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JP3137711B2 - Combustion air supply device - Google Patents

Combustion air supply device

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Publication number
JP3137711B2
JP3137711B2 JP04028227A JP2822792A JP3137711B2 JP 3137711 B2 JP3137711 B2 JP 3137711B2 JP 04028227 A JP04028227 A JP 04028227A JP 2822792 A JP2822792 A JP 2822792A JP 3137711 B2 JP3137711 B2 JP 3137711B2
Authority
JP
Japan
Prior art keywords
burner
combustion air
wind box
resistor
duct
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 - Fee Related
Application number
JP04028227A
Other languages
Japanese (ja)
Other versions
JPH05223240A (en
Inventor
秀久 吉廻
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 Power Ltd
Original Assignee
Babcock Hitachi KK
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 Babcock Hitachi KK filed Critical Babcock Hitachi KK
Priority to JP04028227A priority Critical patent/JP3137711B2/en
Publication of JPH05223240A publication Critical patent/JPH05223240A/en
Application granted granted Critical
Publication of JP3137711B2 publication Critical patent/JP3137711B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は燃焼装置に係わり、特
に、ダクトと風箱とバーナとからなり、ダクトから流れ
込んだ燃焼用空気を一旦風箱に導いた後、バーナに供給
する燃焼用空気供給装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a combustion apparatus, and more particularly, to a combustion apparatus comprising a duct, a wind box and a burner. The combustion air flowing from the duct is guided to the wind box and then supplied to the burner. It relates to a supply device.

【0002】[0002]

【従来の技術】最近のバーナは低NOx・低煤塵で燃焼
する低公害燃焼、低未燃分で燃焼する高効率燃焼、低負
荷から高負荷まで安定に燃焼する広範囲運転燃焼が要求
されている。そのため、特に大容量のバーナを有した事
業用ボイラでは可能な限り燃焼器の最適設計が計られて
いる。
2. Description of the Related Art Recent burners require low-pollution combustion burning with low NOx and low dust, high-efficiency combustion burning with low unburned components, and wide-range operation combustion burning stably from low load to high load. . For this reason, especially for a commercial boiler having a large-capacity burner, the optimal design of the combustor is made as much as possible.

【0003】その一つに風箱がある。風箱はダクトでバ
ーナまで導かれた燃焼用空気を一旦減速させ、バーナへ
の流入空気量を周方向に均一化させるものである。
One of them is a wind box. The wind box is used to temporarily reduce the combustion air guided to the burner by the duct, and to make the amount of air flowing into the burner uniform in the circumferential direction.

【0004】代表的な風箱の構造を図と図および図
に示す。図において、燃焼用空気は押し込み送風器
で大気から吸い込まれ、熱交換器で約300℃に加熱さ
れた後、ダクト5を経由して風箱6に送られる。ここ
で、ダクト5内の燃焼用空気の運動エネルギはダクト内
風速が15m/sなので、圧力に換算して11mmAq
である。普通、バーナ差圧(風箱静圧−火炉静圧)は8
0mmAq程度なので、このままではバーナ1への流入
速度に大きなアンバランスが生じる。
FIGS. 6 and 7 show a typical structure of a wind box.
FIG . In FIG. 6 , combustion air is sucked from the atmosphere by a forced air blower, heated to about 300 ° C. by a heat exchanger, and then sent to a wind box 6 via a duct 5. Here, the kinetic energy of the combustion air in the duct 5 is 11 mmAq in terms of pressure since the wind speed in the duct is 15 m / s.
It is. Normally, the burner differential pressure (wind box static pressure-furnace static pressure) is 8
Since it is about 0 mmAq, a large imbalance occurs in the inflow speed into the burner 1 as it is.

【0005】一方、風箱6で燃焼用空気の風速を8m/
s以下に低下させると、運動エネルギは3.2mmAq
となり、バーナ1への流入速度のアンバランスは大きく
改善される。なお、図において2は火炉、3は火炉壁、
4は火炎、7は燃料配管である。
On the other hand, the wind speed of the combustion air is set to 8 m /
s, the kinetic energy becomes 3.2 mmAq
Thus, the imbalance of the inflow speed into the burner 1 is greatly improved. In the figure, 2 is a furnace, 3 is a furnace wall,
4 is a flame and 7 is a fuel pipe.

【0006】図、図の例は1個の風箱6の中に複数
のバーナ1を内蔵したものである。この場合も原理は同
じである。
FIGS. 7 and 8 show examples in which a plurality of burners 1 are built in one wind box 6. In this case, the principle is the same.

【0007】[0007]

【発明が解決しようとする課題】このように、風箱はバ
ーナへ燃焼用空気を均一に供給するために考案されたも
のであるが、その原理から明らかなように、風箱は大き
な空間を持たないと用をなさない。つまり、事業用ボイ
ラのようにバーナが多段・多列に装着され、バーナとバ
ーナの間隔が制限されている場合には、風箱を厚くする
しかない。しかし、風箱を厚くするとボイラの重量と占
有面積が増えるのでボイラを支える鉄骨が大きくなり、
建設費が大幅に増加する。
As described above, the wind box is designed to uniformly supply the combustion air to the burner. However, as is clear from the principle, the wind box occupies a large space. If you do not have it, you will not use it. In other words, when the burners are mounted in multiple stages and multiple rows as in a commercial boiler and the interval between the burners is limited, the only option is to make the wind box thicker. However, thickening the wind box increases the weight and occupied area of the boiler, so the steel frame supporting the boiler increases,
Construction costs increase significantly.

【0008】この問題を解決するために、例えば図
ように風箱とバーナの間に整流板16を設け、風箱を大
きくしないでバーナへの均一供給を計ろうとしたものが
ある。しかし、整流板16では圧力損失が小さいのでバ
ーナの旋回羽根8の開度が設定条件と変わつたときに対
応することができない。
In order to solve this problem, for example, as shown in FIG. 9 , a rectifying plate 16 is provided between a wind box and a burner so as to make uniform supply to the burner without increasing the size of the wind box. However, since the pressure loss is small in the rectifying plate 16, it is not possible to cope with the case where the opening degree of the swirling blade 8 of the burner changes from the set condition.

【0009】本発明は、ボイラを大型化することなく、
バーナに均一に燃焼用空気を供給することができる燃焼
用空気供給装置を提供することを目的とする。
According to the present invention, without increasing the size of the boiler,
An object of the present invention is to provide a combustion air supply device capable of uniformly supplying combustion air to a burner.

【0010】[0010]

【課題を解決するための手段】上記目的を達成するため
には、風箱の内側に円筒状の抵抗体を前記バーナを囲む
ように配置し、抵抗体の中心軸がバーナの中心軸に対し
てダクト側からみて燃焼用空気の流れ方向下流側に偏心
させればよい。
In order to achieve the above object , a cylindrical resistor is provided inside a wind box to surround the burner.
So that the center axis of the resistor is aligned with the center axis of the burner.
Eccentric to the downstream side in the combustion air flow direction as viewed from the duct side
It should be done.

【0011】[0011]

【作用】ダクトから風箱に流入した燃焼用空気は、円筒
状の抵抗体によつて風箱内に均一分散される。しかも、
抵抗体がダクト側からみて下流側に偏心しているので、
風箱内において、上流側と下流側との流速が殆ど同じに
なる。その結果、バーナには均一に燃焼用空気が供給さ
れる。
The combustion air flowing into the wind box from the duct is uniformly dispersed in the wind box by the cylindrical resistor. Moreover,
Since the resistor is eccentric downstream from the duct side,
In the wind box, the flow rates on the upstream side and the downstream side are almost the same. As a result, the combustion air is uniformly supplied to the burner.

【0012】[0012]

【実施例】図1、図2に本発明の実施例を示す。バーナ
1は微粉炭焚き用で燃料消費量は5t/hである。バー
ナ1のスロート径は1,000mmで、バーナ1を包む
ように円筒状の抵抗体10が囲んでいる。抵抗体10の
直径は1,600mmで、バーナ1の中心と100mm
だけずらして取り付けてある。抵抗体10は厚さ6m
m、開口率30%の多孔板である。燃焼用空気はダクト
5内を風速15m/sで流れるが、多孔板で均等配分さ
れ旋回羽根8を通つてスロートに至る。旋回羽根8の角
度は最適な燃焼が行われるようにハンドル9で調整され
る。
1 and 2 show an embodiment of the present invention. The burner 1 is for pulverized coal combustion and has a fuel consumption of 5 t / h. The throat diameter of the burner 1 is 1,000 mm, and a cylindrical resistor 10 surrounds the burner 1. The diameter of the resistor 10 is 1,600 mm, and the center of the burner 1 is 100 mm.
It is attached only by shifting. Resistor 10 is 6m thick
m, a perforated plate having an aperture ratio of 30%. The combustion air flows through the duct 5 at a wind speed of 15 m / s, but is equally distributed by the perforated plate and reaches the throat through the swirling vanes 8. The angle of the swirling vanes 8 is adjusted by the handle 9 so that optimal combustion is performed.

【0013】図3は本発明の作用を確認するために旋回
羽根8の入口側に静圧測定用の孔を設け、起点から静圧
を周方向に9点測定した結果を示す。横軸は起点11か
らの角度である。イは抵抗体を入れない場合、ロは入れ
た場合を示す。イの場合、静圧は一旦最低になつた後、
除々に回復している。この現象は流体の運動エネルギー
と静圧との和が一定であることを述べたベルヌーイの式
で説明することができる。つまり、ダクトからの空気が
真正面にぶつかる起点では速度が0になるので、運動エ
ネルギーがそのまま静圧に変換される。その後、燃焼用
空気は左右に分かれるが、その時、流速が最大となるの
で静圧は最低となる。さらに、燃焼用空気が下流側に回
るに連れて、一部の燃焼用空気は旋回羽根8を通つてバ
ーナ1に入るので流量が減少し、流速が次第に低下す
る。その結果、静圧は除々に上昇する。
FIG. 3 shows the results of measuring the static pressure at nine points in the circumferential direction from the starting point by providing a hole for measuring the static pressure on the inlet side of the swirling blade 8 to confirm the operation of the present invention. The horizontal axis is the angle from the starting point 11. A indicates the case where the resistor is not inserted, and B indicates the case where the resistor is inserted. In the case of b, once the static pressure has reached a minimum,
He is recovering gradually. This phenomenon can be explained by Bernoulli's equation which states that the sum of the kinetic energy of the fluid and the static pressure is constant. That is, the velocity becomes 0 at the starting point where the air from the duct collides directly in front, and the kinetic energy is directly converted to static pressure. After that, the combustion air is divided into left and right. At that time, the flow velocity becomes maximum and the static pressure becomes minimum. Further, as the combustion air goes downstream, a part of the combustion air enters the burner 1 through the swirling vanes 8, so that the flow rate decreases, and the flow velocity gradually decreases. As a result, the static pressure gradually increases.

【0014】これに対し、抵抗10を設けたロの場合
には流速の低下がないので静圧は変化しない。
[0014] In contrast, the static pressure does not change because there is no decrease in the flow rate in the case of the resistor 10 is provided b.

【0015】バーナ1に流入する空気量は火炉2側の静
圧が一定だから、測定した静圧分布に比例して分布す
る。従つて、本発明によつて小さな風箱でもバーナ1へ
流入する燃焼用空気がほぼ均一になることが分かる。
The amount of air flowing into the burner 1 is distributed in proportion to the measured static pressure distribution because the static pressure on the furnace 2 side is constant. Therefore, according to the present invention, it can be seen that the combustion air flowing into the burner 1 becomes almost uniform even in a small wind box.

【0016】なお、最適な偏心量(抵抗体10の中心と
バーナ1中心とのずれ)を求めるために、偏心量とその
時の各旋回羽根8間の流入速度との関係を調べた結果を
図4に示す。図4の横軸は偏心量を多孔板の直径で割つ
た偏心率、縦軸は各流入速度から算出した変動率を示
す。これより、多孔板をダクト5と反対側にずらしたと
ころに最適値があることが分かる。多孔板を設置しない
ときの変動率は40%であるから、偏心率が−20%
(ダクト側へ偏心)から+40%の範囲で有効なことが
分かる。
The relationship between the amount of eccentricity and the inflow speed between the respective swirling blades 8 at that time is shown in FIG. It is shown in FIG. The horizontal axis in FIG. 4 shows the eccentricity obtained by dividing the amount of eccentricity by the diameter of the perforated plate, and the vertical axis shows the fluctuation rate calculated from each inflow velocity. From this, it can be seen that there is an optimum value when the perforated plate is shifted to the side opposite to the duct 5. The eccentricity is -20% because the variation rate when no perforated plate is installed is 40%.
(Eccentric to the duct side) from + 40% is effective.

【0017】図5は起点になる部分に遮蔽板15を設
け、この部分の流量が多くなるのを防止するようにした
ものである。これによつて、流量のアンバランスは10
%以下にすることができた。
FIG. 5 shows a structure in which a shielding plate 15 is provided at a portion serving as a starting point to prevent an increase in the flow rate at this portion. As a result, the flow rate imbalance is 10
%.

【0018】[0018]

【0019】[0019]

【0020】[0020]

【発明の効果】以上説明したように、本発明によれば、
バーナと風箱との間に円筒状の抵抗体を置き、しかも、
抵抗体の中心がバーナの中心軸と異なるように偏心させ
て配置したので、風箱を大きくすることなく、即ち、ボ
イラを大きくすることなくバーナに均一に燃焼用空気を
供給することができる。
As described above, according to the present invention,
Place a cylindrical resistor between the burner and the wind box, and
Since the resistor is disposed eccentrically so that the center of the resistor is different from the center axis of the burner, combustion air can be uniformly supplied to the burner without increasing the size of the wind box, that is, without increasing the size of the boiler.

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

【図1】本発明の実施例に係る風箱の側断面図である。FIG. 1 is a side sectional view of a wind box according to an embodiment of the present invention.

【図2】本発明の実施例に係る風箱の正面図である。FIG. 2 is a front view of a wind box according to the embodiment of the present invention.

【図3】バーナ周方向の静圧分布特性図である。FIG. 3 is a graph showing static pressure distribution characteristics in a circumferential direction of a burner.

【図4】偏心量と速度変動率の関係を示す特性図であ
る。
FIG. 4 is a characteristic diagram showing a relationship between an eccentric amount and a speed variation rate.

【図5】遮蔽板を付け加えた風箱の正面図である。FIG. 5 is a front view of a wind box to which a shielding plate is added.

【図6】従来の風箱の側断面図である。 FIG. 6 is a side sectional view of a conventional wind box.

【図7】複数個のバーナを有した従来の風箱の正面図で
ある。
FIG. 7 is a front view of a conventional wind box having a plurality of burners.
is there.

【図8】複数個のバーナを有した従来の風箱の平面図で
ある。
FIG. 8 is a plan view of a conventional wind box having a plurality of burners.
is there.

【図9】整流板を取り付けた従来の風箱の正面図であ
る。
FIG. 9 is a front view of a conventional wind box to which a current plate is attached.
You.

【符号の説明】[Explanation of symbols]

1 バーナ 2 火炉 3 火炉壁 4 火炎 5 ダクト 6 風箱 7 燃料配管 8 旋回羽根 9 旋回調整ハンドル 10 抵抗体 11 起点 DESCRIPTION OF SYMBOLS 1 Burner 2 Furnace 3 Furnace wall 4 Flame 5 Duct 6 Wind box 7 Fuel pipe 8 Swirl blade 9 Swirl adjustment handle 10 Resistor 11 Starting point

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 ダクトと風箱とバーナとを備えて燃焼用
空気をバーナに供給する燃焼用空気供給装置において、
前記風箱の内側に円筒状の抵抗体を前記バーナを囲むよ
うに配置し、抵抗体の中心軸がバーナの中心軸に対して
ダクト側からみて燃焼用空気の流れ方向下流側に偏心し
ていることを特徴とする燃焼用空気供給装置。
1. A combustion device comprising a duct, a wind box, and a burner .
In a combustion air supply device for supplying air to a burner,
A cylindrical resistor inside the wind box surrounds the burner.
So that the center axis of the resistor is aligned with the center axis of the burner.
It is eccentric to the downstream side in the flow direction of the combustion air as viewed from the duct side.
And combustion air supply device, characterized in that it is.
【請求項2】 請求項1記載の燃焼用空気供給装置にお
いて、前記抵抗体が多孔板から構成されていることを特
徴とする燃焼用空気供給装置。
2. The combustion air supply device according to claim 1 ,
Wherein the resistor comprises a perforated plate .
JP04028227A 1992-02-14 1992-02-14 Combustion air supply device Expired - Fee Related JP3137711B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04028227A JP3137711B2 (en) 1992-02-14 1992-02-14 Combustion air supply device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04028227A JP3137711B2 (en) 1992-02-14 1992-02-14 Combustion air supply device

Publications (2)

Publication Number Publication Date
JPH05223240A JPH05223240A (en) 1993-08-31
JP3137711B2 true JP3137711B2 (en) 2001-02-26

Family

ID=12242722

Family Applications (1)

Application Number Title Priority Date Filing Date
JP04028227A Expired - Fee Related JP3137711B2 (en) 1992-02-14 1992-02-14 Combustion air supply device

Country Status (1)

Country Link
JP (1) JP3137711B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4831815B2 (en) * 2006-02-28 2011-12-07 三菱重工業株式会社 Burner nozzle, pulverized fuel burning burner, and pulverized fuel combustion device
CN115560354A (en) * 2022-10-19 2023-01-03 国家电投集团江西电力有限公司新昌发电分公司 Air inducing device for combustor and design method thereof

Also Published As

Publication number Publication date
JPH05223240A (en) 1993-08-31

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