuring method and optical measuring aid

Publications (1)

Publication Number Publication Date
JPH09257582A true JPH09257582A (en) 1997-10-03

Family

ID=13245009

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8063982A Pending JPH09257582A (en) 1996-03-21 1996-03-21 Optical measuring method and optical measuring aid

Country Status (1)

Country Link
JP (1) JPH09257582A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009515079A (en) * 2005-11-04 2009-04-09 ゾロ テクノロジーズ,インコーポレイティド Method and apparatus for spectroscopic measurements in a combustor of a gas turbine engine
CN105157848A (en) * 2015-07-31 2015-12-16 南京理工大学 Device for measuring temperature of solid propellant during laser loading by using infrared thermometer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009515079A (en) * 2005-11-04 2009-04-09 ゾロ テクノロジーズ,インコーポレイティド Method and apparatus for spectroscopic measurements in a combustor of a gas turbine engine
CN105157848A (en) * 2015-07-31 2015-12-16 南京理工大学 Device for measuring temperature of solid propellant during laser loading by using infrared thermometer

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