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JPH0260934B2 - - Google Patents
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JPH0260934B2 - - Google Patents

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Publication number
JPH0260934B2
JPH0260934B2 JP59072711A JP7271184A JPH0260934B2 JP H0260934 B2 JPH0260934 B2 JP H0260934B2 JP 59072711 A JP59072711 A JP 59072711A JP 7271184 A JP7271184 A JP 7271184A JP H0260934 B2 JPH0260934 B2 JP H0260934B2
Authority
JP
Japan
Prior art keywords
combustion
burner
nox
stage
fuel
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
Application number
JP59072711A
Other languages
Japanese (ja)
Other versions
JPS60218525A (en
Inventor
Hiroshi Matsumoto
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP7271184A priority Critical patent/JPS60218525A/en
Publication of JPS60218525A publication Critical patent/JPS60218525A/en
Publication of JPH0260934B2 publication Critical patent/JPH0260934B2/ja
Granted legal-status Critical Current

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Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F23COMBUSTION APPARATUS; COMBUSTION PROCESSES
    • F23NREGULATING OR CONTROLLING COMBUSTION
    • F23N5/00Systems for controlling combustion
    • F23N5/003Systems for controlling combustion using detectors sensitive to combustion gas properties
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F23COMBUSTION APPARATUS; COMBUSTION PROCESSES
    • F23NREGULATING OR CONTROLLING COMBUSTION
    • F23N5/00Systems for controlling combustion
    • F23N5/02Systems for controlling combustion using devices responsive to thermal changes or to thermal expansion of a medium
    • F23N5/08Systems for controlling combustion using devices responsive to thermal changes or to thermal expansion of a medium using light-sensitive elements
    • F23N5/082Systems for controlling combustion using devices responsive to thermal changes or to thermal expansion of a medium using light-sensitive elements using electronic means

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Regulation And Control Of Combustion (AREA)
  • Control Of Combustion (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の利用分野〕 本発明は燃焼制御方法に係り、特に燃料の性状
が時々刻々変化する微粉炭を燃料とする燃焼の燃
焼効率の向上及びNOx発生の低減に好適な燃焼
制御方法に関する。 〔発明の背景〕 従来の燃焼制御は、主として空燃比(燃焼室に
投入する全燃料流量に対する空気流量の比)が規
定値となるように制御することにより排ガス損失
を低減し、燃焼の高効率化を図る技術と、火炎の
終端部に投入する空気量を制御することにより排
ガス中のNOx濃度を制限値以下に抑制する技術
で構成されていた。 しかし、上記従来方式は燃焼室内の燃焼状態を
直接観測していないため、微粉炭燃料などのよう
に時々刻々変動する燃料性状(固定炭素分、揮発
分、灰分、水分など含有率及びその性質)及び運
転条件(燃焼負荷、環境上の制約値、空気温度な
ど)のもとで常に最適な燃焼状態を維持すること
は不可能であつた。 〔発明の目的〕 本発明の目的は、時々刻々変化する燃料性状及
び運転条件のもとで常に運転制限条件を守り、か
つ最大燃焼効率を得るための燃焼室内の最適火炎
形状を決定し、維持するための燃焼制御方法を提
供するにある。 〔発明の概要〕 本発明は、燃焼効率がCO濃度と強い相関があ
ること、CO濃度及びNOx濃度が火炎形状即ち燃
焼室内への燃料及び空気の導入方法に大きく依存
することに着目したものである。本発明の目的で
ある燃焼の高効率化及び低NOx化の問題は、
NOx濃度を制約条件とし燃焼効率を評価関数と
する非線形最適化制御問題として定式化した。本
制御の機能は、大きく分けて、最適目標火炎形状
探索機能と、この最適目標火炎形状を維持するた
めの火炎形状制御機能の2つの機能で構成したこ
とに特徴がある。最適目標火炎形状探索機能は燃
料供給系及び空気供給系の操作量を変更すること
により、NOx濃度が運転制限値以下でかつ燃焼
効率が最大となつたときの火炎形状を最適目標火
炎形状とする。ただし、火炎形状は火炎形状計測
機能で計測する。火炎形状制御機能は計測した火
炎形状が上記最適目標火炎形状となるように操作
量を調節する。火炎形状制御中に前記燃料性状あ
るいは運転条件が変動した場合は、再び最適目標
火炎形状を探索し、変動した条件のもとでの最適
目標火炎形状を決定し、燃料性状の変化にかゝわ
らず最適燃焼状態を維持する。 〔発明の実施例〕 本発明を火力発電プラントのボイラ燃焼制御に
適用した場合について、以下に説明する。 ボイラ用燃料として使用量が増してきた石炭
は、石油あるいは天然ガスと比較して、排ガス中
の窒素酸化物(NOx),硫黄酸化物(SOx),一
酸化炭素(CO)など有害物質の低減が困難と言
われている。石炭に含まれる窒素分(以下Fuel
―Nと表記する)は比較的多いため、特にNOx
の低減が困難とされている。燃焼によつて発生す
るNOxは、Fuel―Nの酸化によるもの(これを
以下Fuel―NOxと表記する)と、高温場におけ
る空気中の窒素の酸化によるもの(これを以下
Thermal―NOxと表記する)に分けられる。石
油やガスを燃料とした場合に発生するNOxは大
部分がThermal―NOxであり、石炭を燃料とし
た場合は大部分がFuel―NOxである。従つて、
石油やガスを対象として開発されてきた従来の燃
焼方式は、燃焼温度に着目したものであり、
Thermal―NOxの低減には効果があるが、石炭
燃焼に適用した場合はFuel―NOxの問題が依然
として残る。 一方、発電用ボイラは一般に複数のバーナを有
し、燃焼ガスの流れ方向に多段に配置された複雑
な構造をしている。そのため、従来、数多くある
操作端は試運転時あるいは定検時に制定した操作
規準に従つて運転されていた。石炭は産炭地、名
柄により性状が大きく異なるため多種燃料を使う
プラントでは上記操作規準にマージンを十分とる
必要が有り、燃焼効率が必ずしも最大値となるよ
うに運転されていなかつた。常時、低NOxかつ
高効率運転を実現するためには高度で複雑な判断
能力を持つ熟練運転員が必要である。しかし、新
鋭ボイラのように構造が複雑化し、多様化してく
ると熟練運転員の養成がむつかしいばかりでな
く、熟練運転員であつても燃料性状や運転条件の
時間変動に直ちに対応することが困難である。 低NOx高効率化を基本目標とする燃焼制御は、
次のような非線形最適化問題として定式化でき
る。 評価関数η(x)→Max ……(1) 等式制約条件g(x)=0 ……(2) 不等式制約条件h(x)<h0 ……(3) ここで、x(∈Rn)はプラント状態値(ベクト
ル)、ηは燃焼効率(スカラ関数)、g(∈Rk)は
運転条件、h(∈Rl)は運転制限要因(ベクトル
関数)、h0(∈Rl)は運転制限値(ベクトル)であ
る。等式制約条件((2)式)は、プラントの出力及
び蒸気温度並びに圧力などのように燃焼制御機能
よりも上位の制御機能によつて制御される運転条
件に関するものであり、上位制御機能が健全であ
れば常に満足されるものである。運転制限要因h
は排ガス中のNOx濃度、CO濃度及び操作量であ
り、h0はその制限値である。従つて、実質的には
(1),(3)式を満足する操作量x(∈Rm,m=l−
2)を求めることになる。 第1図はボイラ火炉20におけるバーナ配置、
燃料供給系30及び空気・ガス系40を示す。第
2図はバーナ80の構造を示す。押込通風フアン
(FDF)41により取り込まれた空気は空気予熱
器(SAH42及びYAH43)に送られ、排ガス
の保有熱により予熱される。この予熱された空気
は2次空気44と呼ばれる。2次空気44は、混
合用ガス(再循環ガス46の一部であり、集塵器
(HEP)47出口から抽出したもの)45と混合
され、ウインドボツクス79に導かれる。ウイン
ドボツクス79は火炉20の前面21と後面22
に配置されたA〜Fの各バーナ段(23A〜23F
及びNOポート24,25に対応して設置されて
いる。各ウインドボツクスへ流入する2次空気及
び混合用ガス48の流量は、入口に設けた各ダン
パ49の開度で定まる。各バーナ段は複数本(本
実施例では8本)の微粉炭バーナ80から構成さ
れている。一方、再循環ガス46は、一次ガス5
0、火炉ホツパガス51及び前記混合用ガス45
の3つに分流される。1次ガス50は、第2図に
示すようにバーナ80の外周にある1次ガスポー
ト52から火炉20に噴射される。また、火炉ホ
ツパガス51は火炉底にあるホツパ部に導入され
る。混合用ガス45は前記2次空気44と混合さ
れ、1次ガスポートの外周から火炉20に噴射さ
れる。これら3つのガスの流量比は、1次ガスダ
ンパ(PGD)53、火炉ホツパガスダンパ
(FHGD)54及び混合ダンパ(GMD)55の
開度で定まる。一方、石炭フイーダ31と微粉炭
ミル32から成る燃料供給系30は各バーナ段に
対応してA〜Fの6系統設置されている。FDF
出口から抽出した1次空気56は、1次空気予熱
器(PAH)57で予熱されたのち微粉炭ミル3
2に送られ、微粉炭の乾燥及び搬送に使われる。
1次空気の1部58は、1次空気フアン(PAF)
59を出たのちPAHをバイパスされる。このバ
イパス量の調整により微粉炭ミル出口の微粉炭及
び1次空気33の温度を一定に保つことができ
る。また、図には示さなかつたが、節炭器出口部
には再熱蒸気温度制御用のパラレルダンパを設け
てあり、このダンパ開度を調節することにより1
次過熱器と1次再熱器側に流れるガス量配分を変
更でき、再熱蒸気温度は一定に制御される。 第3図は火炉内火炎構造と各バーナ段への空気
比(理論空気量に対する実際の使用空気量の比)
配分方式を示す。各バーナ段に対して、 (1) 下段バーナ(A,D段)23A,23Dには環
元性物質を積極的に生成させる領域91を形成
させる。 (2) 中段バーナ(B,E段)23B,23Eには
Fuel―Nを積極的に放出させる領域92を形
成させる。 (3) 下段バーナと中段バーナの火炎先端を合流さ
せ、NOxの還元領域93を形成させる。 (4) 上段バーナ(C,F段)には下、中段バーナ
からの未燃分を完全燃焼させる領域94を形成
させる。 以上の機能を実現するために、次のような手段
をとる。 下段バーナに関しては、噴射される燃料の火炉
内滞留時間が他段のそれよりも長いことに着目
し、空気比(λ1と表記する)を1より小さくし、
比較的低温で時間をかけて燃焼させる方式とす
る。すなわち、低酸素雰囲気にて微粉炭が熱分解
される時に放出する揮発成分中の窒素が環元性物
質であるNH3やHCNに転換される割合が、高酸
素雰囲気でのそれと比較して高いことを利用す
る。従つて、下段バーナの火炎はNOx濃度が低
く、還元性物質に豊む。しかし、λ1<1で燃焼さ
せているため未燃分が比較的多く存在し、この未
燃分中にはFuel―Nが存在する。 一方、中段バーナに関しては、空気比(λ2と表
記する)を1より少し大きくし、比較的高温で短
時間で燃焼させる方式とする。すなわち、高酸素
雰囲気での燃焼は、Thermal―NOxは多く発生
するが、Fuel―Nの放出が活発となることを利
用する。従つて、中段バーナの火炎はNOx濃度
は高いが、未燃分中にはFuel―Nが殆ど存在し
ない。 また、上段バーナに関しては、空気比(λ3と表
記する)をλ2よりも更に大きくし、主として下段
バーナから発生する未燃分を完全燃焼させる方式
とする。 以上述べたような機能を各段に分担させること
により、上段バーナの火炎先端部ではNOxの還
元領域が形成され、主として中段バーナで発生し
たNOxが、主として下段バーナで発生したNH3
やHCNなどの還元性物質により還元され、NOx
低減が可能となる。 燃焼制御システムでは、上記空気比配分(λ1
1,λ2>1,λ3≫1)の条件を満たす範囲で、更
に最適な空気比配分を決定することになる。 低NOxかつ高効率燃焼は、(1)〜(3)式で定式化
した非線形最適化問題を解くことにより実現でき
る。ここでは、燃焼効率向上のための基本的考え
方を述べ、評価関数としての燃焼効率ηを定義す
る。 微粉炭が完全燃焼して理論発熱量が得られる場
合の燃焼効率は100%である。しかし、実際のボ
イラでは、火炉内ガス流動の乱れによる未燃分が
残り、燃焼効率の低下の原因となる。末燃分は主
として固形炭素Cと一酸化炭素COから成る。燃
焼効率を上げるには酸素過剰率(理論酸素量に対
する過剰酸素量の比:以下、Z02と表記する)を
大きくすれば良いが、大きくし過ぎるとボイラの
排ガス損失が増して、ボイラ効率は低下する。従
つて、実際のボイラでは、燃焼効率を広義にとら
え、排ガス損失も考慮する必要がある。以下では
燃焼効率を広義に使用する。未燃分のうちC分は
粉体であり、火炉ホツパや集塵器で捕獲されるた
め、現在の計測技術ではオンライン計測が不可能
である。一方、CO分はガス体のためオンライン
計測が可能であり、ボイラ全体のZ02に対するCO
濃度と燃焼効率は一般に第4図A,Bの実線で示
す関係にある。すなわち、CO濃度ZCOがZCO,U以下
の条件ではZ02が小さいほど燃焼効率は高いこと
を示している。Z02=aのとき、燃焼効率ηは最
大(ηa)となつている。この実線で示す特性は従
来の非最適運転用時のものであるが、本発明を適
用した最適運用の場合は破線で示す特性が期待で
きる。すなわち、同じZ02のもとでも良好な燃焼
が期待でき、CO濃度が低下するため、燃焼効率
が向上する。この場合でもZCO=ZCO,Uとなる。Z02
=bの条件で燃焼効率は最大(ηb)に近い値と
なることが期待できる。すなわち、NOx濃度を
ZNOX及びその制限値をZZOX,Uとすれば、ZCO<ZCO,U
かつZNOX<ZZOX,Uを満足し、かつ再熱蒸気温度制
御のためのパラレルダンパ開度APDはその上、下
限値A APD,U,APD,Lに対してAPD,L<APD,Uを満足
し、Z02を最小にする操作量が最適操作量となる。
よつて、燃焼効率は絶対量を知る必要がないから
次式で等価的に定義して良い。 η=100−Z02 ……(4) 燃焼制御システムの機能構成を第5図に示し、
また制御のための基本処理手順を第6図に示す。
制御システムは運転員97からの指令で動作を開
始し、まず最適目標火炎形状探索機能200によ
り最適目標火炎形状(y^*)101及び最適操作
量(x^*)102を決定する。ここで、y^*は前述
の最適化問題を満足する操作ベクトルであり、
y^*はこのときの火炉内火炎に関する形状ベクト
ルである。操作ベクトルは次のように定義する。
[Field of Application of the Invention] The present invention relates to a combustion control method, and particularly to a combustion control method suitable for improving combustion efficiency and reducing NOx generation in combustion using pulverized coal as a fuel whose fuel properties change from time to time. [Background of the Invention] Conventional combustion control mainly controls the air-fuel ratio (the ratio of the air flow rate to the total fuel flow rate injected into the combustion chamber) to a specified value, thereby reducing exhaust gas loss and achieving high combustion efficiency. It consisted of technology to reduce NOx concentration in the exhaust gas to below a limit value by controlling the amount of air injected into the end of the flame. However, the conventional method described above does not directly observe the combustion state inside the combustion chamber, so fuel properties such as pulverized coal fuel change from time to time (content rate and properties such as fixed carbon content, volatile content, ash content, and moisture content). It has been impossible to maintain optimal combustion conditions at all times under various operating conditions (combustion load, environmental constraints, air temperature, etc.). [Object of the Invention] The object of the present invention is to determine and maintain the optimum flame shape within the combustion chamber in order to always observe the operating limit conditions and obtain maximum combustion efficiency under constantly changing fuel properties and operating conditions. The purpose of the present invention is to provide a method for controlling combustion. [Summary of the Invention] The present invention focuses on the fact that combustion efficiency has a strong correlation with CO concentration, and that CO concentration and NOx concentration greatly depend on the flame shape, that is, the method of introducing fuel and air into the combustion chamber. be. The problems of high combustion efficiency and low NOx, which are the objectives of the present invention, are as follows:
It was formulated as a nonlinear optimization control problem with NOx concentration as a constraint and combustion efficiency as an evaluation function. The function of this control is characterized by being broadly divided into two functions: an optimal target flame shape search function and a flame shape control function for maintaining this optimal target flame shape. The optimal target flame shape search function changes the manipulated variables of the fuel supply system and air supply system to determine the flame shape when the NOx concentration is below the operating limit value and the combustion efficiency is maximum as the optimal target flame shape. . However, the flame shape is measured using the flame shape measurement function. The flame shape control function adjusts the manipulated variable so that the measured flame shape becomes the optimal target flame shape. If the fuel properties or operating conditions change during flame shape control, the optimum target flame shape is searched again, the optimum target flame shape is determined under the changed conditions, and the optimum target flame shape is determined in spite of the change in fuel properties. maintain optimal combustion conditions. [Embodiments of the Invention] A case where the present invention is applied to boiler combustion control of a thermal power plant will be described below. Coal, which has been increasingly used as boiler fuel, reduces harmful substances such as nitrogen oxides (NOx), sulfur oxides (SOx), and carbon monoxide (CO) in exhaust gas compared to oil or natural gas. is said to be difficult. Nitrogen contained in coal (hereinafter referred to as "Fuel")
- written as N) is relatively large, so NOx
is said to be difficult to reduce. NOx generated by combustion is caused by the oxidation of Fuel-N (hereinafter referred to as Fuel-NOx) and the oxidation of nitrogen in the air in high-temperature areas (hereinafter referred to as Fuel-NOx).
Thermal - written as NOx). Most of the NOx generated when oil or gas is used as fuel is thermal-NOx, and when coal is used as fuel, most of it is fuel-NOx. Therefore,
Conventional combustion methods that have been developed for oil and gas focus on combustion temperature.
Although effective in reducing thermal NOx, the problem of fuel NOx still remains when applied to coal combustion. On the other hand, a power generation boiler generally has a plurality of burners and has a complicated structure arranged in multiple stages in the direction of flow of combustion gas. Therefore, conventionally, many operating terminals have been operated in accordance with operating standards established during test runs or periodic inspections. Because the properties of coal vary greatly depending on the region where it is produced and the name of the coal, plants that use a variety of fuels must have a sufficient margin in the operating standards mentioned above, and are not always operated to maximize combustion efficiency. In order to achieve constant low NOx and high efficiency operation, skilled operators with advanced and complex decision-making abilities are required. However, as the structures of new boilers become more complex and diversified, it is not only difficult to train skilled operators, but even experienced operators find it difficult to immediately respond to changes in fuel properties and operating conditions over time. It is. Combustion control whose basic goal is low NOx and high efficiency,
It can be formulated as a nonlinear optimization problem as follows. Evaluation function η(x)→Max...(1) Equality constraint g(x)=0...(2) Inequality constraint h(x)<h 0 ...(3) Here, x(∈R n ) is the plant state value (vector), η is the combustion efficiency (scalar function), g (∈R k ) is the operating condition, h (∈R l ) is the operation limiting factor (vector function), h 0 (∈R l ) is the operating limit value (vector). The equality constraint (Equation (2)) relates to operating conditions that are controlled by a control function higher than the combustion control function, such as plant output, steam temperature, and pressure. If you are healthy, you will always be satisfied. Driving restriction factor h
are the NOx concentration in the exhaust gas, the CO concentration, and the manipulated variable, and h 0 is its limit value. Therefore, in effect
The manipulated variable x (∈R m , m=l−
2) is required. Figure 1 shows the burner arrangement in the boiler furnace 20,
A fuel supply system 30 and an air/gas system 40 are shown. FIG. 2 shows the structure of burner 80. The air taken in by the forced draft fan (FDF) 41 is sent to the air preheater (SAH 42 and YAH 43) and is preheated by the heat retained in the exhaust gas. This preheated air is called secondary air 44. The secondary air 44 is mixed with a mixing gas 45 (part of the recirculated gas 46 and extracted from the exit of the dust collector (HEP) 47) and directed to the wind box 79. The wind box 79 is located between the front side 21 and the rear side 22 of the furnace 20.
Each burner stage A to F (23 A to 23 F
and NO ports 24 and 25. The flow rate of the secondary air and the mixing gas 48 flowing into each window box is determined by the opening degree of each damper 49 provided at the inlet. Each burner stage is composed of a plurality of (eight in this embodiment) pulverized coal burners 80. On the other hand, the recirculating gas 46 is the primary gas 5
0, Furnace hopper gas 51 and the mixing gas 45
It is divided into three parts. The primary gas 50 is injected into the furnace 20 from a primary gas port 52 located on the outer periphery of the burner 80, as shown in FIG. Further, the furnace hopper gas 51 is introduced into a hopper portion at the bottom of the furnace. The mixing gas 45 is mixed with the secondary air 44 and injected into the furnace 20 from the outer periphery of the primary gas port. The flow rate ratio of these three gases is determined by the opening degrees of the primary gas damper (PGD) 53, the furnace hot gas damper (FHGD) 54, and the mixing damper (GMD) 55. On the other hand, six fuel supply systems 30 consisting of a coal feeder 31 and a pulverized coal mill 32 are installed, A to F, corresponding to each burner stage. FDF
The primary air 56 extracted from the outlet is preheated by a primary air preheater (PAH) 57 and then sent to the pulverized coal mill 3.
2 and used for drying and transporting pulverized coal.
One part of the primary air 58 is a primary air fan (PAF)
After leaving 59, PAH is bypassed. By adjusting the amount of bypass, the temperature of the pulverized coal and the primary air 33 at the pulverized coal mill outlet can be kept constant. Although not shown in the figure, a parallel damper for controlling the temperature of reheated steam is installed at the outlet of the economizer, and by adjusting the opening degree of this damper,
The gas amount distribution flowing to the secondary superheater and primary reheater sides can be changed, and the reheated steam temperature can be controlled to be constant. Figure 3 shows the flame structure in the furnace and the air ratio to each burner stage (ratio of the actual amount of air used to the theoretical amount of air).
Indicates the allocation method. For each burner stage: (1) A region 91 is formed in the lower stage burners (stages A and D) 23 A and 23 D to actively generate a cyclic substance. (2) Middle stage burners (B, E stages) 23 B and 23 E have
A region 92 is formed in which Fuel-N is actively released. (3) The flame tips of the lower burner and the middle burner are merged to form a NOx reduction region 93. (4) A region 94 is formed in the upper stage burners (stages C and F) in which unburned content from the lower and middle stage burners is completely combusted. In order to realize the above functions, the following measures are taken. Regarding the lower stage burner, we focused on the fact that the residence time of the injected fuel in the furnace is longer than that in other stages, and set the air ratio (denoted as λ 1 ) to be less than 1.
The method involves burning at a relatively low temperature over a long period of time. In other words, the rate at which nitrogen in the volatile components released when pulverized coal is thermally decomposed in a low-oxygen atmosphere is converted into cyclic substances such as NH 3 and HCN is higher than that in a high-oxygen atmosphere. Take advantage of that. Therefore, the flame of the lower burner has a low NOx concentration and is rich in reducing substances. However, since the combustion is performed at λ 1 <1, there is a relatively large amount of unburned matter, and Fuel-N is present in this unburned matter. On the other hand, for the middle stage burner, the air ratio (denoted as λ 2 ) is set slightly larger than 1, and combustion is performed at a relatively high temperature in a short time. That is, combustion in a high oxygen atmosphere generates a large amount of thermal NOx, but utilizes the fact that fuel-N is actively released. Therefore, although the flame of the middle burner has a high NOx concentration, there is almost no Fuel-N in the unburned content. Further, regarding the upper stage burner, the air ratio (denoted as λ 3 ) is made larger than λ 2 to completely burn the unburned content mainly generated from the lower stage burner. By distributing the functions described above to each stage, a NOx reduction region is formed at the flame tip of the upper stage burner, and NOx mainly generated in the middle stage burner is reduced to NH3 mainly generated in the lower stage burner.
NOx is reduced by reducing substances such as and HCN.
reduction is possible. In the combustion control system, the above air ratio distribution (λ 1 <
A further optimal air ratio distribution is determined within the range that satisfies the following conditions: 1, λ 2 > 1, λ 3 ≫ 1). Low NOx and high efficiency combustion can be achieved by solving the nonlinear optimization problem formulated by equations (1) to (3). Here, we will describe the basic concept for improving combustion efficiency and define combustion efficiency η as an evaluation function. Combustion efficiency is 100% when pulverized coal is completely combusted and the theoretical calorific value is obtained. However, in actual boilers, unburned gas remains due to disturbances in gas flow within the furnace, causing a reduction in combustion efficiency. The end combustion mainly consists of solid carbon C and carbon monoxide CO. In order to increase combustion efficiency, the excess oxygen ratio (ratio of excess oxygen amount to theoretical oxygen amount: hereinafter referred to as Z 02 ) can be increased, but if it is increased too much, the exhaust gas loss of the boiler will increase and the boiler efficiency will decrease. descend. Therefore, in actual boilers, combustion efficiency must be viewed in a broad sense and exhaust gas loss must also be considered. In the following, combustion efficiency will be used in a broad sense. Among the unburned components, the C component is a powder and is captured in the furnace hopper and dust collector, so online measurement is impossible with current measurement technology. On the other hand, the CO content can be measured online because it is a gas, and the CO content relative to Z 02 of the entire boiler can be measured.
Concentration and combustion efficiency generally have the relationship shown by the solid lines in FIG. 4A and B. That is, under the condition that the CO concentration Z CO is less than or equal to Z CO,U, the smaller Z 02 is, the higher the combustion efficiency is. When Z 02 =a, the combustion efficiency η is maximum (η a ). The characteristics shown by the solid line are those for conventional non-optimal operation, but the characteristics shown by the broken line can be expected for optimal operation to which the present invention is applied. In other words, good combustion can be expected even under the same Z 02 , and the CO concentration decreases, resulting in improved combustion efficiency. In this case as well, Z CO =Z CO,U . Z 02
It can be expected that the combustion efficiency will be close to the maximum value (ηb) under the condition of =b. In other words, NOx concentration
If Z NOX and its limit value are Z ZOX,U , then Z CO <Z CO,U
and Z NOX <Z ZOX,U , and the parallel damper opening A PD for reheating steam temperature control is furthermore A PD,L with respect to the lower limit values A A PD,U , A PD,L . The manipulated variable that satisfies <A PD,U and minimizes Z 02 is the optimal manipulated variable.
Therefore, since there is no need to know the absolute amount of combustion efficiency, it can be equivalently defined using the following equation. η=100−Z 02 ...(4) The functional configuration of the combustion control system is shown in Figure 5.
Further, the basic processing procedure for control is shown in FIG.
The control system starts operating in response to a command from an operator 97, and first determines an optimal target flame shape (y^ * ) 101 and an optimal manipulated variable (x^ * ) 102 by an optimal target flame shape search function 200. Here, y^ * is the operation vector that satisfies the optimization problem mentioned above,
y^ * is the shape vector related to the flame in the furnace at this time. The operation vector is defined as follows.

【表】 また、火炎の形状ベクトルの選び方は種々考え
られるが、ここでは火炉内の各火炎配置を表すの
に都合の良い第7図のように定義する。この形状
はITVカメラで撮映した火炎画像を計算機処理
(画像処理)して求める。但し、(5)式で定義した
ように、火炉の前面と後面に配置されたバーナは
同一運用をするから、A段とD段,B段とE段,
C段とF段の火炎形状は対称となる。また、形状
ベクトルは、各火炎の中心線上の輝度が規定値ま
で減衰する点から炉壁及びバーナ中心までの距離
とする。 火炎形状制御機能300は、燃料性状や大気温
度などの僅かな変化が燃焼特性に対する外乱とな
つても安定な火炎形状を維持するためのものであ
る。火炎形状制御の目標値は、既に最適目標火炎
形状探索機能により決定されている最適目標火炎
形状y^*である。この場合、‖y―y^*‖を最小とす
る準最適操作量x^103を決定する。ここで、x^
を準最適操作量と呼ぶ理由は、x^の決定に際し燃
焼効率及びNOx濃度を評価していないためであ
る。すなわち、外乱が小さい場合は、火炎形状を
y^*に追従制御しておけば ‖x^―x^*‖<εx ……(6) が満足され、燃焼特性は最適値近傍に維持される
ことが期待できる。但し、(6)式でのx^,x^*は正規
化値である。外乱としての燃料性状の変動を実測
することは困難であるが、‖x^−x^*‖の大きさが
外乱の大きさを代表していると言える。これに着
目し、次式が満足される場合は最適目標火炎形状
は変更されるべきものと判断し、再び最適目標火
炎形状探索機能200を動作させ、新たなy^*
求める。 ‖x^―x^*‖εx ……(7) 最適目標火炎形状探索機能200は、負荷変動
完了時にも動作する。これは、運転負荷レベルが
変化すれば、最適火炎形状も当然のこととして変
化するからである。負荷変動中あるいは制御周期
以外では操作量を保持するための制御周期管理2
10及び操作量保持220の各機能を設けた。操
作量管理機能230は、制御操作量235として
のx^*あるいはx^と、これらを探索により求めるた
めの探索操作量237を区別して操作器240に
出力するためのものである。計測管理機能250
は試行操作に対応して火炎形状や排ガス濃度を計
測するタイミングを管理するものである。すなわ
ち、試行操作後、定常燃焼に達するまで待つてか
ら火炎形状計測機能260あるいは排ガス濃度の
計測機能270を作動させるものである。CRT
インターフエイス機能280は、運転員97から
のシステム動作指令を受けたり、運転員のリクエ
ストに応じて各種燃焼制御状態をCRT290の
画面に表示させるためのもののである。 ボイラの燃焼過程は複雑であり、オンライン制
御で使用できるモデル用として定式化することは
困難である。ここでは、前記非線形最適化問題を
解くために、非線形計画法の一種であるコンプレ
ツクス法を適用することにし、実際のプラントに
対して試行操作を与え、実測値を評価することに
より最適目標火炎形状を決定する方法をとる。 いま、CO濃度(ZCO),NOx濃度(ZNOX)パラ
レルダンパ開度(APD)を x10=ZCO x11=ZNOX X12=APD ……(8) で定義すると、(3)式で示した制約関数(ベクト
ル)h(x)及びその制御値(ベクトル)h0は次
式で定義できる。
[Table] Although there are various ways to select the flame shape vector, we will define it here as shown in FIG. 7, which is convenient for representing the arrangement of each flame in the furnace. This shape is determined by computer processing (image processing) of flame images captured by an ITV camera. However, as defined in equation (5), the burners placed at the front and rear of the furnace operate in the same way, so stage A and stage D, stage B and stage E,
The flame shapes of stage C and stage F are symmetrical. Further, the shape vector is defined as the distance from the point on the center line of each flame where the brightness attenuates to a specified value to the furnace wall and the center of the burner. The flame shape control function 300 is for maintaining a stable flame shape even if slight changes in fuel properties, atmospheric temperature, etc. cause disturbances to combustion characteristics. The target value for flame shape control is the optimal target flame shape y * , which has already been determined by the optimal target flame shape search function. In this case, a quasi-optimal manipulated variable x^103 that minimizes |y−y^ * | is determined. Here, x^
The reason why is called a sub-optimal manipulated variable is that combustion efficiency and NOx concentration are not evaluated when determining x^. In other words, when the disturbance is small, the flame shape
If the control is performed to follow y^ * , ‖x^−x^ * ‖<εx ...(6) is satisfied, and the combustion characteristics can be expected to be maintained near the optimum value. However, x^ and x^ * in equation (6) are normalized values. Although it is difficult to actually measure fluctuations in fuel properties due to disturbances, it can be said that the magnitude of ‖x^−x^ * ‖ represents the magnitude of the disturbance. Focusing on this, if the following equation is satisfied, it is determined that the optimal target flame shape should be changed, and the optimal target flame shape search function 200 is operated again to find a new y * . ‖x^−x^ * ‖εx ...(7) The optimum target flame shape search function 200 also operates when the load change is completed. This is because if the operating load level changes, the optimal flame shape will naturally change as well. Control cycle management 2 to maintain the manipulated variable during load fluctuations or outside the control cycle
10 and operation amount holding 220 are provided. The operation amount management function 230 is for distinguishing between x^ * or x^ as the control operation amount 235 and a search operation amount 237 for finding these by search, and outputting them to the operating device 240. Measurement management function 250
This controls the timing of measuring the flame shape and exhaust gas concentration in response to trial operations. That is, after a trial operation, the flame shape measurement function 260 or the exhaust gas concentration measurement function 270 is activated after waiting until steady combustion is reached. CRT
The interface function 280 is for receiving system operation commands from the operator 97 and for displaying various combustion control states on the screen of the CRT 290 in response to requests from the operator. The boiler combustion process is complex and difficult to formulate for a model that can be used for online control. Here, in order to solve the nonlinear optimization problem mentioned above, we decided to apply the complex method, which is a type of nonlinear programming method, to perform trial operations on an actual plant and evaluate the actual values to determine the optimal target flame. A method is used to determine the shape. Now, if we define the CO concentration (Z CO ), NOx concentration (Z NOX ), and parallel damper opening degree ( A PD ) as x 10 = Z CO x 11 = Z NOX ) The constraint function (vector) h(x) and its control value (vector) h 0 can be defined by the following equation.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、排ガス中に含まれるNOx濃
度、CO濃度などの環境規制値を守り、最大効率
を維持した運転が可能となる。
According to the present invention, it is possible to operate while maintaining maximum efficiency while observing environmental regulation values such as NOx concentration and CO concentration contained in exhaust gas.

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

第1図は、本発明の実施例におけるボイラ火炉
のバーナ配置、燃料供給系及び空気・ガス系の配
置を説明するためのもの。第2図は、本発明の実
施例におけるバーナの構造を示すもの。第3図
は、本発明の実施例における火炉内火炎構造と各
バーナ段への空気比配分方式を説明するためのも
の。第4図は、本発明の実施例において、本発明
を適用することによる燃焼特性に関する期待効果
を説明するためのもの。第5図は、本発明の実施
例における燃焼制御システムの機能構成を説明す
るためのもの。第6図は、本発明の実施例におけ
る制御の基本処理手段を説明するためのもの。第
7図は、本発明の実施例における火炎形状の定義
を示すもの。第8図は、本発明の実施例における
最適目標火炎形状探索の基本アルゴリズムを説明
するためのもの。第9図は、本発明の実施例にお
ける火炎形状制御の基本アルゴリズムを説明する
ためのもの、をそれぞれ示す。 20…ボイラ火炉、30…燃料供給系、31…
石炭フイーダ、40…空気ガス系、41…押込通
風フアン(FDF)、50…一次ガス、200…最
適目標火炎形状探索、300…火炎形状制御、9
7…運転員、101…最適目標火炎形状y^*、1
02…最適操作量x^*、103…準最適操作量x^、
210…制御周期管理、220…操作量保持、2
30…操作量管理、235…制御操作量、237
…探索操作量、240…操作器、400…プラン
ト、250…計測管理、260…火炎形状計測、
270…排ガス濃度計測、280…CRTインタ
ーフエイス、290…CRT、500…中央給電
指令所、600…負荷変動監視。
FIG. 1 is for explaining the burner arrangement, fuel supply system, and air/gas system arrangement of a boiler furnace in an embodiment of the present invention. FIG. 2 shows the structure of a burner in an embodiment of the present invention. FIG. 3 is for explaining the flame structure in the furnace and the air ratio distribution method to each burner stage in the embodiment of the present invention. FIG. 4 is for explaining the expected effect on combustion characteristics by applying the present invention in an example of the present invention. FIG. 5 is for explaining the functional configuration of a combustion control system in an embodiment of the present invention. FIG. 6 is for explaining the basic processing means for control in the embodiment of the present invention. FIG. 7 shows the definition of flame shape in an embodiment of the present invention. FIG. 8 is for explaining the basic algorithm for searching for an optimal target flame shape in an embodiment of the present invention. FIG. 9 shows diagrams for explaining the basic algorithm of flame shape control in the embodiment of the present invention. 20... Boiler furnace, 30... Fuel supply system, 31...
Coal feeder, 40...Air gas system, 41...Forced draft fan (FDF), 50...Primary gas, 200...Optimum target flame shape search, 300...Flame shape control, 9
7...Operator, 101...Optimum target flame shape y^ * , 1
02...optimal operation amount x^ * , 103...semi-optimal operation amount x^,
210...Control cycle management, 220...Manipulated amount retention, 2
30...Manipulation amount management, 235...Control operation amount, 237
...Search operation amount, 240...Control device, 400...Plant, 250...Measurement management, 260...Flame shape measurement,
270...Exhaust gas concentration measurement, 280...CRT interface, 290...CRT, 500...Central power dispatch center, 600...Load fluctuation monitoring.

Claims (1)

【特許請求の範囲】 1 燃料、空気を供給して燃焼を行なう複数のバ
ーナを火炉の燃焼ガスの流れ方向に多段に具備
し、各段のバーナに供給する燃料或いは/及び空
気の流量を制御する燃焼制御方法において、 前記火炉の燃焼ガスの流れ方向に下段バーナと
中段バーナと上段バーナよりなる前記複数のバー
ナを備え、該下段バーナの空気比を1よりも小さ
くして還元性物質を生成する燃焼を行ない、該中
段バーナの空気比を1よりも大きくしてNOxを
生成する燃焼を行ない、該上段バーナの空気比を
該中段バーナの空気比よりも更に大きくして
NOx還元領域を形成し前記中段バーナで生成し
たNOxを前記下段バーナで生成した還元性物質
により還元する燃焼を行ない、 前記各段のバーナに供給する燃料或いは/及び
空気の流量を変えて複数回の試行操作を行ない、
各試行時の前記下段バーナと中段バーナ及び上段
バーナの火炎形状を夫々計測記憶し、 前記各試行時のCO濃度およびNOx濃度を検出
して該CO濃度に基づいて炉内燃焼効率を推定し、 前記複数回の試行操作の中でNOx濃度が予め
定めた規定値以下でかつ最大の推定燃焼効率が得
られたときの火炎形状を目標火炎形状とし、 前記各段のバーナによる火炎形状が夫々目標火
炎形状となるように前記各段のバーナに供給する
燃料あるいは空気の流量を制御することを特徴と
する燃焼制御方法。
[Scope of Claims] 1. A plurality of burners that supply fuel and air to perform combustion are provided in multiple stages in the direction of flow of combustion gas in a furnace, and the flow rate of fuel and/or air supplied to the burners in each stage is controlled. In the combustion control method, the plurality of burners consisting of a lower stage burner, a middle stage burner, and an upper stage burner are provided in the flow direction of the combustion gas of the furnace, and the air ratio of the lower stage burner is made smaller than 1 to generate reducing substances. The air ratio of the middle stage burner is made larger than 1 to perform combustion that generates NOx, and the air ratio of the upper stage burner is made even larger than the air ratio of the middle stage burner.
Combustion is performed to form a NOx reduction region and reduce NOx generated in the middle stage burner with a reducing substance generated in the lower stage burner, and the flow rate of fuel and/or air supplied to each stage burner is changed multiple times. Perform the trial operation of
Measuring and storing the flame shapes of the lower burner, middle burner, and upper burner during each trial, detecting the CO concentration and NOx concentration during each trial, and estimating the in-furnace combustion efficiency based on the CO concentration; The flame shape when the NOx concentration is below a predetermined value and the maximum estimated combustion efficiency is obtained during the plurality of trial operations is set as the target flame shape, and the flame shape by the burners at each stage is set as the target flame shape. A combustion control method comprising controlling the flow rate of fuel or air supplied to the burners in each stage so as to form a flame shape.
JP7271184A 1984-04-13 1984-04-13 Combustion control method Granted JPS60218525A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7271184A JPS60218525A (en) 1984-04-13 1984-04-13 Combustion control method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7271184A JPS60218525A (en) 1984-04-13 1984-04-13 Combustion control method

Publications (2)

Publication Number Publication Date
JPS60218525A JPS60218525A (en) 1985-11-01
JPH0260934B2 true JPH0260934B2 (en) 1990-12-18

Family

ID=13497208

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7271184A Granted JPS60218525A (en) 1984-04-13 1984-04-13 Combustion control method

Country Status (1)

Country Link
JP (1) JPS60218525A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012181003A (en) * 2011-03-03 2012-09-20 Ihi Corp Boiler device and high temperature air combustion system

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5707897B2 (en) * 2010-11-25 2015-04-30 株式会社Ihi Fine fuel fired boiler equipment
US10865985B2 (en) * 2018-02-20 2020-12-15 General Electric Technology Gmbh System and method for operating a combustion chamber
US12044641B2 (en) * 2020-05-29 2024-07-23 Baker Hughes Oilfield Operations Llc Emission monitoring of flare systems

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55131623A (en) * 1979-03-30 1980-10-13 Babcock Hitachi Kk Method of proper combustion for combustor
JPS614100Y2 (en) * 1979-07-23 1986-02-07
JPS58108326A (en) * 1981-12-22 1983-06-28 Mitsubishi Heavy Ind Ltd Burning method of burner

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012181003A (en) * 2011-03-03 2012-09-20 Ihi Corp Boiler device and high temperature air combustion system

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