JP3083633B2 - Combustion diagnostic device - Google Patents
Combustion diagnostic deviceInfo
- Publication number
- JP3083633B2 JP3083633B2 JP04081133A JP8113392A JP3083633B2 JP 3083633 B2 JP3083633 B2 JP 3083633B2 JP 04081133 A JP04081133 A JP 04081133A JP 8113392 A JP8113392 A JP 8113392A JP 3083633 B2 JP3083633 B2 JP 3083633B2
- Authority
- JP
- Japan
- Prior art keywords
- combustion
- flame
- soot
- flow rate
- spectral
- 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
- 238000002485 combustion reaction Methods 0.000 title claims description 84
- 238000002835 absorbance Methods 0.000 claims description 41
- 239000004071 soot Substances 0.000 claims description 40
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 33
- 238000003745 diagnosis Methods 0.000 claims description 28
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 claims description 26
- 230000003595 spectral effect Effects 0.000 claims description 25
- 238000001514 detection method Methods 0.000 claims description 18
- 239000000446 fuel Substances 0.000 claims description 16
- UGFAIRIUMAVXCW-UHFFFAOYSA-N Carbon monoxide Chemical compound [O+]#[C-] UGFAIRIUMAVXCW-UHFFFAOYSA-N 0.000 claims description 15
- 238000004020 luminiscence type Methods 0.000 claims description 15
- 239000003546 flue gas Substances 0.000 claims description 14
- 229910002092 carbon dioxide Inorganic materials 0.000 claims description 13
- 239000001569 carbon dioxide Substances 0.000 claims description 13
- 238000012545 processing Methods 0.000 claims description 8
- 238000010183 spectrum analysis Methods 0.000 claims description 6
- 238000004458 analytical method Methods 0.000 claims description 5
- 238000007405 data analysis Methods 0.000 claims description 5
- 238000004611 spectroscopical analysis Methods 0.000 claims 2
- 238000000295 emission spectrum Methods 0.000 description 16
- 238000001228 spectrum Methods 0.000 description 15
- 230000007423 decrease Effects 0.000 description 14
- 230000003287 optical effect Effects 0.000 description 11
- 239000007789 gas Substances 0.000 description 8
- 239000013307 optical fiber Substances 0.000 description 8
- MWUXSHHQAYIFBG-UHFFFAOYSA-N nitrogen oxide Inorganic materials O=[N] MWUXSHHQAYIFBG-UHFFFAOYSA-N 0.000 description 6
- 239000000523 sample Substances 0.000 description 6
- 238000010521 absorption reaction Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 238000012423 maintenance Methods 0.000 description 5
- 230000005855 radiation Effects 0.000 description 5
- 238000004364 calculation method Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 230000006399 behavior Effects 0.000 description 3
- 239000000295 fuel oil Substances 0.000 description 3
- 238000009434 installation Methods 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 239000003921 oil Substances 0.000 description 3
- 239000003245 coal Substances 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 229910002091 carbon monoxide Inorganic materials 0.000 description 1
- 239000000567 combustion gas Substances 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 238000010248 power generation Methods 0.000 description 1
- 230000003134 recirculating effect Effects 0.000 description 1
- 239000004449 solid propellant Substances 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Landscapes
- Control Of Combustion (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、燃焼診断装置に係り、
特に低NOx燃焼等の目的から、排ガス再循環を行なう
バーナが設置される燃焼炉内の、個々のバーナ火炎の燃
焼状態を、火炎発光スペクトルをもとに診断する燃焼診
断装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a combustion diagnostic device,
In particular, the present invention relates to a combustion diagnostic apparatus for diagnosing the combustion state of each burner flame in a combustion furnace provided with a burner for recirculating exhaust gas for the purpose of low NOx combustion or the like, based on a flame emission spectrum.
【0002】[0002]
【従来の技術】公害防止の目的から、ボイラ等の燃焼炉
においては、窒素酸化物、すすおよび一酸化炭素を発生
させないことが必要である。このような燃焼状態を形成
するには、各バーナでの燃料流量、空気流量および燃料
と空気の混合状態等を所定状態に保ち、これにより、燃
焼炉内に極端な高温度領域および極端な低温度領域を形
成させないことが必要である。このような燃焼状態を形
成する際に使用する計測器の一つに、火炎発光スペクト
ルを検出し、このスペクトル特性から燃焼状態を診断す
る装置(以下、燃焼診断装置という)がある。2. Description of the Related Art For the purpose of preventing pollution, it is necessary not to generate nitrogen oxides, soot and carbon monoxide in a combustion furnace such as a boiler. In order to form such a combustion state, the fuel flow rate, the air flow rate, the mixed state of fuel and air, and the like in each burner are maintained in a predetermined state, so that an extremely high temperature region and an extremely low temperature It is necessary not to form a temperature region. As one of the measuring instruments used for forming such a combustion state, there is a device that detects a flame emission spectrum and diagnoses the combustion state from the spectrum characteristic (hereinafter, referred to as a combustion diagnosis device).
【0003】しかし、この燃焼診断装置においては、火
炎発光スペクトルが火炎の揺らぎ、バーナ火炎の相互干
渉のために不規則な変動をしており、燃焼診断を困難に
していた。従来の燃焼診断装置の多くは、この火炎発光
スペクトルの変動について十分な配慮がされておらず、
このため、燃焼診断精度が低下する問題および診断時間
が長くなる問題があった。[0003] However, in this combustion diagnosis apparatus, the flame emission spectrum fluctuates due to the fluctuation of the flame and the mutual interference of the burner flame, making the combustion diagnosis difficult. Many conventional combustion diagnostic devices do not give sufficient consideration to fluctuations in the flame emission spectrum,
For this reason, there has been a problem that the combustion diagnosis accuracy is reduced and a diagnosis time is long.
【0004】この発光スペクトル変動の問題に対し、特
願平3−50252号では、スペクトルの変動は燃料流
量および空気流量等の変動に関係することに着眼し、燃
料流量計および空気流量計等を設置し、測定される火炎
発光スペクトルをそれぞれの流量に基づいて標準化し、
そして標準化した火炎発光スペクトルを燃焼診断ロジッ
クにかける方法が提案された。To cope with this problem of emission spectrum variation, Japanese Patent Application No. 50252/1991 focuses on the fact that spectrum variation relates to variations in fuel flow rate and air flow rate. Installed and standardize the measured flame emission spectrum based on each flow rate,
Then, a method of applying the standardized flame emission spectrum to combustion diagnosis logic was proposed.
【0005】この方法は、診断時間は短縮されたが、各
系統ごとに流量計を設置する必要から装置コストが増大
すること、この流量計の保守に多くの労力が消費される
こと等の経済的問題があった。[0005] Although this method shortens the diagnosis time, it requires the installation of a flow meter for each system, which increases the equipment cost, and the maintenance of the flow meter consumes much labor. Problem.
【0006】[0006]
【発明が解決しようとする課題】上記先行技術は、燃焼
診断精度を低下させる問題および診断時間が長くなる問
題、または各種流量計設置による装置コストの上昇およ
びこれら計器への保守労力の増加等の問題を有してい
た。本発明の目的は、装置コストの上昇および保守労力
の増加を生じることなく、燃焼診断精度を向上でき、か
つ診断時間を短縮できる燃焼診断装置を提供することに
ある。The above prior arts involve problems such as a decrease in the accuracy of combustion diagnosis and a problem of a long diagnosis time, an increase in equipment costs due to the installation of various flow meters, and an increase in maintenance labor for these meters. Had a problem. It is an object of the present invention to provide a combustion diagnostic device that can improve the accuracy of combustion diagnosis and reduce the diagnosis time without increasing the cost of the device and the maintenance labor.
【0007】[0007]
【課題を解決するための手段】上記目的を達成するため
本願の第1の発明は、火炎に対して配置された火炎検出
手段と、その火炎検出手段からの光検出信号を入力する
分光分析手段と、その分光分析手段からの信号を入力し
て演算処理するデータ解析手段とを備え、分光分析手段
により求めた波長ごとのスペクトル強度に基づき、前記
解析手段により、正常燃焼時のスート発光度と水蒸気吸
光度の基準データと燃焼診断すべき検出時のスート発光
度と水蒸気吸光度のデータとを作成してこれにより火炎
の燃焼状態を診断するように構成したことを特徴とする
燃焼診断装置に関する。To achieve the above object, a first invention of the present application is a flame detecting means arranged for a flame, and a spectral analysis means for inputting a light detection signal from the flame detecting means. And data analysis means for inputting a signal from the spectrum analysis means and performing arithmetic processing, based on the spectrum intensity for each wavelength determined by the spectrum analysis means, the soot emission degree during normal combustion by the analysis means, The present invention relates to a combustion diagnostic apparatus characterized in that reference data of water vapor absorbance and data of soot light emission and water vapor absorbance at the time of detection to be diagnosed for combustion are created and the combustion state of the flame is diagnosed based on the data.
【0008】第2の発明は、火炎に対して配置された火
炎検出手段と、その火炎検出手段からの光検出信号を入
力する分光分析手段と、その分光分析手段からの信号を
入力して演算処理するデータ解析手段とを備え、分光分
析手段により求めた波長ごとのスペクトル強度に基づ
き、前記解析手段により、正常燃焼時のスート発光度と
二酸化炭素吸光度の基準データと燃焼診断すべき検出時
のスート発光度と二酸化炭素吸光度のデータとを作成し
てこれにより火炎の燃焼状態を診断するように構成した
ことを特徴とする燃焼診断装置に関する。According to a second aspect of the present invention, there is provided a flame detecting means arranged for a flame, a spectral analyzing means for inputting a light detection signal from the flame detecting means, and a signal input from the spectral analyzing means for calculation. And a data analyzing means for processing, based on the spectral intensity for each wavelength obtained by the spectral analyzing means, by the analyzing means, soot luminescence during normal combustion and reference data of carbon dioxide absorbance and at the time of detection to perform combustion diagnosis The present invention relates to a combustion diagnostic apparatus characterized in that data on soot luminous intensity and carbon dioxide absorbance are created and the combustion state of a flame is diagnosed based on the data.
【0009】第3の発明は、火炎に対して配置された火
炎検出手段と、その火炎検出手段からの光検出信号を入
力する分光分析手段と、その分光分析手段からの信号を
入力して演算処理するデータ解析手段とを備え、分光分
析手段により求めた波長ごとのスペクトル強度に基づ
き、前記解析手段により、正常燃焼時のスート発光度と
水蒸気吸光度の値と変動幅および燃焼診断すべき検出時
のスート発光度と水蒸気吸光度の値および/または変動
幅を求め、かつこれにより燃料流量、空気流量、再循環
燃焼排ガス流量のいずれか一つ以上の状態を診断するご
とく構成したことを特徴とする燃焼診断装置に関する。According to a third aspect of the present invention, there is provided a flame detecting means arranged for a flame, a spectral analyzing means for inputting a light detection signal from the flame detecting means, and a signal input from the spectral analyzing means for calculation. A data analyzing means for processing, based on the spectral intensity for each wavelength obtained by the spectral analyzing means, by the analyzing means, the value of soot luminescence and water vapor absorbance during normal combustion, the fluctuation range, and the time of detection for combustion diagnosis The value and / or fluctuation range of the soot luminous intensity and water vapor absorbance of the soot are determined, and thereby any one or more of a fuel flow rate, an air flow rate, and a recirculation flue gas flow rate is diagnosed. The present invention relates to a combustion diagnostic device.
【0010】第4の発明は、火炎に対して配置された火
炎検出手段と、その火炎検出手段からの光検出信号を入
力する分光分析装置と、その分光分析手段からの信号を
入力して演算処理するデータ解析手段とを備え、分光分
析手段により求めた波長ごとのスペクトル強度に基づ
き、前記解析手段により、正常燃焼時のスート発光度と
二酸化炭素吸光度の値と変動幅および燃焼診断すべき検
出時のスート発光度と二酸化炭素吸光度の値および/ま
たは変動幅とを求め、かつこれにより燃料流量、空気流
量、再循環燃焼排ガス流量のいずれか一つ以上の状態を
診断するように構成したことを特徴とする燃焼診断装置
に関する。According to a fourth aspect of the present invention, there is provided a flame detecting means arranged for a flame, a spectrum analyzer for inputting a light detection signal from the flame detecting means, and a signal input from the spectrum analyzing means for calculation. Data analyzing means for processing, based on the spectrum intensity for each wavelength obtained by the spectral analyzing means, the soot luminous intensity and carbon dioxide absorbance value during normal combustion, the fluctuation range and the detection to be diagnosed by combustion by the analyzing means. Determining the value and / or fluctuation range of the soot luminosity and the carbon dioxide absorbance at the time, and diagnosing at least one of the fuel flow rate, the air flow rate, and the recirculation flue gas flow rate based on the value. The present invention relates to a combustion diagnostic device characterized by the following.
【0011】[0011]
【作用】正常運転燃焼時と燃焼診断すべき運転時につい
て、火炎発光スペクトルの内、スートの発光特性と水蒸
気の吸光特性を検出し、上記2つの場合について比較
し、後述する表1に示される各種燃焼調整と火炎発光ス
ペクトル挙動の関係から、燃料流量、空気流量、再循環
排ガス流量または空気・再循環排ガス混合ガスの旋回力
の変化を知ることができる。The soot emission characteristic and the water vapor absorption characteristic of the flame emission spectrum are detected for the normal operation combustion and the operation for which combustion diagnosis is to be performed, and the above two cases are compared. From the relationship between the various combustion adjustments and the flame emission spectrum behavior, it is possible to know the change in the fuel flow rate, the air flow rate, the recirculation exhaust gas flow rate, or the swirl force of the air / recirculation exhaust gas mixed gas.
【0012】[0012]
i)全体の構成 図1に、この燃焼診断方法を適用する燃焼診断装置の一
例を示す。この燃焼診断装置は、複数個の光プローブ
1、複数個の中継光ファイバ2、光チャンネルセレクタ
3、分光分析装置4、データ解析装置5から主に構成さ
れる。光プローブ1は、一個以上の視野を有している。i) Overall Configuration FIG. 1 shows an example of a combustion diagnosis apparatus to which the combustion diagnosis method is applied. This combustion diagnostic apparatus mainly includes a plurality of optical probes 1, a plurality of relay optical fibers 2, an optical channel selector 3, a spectroscopic analyzer 4, and a data analyzer 5. The optical probe 1 has one or more visual fields.
【0013】これにより、火炎10からの光は、各光プ
ローブ1で受光され、中継光ファイバ2を通して、光チ
ャンネルセレクタ3に移送される。光チャンネルセレク
タ3によって、解析対象の中継光ファイバ2が選ばれ、
この中継光ファイバ2によって移送された火炎光が分光
分析装置4によってスペクトル分析されたのち電気信号
に変換される。データ解析装置5は、このスペクトル分
析結果に基づいて、このときの燃焼状態を明示する。Thus, the light from the flame 10 is received by each optical probe 1 and transferred to the optical channel selector 3 through the relay optical fiber 2. The relay optical fiber 2 to be analyzed is selected by the optical channel selector 3,
The flame light transferred by the relay optical fiber 2 is spectrally analyzed by the spectroscopic analyzer 4 and then converted into an electric signal. The data analyzer 5 specifies the combustion state at this time based on the spectrum analysis result.
【0014】図2に、重油燃焼火炎の発光スペクトルの
一例を示す。中継光ファイバの光伝送損失が小さい0.
4〜1.6μmの波長域において、0.7μmより長波
長側にスート(炭素質粒子)の発光スペクトルが見ら
れ、この発光スペクトル上の1.1μmおよび1.4μ
m近傍には水蒸気の吸光によるスペクトル強度の減少が
見られる。FIG. 2 shows an example of the emission spectrum of a heavy oil combustion flame. Optical transmission loss of relay optical fiber is small.
In the wavelength range of 4 to 1.6 μm, an emission spectrum of soot (carbonaceous particles) was observed on the longer wavelength side than 0.7 μm, and 1.1 μm and 1.4 μm on this emission spectrum.
Near m, a decrease in the spectrum intensity due to the absorption of water vapor is observed.
【0015】スートの発光特性から、プランクの輻射則
の関係を用い、火炎温度を知ることができる。プランク
の輻射則とは図5に示すように、ある温度での輻射波長
と輻射強度の関係は定まっていることをいう。したがっ
て、火炎の温度を求めるには、波長と強度の関係を求め
ればよい。全波長域にわたって測定するのは困難である
ので、高温のものは通常では波長λ<1μm以下の可視
−近赤外光波長域で測定する。火炎ではこの波長域でス
ート(すすorカーボン)からの発光が優勢といわれて
いる。火炎温度は通常1200°K〜2000°Kの範
囲にあり、この温度範囲では図5から推測されるように
λ=0.8〜1.0μm波長域での強度はほぼ波長にリ
ニアに依存しているので、2〜3点での波長で強度を測
定するだけで、測定点を結ぶ線の傾きにより温度を演算
できる。λ<0.8μm以下で演算しても原理的には問
題ないが、波長が短いほど強度は減少するので測定がむ
つかしくなる。本発明では、0.8〜1.0μm波長域
のスペクトル強度の傾斜値をスート発光度という。温度
測定方法を示すと、あらかじめ実験的に任意の複数波長
のスペクトル強度、例えば0.8μmにおけるスペクト
ル強度と1.0μmのスペクトル強度を測定し、測定値
と温度の関係を求めると図6の関係が得られる。この関
係を用いスペクトル特性から火炎温度の換算が可能とな
る。From the emission characteristics of the soot, the flame temperature can be known by using the relationship of Planck's radiation law. Planck's radiation law means that the relationship between the radiation wavelength and the radiation intensity at a certain temperature is determined as shown in FIG. Therefore, to determine the temperature of the flame, the relationship between the wavelength and the intensity may be determined. Since it is difficult to measure over the entire wavelength range, high-temperature ones are usually measured in the visible-near-infrared light wavelength range having a wavelength λ <1 μm or less. It is said that the flame emits light from soot (soot or carbon) in this wavelength range. The flame temperature is usually in the range of 1200 ° K to 2000 ° K, and in this temperature range, the intensity in the λ = 0.8 to 1.0 μm wavelength region almost linearly depends on the wavelength, as estimated from FIG. Therefore, the temperature can be calculated from the slope of the line connecting the measurement points only by measuring the intensity at the wavelengths at two or three points. Although there is no problem in principle even if the calculation is performed at λ <0.8 μm or less, the shorter the wavelength, the lower the intensity, so that the measurement becomes difficult. In the present invention, the slope value of the spectrum intensity in the wavelength range of 0.8 to 1.0 μm is called soot luminous intensity. The method of measuring the temperature is as follows. When the spectrum intensity at arbitrary plural wavelengths, for example, the spectrum intensity at 0.8 μm and the spectrum intensity at 1.0 μm are experimentally measured in advance, and the relationship between the measured value and the temperature is obtained, the relationship shown in FIG. Is obtained. Using this relationship, it is possible to convert the flame temperature from the spectral characteristics.
【0016】水蒸気の吸光は、火炎と光プローブの間を
水蒸気を含む再循環燃焼排ガスが流れることから生じる
現象である。このスペクトル強度の減少量は、水蒸気の
濃度、流量が増加すると大きくなる。火力発電所のボイ
ラにおいては、負荷ごとにそれに対する空気量と再循環
ガス量を調整しており、負荷一定のときは、空気流量+
再循環ガス流量はボイラ全体の総流量が一定となるよう
に制御されているが、個別バーナを対象とした制御は行
なわれていない。このため、厳密ではないが、平均的に
みて各バーナについても、空気流量が増加すると再循環
排ガス流量が減少する。スペクトル強度の減少量(=水
蒸気の吸光によるスペクトル強度の減少量)の変化から
空気流量、再循環燃焼排ガス流量または燃焼空気と再循
環燃焼排ガスの混合比率の変化を知ることができる(こ
のスペクトル強度の減少量を水蒸気吸光度と称す。実際
には、1.4μm近傍におけるスペクトル強度の減少量
である凹みの面積を求める)。The absorption of water vapor is a phenomenon caused by the flow of recirculated flue gas containing water vapor between the flame and the optical probe. This decrease in spectral intensity increases as the concentration and flow rate of water vapor increase. In a boiler of a thermal power plant, the amount of air and the amount of recirculated gas corresponding to each load are adjusted, and when the load is constant, the air flow rate +
The recirculation gas flow rate is controlled so that the total flow rate of the entire boiler is constant, but control for individual burners is not performed. For this reason, although not strict, for each burner on average, as the air flow rate increases, the recirculation exhaust gas flow rate decreases. From the change in the decrease in the spectral intensity (= the decrease in the spectral intensity due to the absorption of water vapor), it is possible to know the change in the air flow rate, the flow rate of the recirculated flue gas, or the change in the mixing ratio of the combustion air and the recirculated flue gas. Is referred to as water vapor absorbance. In practice, the area of the dent, which is the amount of decrease in the spectrum intensity near 1.4 μm, is obtained).
【0017】図3に重油燃焼における火炎正常燃焼時
(各負荷帯でそれぞれ燃焼調整が完了している最適燃焼
状態時をいう、すなわち、試運転調整時において、運転
指導員が最適とした燃焼状態時をいう)と正常燃焼時よ
り燃料流量のみを平均値が20%減少した時(したがっ
て、空気流量、再循環燃焼排ガス流量は運転指導員が最
適とした流量のままである。)のスート発光度と水蒸気
吸光度の変動状況の関係を示す。負荷一定(燃料流量、
空気流量、再循環燃焼排ガス流量がボイラ全体では一
定)で運転していても、各バーナについてみれば、空
気、再循環燃焼排ガス流量はバーナの相互干渉のため変
動している。例えば、対象バーナの空気または再循環燃
焼排ガス流量が増加すると、隣接バーナの空気または再
循環燃焼排ガス流量が減少する。したがって、火炎発光
スペクトルを観察していると、バーナ相互干渉のため、
水蒸気吸光度およびスートの発光度の変動が図3のよう
に観測される。図4に正常燃焼時と正常燃焼時より空気
流量の平均値が15%増加したときのスート発光度と水
蒸気吸光度の変動状況の関係を示す。FIG. 3 shows the normal combustion state of the flame in the heavy oil combustion (the optimum combustion state in which the combustion adjustment is completed in each load zone, that is, the combustion state optimized by the operation instructor during the test operation adjustment). ) And when the average value of only the fuel flow rate is reduced by 20% from the normal combustion state (therefore, the air flow rate and the recirculated flue gas flow rate remain at the flow rates optimized by the operation instructor). 6 shows the relationship between the fluctuation states of the absorbance. Constant load (fuel flow,
Even when operating at a constant air flow rate and recirculated flue gas flow rate throughout the boiler), the air and recirculated flue gas flow rates vary for each burner due to the mutual interference of the burners. For example, as the air or recirculated flue gas flow of the target burner increases, the air or recirculated flue gas flow of the adjacent burner decreases. Therefore, when observing the flame emission spectrum, because of the burner mutual interference,
Fluctuations in water vapor absorbance and soot luminescence are observed as shown in FIG. FIG. 4 shows a relationship between the soot luminous intensity and the fluctuation state of the water vapor absorbance at the time of normal combustion and when the average value of the air flow rate is increased by 15% from that at the time of normal combustion.
【0018】図3、図4からわかるように、火炎発光ス
ペクトル内のスート発光度および水蒸気吸光度は、正常
燃焼時および燃料流量、空気流量など(の平均値)が変
化した異常燃焼時においても、ある一定範囲内で変動し
ている。このとき、スート発光度が減少すると水蒸気吸
光度が増加する反比例の関係が見られる。この現象は、
水蒸気吸光度が増加するような再循環燃焼排ガスが増加
しているときは、燃焼が緩慢になり、火炎温度が低下
し、スートの発光度が減少することを示すものと考えら
れる。As can be seen from FIGS. 3 and 4, the soot luminous intensity and water vapor absorbance in the flame luminous spectrum show the normal combustion and the abnormal combustion in which the fuel flow rate, air flow rate and the like (the average value) have changed. It fluctuates within a certain range. At this time, there is an inverse relationship that the water vapor absorbance increases as the soot luminescence decreases. This phenomenon is
An increase in recirculated flue gas, such as an increase in water vapor absorbance, is believed to indicate slow combustion, lower flame temperature, and lower soot luminescence.
【0019】空気流量が増加すると、スート発光度の変
動領域(X)は変化しないが、水蒸気吸光度の変動領域
は減少する(変動幅がY1 からY2 に減少するととも
に、吸光度そのものも低い変動領域へ移行する)関係が
見られる。燃料流量が減少すると、スート発光度の変動
領域および水蒸気吸光度の変動領域がともに減少する
(低い変動領域に移行する)。以上述べた燃料流量、空
気流量の変化時における、スート発光度および水蒸気吸
光度の変動領域の変化をまとめて示すと表1のようにな
る。When the air flow rate increases, the fluctuation area (X) of the soot luminous intensity does not change, but the fluctuation area of the water vapor absorbance decreases (the fluctuation width decreases from Y 1 to Y 2 , and the absorbance itself also changes at a low level). (Transition to the domain). When the fuel flow rate decreases, both the soot luminous intensity fluctuation region and the water vapor absorbance fluctuation region decrease (shift to a low fluctuation region). Table 1 summarizes changes in the soot luminous intensity and water vapor absorbance fluctuation region when the fuel flow rate and the air flow rate change as described above.
【0020】[0020]
【表1】 [Table 1]
【0021】表1において、発電負荷増加とは、燃料流
量が増加し、それに伴って燃焼用空気流量と再循環燃焼
排ガス流量が増加することを意味する。以上重油燃焼火
炎を対象とした実施例について述べたが、ガス燃料につ
いての燃焼火炎における燃焼診断は、油燃焼火炎の場合
と同じように、火炎発光スペクトルのスート発光度およ
び水蒸気吸光度を検出して同様に行なうことができる。In Table 1, an increase in the power generation load means that the fuel flow rate increases, and accordingly, the combustion air flow rate and the recirculated flue gas flow rate increase. Although the embodiment for heavy oil combustion flame has been described above, the combustion diagnosis in the combustion flame for gas fuel detects the soot luminescence and water vapor absorbance of the flame emission spectrum in the same manner as in the case of oil combustion flame. The same can be done.
【0022】しかし、石炭などの固体燃料(例えば微粉
炭)の場合は、燃焼生成物中に含まれる水蒸気の割合が
小さいために、水蒸気吸光度の変化が顕著に現われな
い。このため、水蒸気吸光度に代わって、二酸化炭素の
吸光度を用いると、油燃焼火炎と同様にして燃焼診断で
きる。この場合、二酸化炭素の吸光波長は2.7μmお
よび4.3μmにあるのでこの波長付近について、スペ
クトルの強度の減少量、凹みの面積を求める。なお、二
酸化炭素の吸光度は光ファイバを通過させると測定でき
ないので、光プローブで検出したものを中継光ファイバ
を通すことなく分光分析装置に直接送って分析する必要
がある。However, in the case of a solid fuel such as coal (for example, pulverized coal), a change in water vapor absorbance does not appear significantly because the proportion of water vapor contained in the combustion product is small. Therefore, when the absorbance of carbon dioxide is used instead of the water vapor absorbance, combustion diagnosis can be performed in the same manner as in the case of oil combustion flame. In this case, since the absorption wavelengths of carbon dioxide are at 2.7 μm and 4.3 μm, the amount of decrease in the intensity of the spectrum and the area of the dent are determined around this wavelength. Since the absorbance of carbon dioxide cannot be measured when the light passes through an optical fiber, it is necessary to directly send the light detected by an optical probe to a spectrometer without passing through a relay optical fiber for analysis.
【0023】本発明を実施するにあたっては、図3に示
すように、あらかじめ正常燃焼時の火炎についてのスー
ト発光度と水蒸気吸光度の関係データ域(正常データ
域)を実験的に求めておき(実験式として表現でき
る)、これを基準値とし、実際に運転しているときのバ
ーナ火炎についてのスート発光度と水蒸気吸光度の検出
関係データ(図3についていえば、燃料20%減のデー
タ域についての全データ、またはその一部データ)を求
め、表1に示すスペクトル挙動の関係を考慮して、両デ
ータを比較してバーナの燃焼状態を診断する。例えば、
基準値と検出値を比較して、スート発光特性に変化が見
られず、水蒸気吸光度が小さくなっている火炎挙動が得
られたバーナは、空気流量が増加していると診断され、
このような場合、燃焼ガス中に窒素酸化物が多く発生し
ていることが推定される。In carrying out the present invention, as shown in FIG. 3, a relational data area (normal data area) between the soot luminous intensity and the water vapor absorbance of a flame during normal combustion is previously experimentally obtained (experimental). Using this as a reference value, detection relation data of soot luminous intensity and water vapor absorbance of a burner flame during actual operation (in FIG. 3, the data area of a data area where fuel is reduced by 20%) All the data or a part of the data is obtained, and considering the relationship between the spectral behaviors shown in Table 1, the two data are compared to diagnose the burner combustion state. For example,
Comparing the reference value and the detection value, the burner in which the soot emission characteristic does not show a change and the flame behavior in which the water vapor absorbance is small is obtained is diagnosed that the air flow rate is increasing,
In such a case, it is estimated that a large amount of nitrogen oxide is generated in the combustion gas.
【0024】本発明によれば正常運転時について、スー
ト発光度と水蒸気吸光度(二酸化炭素吸光度)の基準値
をあらかじめ測定しておけば、診断すべき運転時のスー
ト発光度と水蒸気吸光度(二酸化炭素吸光度)の変動域
全部のデータを求めなくても、その一部データを求めて
基準値と比較することによっても、燃焼診断をすること
ができるので診断時間が短縮できる。According to the present invention, when the reference values of the soot luminescence and the water vapor absorbance (carbon dioxide absorbance) are measured in advance during normal operation, the soot luminescence and the water vapor absorbance (carbon dioxide absorbance) during the operation to be diagnosed are determined. Even if the data of the entire fluctuation range of the absorbance is not obtained, the combustion diagnosis can also be performed by obtaining a part of the data and comparing it with the reference value, so that the diagnosis time can be shortened.
【0025】[0025]
【発明の効果】本発明によれば、従来の燃焼診断装置に
あった燃焼診断精度を低下させる問題および診断時間が
長くなる問題、または、各種流量計設置による装置コス
トの上昇およびこれら計器への保守労力の増加等の問題
がなくなり、装置コストの上昇および保守労力の増加を
生じることなく、燃焼診断精度を向上でき、かつ診断時
間を短縮できる燃焼診断ソフトを提供できるようにな
る。According to the present invention, there is a problem that the accuracy of combustion diagnosis is reduced and a diagnosis time is long, which is a problem with the conventional combustion diagnosis device, or the cost of the device is increased due to the installation of various flow meters, and the cost for these devices is reduced. Problems such as an increase in maintenance labor are eliminated, and it is possible to provide combustion diagnosis software that can improve the accuracy of combustion diagnosis and reduce the diagnosis time without increasing the cost of the apparatus and the maintenance labor.
【図1】本発明になる一実施例の燃焼診断システムの構
成図。FIG. 1 is a configuration diagram of a combustion diagnosis system according to an embodiment of the present invention.
【図2】油燃焼火炎の発光スペクトルの一例を示す図。FIG. 2 is a diagram showing an example of an emission spectrum of an oil combustion flame.
【図3】、FIG.
【図4】火炎発光スペクトルのスートの発光度および水
蒸気の吸光度の測定値と両者の関係を示す図。FIG. 4 is a diagram showing measured values of soot luminescence and water vapor absorbance in a flame emission spectrum and the relationship between the two.
【図5】プランクの輻射則を示す図。FIG. 5 is a diagram showing Planck's radiation law.
【図6】スペクトル強度の測定から火炎温度を求める関
係図。FIG. 6 is a relationship diagram for obtaining a flame temperature from measurement of spectrum intensity.
1…光プローブ、2…中継光ファイバ、3…光チャンネ
ルセレクタ、4…分光分析装置、5…データ解析装置。1 optical probe, 2 relay optical fiber, 3 optical channel selector, 4 spectral analyzer, 5 data analyzer.
フロントページの続き (56)参考文献 特開 昭62−276326(JP,A) 特開 平4−270820(JP,A) (58)調査した分野(Int.Cl.7,DB名) F23N 5/08 F23M 11/04 104 Continuation of the front page (56) References JP-A-62-276326 (JP, A) JP-A-4-270820 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) F23N 5 / 08 F23M 11/04 104
Claims (4)
と、その火炎検出手段からの光検出信号を入力する分光
分析手段と、その分光分析手段からの信号を入力して演
算処理するデータ解析手段とを備え、分光分析手段によ
り求めた波長ごとのスペクトル強度に基づき、前記解析
手段により、正常燃焼時のスート発光度と水蒸気吸光度
の基準データと燃焼診断すべき検出時のスート発光度と
水蒸気吸光度のデータとを作成してこれにより火炎の燃
焼状態を診断するように構成したことを特徴とする燃焼
診断装置。1. Flame detecting means arranged for a flame, spectral analyzing means for inputting a light detection signal from the flame detecting means, and data analysis for inputting and processing a signal from the spectral analyzing means. Means, based on the spectral intensity for each wavelength determined by the spectral analysis means, by the analysis means, soot luminescence during normal combustion and reference data of water vapor absorbance and soot luminescence and water vapor at the time of detection for combustion diagnosis A combustion diagnostic apparatus characterized in that data on absorbance is created and the combustion state of the flame is diagnosed based on the data.
と、その火炎検出手段からの光検出信号を入力する分光
分析手段と、その分光分析手段からの信号を入力して演
算処理するデータ解析手段とを備え、分光分析手段によ
り求めた波長ごとのスペクトル強度に基づき、前記解析
手段により、正常燃焼時のスート発光度と二酸化炭素吸
光度の基準データと燃焼診断すべき検出時のスート発光
度と二酸化炭素吸光度のデータとを作成してこれにより
火炎の燃焼状態を診断するように構成したことを特徴と
する燃焼診断装置。2. Flame detecting means arranged for a flame, spectral analyzing means for inputting a light detection signal from the flame detecting means, and data analysis for inputting a signal from the spectral analyzing means and performing arithmetic processing. With means, based on the spectral intensity for each wavelength determined by the spectral analysis means, by the analysis means, soot luminescence at normal combustion and reference data of carbon dioxide absorbance and soot luminescence at the time of detection for combustion diagnosis and A combustion diagnostic apparatus characterized in that data of carbon dioxide absorbance is created and the combustion state of the flame is diagnosed based on the data.
と、その火炎検出手段からの光検出信号を入力する分光
分析手段と、その分光分析手段からの信号を入力して演
算処理するデータ解析手段とを備え、分光分析手段によ
り求めた波長ごとのスペクトル強度に基づき、前記解析
手段により、正常燃焼時のスート発光度と水蒸気吸光度
の値と変動幅および燃焼診断すべき検出時のスート発光
度と水蒸気吸光度の値および/または変動幅を求め、か
つこれにより燃料流量、空気流量、再循環燃焼排ガス流
量のいずれか一つ以上の状態を診断するように構成した
ことを特徴とする燃焼診断装置。3. A flame detecting means arranged for a flame, a spectral analyzing means for inputting a light detection signal from the flame detecting means, and a data analysis for inputting a signal from the spectral analyzing means and performing arithmetic processing. Means, based on the spectral intensity for each wavelength determined by the spectroscopic analysis means, the analysis means, soot luminescence during normal combustion and the value and variation of water vapor absorbance and soot luminescence at the time of detection to be diagnosed combustion A combustion diagnostic apparatus characterized by determining a value of a water vapor absorbance and / or a fluctuation range, and diagnosing at least one of a fuel flow rate, an air flow rate, and a recirculation flue gas flow rate. .
と、その火炎検出手段からの光検出信号を入力する分光
分析装置と、その分光分析手段からの信号を入力して演
算処理するデータ解析手段とを備え、分光分析手段によ
り求めた波長ごとのスペクトル強度に基づき、前記解析
手段により、正常燃焼時のスート発光度と二酸化炭素吸
光度の値と変動幅および燃焼診断すべき検出時のスート
発光度と二酸化炭素吸光度の値および/または変動幅と
を求め、かつこれにより燃料流量、空気流量、再循環燃
焼排ガス流量のいずれか一つ以上の状態を診断するよう
に構成したことを特徴とする燃焼診断装置。4. A flame detecting means arranged for a flame, a spectroscopic analyzer for inputting a light detection signal from the flame detecting means, and a data analysis for inputting a signal from the spectroscopic analyzing means and performing arithmetic processing. Means, based on the spectral intensity for each wavelength determined by the spectroscopic analysis means, the soot emission at the time of normal combustion, soot emission and carbon dioxide absorbance values and fluctuation range and soot emission at the time of detection to be diagnosed by combustion And a value and / or a fluctuation range of the carbon dioxide absorbance are obtained, and a state of at least one of a fuel flow rate, an air flow rate, and a recirculation flue gas flow rate is diagnosed based on the determined value. Combustion diagnostic device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP04081133A JP3083633B2 (en) | 1992-04-02 | 1992-04-02 | Combustion diagnostic device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP04081133A JP3083633B2 (en) | 1992-04-02 | 1992-04-02 | Combustion diagnostic device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH05288343A JPH05288343A (en) | 1993-11-02 |
| JP3083633B2 true JP3083633B2 (en) | 2000-09-04 |
Family
ID=13737904
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP04081133A Expired - Lifetime JP3083633B2 (en) | 1992-04-02 | 1992-04-02 | Combustion diagnostic device |
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| Country | Link |
|---|---|
| JP (1) | JP3083633B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN120314284B (en) * | 2025-06-16 | 2025-09-12 | 浙江大合检测有限公司 | Method and system for detecting alkali content in concrete |
| CN120760133B (en) * | 2025-07-31 | 2026-01-02 | 佛山市顺德区豫锐涂装设备有限公司 | A smart air-gas linkage control system for a gas burner |
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1992
- 1992-04-02 JP JP04081133A patent/JP3083633B2/en not_active Expired - Lifetime
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|---|---|
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