JPS5965230A - Flame air ratio detecting device - Google Patents

Flame air ratio detecting device

Info

Publication number
JPS5965230A
JPS5965230A JP17590982A JP17590982A JPS5965230A JP S5965230 A JPS5965230 A JP S5965230A JP 17590982 A JP17590982 A JP 17590982A JP 17590982 A JP17590982 A JP 17590982A JP S5965230 A JPS5965230 A JP S5965230A
Authority
JP
Japan
Prior art keywords
intensity
light
air ratio
ratio
flame
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
JP17590982A
Other languages
Japanese (ja)
Inventor
Yasutsugu Matsui
松井 安次
Hideki Komori
秀樹 古森
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP17590982A priority Critical patent/JPS5965230A/en
Publication of JPS5965230A publication Critical patent/JPS5965230A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/314Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Spectrometry And Color Measurement (AREA)

Abstract

PURPOSE:To detect an air ratio quickly and accurately, by dividing the spectrum in the vicinity of the peak wavelength of light emitted from a flame, obtaining the intensity of the light rays, and obtaining the air ratio from the intensity ratio between the two different peaks. CONSTITUTION:Light emitted from a preliminarily mixed flame 1 passes through an objective lens 2 and a slit 3. The light is sequentially transmitted through windows A-C of a rotary disk 4 and inputted to a light detecting element 6. The window A can pass the light having all wavelengths. The windows B and C have interference filters, which transmit the light rays, whose peak wavelengths are in the vicinities of (3100Angstrom ) for an OH group and (5165Angstrom ) for C2 group. The detected signals are inputted to an operation circuit 8, and the detected signal intensity ratio I1/I2 between the OH group and the C2 group is computed. An air ratio is computed by a computing circuit 9 based on the computed value from the circuit 8, and the result is displayed on a display device 10. Thus the air ratio is detected quickly and accurately.

Description

【発明の詳細な説明】 本発明は予混合火炎等の火炎の空気比(供給空5気量/
理論空気片)を検出する装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention improves the air ratio of a flame such as a premixed flame (supplied air 5 volume/
The present invention relates to a device for detecting air particles (theoretical air particles).

予混合火炎の燃焼特性は空気比でtデは決定されること
は周知の事実でアシ、燃焼制御においてはこの空気比を
敏速かつ正確に検出することが大きく影響する。
It is a well-known fact that the combustion characteristics of a premixed flame are determined by the air ratio, and rapid and accurate detection of this air ratio has a great influence on combustion control.

ところで、通常の炭化水素系燃料の火炎からの発光は第
1図に示すようなスペクトル分布を持つことはよく知ら
れてお、り、0)I(λ=3100^)、C2(λ:5
165^)、CH(λ=4315A)等のラジカルから
の発光が顕著でおることがわかる。そして、これらのラ
ジカルからの光強度11.Iz、Isは空気比に対して
第2図(a)の如く多価関数型の関係となることも調べ
られる。
By the way, it is well known that the light emitted from the flame of ordinary hydrocarbon fuel has a spectral distribution as shown in Figure 1.
It can be seen that light emission from radicals such as 165^) and CH (λ=4315A) is remarkable. Then, the light intensity from these radicals11. It can also be investigated that Iz and Is have a multivalued function type relationship with the air ratio as shown in FIG. 2(a).

本発明は上記に鑑みて為されたもので、火炎から放射さ
れる光のピーク波長近傍部を分光して強度を求め、異な
る2つの強度の比が空気比に対して第2図(C)の如く
略−伝関数型となることに着目して前記強度比から空気
比を求めるようにしたものでおる。
The present invention has been made in view of the above, and the intensity is determined by spectroscopy near the peak wavelength of the light emitted from the flame, and the ratio of the two different intensities to the air ratio is shown in Figure 2 (C). The air ratio is determined from the intensity ratio by paying attention to the fact that it has a substantially -transfer type as shown in FIG.

以下本発明の1実施例を第3図(a)、(b)。An embodiment of the present invention is shown in FIGS. 3(a) and 3(b) below.

(e)に基づいて説明する。The explanation will be based on (e).

図において、1は予混合火炎、2は対物レンズ、3はス
リット、4はスリット3を通過した火炎からの光のピー
ク波長近傍部を分光する光選別手段としての光干渉フィ
ルターを有した回転円板で、周方向等間隔に全波長の光
が通過可能な窓A10Hのビーク波長(3100^)近
傍部が通過可能な光学干渉フィルターが取付けられた窓
BとC2のビーク波長(5165A)近傍部が通過可能
な光学干渉フィルターが取付けられた窓Cを有する。5
は回転用板4を回転駆動して順次窓A。
In the figure, 1 is a premixed flame, 2 is an objective lens, 3 is a slit, and 4 is a rotating circle with an optical interference filter as a light selection means for separating the light from the flame that has passed through the slit 3 in the vicinity of the peak wavelength. The area near the peak wavelength (5165A) of windows B and C2 is installed with an optical interference filter that allows light of all wavelengths to pass through the plate at equal intervals in the circumferential direction and allows the area near the peak wavelength (3100^) of window A10H to pass through. It has a window C equipped with an optical interference filter that allows the light to pass therethrough. 5
The rotating plate 4 is rotated to sequentially open the windows A.

B、Cをスリット3に位置せしめる電動機、6は窓A、
B、Cを通過した光をその強度に応じた強さの電気エネ
ルギに変換する光検出素子、Tは対物レンズ2、スリッ
ト3、回転円板4、電動機5と光検出素子6等を収容し
た本体ケース、8は窓Aを通過した光に応じた光検出素
子6からの゛信号強度Ioを受けて動作開始し、所定時
間後に順に窓B全通過した光に応じた信号強度11と窓
Cfc通過した光に応じた信号強度工2とを受けて11
/I2の演η:を行なう演算回路で、前ムピ光検出素子
6とともに光強夏検出手段並びに強度比演算手段として
作用する。9は演算回路8の出力から工1/I2の値に
応じた空気比μを算出する算出回路で、空気比判定手段
として作用する。10は算出回路9からの信号を受けて
算出した空気比μの値を表示する表示装置である。
Electric motor that positions B and C in slit 3, 6 is window A,
A photodetection element that converts the light passing through B and C into electrical energy with an intensity corresponding to the intensity of the light; T houses an objective lens 2, a slit 3, a rotating disk 4, an electric motor 5, a photodetection element 6, etc. The main body case 8 starts operating upon receiving the signal intensity Io from the photodetector element 6 corresponding to the light that has passed through the window A, and after a predetermined time, it sequentially detects the signal intensity 11 corresponding to the light that has completely passed through the window B and the window Cfc. Signal strength adjustment 2 and 11 according to the passed light
It is an arithmetic circuit that performs the calculation η: of /I2, and functions together with the front light detection element 6 as a light intensity/summer detection means and an intensity ratio calculation means. Reference numeral 9 denotes a calculation circuit that calculates the air ratio μ according to the value of 1/I2 from the output of the arithmetic circuit 8, and acts as an air ratio determination means. A display device 10 displays the value of the air ratio μ calculated in response to the signal from the calculation circuit 9.

かかる構成の空気比検出装置では、予混合火炎1の前に
本体ケース7を位置させ、図示しない動作スイッチを操
作すると、電動機5が動作開始し回転円板4が回転する
。そして、スリット3と回転円板4の窓Aとが一致する
と光検出素子6を介して信号強度Ioが演算回路8に入
力され、演算回路8が動作開始する。演算回路8が窓B
、Cを介して順にOHの信号強度11とC2の信号強度
工2を受け、それらの強度比It/I2を演算する。3
1出回路9はこの演算値を受け、これに応じた空気比μ
k 7J−出して表示装置1oに出力するので、表示装
置10がこの値を速やかに表示する。そして、再びスリ
ット3と窓Aとが一致すると演算回路8がリセットされ
、上記と同様に空気比μが算出されて表示装置10に新
たな値が表示され、常時空気比μを監視できる。
In the air ratio detection device having such a configuration, when the main body case 7 is positioned in front of the premix flame 1 and an operation switch (not shown) is operated, the electric motor 5 starts operating and the rotating disk 4 rotates. When the slit 3 and the window A of the rotary disk 4 match, the signal intensity Io is input to the arithmetic circuit 8 via the photodetector element 6, and the arithmetic circuit 8 starts operating. Arithmetic circuit 8 is window B
, C in order to receive the signal strength 11 of OH and the signal strength 2 of C2, and calculate their strength ratio It/I2. 3
The 1 output circuit 9 receives this calculated value and calculates the air ratio μ accordingly.
k7J- and outputs it to the display device 1o, so the display device 10 quickly displays this value. Then, when the slit 3 and the window A match again, the arithmetic circuit 8 is reset, the air ratio μ is calculated in the same way as above, and a new value is displayed on the display device 10, so that the air ratio μ can be constantly monitored.

また、1つの光検出素子6を介して光の強度を求める構
成であるから該光検出素子6の経時変化や受光面の塵埃
等の付着にょシ強度比が影響されることがなく検出精度
の悪化を招くこともない。
In addition, since the light intensity is determined through one photodetection element 6, the intensity ratio is not affected by changes in the photodetection element 6 over time or adhesion of dust etc. to the light receiving surface, which improves the detection accuracy. It will not cause any deterioration.

尚、この実施例では強度比を算出する対象としてOH”
とC2“ のラジカルを選択したが、この理由はOH”
とC2” の強度比が燃焼量、バーナ壁温度等の燃焼条
件の変動にかかわらずtデとんど一定となることを発明
者等が確認して高検出精度を得られることがわかったか
らであシ、多少の検出精度の低下を許容できるならば、
OH“とCH“或イハ02″′ とCH等の組合せでも
よい。
In this example, the object for calculating the intensity ratio is OH"
The reason for this is OH”.
This is because the inventors confirmed that the intensity ratio of t and C2'' remains almost constant regardless of fluctuations in combustion conditions such as combustion amount and burner wall temperature, and found that high detection accuracy can be obtained. Yes, if you can tolerate a slight decrease in detection accuracy,
A combination of OH" and CH" or IHA02"' and CH may also be used.

第4図(a )、(b )、(e )は他の実施例を表
わしたもので、このものは上記実施例を更に改良して検
出精度を良好としたものである。即ち、回転円板4に、
全波長の光が通過可能々窓A、OH“のビーク波長(3
100X)近傍部が通過可能な光学干渉フィルターが取
付けられた窓B、3100人近傍の連続スペクトルを検
出するだめの2950Xの光学干渉フィルターが取付け
られ窓B′。
FIGS. 4(a), (b), and (e) show another embodiment, which is a further improvement of the above embodiment to improve the detection accuracy. That is, on the rotating disk 4,
All wavelengths of light can pass through.Beak wavelength of window A, OH" (3
Window B is equipped with an optical interference filter that allows the 100X) vicinity to pass through, and window B' is equipped with a 2950X optical interference filter that allows the detection of a continuous spectrum in the vicinity of 3100 people.

c 2+  のビーク波長(51655,)近傍部が通
過可能な光学干渉フィルターが取付けられた窓C1と5
165人近傍の連続スペクトルを検出するだめの530
0Xの光学干渉フィルターが取付けられた窓C′を周方
向等間隔に設ける。そして、演算回路8で窓Aを介して
得られた信号強度I、/からピーク波長(3100X)
近傍の窓A′を介して得られた連続スペクトルの信号強
度工l″を差し引いて正味の信号強度工lII/ を求
めるとともに窓Bを介して得られた信号強度I 2’か
らビーク波長(5165′A)近傍の窓B′を介して得
られた連続スペクトルの信号強度工2″を差し引いて正
味のイa号強度I 2”  ’c求メ、強度比I r”
’/ I z″′fn出し、これを算出回路9へ出力す
る。この他の実施例でtゴ黄炎が混在した場合或いは火
炎以外の物体からの光が測定部に入射した場合でも連続
スペクトルを差し引くものだから正確な空気比μを検出
できる利点もある。
Windows C1 and 5 are equipped with optical interference filters that allow the vicinity of the peak wavelength (51655,) of c 2+ to pass through.
530 to detect continuous spectra in the vicinity of 165 people
Windows C' to which 0X optical interference filters are attached are provided at equal intervals in the circumferential direction. Then, the peak wavelength (3100
The signal intensity factor l'' of the continuous spectrum obtained through the nearby window A' is subtracted to obtain the net signal intensity factor lII/, and the peak wavelength (5165 'A) Subtract the signal strength of the continuous spectrum obtained through the nearby window B' to obtain the net intensity I2"'c, intensity ratio Ir'
'/I z'''fn and outputs this to the calculation circuit 9. In other embodiments, even if yellow flame is present or light from an object other than flame is incident on the measuring section, a continuous spectrum can be obtained. Since it subtracts , it also has the advantage of being able to accurately detect the air ratio μ.

以上説明したように本発明によれば火炎から放射される
光のピーク波長近傍部を分光して強度を求め、異なる2
つのピーク波長近傍部の強度比を算出して、この値に応
じて空気比を検出する構成としたので、空気比を敏速か
つ正確に知ることができ、燃焼制御性能を良好とするこ
とができる。
As explained above, according to the present invention, the intensity of the light emitted from the flame is determined by spectroscopy in the vicinity of the peak wavelength.
The configuration calculates the intensity ratio near the two peak wavelengths and detects the air ratio according to this value, so the air ratio can be quickly and accurately determined and combustion control performance can be improved. .

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

第1図は炭素水素炎からの発光スペクトル分布を示す図
、第2図(a)はOH’ 、、Cz”  、CM”の発
光強度Ix、Iz、Iaと空気比μとの関係を示す図、
第2図(b)は上記発光強度の比即ち、I+ /I2 
、I3 /Iz 、Is /It と空気比μとの関係
を示す図、第3図(lは本発明の1実施例を示す概略構
成図、第3図(b)は同上の回転円板の正面図、第3図
(c)は同上の光検出素子から出力される信号強度の出
力図、第4図(a)は他の実施例を示す軌路構成図、第
4図(b)は同上回転円板の正面図、第4図(c)は同
上の光検出素子から出力される信号強度の出力図である
。 1・・・予混合火炎  2・・・対物レンズ  3・・
・スリット  4・・・回転円板  5・・・電動機 
 6・・・光検出素子  8・・・演算回路  9・・
・算出回路A、 A’ 、 B、 B’・・・窓 代理人葛野信−(#1か1名) 手続補正書!”、(3+ 2’? 昭和  年  月  日 ′41・許庁長官殿 1、事件の表示    特願昭 57−175909号
2、発明の名称    火炎の空気比検出装置3、補正
をする者 事件との関係   91間作出願人 6、補正の内容 0)明細書第3頁第2行に「第2図(C)」とあるを「
第2図(b)」と補正する。 (2)明細@第3頁第16行に「回転用板4」とあるを
「回転円板4」と補正する。 以上 189
Figure 1 is a diagram showing the emission spectrum distribution from a carbon-hydrogen flame, and Figure 2 (a) is a diagram showing the relationship between the emission intensities Ix, Iz, Ia of OH', Cz", CM" and the air ratio μ. ,
FIG. 2(b) shows the ratio of the above emission intensity, that is, I+ /I2
, I3 /Iz , Is /It and the air ratio μ, FIG. A front view, FIG. 3(c) is an output diagram of the signal intensity output from the same photodetecting element as above, FIG. 4(a) is a track configuration diagram showing another embodiment, and FIG. 4(b) is The front view of the rotating disk same as the above, and FIG. 4(c) is an output diagram of the signal intensity output from the light detection element same as the above. 1... Premixed flame 2... Objective lens 3...
・Slit 4... Rotating disk 5... Electric motor
6... Photodetection element 8... Arithmetic circuit 9...
・Calculation circuit A, A', B, B'... Window agent Shin Kuzuno - (#1 or 1 person) Procedural amendment! ”, (3+2'? Showa year, month, day, '41, Director-General of the License Agency, 1, Indication of the case, Patent Application No. 57-175909, 2, Title of the invention, Flame air ratio detection device 3, Compliance with the case of the person making the amendment. Relationship 91 Intercropping Applicant 6, Contents of Amendment 0) In the second line of page 3 of the specification, the phrase “Figure 2 (C)” has been changed to “
2(b)". (2) In the specification @ page 3, line 16, "rotating plate 4" is corrected to "rotating disc 4." More than 189

Claims (3)

【特許請求の範囲】[Claims] (1)火炎から放射される光のピーク波長近傍部を分光
する光学干渉フィルター等の光選別手段と、該光選別手
段によシ分光された波長部の強度を検出する光強度検出
手段と、該光強度検出手段の出力の:異なる2つの強度
から強度比を演算する強度比演算手段と、該強度比演算
手段の出力から強度比に基づいて空気比を判定する空気
比判定手段と、全備えたことを特徴とする火炎の空気比
検出装置。
(1) a light sorting means such as an optical interference filter that separates light emitted from a flame near its peak wavelength, and a light intensity detection means that detects the intensity of the wavelength portion separated by the light sorting means; an intensity ratio calculation means for calculating an intensity ratio from two different intensities of the output of the light intensity detection means; an air ratio determination means for determining an air ratio based on the intensity ratio from the output of the intensity ratio calculation means; A flame air ratio detection device characterized by comprising:
(2)光選別手段はOR(3100人)とC2”(51
65^)の各ラジカルから放射された光のピーク波長近
傍部を分光することを特徴とする特許請求の範囲第1項
記載の火炎の空気比検出装置。
(2) The optical selection means is OR (3100 people) and C2'' (51 people).
65^) The flame air ratio detection device according to claim 1, characterized in that the light emitted from each radical of 65^) is spectrally analyzed in the vicinity of the peak wavelength.
(3)光選別手段はピーク波長近傍部の連続スペクトル
を分光し、演算手段はピーク波長近傍部の強1現と連続
スペクトルの強度との差を演算して強度比を演算するこ
とを特徴とする特許請求の範囲第1項又は第2項に記載
の火炎の空気比検出装置。
(3) The optical sorting means separates the continuous spectrum in the vicinity of the peak wavelength, and the calculation means calculates the difference between the intensity in the vicinity of the peak wavelength and the intensity of the continuous spectrum to calculate an intensity ratio. A flame air ratio detection device according to claim 1 or 2.
JP17590982A 1982-10-06 1982-10-06 Flame air ratio detecting device Pending JPS5965230A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17590982A JPS5965230A (en) 1982-10-06 1982-10-06 Flame air ratio detecting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17590982A JPS5965230A (en) 1982-10-06 1982-10-06 Flame air ratio detecting device

Publications (1)

Publication Number Publication Date
JPS5965230A true JPS5965230A (en) 1984-04-13

Family

ID=16004355

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17590982A Pending JPS5965230A (en) 1982-10-06 1982-10-06 Flame air ratio detecting device

Country Status (1)

Country Link
JP (1) JPS5965230A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6280523A (en) * 1985-10-04 1987-04-14 Hitachi Ltd Method and circuit for detecting flame in gas turbine combustor
JP2013072574A (en) * 2011-09-27 2013-04-22 Tokyo Gas Co Ltd Combustion diagnostic device and method of diagnosing combustion

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS53107890A (en) * 1977-03-03 1978-09-20 Mitsubishi Heavy Ind Ltd Air ratio detecting method in combustion furnace

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS53107890A (en) * 1977-03-03 1978-09-20 Mitsubishi Heavy Ind Ltd Air ratio detecting method in combustion furnace

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6280523A (en) * 1985-10-04 1987-04-14 Hitachi Ltd Method and circuit for detecting flame in gas turbine combustor
JP2013072574A (en) * 2011-09-27 2013-04-22 Tokyo Gas Co Ltd Combustion diagnostic device and method of diagnosing combustion

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