JPS60202230A - Combustion device - Google Patents

Combustion device

Info

Publication number
JPS60202230A
JPS60202230A JP59057851A JP5785184A JPS60202230A JP S60202230 A JPS60202230 A JP S60202230A JP 59057851 A JP59057851 A JP 59057851A JP 5785184 A JP5785184 A JP 5785184A JP S60202230 A JPS60202230 A JP S60202230A
Authority
JP
Japan
Prior art keywords
sensors
specific gravity
fuel
burner
gas
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP59057851A
Other languages
Japanese (ja)
Inventor
Masahiro Indo
引頭 正博
Hideki Kaneko
秀樹 金子
Yoshifumi Moriya
好文 守屋
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59057851A priority Critical patent/JPS60202230A/en
Publication of JPS60202230A publication Critical patent/JPS60202230A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • F23N5/12Systems for controlling combustion using devices responsive to thermal changes or to thermal expansion of a medium using ionisation-sensitive elements, i.e. flame rods
    • F23N5/126Systems for controlling combustion using devices responsive to thermal changes or to thermal expansion of a medium using ionisation-sensitive elements, i.e. flame rods using electrical or electromechanical means
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F23COMBUSTION APPARATUS; COMBUSTION PROCESSES
    • F23NREGULATING OR CONTROLLING COMBUSTION
    • F23N2229/00Flame sensors
    • F23N2229/16Flame sensors using two or more of the same types of flame sensor

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)

Abstract

PURPOSE:To perform high precise detection of a combustion condition by a method wherein sensors, detecting a combustion condition, are respectively located to both ends of the burner port of a line burner, and a control means, which detects a combustion condition through comparison of sensor outputs therfrom with each other, is provided. CONSTITUTION:Sensors 7 and 8 are located to the both ends of a total primary line burner, and various combustion conditions are detected by means of outputs from the two sensors. Fuel, for example, LPG, having high gas specific gravity, forms flame distribution like a flow alpha with a main flow flowing on the bottom of a baurner body 2 since a specific gravity after incoming of the air is increased over 1 of the air, gas specific gravity of LPG is about 1.6, and concentration distribution also tends to become alpha. Conversely, the specific gravity of gas such as methane is 0.5-0.6, and since gas body is apt to flow to the upper surface side of a burner body, concentration distribution is apt to form the shape of beta. Thus, when either the two sensors attains a threshold, a fuel velve 10 is closed to stop the supply of fuel to ensure safety. Detection of either sensor outputs at opposite ends of a bruner enables detection of safe rise and an oxygen deficiency condition before either of burthers is brought to poor combustion condition.

Description

【発明の詳細な説明】 産業上の利用分野 本発明はライン状の全−次燃焼装置に関する。[Detailed description of the invention] Industrial applications The present invention relates to a line-shaped post-combustion device.

従来例の構成とその問題点 従来この種の全−次燃焼装置の検出装置として、熱電対
、フレームロッド、各種02センサ等があり、最近は着
火、燃焼状態、酸欠、バツクファイヤー等検出項目も増
大し、より高い安全性がめられるようになり、複数のヒ
ンサの組み合せ検出も増大しめきているが、特に全−次
バーナの場合着火範囲(空燃比1.0〜1.6)、酸欠
(を燃比1.0以下では不完全燃焼)等規制条件ケ越え
ると極端にcoが発生したり、全熱着火しない等の課題
があり、かつ長方形のライン状に燃せずバーナにおいて
は、長手方向に空燃比および火炎長等均一化することは
設計的にもむつかしい。第1図の全−次の炎孔1上に形
成される火炎は、実線で示1−α、点線で示すβのよう
に、燃焼量あるいは燃料ガスの種類によって火炎長が異
なりやすいものであり、適切な検出状1g’に得にくい
のが実情である。
Conventional structure and its problems Traditionally, detection devices for this type of primary combustion device include thermocouples, flame rods, and various 02 sensors.Recently, detection items such as ignition, combustion status, oxygen deficiency, backfire, etc. have been used. As the number of burners increases, higher safety is required, and the detection of combinations of multiple hinges is also increasing. (If the fuel ratio is less than 1.0, combustion will be incomplete.) If the regulation conditions are exceeded, there will be problems such as excessive CO generation and failure to ignite with full heat. It is difficult from a design standpoint to make the air-fuel ratio and flame length uniform in both directions. The flame formed on the full flame hole 1 in Figure 1 tends to have a different flame length depending on the amount of combustion or the type of fuel gas, as shown by the solid line 1-α and the dotted line β. The reality is that it is difficult to obtain a suitable detection letter 1g'.

発明の目的 本発明は、燃焼状態の検知會精度を良く行うこと?目的
と1−る。
Purpose of the Invention The present invention is to detect combustion conditions with high precision. Purpose and 1-ru.

発明の構成 この目的を達成するためにライン状バーナの炎孔部の両
端に、燃焼状匙紮検出するセンサ葡それぞれ設け、その
センサ出力の比較で、燃焼状F?に検出する制御手段を
備えたものである。
Structure of the Invention In order to achieve this object, sensors for detecting the combustion state are provided at both ends of the flame hole of the line-shaped burner, and by comparing the sensor outputs, it is possible to determine whether the combustion state is F? It is equipped with a control means for detecting the

この構成によって、炎孔の両端での火炎長あるいは突気
・燃料の混合気等の分布があっても、両者センサの出力
比較により、燃焼状態全検知できるものであり、燃料の
制御が適正にできるという作用を有する。
With this configuration, even if there is a distribution of flame length or sudden air/fuel mixture at both ends of the flame hole, the entire combustion state can be detected by comparing the outputs of both sensors, and the fuel can be controlled appropriately. It has the effect of being able to do something.

実施例の説明 以下本発明の一実施例を第1図を設いて説明する。第1
図において、ライプ状で金網よりなる全−次の炎孔1の
下方のバーナ体2の右端には一次空気孔3を有し′てい
る。またこの部分には絞り部4、炎孔1の右端下方には
を気4・燃料の混合均一化のための均−板5を設けてい
る0炎孔1の上部には燃焼室6を設け、その燃焼室壁を
絶縁貫通してセンサとして左側の炎孔1の上部にはフレ
ームロッド7、右側の炎孔1の上部には酸化錫8を設け
、センサ出力は制御装置9で演算判断され、燃料弁10
會開閉している。11は燃料供給ノズル?示す。上記構
成において、均−板5により、ノズル11から供給され
る燃料と、−次突気孔3から吸引される空気が均一混合
され、炎孔1に均一分布されるようにバーナ体2の設計
は行われているが、燃料としてガスを考えると比重が0
.5の都市ガスから2.1のブタンまでバラツキも太き
く、更に燃料の絞り巾を広くとると、真の均一分布およ
び均一濃度分布は非常に困難なものである。第1図炎孔
1上の曲線aおよびβの火炎分布が全く逆になる場合も
ある。例えばLPGのようにガス比重の大きいものは、
全気流人後の比重がやはり空気の1より犬きくなるため
バーナ体2の底辺全主流として流れαのような火炎分布
でありかつLPGのガス比重1.6前後であり濃度分布
もαのようになる傾向にある。逆にメタン等のガス比重
は0.5〜0.6であり、ガス体はバーナ体の上面側に
流れ易いため濃度分布はβの形状となり易い。
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. 1st
In the figure, a primary air hole 3 is provided at the right end of the burner body 2 below a full-length flame hole 1 which is rib-shaped and made of wire mesh. In addition, a throttle part 4 is provided in this part, and a leveling plate 5 is provided below the right end of the flame hole 1 to ensure a uniform mixture of air 4 and fuel.A combustion chamber 6 is provided in the upper part of the flame hole 1. A flame rod 7 is installed at the top of the left flame hole 1 and a tin oxide 8 is installed at the top of the right flame hole 1 as a sensor by penetrating the insulation of the combustion chamber wall, and the sensor output is calculated and judged by the control device 9. , fuel valve 10
Meetings are open and closed. Is 11 the fuel supply nozzle? show. In the above configuration, the burner body 2 is designed so that the equalizing plate 5 uniformly mixes the fuel supplied from the nozzle 11 and the air sucked from the secondary blow hole 3 and uniformly distributes it to the flame hole 1. However, when considering gas as a fuel, the specific gravity is 0.
.. There is wide variation from city gas at 5.0 to butane at 2.1, and if the aperture width of the fuel is widened, it is extremely difficult to achieve truly uniform distribution and uniform concentration distribution. The flame distributions of curves a and β on flame hole 1 in FIG. 1 may be completely opposite. For example, gases with high specific gravity such as LPG,
Since the specific gravity of the total air flow is still much higher than that of air (1), it flows as the entire main stream at the bottom of the burner body 2, and the flame distribution is like α, and the gas specific gravity of LPG is around 1.6, so the concentration distribution is also like α. It tends to become. Conversely, the specific gravity of a gas such as methane is 0.5 to 0.6, and the gas tends to flow toward the upper surface of the burner body, so the concentration distribution tends to be in the shape of β.

これら?均−板5で均一化するようにしているが、ガス
種がLPGの場合で絞り比?大きくしていくと、分布は
a→βの曲線のように変化していく、従って燃料の種類
および絞り巾の拡大全てにわたって同一形状のライン状
バーナで均一濃度および均一火炎分布にすることは設計
的にも非常にむっかしい。第2図に立上りのセンサ出力
を示すが、実線の■@はαの火炎及び濃度分布時、点線
の■′O牡βの火炎及び濃度分布時の特性であり、燃料
ガスの混合気に点火し立上りを検出するのにαの分布で
は、■のイオン電流の立上りが濃度お・よび火炎分布に
応じ早く、図示の如(t、secでフレーム電流のしき
い値Aに到達するが、濃度火炎分布の低い右端の酸化錫
センサ部は@で示すように火炎湯度の立上がりも遅く、
火炎高さ低いため燃焼室6の上部からのを気の流入もあ
り、火炎帯内に酸化錫8か入らないため徐々に抵抗値が
低下する。
these? I try to equalize it with the equalizing plate 5, but what about the aperture ratio when the gas type is LPG? As the size increases, the distribution changes like a curve from a to β. Therefore, it is difficult to achieve uniform concentration and flame distribution with a linear burner of the same shape across all types of fuel and expansion of throttle width. It's also very difficult. Figure 2 shows the sensor output at the rise. The solid line ■@ is the characteristic when the flame and concentration distribution is α, and the dotted line ■@ is the characteristic when the flame and concentration distribution is β. In order to detect the rise, the rise of the ion current in (■) is early depending on the concentration and flame distribution, and reaches the threshold value A of the flame current at (t, sec) as shown in the figure. In the tin oxide sensor section on the right end where the flame distribution is low, the flame temperature rises slowly as shown by @.
Since the flame height is low, air flows in from the upper part of the combustion chamber 6, and since the tin oxide 8 does not enter the flame zone, the resistance value gradually decreases.

従ってしきい値Bになるまでt4 S e Cとイオン
電流のt、に比べ大巾に遅くなる。従って着火検出とし
てイオン電流の■とセンサ抵抗Oそれぞれのしきい値の
早い方を判定すれば良い。反対にβの火炎および濃度分
布の場合は、図示の如くセンサ抵抗の変化の方が急とな
りしきい値B検知までにt2sec、逆にイオン電流は
t s s e Cと遅くなる。従ってこの場合の着火
検知はセンサ抵抗で検知すれば良い。また第3図に示す
ように酸欠に対する酸化錫8 (Sn02)の抵抗値変
化とフレームロッド7電流値変化を示す。θOの曲線は
αの火炎および濃度分布時の特性、θ0の曲線βは分布
時の特性全示す。aの分布の時は5n028の雰囲気は
初期から02濃度高いので酸欠により〜濃度の低下し0
キO%となるのは17′チ位であるがβの分布の時は逆
に雰囲気0 濃度は初期から火炎帯内にあるため低く図
示の如< 18.5%位でo22O27の電流は酸化錫
(SnO)8と逆の特性となる。
Therefore, until the threshold value B is reached, it is much slower than t4 S e C and t of the ion current. Therefore, for ignition detection, it is sufficient to determine whichever is earlier of the threshold values of the ion current (■) and the sensor resistance O. On the other hand, in the case of the flame and concentration distribution of β, as shown in the figure, the change in sensor resistance becomes steeper, and it takes t2 seconds to detect the threshold value B, whereas the ion current slows down to t s se C. Therefore, ignition detection in this case may be performed using a sensor resistance. Furthermore, as shown in FIG. 3, changes in the resistance value of tin oxide 8 (Sn02) and changes in the current value of the frame rod 7 due to oxygen deficiency are shown. The θO curve shows the characteristics when α is flame and concentration distribution, and the θ0 curve β shows all the characteristics when distributed. When the distribution is a, the atmosphere of 5n028 has a high 02 concentration from the beginning, so the concentration decreases due to oxygen deficiency and 0.
KiO% is at the 17' position, but in the case of β distribution, on the contrary, the atmosphere is 0. Since the concentration is within the flame zone from the beginning, it is low, as shown in the figure, at about <18.5%, the current of o22O27 is oxidized. The properties are opposite to those of tin (SnO) 8.

となり抵抗値が急変している。フレームロッド図中R、
E は酸化錫(Sn○)8の抵抗値のし べt 1. 
2 。
The resistance value changes suddenly. Frame rod R in the diagram,
E is the resistance value of tin oxide (Sn○)8.
2.

きい値、フレームロッド7のイオン電流値のしき ・い
値を示す。従って両センザのどちらかしきい値に達すれ
ば、燃料弁10?閉じ燃焼をストップさせ安全會保つ等
、バーナ両端のどちらかのセンサ出力を検出することに
より、バーナのどちらかが燃焼不良奮起こす前に安全に
立上りや酸欠状態音検知する効果がある。センサとして
フレーム0.2ドばがり2本、あるいはその他のセンサ
全般いても良いし、検知方法の制御手段を変えても良い
のは勿論のことである。
Threshold value indicates the threshold value of the ion current value of frame rod 7. Therefore, if the threshold value of either sensor is reached, the fuel valve 10? By detecting sensor output from either end of the burner, such as stopping closed combustion and maintaining safety, it is effective to safely detect start-up or oxygen deficient sound before either burner starts to suffer from poor combustion. It goes without saying that the sensors may be two 0.2mm sensors or any other type of sensor, or that the control means for the detection method may be changed.

発明の効果 以上のように°本発明の燃焼装置によれば次の効果が得
られる。
Effects of the Invention As described above, the combustion apparatus of the present invention provides the following effects.

(1)全−次ラインバーナの両端にセンサをそれぞれ設
け、その両センサの出力で各種燃焼状態音検出するので
、バーナ全体の燃焼状%’に常に判断しながら適正な制
御手段がとれる。
(1) Sensors are provided at both ends of the primary line burner, and various combustion state sounds are detected using the outputs of both sensors, so that appropriate control means can be taken while constantly determining the combustion state of the burner as a whole.

(2)分布の悪い全−次ラインバーナにおいて、両端に
センサを設けることにより、絞り比を大きくとって・も
、燃焼状餓全適切に検出できる。
(2) In a full-order line burner with poor distribution, by providing sensors at both ends, combustion state starvation can be appropriately detected even if the aperture ratio is set large.

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

第1図は本発明の一実施例の構成図、第2図はセンサ出
力の経通時間変化の特性図、第3図は酸欠時のセンサ出
力変化の特性図である。 1・・・“・炎孔、7 ・・・・フレームロッド、8・
・・・・・酸化錫、9・・・・・・制御装置。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第21箇 第 3 N
FIG. 1 is a block diagram of an embodiment of the present invention, FIG. 2 is a characteristic diagram of changes in sensor output over time, and FIG. 3 is a characteristic diagram of changes in sensor output during oxygen deficiency. 1..."・Flame hole, 7...Frame rod, 8.
...Tin oxide, 9...Control device. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 21, 3rd N

Claims (1)

【特許請求の範囲】[Claims] (1)ライン状バーナの炎孔部両端に火炎状態全検出す
るセンサをそれぞれ設け、そのセンサー出力を比較して
燃焼状態を検知する制御手段を備えた燃焼装置。 (巧 センサとして一方をフレームロッドとし、他方を
酸化ジルコニア、酸化錫等の02センサとした特許請求
の範囲第1項記載の燃焼装置。
(1) A combustion device that includes sensors for detecting all flame conditions at both ends of the flame hole of a line-shaped burner, and a control means that compares the outputs of the sensors to detect the combustion condition. (Takumi) The combustion device according to claim 1, wherein one of the sensors is a flame rod, and the other is an 02 sensor made of zirconia oxide, tin oxide, or the like.
JP59057851A 1984-03-26 1984-03-26 Combustion device Pending JPS60202230A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59057851A JPS60202230A (en) 1984-03-26 1984-03-26 Combustion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59057851A JPS60202230A (en) 1984-03-26 1984-03-26 Combustion device

Publications (1)

Publication Number Publication Date
JPS60202230A true JPS60202230A (en) 1985-10-12

Family

ID=13067484

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59057851A Pending JPS60202230A (en) 1984-03-26 1984-03-26 Combustion device

Country Status (1)

Country Link
JP (1) JPS60202230A (en)

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