JPH03260504A - Fluidized bed type combustion device and combustion method - Google Patents

Fluidized bed type combustion device and combustion method

Info

Publication number
JPH03260504A
JPH03260504A JP5664990A JP5664990A JPH03260504A JP H03260504 A JPH03260504 A JP H03260504A JP 5664990 A JP5664990 A JP 5664990A JP 5664990 A JP5664990 A JP 5664990A JP H03260504 A JPH03260504 A JP H03260504A
Authority
JP
Japan
Prior art keywords
reaction chamber
fluidized bed
combustion
air
circulating
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.)
Granted
Application number
JP5664990A
Other languages
Japanese (ja)
Other versions
JP2622299B2 (en
Inventor
Yuichi Fujioka
祐一 藤岡
Nobuaki Murakami
信明 村上
Naoharu Hayashida
直治 林田
Yukihisa Fujima
藤間 幸久
Keisuke Sonoda
圭介 園田
Satoki Motai
甕 聰樹
Shigeyasu Ishigami
石神 重泰
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 Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries 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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP5664990A priority Critical patent/JP2622299B2/en
Publication of JPH03260504A publication Critical patent/JPH03260504A/en
Application granted granted Critical
Publication of JP2622299B2 publication Critical patent/JP2622299B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Fluidized-Bed Combustion And Resonant Combustion (AREA)

Abstract

PURPOSE:To perform a high efficient combustion of not-yet burned particles at a free board under an occurrence of a Rankin type circulation flow at the free board formed within the second reaction chamber by a method wherein a circulating vane fixed at an inlet port of the second reaction chamber and an air supplying pipe for injecting air in the same direction as the circulating direction of the circulating vane are provided. CONSTITUTION:Combustion gas is circulated by a circulating vane 13 mounted at an inlet port of a second reaction chamber B and then fed into the second reaction chamber B. The circulating vane is not connected to the outer wall 15 of the second reaction chamber B, but there is a clearance (d) between them, so that the gas at the outer wall 15 of the second reaction chamber does not receive any circulating force from the circulating vane 13. This clearance (d) and an angle theta between the circulating vane 13 and the center of the shaft may also influence over a formation of Rankine eddy flow within the second reaction chamber B. An air supplying pipe 116 is arranged in the center of the shaft in the second reaction chamber B and then a free board air supplying nozzle 14 is opened. This air supplying nozzle 14 has its blowing port mounted in such a direction as one having an angle phi in respect to a radial direction. Under such an arrangement of the angle phi, circulation of combustion gas 108 within the second reaction chamber B is assisted under an injection of the free board air. Accordingly, mean staying time of particle is extended and combustion efficiency of the particles at the free board within the second reaction chamber B is increased.

Description

【発明の詳細な説明】 〔産業上の利用分野] 本発明は、石炭等の固体燃料やCWM、重質油等の液体
燃料の燃焼に適用される装置および方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an apparatus and method applied to the combustion of solid fuels such as coal and liquid fuels such as CWM and heavy oil.

〔従来の技術] 従来、石灰石やドロマイト等を流動媒体として、石炭等
を燃焼させると同時に脱硫も行なうという流動床燃焼装
置および方法が実用化されている。
[Prior Art] Conventionally, fluidized bed combustion apparatuses and methods have been put into practical use that use limestone, dolomite, or the like as a fluidized medium to combust coal or the like and simultaneously perform desulfurization.

そのような従来の代表的な例を第7図に基づいて説明す
る。
A typical example of such a conventional method will be explained based on FIG. 7.

流動床(11)は、水冷壁(5)に囲まれた、分散板(
6)上に形成されている。流動床とは分散板の下方から
供給されるガスによって粒子が浮遊し、ガスにより混合
攪拌されている状態であり、その上方には粒子の存在割
合が流動床よりも1桁以上小さくなったフリーボード(
12)が存在する。石炭(102)と石灰石(103)
は供給ノズル(2) 、 (3)からそれぞれ流動床(
11)へ供給され、空気(101)は空気供給ノズル(
1)から風箱(10)を経て、多数の小孔を有する分散
板(6)から流動床(11)へ供給される。
The fluidized bed (11) consists of a dispersion plate (
6) Formed on top. A fluidized bed is a state in which particles are suspended by gas supplied from below the dispersion plate and mixed and stirred by the gas. board(
12) exists. Coal (102) and limestone (103)
are the fluidized bed (
11), and the air (101) is supplied to the air supply nozzle (
1), passes through a wind box (10), and is supplied to a fluidized bed (11) from a distribution plate (6) having a large number of small holes.

水冷壁(5)と流動床(11)内に設置された冷却管(
4)とには、流動床(11)内の反応熱を除去するため
、それぞれ冷却水(105)、 (104)が供給され
ている。
Cooling pipes (
4) are supplied with cooling water (105) and (104), respectively, in order to remove the reaction heat in the fluidized bed (11).

流動床(11)内の粗大粒子は排出管(9)から排出さ
れる。燃焼ガスはフリーボード(12)で燃焼ガスに随
伴された未燃粒子および脱硫剤粒子を重力分級により分
離した後、排出口(7)からダストを含んだ燃焼排ガス
(107)として排出される。
Coarse particles in the fluidized bed (11) are discharged from the discharge pipe (9). The combustion gas is separated by gravity classification from unburned particles and desulfurization agent particles entrained in the combustion gas in a freeboard (12), and then is discharged from an exhaust port (7) as a combustion exhaust gas (107) containing dust.

低No、燃焼を指向しない場合、空気比は1.1〜1.
2である。
Low No., when combustion is not oriented, the air ratio is 1.1 to 1.
It is 2.

低No、燃焼を指向する場合は、空気(101)の量を
減少させて流動床の空気比(供給空気量/完全燃焼に必
要な空気量の比)を1.0〜1.05に小さくすること
により、No、(No、No2等)の発生量を低く抑え
ている。流動床の空気比を小さくしたことにより、低N
Ox燃焼を指向しない場合に較べると、発生するガス中
のCOおよびガスに随伴された未燃粒子が増加する。そ
こで、ノズル(16)から空気(106)を供給して、
COおよび未燃粒子をフリーボード(12)において燃
焼させ、燃焼効率の低下を防いでいる。
When aiming for low No. combustion, reduce the amount of air (101) to reduce the air ratio of the fluidized bed (ratio of supplied air amount/air amount required for complete combustion) to 1.0 to 1.05. By doing so, the amount of No. (No. No. 2, etc.) generated is kept low. By reducing the air ratio of the fluidized bed, low N
Compared to the case where Ox combustion is not directed, CO in the generated gas and unburned particles accompanying the gas increase. Therefore, air (106) is supplied from the nozzle (16),
CO and unburned particles are combusted in the freeboard (12) to prevent a decrease in combustion efficiency.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来の流動床燃焼装置では、低No、燃焼を実現するた
めに空気比を小さくすると燃焼効率が低下し、SOXが
増大した。また空気比を小さくしても、Neoの発生量
までは低下させることができなかった。更に、フリーボ
ードへ空気を吹き込んで流動床で発生した未燃粒子を燃
焼する場合でも、フリーボードに未燃粒子が滞留する時
間が短いので、高い燃焼効率で未燃粒子を燃焼させるこ
とは難しかった。加えて、フリーボードの周壁が水冷壁
で構成されているので、フリーボードの温度を容易に高
温化できなかった。
In conventional fluidized bed combustion equipment, when the air ratio was reduced to achieve low No. combustion, combustion efficiency decreased and SOX increased. Furthermore, even if the air ratio was reduced, the amount of Neo generated could not be reduced. Furthermore, even when unburned particles generated in a fluidized bed are combusted by blowing air into the freeboard, the residence time of the unburned particles in the freeboard is short, so it is difficult to combust the unburned particles with high combustion efficiency. Ta. In addition, since the peripheral wall of the freeboard is constituted by a water-cooled wall, the temperature of the freeboard cannot be easily increased.

〔課題を解決するための手段〕[Means to solve the problem]

本発明は、前記従来の課題を解決するために、側壁が冷
却水のチューブで構成され、空気供給口、固体燃料また
は液体燃料の供給口、脱硫剤供給口および燃焼残渣排出
口を有する第1の反応室と、同第1の反応室の上端に連
通してその上方に配され、周壁が耐火断熱材で構成され
るとともに、上部にガスの出口を有する第2の反応室と
、上記第1の反応室の内部に設けられた冷却水管と、上
記第2の反応室の入口部に固着された旋回羽根と、上記
第2の反応室内に開口し、上記旋回羽根の旋回方向と同
方向に空気を噴出する空気供給管とを備えたことを特徴
とする流動床燃焼装置;ならびに上記流動床燃焼装置に
おいて、第1の反応室でカルシウムを含む脱硫剤を空気
により流動化させて流動床を形成するとともに、その流
動床中で燃料を800℃ないし870℃で燃焼させ、発
生したガスを次に第2の反応室内で旋回させてランキン
渦を発生させ、更に同第2の反応室内に吹込まれた空気
によりガス中の未燃粒子を880℃ないし1000℃で
燃焼させることを特徴とする流動床燃焼方法を提案する
ものである。
In order to solve the above-mentioned conventional problems, the present invention provides a first tube whose side wall is composed of a cooling water tube and has an air supply port, a solid fuel or liquid fuel supply port, a desulfurization agent supply port, and a combustion residue discharge port. a second reaction chamber communicating with and disposed above the upper end of the first reaction chamber, the peripheral wall of which is made of a fireproof and insulating material, and having a gas outlet at the top; A cooling water pipe provided inside the first reaction chamber, a swirling vane fixed to the inlet of the second reaction chamber, and a swirling vane opening into the second reaction chamber in the same direction as the swirling direction of the swirling vane. A fluidized bed combustion apparatus characterized by comprising: an air supply pipe that blows air into the fluidized bed; At the same time, the fuel is burned at 800°C to 870°C in the fluidized bed, and the generated gas is then swirled in the second reaction chamber to generate a Rankine vortex, and further in the second reaction chamber. This paper proposes a fluidized bed combustion method characterized by burning unburned particles in gas at 880°C to 1000°C using blown air.

〔作用〕[Effect]

本発明においては、従来のフリーボード部に相当する第
2の反応室を耐火断熱構造とすることにより、伝熱によ
り壁から系外へ放散される発生ガスの顕熱量を減少させ
ることができ、そこで発生するガスの温度を容易に高温
化することができる。
In the present invention, by making the second reaction chamber, which corresponds to the conventional freeboard part, have a fireproof and insulating structure, the amount of sensible heat of the generated gas dissipated from the wall to the outside of the system due to heat transfer can be reduced. The temperature of the gas generated therein can be easily increased.

また、第2の反応室の入口に設けられた旋回羽根と第2
の反応室に吹き込まれる空気とによって第2の反応室内
のガスを旋回させ、その旋回流を、旋回方向流速が半径
方向で一定となるような、ランキン渦とすることにより
、粒子は第2の反応室の空間内を旋回するが粒子が壁に
近づく速度は非常に遅いという状態が出現し、粒子濃度
の高い領域が旋回流中に生しる。このように第2の反応
室のガスをランキン渦の旋回流とすることにより、粒子
の滞留時間をガスよりも長くすることが可能となる。
In addition, a swirl vane provided at the entrance of the second reaction chamber and a second
The gas in the second reaction chamber is swirled by the air blown into the second reaction chamber, and the swirling flow is made into a Rankine vortex where the flow velocity in the swirling direction is constant in the radial direction. A situation arises in which the particles swirl within the space of the reaction chamber, but the speed at which they approach the walls is very slow, and regions with high particle concentration occur in the swirling flow. By making the gas in the second reaction chamber a swirling flow of a Rankine vortex in this way, it becomes possible to make the residence time of the particles longer than that of the gas.

更に本発明では第2の反応室内の温度を第1の反応室内
の流動床よりも高くするので、SZOの分解量が増大す
る。しかし、その上昇値によっては、カルシウムを含む
脱硫剤が温度上昇により再分解してSOzの放出が生し
る。流動床と同一温度にすると、常圧では加圧した場合
よりも脱流剤からのSO2放出量が多くなるので、加圧
状況やN、0. SO□未燃分の発生量に応して第2の
反応室の温度を選定し、N、Oの分解量が太きく802
の再放出が小さな温度を選定する。常圧では880℃+
 16a taの加圧時には1000”Cまで必要であ
る。
Furthermore, in the present invention, since the temperature in the second reaction chamber is made higher than that in the fluidized bed in the first reaction chamber, the amount of SZO decomposed increases. However, depending on the increased value, the desulfurizing agent containing calcium is re-decomposed due to the temperature increase, resulting in the release of SOz. If the temperature is the same as that of the fluidized bed, the amount of SO2 released from the deflow agent will be greater at normal pressure than when pressurized, so depending on the pressurization situation, N, 0. SO□The temperature of the second reaction chamber is selected according to the amount of unburned matter generated, and the amount of decomposition of N and O is large.802
Select a temperature at which re-emission of is small. 880℃+ at normal pressure
When pressurizing at 16a ta, up to 1000''C is required.

〔実施例〕〔Example〕

第1図は本発明の一実施例を示す流動床燃焼装置の縦断
面図、第2図は第1図の■−■断面図、第3図は第2図
の■−■断面図、第4図は第1図のIV−IV断面図で
ある。
Fig. 1 is a longitudinal cross-sectional view of a fluidized bed combustion apparatus showing an embodiment of the present invention, Fig. 2 is a cross-sectional view taken along ■-■ in Fig. 1, and Fig. 3 is a cross-sectional view taken along ■-■ in Fig. 2; FIG. 4 is a sectional view taken along line IV-IV in FIG. 1.

まず第1図において、Aは第1の反応室であって、その
側壁は冷却水のチューブで構成されて水冷壁(5)を形
成している。そして空気供給ノズル(1)、石炭供給ノ
ズル(2)、石灰石供給ノズル(3)および燃焼残渣の
排出管(9)が設けられている。
First, in FIG. 1, A is a first reaction chamber, the side wall of which is composed of cooling water tubes to form a water-cooled wall (5). An air supply nozzle (1), a coal supply nozzle (2), a limestone supply nozzle (3) and a combustion residue discharge pipe (9) are provided.

またBは第2の反応室であって、上記第1の反応室Aの
上端に連通してその上方に配され、周壁(15)が耐火
断熱材で構成されていて、上部に排出ガス管(17)が
設けられている。
Reference numeral B designates a second reaction chamber, which communicates with and is disposed above the upper end of the first reaction chamber A, and has a peripheral wall (15) made of a fireproof heat insulating material, and has an exhaust gas pipe in the upper part. (17) is provided.

流動床(11)は、水冷壁(5)に囲まれた上記第1の
反応室A内の分散板(6)上に形成されている。
A fluidized bed (11) is formed on a distribution plate (6) in the first reaction chamber A surrounded by a water-cooled wall (5).

石炭(102) 、石灰石(103)は石炭供給ノズル
(2)1石灰石供給ノズル(3)から流動床(11)へ
供給され、空気(101)は空気供給ノズル(1)から
風箱(10)を経て多数の小孔を有する分散板(6)を
通り流動床(11)へ供給される。流動床(11)内に
設置された冷却管(4)および水冷壁(5)には、流動
床(11)内の反応熱を除去するため、それぞれ冷却水
(104) 、 (105)が供給されている。流動床
(11)内の粗大粒子は排出管(9)から排出される。
Coal (102) and limestone (103) are supplied from the coal supply nozzle (2) 1 limestone supply nozzle (3) to the fluidized bed (11), and air (101) is supplied from the air supply nozzle (1) to the wind box (10). The liquid is then supplied to the fluidized bed (11) through a distribution plate (6) having a large number of small holes. Cooling water (104) and (105) are supplied to the cooling pipe (4) and water cooling wall (5) installed in the fluidized bed (11), respectively, in order to remove the reaction heat in the fluidized bed (11). has been done. Coarse particles in the fluidized bed (11) are discharged from the discharge pipe (9).

燃焼ガスは、第2の反応室Bの入口に設置された旋回羽
根(13)で、旋回を与えられて第2の反応室内Bへ導
入される。旋回羽根は、第2図および第3図に示したよ
うな構造をしている。旋回羽根は、第2の反応室Bの外
壁(15)とは連結しておらず、間隙dがあるので、第
2の反応室の外壁(15)側のガスは旋回羽根(13)
から旋回力を受けない。
The combustion gas is given a swirl by a swirl vane (13) installed at the entrance of the second reaction chamber B and is introduced into the second reaction chamber B. The swirl vane has a structure as shown in FIGS. 2 and 3. The swirl vane is not connected to the outer wall (15) of the second reaction chamber B, and there is a gap d, so the gas on the outer wall (15) side of the second reaction chamber flows through the swirl vane (13).
Does not receive turning force from

したがって、旋回方向流速は中心部が速く外周部が遅い
流速分布とすることができる。第2図に示されて旋回羽
根(13)と第2の反応室外壁(15)との間のこのよ
うな間隙dは、第2の反応室B内のランキン渦形成に大
きな影響を与える。また、旋回方向流速は、第3図に示
されている旋回羽根(13)と軸心のなす角度θも、第
2の反応室B内のランキン渦形成に大きな影響を与える
。したがって、dとθは第2の反応室B内の未燃粒子の
燃焼効率を左右する因子であるので、最適な値となるよ
う実験斡により決定する。
Therefore, the flow velocity in the swirling direction can be distributed such that the flow velocity is high at the center and slow at the outer circumference. Such a gap d between the swirl vane (13) and the second reaction chamber outer wall (15) shown in FIG. 2 has a great influence on the Rankine vortex formation in the second reaction chamber B. Furthermore, the flow velocity in the swirling direction and the angle θ between the swirling vane (13) and the axis shown in FIG. Therefore, since d and θ are factors that influence the combustion efficiency of unburned particles in the second reaction chamber B, they are determined through experiments so as to have optimal values.

第2の反応室Bの細心部には、空気供給管(116)が
配され、フリーボード空気の供給ノズル(14)が開口
している。この空気供給ノズル(14)は、第4図に示
されるように、半径方向に対して角φをなすような方向
に吹出口が設置されている。このような角度φを有する
ので、フリーボード空気の吹き出しにより、第2の反応
室B内の燃焼ガス(108)の旋回が助長される。した
がって角度φは、最適な値となるよう実験的に決定する
An air supply pipe (116) is arranged in the narrow part of the second reaction chamber B, and a freeboard air supply nozzle (14) is opened. As shown in FIG. 4, this air supply nozzle (14) has an outlet installed in a direction forming an angle φ with respect to the radial direction. With such an angle φ, swirling of the combustion gas (108) in the second reaction chamber B is facilitated by blowing out freeboard air. Therefore, the angle φ is experimentally determined to be the optimum value.

第5図(al、 (blは第2の反応室B内の旋回方向
流速分布を示す図である。第5図ta)は、第5図(C
1の(81部(第1図のTV−IV鎖線部)、すなわち
空気の供給ノズル(14)部付近における旋回方向流速
の分布を示し、第5囲い)は第5図(C1の中)部、す
なわち第2の反応室Bの上部における旋回方向流速の分
布を示す。まず(61部では、旋回方向流速が半径方向
にほぼ一様であり、ランキン渦が生している。
Figures 5 (al and bl are diagrams showing the flow velocity distribution in the swirling direction in the second reaction chamber B. Figure 5 ta) are diagrams showing the flow velocity distribution in the swirling direction in the second reaction chamber B.
Part 1 (81 part (TV-IV chain line part in Figure 1), that is, the distribution of the flow velocity in the swirling direction near the air supply nozzle (14) part, box 5) is the part in Figure 5 (center of C1). , that is, the distribution of the flow velocity in the swirling direction in the upper part of the second reaction chamber B. First, in the 61st part, the flow velocity in the swirling direction is almost uniform in the radial direction, and a Rankine vortex is generated.

この部分では、大部分の粒子の軌跡は第1図中に一点鎖
線(109)で示すように旋回している。そして、点線
(110)のように壁まで移動して壁近傍のガスの下降
流に乗り、再度流動床へ落下する粒子の割合は少ない。
In this part, most of the particle trajectories rotate as shown by the dashed line (109) in FIG. Then, as shown by the dotted line (110), a small percentage of particles move to the wall, ride the downward flow of gas near the wall, and fall back into the fluidized bed.

また山)部(第2図の反応室Bの上部)では、第5囲い
)に示されるように、旋回流速は全体に低下するが、ラ
ンキン渦はまだ保持されている。第2の反応室B内にお
ける燃焼ガス主流(Lo8)の平均滞留時間は約3秒で
あるが、粒子はランキン渦に乗って同一高さの位置を旋
回している時間が長くなり、粒子の平均滞留時間は10
秒以上となる0粒子の平均滞留時間が延びることにより
、第2の反応室B内のフリボードにおける粒子の燃焼効
率が上昇する。試験によれば、16ataの加圧状態で
は粒子の燃焼速度が上昇したので、流動床温度850℃
、フリーボード温度900℃で燃焼効率99.5%、 
Sow 40111pm、 NOx 40ppm、Nz
O5pp髄という低公害で、かつ高い燃焼効率を達成す
ることができた。
In addition, as shown in the fifth box (in the upper part of the reaction chamber B in FIG. 2), the swirling flow velocity decreases overall, but the Rankine vortex is still maintained. The average residence time of the main combustion gas (Lo8) in the second reaction chamber B is about 3 seconds, but the particles spend a longer time riding the Rankine vortex and swirling at the same height. Average residence time is 10
By extending the average residence time of zero particles to more than a second, the combustion efficiency of the particles in the friboard in the second reaction chamber B increases. According to the test, the combustion rate of particles increased under a pressurized state of 16ata, so the fluidized bed temperature was 850℃.
, combustion efficiency of 99.5% at freeboard temperature of 900℃,
Sow 40111pm, NOx 40ppm, Nz
We were able to achieve low pollution and high combustion efficiency using O5pp.

なお、燃焼ガス(108)は最後に排出ガス管(17〉
より糸外に排出される。
In addition, the combustion gas (108) is finally passed through the exhaust gas pipe (17).
It is discharged outside the twine.

第2の反応室Bにおいて、旋回ガス流の旋回方向流速が
半径方向で均一となるような、ランキン渦を発生させる
ためには、3つの条件を考慮して、第2の反応室への空
気の吸込方法が選定される。
In order to generate a Rankine vortex in which the flow velocity in the swirling direction of the swirling gas flow is uniform in the radial direction in the second reaction chamber B, three conditions must be considered to The suction method is selected.

その3つの条件とは、■空気供給ノズル(14)の軸方
向位置、■空気供給ノズル(14)の吹き込み方向が半
径方向に対してなす角度φ、■フリーボードへ吹き込む
空気の吹き込み速度である。
The three conditions are: (1) the axial position of the air supply nozzle (14), (2) the angle φ that the blowing direction of the air supply nozzle (14) makes with respect to the radial direction, and (2) the blowing speed of the air into the freeboard. .

第6図は本発明の第2実施例を示す流動床燃焼装置の縦
断面図である。本実施例では、燃焼ガスが、空気供給管
(216)と同心でその外方を囲んで設けられた排出ガ
ス管(27)から、系外に取り出される。その他の構成
および作用・効果は前記第1の実施例と同様なので、詳
しい説明を省く。
FIG. 6 is a longitudinal sectional view of a fluidized bed combustion apparatus showing a second embodiment of the present invention. In this embodiment, combustion gas is taken out of the system through an exhaust gas pipe (27) provided concentrically with and surrounding the air supply pipe (216). The other configurations, functions, and effects are the same as those of the first embodiment, so detailed explanations will be omitted.

〔発明の効果〕〔Effect of the invention〕

本発明においては、第2の反応室Bの入口に旋回羽根を
設けるとともに、その旋回方向と同方向に空気を吹込む
ことにより、第2の反応室B内に形成されたフリーボー
ドにランキン渦型の旋回流を発生させ、フリーボードで
の未燃粒子を従来よりも高効率で燃焼することが可能と
なった。したがって、流動床の空気比を1.0〜1.0
5としても装置全体の燃焼効率は低下せず、かつフリー
ボードでの燃焼効率が上昇するため容易にフリーボード
のガス温度が上昇し、N、Oを分解することが可能とな
った。
In the present invention, by providing a swirling vane at the entrance of the second reaction chamber B and blowing air in the same direction as the swirling direction, a Rankine vortex is created in the freeboard formed in the second reaction chamber B. By generating a swirling flow, it has become possible to burn unburned particles in the freeboard with higher efficiency than before. Therefore, the air ratio of the fluidized bed is 1.0 to 1.0.
5, the combustion efficiency of the entire device did not decrease, and the combustion efficiency in the freeboard increased, so the gas temperature in the freeboard rose easily, making it possible to decompose N and O.

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

第1図は、本発明の一実施例を示す流動床燃焼装置の縦
断面図、第2図は第1図の■−■断面図、第3図は第2
図の■−■断面図、第4図は第1図のIV−fV断面図
である。第5図は第2図の反応室内における旋回方向流
速の半径方向分布を示す図である。第6図は本発明の第
2の実施例を示す流動床燃焼装置の縦断面図である。第
7図は従来の流動床燃焼装置の一例を示す縦断面図であ
る。 A・・・第1の反応室、   B・・・第2の反応室(
1)・・・空気供給ノズル、(2)・・・石炭供給ノズ
ル。 (3)・・・石灰石供給ノズル、(4)・・・冷却管(
5)・・・水冷壁、(6)・・・分散板。 (7)、 (17)、(27)・・・排出ガス管(8)
・・・風箱壁、(9)・・・排出管00)・・・風箱、
00・・・流動床。 0′!J・・・フリーボード、03)・・・旋回羽根。 041・・・空気供給ノズル、051・・・第2の反応
室の周壁。 (16)、(116)・・・空気供給管、 (101)
・・・空気。 (102)・・・石炭、     (103)・・・石
灰石。 (104) 、 (105)・・・冷却水、 (106
)・・・フリーボード空気(107)・・・燃焼排ガス
、  (108)・・・燃焼ガス。 第1囮
FIG. 1 is a longitudinal cross-sectional view of a fluidized bed combustion apparatus showing one embodiment of the present invention, FIG. 2 is a cross-sectional view taken along the line ■-■ in FIG.
FIG. 4 is a sectional view taken along IV-fV in FIG. 1. FIG. 5 is a diagram showing the radial distribution of the flow velocity in the swirling direction in the reaction chamber of FIG. 2. FIG. 6 is a longitudinal sectional view of a fluidized bed combustion apparatus showing a second embodiment of the present invention. FIG. 7 is a longitudinal sectional view showing an example of a conventional fluidized bed combustion apparatus. A...First reaction chamber, B...Second reaction chamber (
1)...Air supply nozzle, (2)...Coal supply nozzle. (3)...Limestone supply nozzle, (4)...Cooling pipe (
5)...Water cooling wall, (6)...Dispersion plate. (7), (17), (27)...Exhaust gas pipe (8)
...Wind box wall, (9)...Exhaust pipe 00)...Wind box,
00...Fluidized bed. 0'! J...Free board, 03)...Swirl blade. 041... Air supply nozzle, 051... Peripheral wall of the second reaction chamber. (16), (116)...Air supply pipe, (101)
···air. (102)...coal, (103)...limestone. (104), (105)...Cooling water, (106
)...Freeboard air (107)...Combustion exhaust gas, (108)...Combustion gas. 1st decoy

Claims (1)

【特許請求の範囲】 1)側壁が冷却水のチューブで構成され、空気供給口、
固体燃料または液体燃料の供給口、脱硫剤供給口および
燃焼残渣排出口を有する第1の反応室と、同第1の反応
室の上端に連通してその上方に配され、周壁が耐火断熱
材で構成されるとともに、上部にガスの出口を有する第
2の反応室と、上記第1の反応室の内部に設けられた冷
却水管と、上記第2の反応室の入口部に固着された旋回
羽根と、上記第2の反応室内に開口し、上記旋回羽根の
旋回方向と同方向に空気を噴出する空気供給管とを備え
たことを特徴とする流動床燃焼装置。 2)請求項1)記載の流動床燃焼装置において、第1の
反応室でカルシウムを含む脱硫剤を空気により流動化さ
せて流動床を形成するとともに、その流動床中で燃料を
800℃ないし870℃で燃焼させ、発生したガスを次
に第2の反応室内で旋回させてランキン渦を発生させ、
更に同第2の反応室内に吹込まれた空気によりガス中の
未燃粒子を880℃ないし1000℃で燃焼させること
を特徴とする流動床燃焼方法。
[Claims] 1) The side wall is composed of a cooling water tube, and has an air supply port,
A first reaction chamber having a solid fuel or liquid fuel supply port, a desulfurization agent supply port, and a combustion residue discharge port, the first reaction chamber communicating with and disposed above the upper end of the first reaction chamber, and having a peripheral wall made of fireproof heat insulating material. a second reaction chamber having a gas outlet at the top, a cooling water pipe provided inside the first reaction chamber, and a swirl fixed to the inlet of the second reaction chamber. A fluidized bed combustion apparatus comprising: a blade; and an air supply pipe that opens into the second reaction chamber and blows out air in the same direction as the swirling direction of the swirling blade. 2) In the fluidized bed combustion apparatus according to claim 1, the calcium-containing desulfurizing agent is fluidized with air in the first reaction chamber to form a fluidized bed, and the fuel is heated in the fluidized bed at 800°C to 870°C. ℃ combustion, the generated gas is then swirled in a second reaction chamber to generate a Rankine vortex,
Furthermore, a fluidized bed combustion method characterized in that unburned particles in the gas are combusted at 880°C to 1000°C by air blown into the second reaction chamber.
JP5664990A 1990-03-09 1990-03-09 Fluid bed combustion apparatus and method Expired - Fee Related JP2622299B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5664990A JP2622299B2 (en) 1990-03-09 1990-03-09 Fluid bed combustion apparatus and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5664990A JP2622299B2 (en) 1990-03-09 1990-03-09 Fluid bed combustion apparatus and method

Publications (2)

Publication Number Publication Date
JPH03260504A true JPH03260504A (en) 1991-11-20
JP2622299B2 JP2622299B2 (en) 1997-06-18

Family

ID=13033210

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5664990A Expired - Fee Related JP2622299B2 (en) 1990-03-09 1990-03-09 Fluid bed combustion apparatus and method

Country Status (1)

Country Link
JP (1) JP2622299B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0596741U (en) * 1992-05-19 1993-12-27 株式会社ガスター Combustion device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0596741U (en) * 1992-05-19 1993-12-27 株式会社ガスター Combustion device

Also Published As

Publication number Publication date
JP2622299B2 (en) 1997-06-18

Similar Documents

Publication Publication Date Title
RU2123637C1 (en) Boiler with pressure inner circulating fluidized layer, electric generating system and furnace with fluidized bed
US5156099A (en) Composite recycling type fluidized bed boiler
US4655148A (en) Method of introducing dry sulfur oxide absorbent material into a furnace
PT88048B (en) FLUIDIFIED BREASTFEEDING PROCESS AND APPARATUS FOR CARRYING OUT THE PROCESS
JPH0391603A (en) Method and apparatus for fluid bed combustion
CA1332685C (en) Composite circulating fluidized bed boiler
US5341753A (en) Circulating fluidized bed power plant with improved mixing of sorbents with combustion gases
JP2731794B2 (en) High performance overfire air system for NOx control
JPS63254303A (en) coal combustion equipment
CN1122812C (en) Method and device for reducing pollutant in smoke of fluidized-bed heating system
JP3504324B2 (en) Pressurized internal circulation type fluidized bed boiler
JPH03260504A (en) Fluidized bed type combustion device and combustion method
JP2776575B2 (en) Pulverized coal combustion equipment
JP2641826B2 (en) Combustion method of liquid fuel in circulating fluidized bed
JP3625818B2 (en) Pressurized fluidized bed furnace
JP4208817B2 (en) Power generation method by gasification of fuel
JPH02122103A (en) Burner of powder particle fuel
JP2003307302A (en) Operation method of fluidized bed furnace
JPS6160322B2 (en)
JPH10205733A (en) Secondary air supply method in fluidized bed combustion furnace
JPS63143408A (en) Coal burner of high fuel ratio
WO2018142772A1 (en) Combustion burner and boiler provided with same
JPH0399106A (en) Fuel supply for fluidized bed burner
JPH07248194A (en) Fluid material circulation method and device
JPH06109210A (en) Fluidized bed combustion apparatus

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees