JP3260580B2 - Thermal storage for thermal storage burners - Google Patents
Thermal storage for thermal storage burnersInfo
- Publication number
- JP3260580B2 JP3260580B2 JP04946295A JP4946295A JP3260580B2 JP 3260580 B2 JP3260580 B2 JP 3260580B2 JP 04946295 A JP04946295 A JP 04946295A JP 4946295 A JP4946295 A JP 4946295A JP 3260580 B2 JP3260580 B2 JP 3260580B2
- Authority
- JP
- Japan
- Prior art keywords
- heat storage
- honeycomb
- combustion
- honeycomb structure
- regenerator
- 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
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E20/00—Combustion technologies with mitigation potential
- Y02E20/34—Indirect CO2mitigation, i.e. by acting on non CO2directly related matters of the process, e.g. pre-heating or heat recovery
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/14—Thermal energy storage
Landscapes
- Air Supply (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、蓄熱式バーナ用蓄熱体
に関し、特に、蓄熱式バーナ等の燃焼装置に好適であ
り、ハニカム構造体を積層した集合体からなる蓄熱式バ
ーナ用蓄熱体に係るものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a regenerator for a regenerative burner, and more particularly, to a regenerator for a regenerative burner which is suitable for a combustion device such as a regenerative burner and which is composed of an aggregate of honeycomb structures. It is related.
【0002】[0002]
【従来の技術】周知のように、蓄熱式バーナにはバーナ
に付随して排熱回収や蓄熱等の目的で蓄熱体が取り付け
られている。公知資料としては、特開平4−25119
0号公報に開示されたハニカム状蓄熱体がある。図3
は、従来の蓄熱式バーナを用いた加熱炉の一例を示して
いる。同図において、3は加熱炉、4a,4bはバー
ナ、5a,5bは蓄熱体、6a,6bは燃料遮断弁、7
は燃焼空気の供給と燃焼排ガスの吸引を切り換えるため
の四方弁、8は燃焼排ガス排気口である。9は加熱炉3
内の被加熱物である。2. Description of the Related Art As is well known, a regenerative burner is provided with a regenerator along with the burner for the purpose of heat recovery or heat storage. As well-known materials, Japanese Patent Laid-Open No.
There is a honeycomb-shaped regenerator disclosed in Japanese Patent Application Publication No. 0-205. FIG.
1 shows an example of a heating furnace using a conventional regenerative burner. In the figure, 3 is a heating furnace, 4a and 4b are burners, 5a and 5b are heat storage bodies, 6a and 6b are fuel cutoff valves, 7
Is a four-way valve for switching between supply of combustion air and suction of combustion exhaust gas, and 8 is a combustion exhaust gas outlet. 9 is heating furnace 3
The object to be heated.
【0003】加熱炉3はバーナ4aが燃焼状態にあるも
のとする。例えば、蓄熱体5aに供給される燃焼空気の
温度は30℃であり、それが蓄熱体5aで加熱されて1
250℃の予熱空気となってバーナ4aに供給される。
予熱空気は燃焼ガスとともに燃焼して加熱炉3内に供給
される。また、燃焼排ガスの一部はバーナ4bを経て1
350℃の温度で蓄熱体5bに吸引されて蓄熱体5bを
加熱して、200℃の燃焼排ガスとして排気される。更
に、残余の燃焼ガスは排気口8から炉外に排気される。
バーナ4aとバーナ4bとの切り替えは、燃料遮断弁6
a,6bと燃焼空気及び燃焼排ガス切り替え四方弁7の
切り替えと連動して行われる。In the heating furnace 3, it is assumed that the burner 4a is in a combustion state. For example, the temperature of the combustion air supplied to the heat storage element 5a is 30 ° C.
The preheated air at 250 ° C. is supplied to the burner 4a.
The preheated air burns together with the combustion gas and is supplied into the heating furnace 3. A part of the combustion exhaust gas passes through the burner 4b,
At a temperature of 350 ° C., the heat is absorbed by the heat storage element 5b to heat the heat storage element 5b and is exhausted as combustion exhaust gas at 200 ° C. Further, the remaining combustion gas is exhausted from the exhaust port 8 to the outside of the furnace.
Switching between the burner 4a and the burner 4b is performed by the fuel cutoff valve 6
a, 6b and the switching of the combustion air and combustion exhaust gas switching four-way valve 7 are performed.
【0004】この加熱炉3には、短時間に蓄熱と放熱を
繰り返してなされる排熱回収システムが組み込まれ、蓄
熱体5a,5bを設けることにより、熱回収効率を高め
たものである。The heating furnace 3 incorporates an exhaust heat recovery system in which heat storage and heat radiation are repeatedly performed in a short period of time, and heat storage bodies 5a and 5b are provided to improve heat recovery efficiency.
【0005】蓄熱体5a,5bは、単位容積当たりの熱
交換面積が大きく、且つ、ガス通過面積が大きく、更
に、流体通過時の圧力損失の小さな構造体が好ましい。
例えば、ハニカム状構造体が適している。このような理
由から蓄熱式バーナの蓄熱体には、ハニカム状蓄熱体が
用いられいる。また、ハニカム状蓄熱体の材質は、例え
ば、1300℃以上の高温の燃焼ガスが通過するため
に、高温で溶融しないセラミックスが用いられている。
このようなセラミックスハニカムは押し出し成型した材
料を焼結して製造する。従って、セラミックスハニカム
による蓄熱体はハニカムの断面形状が流路方向で一定で
ある。The heat storage bodies 5a and 5b preferably have a structure in which the heat exchange area per unit volume is large, the gas passage area is large, and the pressure loss during passage of the fluid is small.
For example, a honeycomb structure is suitable. For this reason, a honeycomb-shaped heat storage element is used as the heat storage element of the regenerative burner. Further, as a material of the honeycomb-shaped regenerator, for example, ceramics that do not melt at a high temperature is used because a high-temperature combustion gas of 1300 ° C. or more passes therethrough.
Such a ceramic honeycomb is manufactured by sintering an extruded material. Therefore, in the heat storage body made of ceramic honeycomb, the cross-sectional shape of the honeycomb is constant in the flow path direction.
【0006】[0006]
【発明が解決しようとする課題】従来、ハニカム状蓄熱
体にセラミックスを使用した場合に割れが発生する問題
があった。その原因は次のようなものであると推定され
ていた。すなわち、ハニカム状蓄熱体の使用状態では、
バーナ側で温度が高く、反バーナ側で温度が低くなり、
ハニカム状蓄熱体の温度勾配が急峻となる。ハニカム状
蓄熱体はこの温度勾配に応じて熱膨張して変形しようと
するが、ハニカム状蓄熱体は力学的に強固な構造体であ
るために、自由な変形が妨げられ、その結果とし、ハニ
カム状蓄熱体には内部応力が発生して割れに至るものと
推定されていた。Heretofore, there has been a problem that cracks occur when ceramics are used for the honeycomb-shaped regenerator. The cause was presumed to be as follows. That is, in the use state of the honeycomb-shaped heat storage body,
The temperature is high on the burner side, the temperature is low on the anti-burner side,
The temperature gradient of the honeycomb-shaped regenerator becomes steep. The honeycomb-shaped regenerator tends to thermally expand and deform in accordance with this temperature gradient.However, since the honeycomb-shaped regenerator is a mechanically strong structure, free deformation is hindered. It was presumed that internal heat was generated in the thermal storage medium and cracked.
【0007】上記のような現象によって、加熱炉のハニ
カム状蓄熱体に割れが発生するものと仮定すると、流路
の一部が拡大して燃焼排ガスの流量が大きくなり、蓄熱
体出側の燃焼排ガス温度が上昇して、排ガス熱損失が増
加し熱効率が悪化する問題があった。このような欠陥の
管理は、蓄熱式バーナ用蓄熱体の燃焼ガス温度の変化等
を観察しながら、蓄熱体の割れを判定して短期間に蓄熱
体を交換する方法でなされていた。その結果、蓄熱体交
換による設備停止期間の生産機会損失、蓄熱体交換費用
が増大する問題があった。更に、割れの原因と推定され
ていた蓄熱体内部応力の値を小さくする方法としては、
ハニカム状蓄熱体を小片に切断分割した上で元の形状に
組み立て使用する方法がある。しかし、この方法では、
蓄熱体の設置、取り替えに手間がかかるばかりでなく、
蓄熱体設置位置が使用中の熱膨張等によって隣合う蓄熱
体間の流路にずれが生じて流路が部分的または全体的に
狭くなるおそれがあり、蓄熱体の流動抵抗が増加する問
題があった。[0007] Assuming that the above-mentioned phenomenon causes cracks in the honeycomb regenerator of the heating furnace, a part of the flow path expands, the flow rate of the combustion exhaust gas increases, and the combustion on the discharge side of the regenerator starts. There has been a problem that the exhaust gas temperature rises, the heat loss of the exhaust gas increases, and the thermal efficiency deteriorates. The management of such a defect has been performed by observing a change in the temperature of the combustion gas of the regenerator for the regenerative burner, determining cracks in the regenerator, and exchanging the regenerator in a short period of time. As a result, there has been a problem that the production opportunity loss during the facility suspension period due to the heat storage material exchange and the heat storage material replacement cost increase. Furthermore, as a method of reducing the value of the heat storage body internal stress that was estimated to be the cause of cracks,
There is a method in which a honeycomb-shaped heat storage body is cut and divided into small pieces and then assembled into an original shape for use. But with this method,
Not only does it take time to install and replace the heat storage body,
There is a possibility that the flow path between the adjacent heat storage bodies may be shifted due to thermal expansion or the like during use of the heat storage body, and the flow path may be partially or entirely narrow, and the flow resistance of the heat storage body increases. there were.
【0008】上記のようにハニカム状蓄熱体の割れの原
因である蓄熱体内部応力の値を小さくし、且つ、分散さ
せて割れを解消する方法とし、ハニカム状蓄熱体を小片
に切断して、元の形状に組み立て直して使用することは
考えられていた。しかしながら、ハニカム状蓄熱体の内
部温度分布を積極的に変化させて蓄熱体内部応力の発生
を抑制する考え方は存在しなかった。[0008] As described above, a method of reducing the internal stress value of the heat storage body, which is the cause of the cracks in the honeycomb heat storage body, and dispersing the cracks to eliminate the cracks, cutting the honeycomb heat storage body into small pieces, It was conceived to reassemble and use it in its original shape. However, there has been no idea that the internal temperature distribution of the honeycomb-shaped heat storage body is positively changed to suppress the generation of the internal stress of the heat storage body.
【0009】本発明は、上述のような課題に鑑みなされ
たものであり、蓄熱体の内部温度分布による割れが発生
しないような温度分布となる蓄熱式バーナ用蓄熱体を提
供することを目的とするものである。SUMMARY OF THE INVENTION The present invention has been made in consideration of the above-described problems, and has as its object to provide a heat storage element for a heat storage type burner having a temperature distribution that does not cause cracking due to an internal temperature distribution of the heat storage element. Is what you do.
【0010】[0010]
【課題を解決するための手段】上述の課題を解決する為
に、第1発明の蓄熱式バーナ用蓄熱体は、燃焼用空気と
燃料用排ガスが流れ方向を変えて交互に通過する多数の
細管が設けられた蓄熱体が少なくとも2個以上のハニカ
ム構造体からなり、且つ、前記燃焼用空気が送り込まれ
る方向に前記ハニカム構造体が積層され、前記蓄熱体を
積層形成するハニカム構造体の細管の断面積が燃焼側ハ
ニカム構造体の細管の断面積に対して反燃焼側ハニカム
構造体の細管の断面積を狭くしたことを特徴とする蓄熱
式バーナ用蓄熱体である。また、第2発明は、前記第1
発明において、前記ハニカム構造体間にスペーサを配置
して間隙を設けたことを特徴とする蓄熱式バーナ用蓄熱
体である。また、第3発明は、上記第1と第2発明にお
いて、前記ハニカム構造体の積層構造からなる蓄熱体の
燃焼側ハニカム構造体の材質がセラミックスであり、反
燃焼側ハニカム構造体の材質が金属からなることを特徴
とする蓄熱式バーナ用蓄熱体である。In order to solve the above-mentioned problems, a regenerator for a regenerative burner according to a first aspect of the present invention comprises a multiplicity of thin tubes through which combustion air and fuel exhaust gas alternately flow while changing their flow directions. Is formed of at least two or more honeycomb structures, and the honeycomb structures are stacked in a direction in which the combustion air is fed, and the thin tubes of the honeycomb structure forming the heat storage bodies in a stacked manner are formed. A heat storage element for a regenerative burner, characterized in that the cross-sectional area of the thin tube of the anti-combustion side honeycomb structure is smaller than that of the thin tube of the combustion side honeycomb structure. Further, the second invention is the first invention.
In the invention, there is provided a heat storage element for a heat storage type burner, wherein a spacer is provided between the honeycomb structures to provide a gap. In a third aspect of the present invention, in the first and second aspects, the material of the combustion-side honeycomb structure of the heat storage body having a stacked structure of the honeycomb structure is ceramics, and the material of the anti-combustion-side honeycomb structure is metal. A heat storage element for a heat storage type burner, comprising:
【0011】[0011]
【作用】蓄熱式バーナに用いられるハニカム蓄熱体は細
管の集合体とみなされる。ハニカム状に形成された細管
とそこを通過するガスとの熱伝達の関係は、一般の細管
中のヌッセルト数Nu〔定義を式(1)に示す〕により
定まり、発明者らの経験測からその値は実測値と一致す
ることが判明している。以下に、ヌッセルト数Nuの関
係式を示す。 Nu= D・h/k ……(1) 但し、 D:細管の水力直径(m) h:ハニカムとガスとの間の熱伝達係数(W/m2 ・
K) k:ガスの熱伝導率(W/m・K)The honeycomb regenerator used in the regenerative burner is regarded as an aggregate of thin tubes. The relationship between the heat transfer between the thin tube formed in a honeycomb shape and the gas passing therethrough is determined by the Nusselt number Nu in a general thin tube (the definition is shown by the formula (1)). The values have been found to be consistent with the measured values. The relational expression of the Nusselt number Nu is shown below. Nu = D · h / k (1) where D: hydraulic diameter of the thin tube (m) h: heat transfer coefficient between the honeycomb and the gas (W / m 2.
K) k: Thermal conductivity of gas (W / m · K)
【0012】図4は、蓄熱式バーナ運転中の蓄熱体内部
の温度分布測定値の時間平均値の例を示したものであ
り、縦軸が温度を示し、横軸がハニカム蓄熱体の位置
A,B,C,Dの温度を示している。この実験で使用し
たハニカム状蓄熱体は流路断面が正方形(縦2.5m
m、横2.5mm)の細管を多数設けた集合体からな
り、ガスの流れる方向(流路方向)に三個のハニカム状
蓄熱体を積層したものである。なお、図中の実線は
(1)式による温度計算値であり、ドット状の記号は図
中に示す蓄熱体の位置A,B,C,Dにおける温度測定
値である。位置Aは高温側であり、Dは低温側である。FIG. 4 shows an example of the time average value of the measured temperature distribution inside the heat storage element during the operation of the heat storage type burner. The vertical axis indicates the temperature, and the horizontal axis indicates the position A of the honeycomb heat storage element. , B, C, and D are shown. The honeycomb-shaped regenerator used in this experiment had a square cross section (2.5 m long).
m, 2.5 mm in width), and is formed by stacking three honeycomb-shaped regenerators in the gas flow direction (flow path direction). Note that the solid line in the figure is the calculated value of the temperature according to the equation (1), and the dot-shaped symbols are the measured temperature values at the positions A, B, C, and D of the heat storage body shown in the figure. Position A is on the high temperature side and D is on the low temperature side.
【0013】細管の流路断面積が同一のハニカム状蓄熱
体を三個用いた蓄熱体では、図4から明らかなように、
その内部の温度勾配が蓄熱体高温側の位置Aで温度勾配
が大きくなることがわかる。この実験では、高温側で蓄
熱体が割れたが、低温側では割れていないことが判明し
た。そこで、割れの原因を調査するために、材質、形状
の異なる蓄熱体について様々な温度分布を与えて割れ発
生の有無について調査した。その結果、蓄熱体の割れ
は、蓄熱体に発生する熱歪と蓄熱体の強度との比、以後
これを割れ指数Sと呼び、その定義を(2)式に示すと
ともに、蓄熱体の割れの発生がこの割れ指数Sによって
判定できることが明らかになった。すなわち、割れ指数
Sが所定の値より小さければ割れないことが判明したも
のである。In a heat storage element using three honeycomb-shaped heat storage elements having the same flow channel cross-sectional area of a thin tube, as is apparent from FIG.
It can be seen that the temperature gradient inside becomes large at the position A on the high-temperature side of the regenerator. In this experiment, it was found that the heat storage body cracked on the high temperature side, but did not crack on the low temperature side. Therefore, in order to investigate the cause of the cracks, various temperature distributions were given to the heat storage bodies having different materials and shapes, and the presence or absence of cracks was investigated. As a result, the crack of the heat storage body is determined by the ratio of the thermal strain generated in the heat storage body to the strength of the heat storage body, hereinafter referred to as a cracking index S. It became clear that the occurrence can be determined by the crack index S. That is, it has been found that if the crack index S is smaller than a predetermined value, no crack occurs.
【0014】 S=(G・b・W・E・L)/T ………(2) G:蓄熱体入り出ガス温度勾配(K/m) b:蓄熱体線膨張係数(1/K) W:蓄熱体代表寸法(m)=ガス通過方向投影面積/蓄
熱体ガス通過方向周囲長さ E:蓄熱体ヤング率(N/m2 ) L:蓄熱体のガス流れ方向長さ(m) T:蓄熱体引っ張り強度(N/m2 ) すなわち、蓄熱体材料を選択すると、蓄熱体の引っ張り
強度T、ヤング率E及び線膨張係数bが決まる。蓄熱体
が割れず、且つ、取扱いを容易にすべく形状(W・L)
を大きくするには蓄熱体入り出ガス温度勾配Gを小さく
することが考えられる。S = (G · b · W · E · L) / T (2) G: Temperature gradient of gas entering and exiting the heat storage unit (K / m) b: Coefficient of linear expansion of the heat storage unit (1 / K) W: typical dimension of heat storage unit (m) = projected area in gas passage direction / perimeter of heat storage unit gas passage direction E: Young's modulus of heat storage unit (N / m 2 ) L: length of heat storage unit in gas flow direction (m) T : Thermal storage material tensile strength (N / m 2 ) That is, when a thermal storage material is selected, the tensile strength T, Young's modulus E, and linear expansion coefficient b of the thermal storage material are determined. Shape (W · L) to prevent heat storage body from cracking and to facilitate handling
In order to increase the temperature, it is conceivable to reduce the temperature gradient G of the gas entering and exiting the regenerator.
【0015】一方、(1)式から明らかなように、細管
の水力直径Dを大きくすれば熱伝達係数が小さくなり、
ガスとセラミックスハニカムとの熱伝達が抑制されるこ
とを示している。従って、このような場合には、蓄熱体
通過中のガスの温度変化は小さくなり、同時にセラミッ
クハニカムの細管長手方向の温度勾配も小さくなって割
れ難くなる。ただし、細管全長に渡って細管を太くする
と、蓄熱体を長くしないと十分な熱交換ができず、蓄熱
体が大きくなる問題が生ずる。従って、流れ方向(流路
方向)に複数に分割されたハニカム構造体を積層した集
合体からなる蓄熱体を形成し、且つ、各ハニカム構造体
の割れ係数Sが所定の値より小さくなるような温度勾配
となる細管の断面積を、それぞれのハニカム構造体につ
いて計算して決めればよいことになる。これらを考え合
わせると、ハニカム状蓄熱体では、各ハニカム構造体の
細管の断面積を、高温側(燃焼側)を大きくし低温側
(反燃焼側)に向かうに従って順次狭くするように選定
すればよいことになる。On the other hand, as is apparent from the equation (1), when the hydraulic diameter D of the thin tube is increased, the heat transfer coefficient decreases,
This indicates that heat transfer between the gas and the ceramic honeycomb is suppressed. Therefore, in such a case, the temperature change of the gas during the passage of the heat accumulator becomes small, and at the same time, the temperature gradient in the longitudinal direction of the narrow tube of the ceramic honeycomb becomes small, so that it becomes difficult to crack. However, if the thin tube is made thicker over the entire length of the thin tube, sufficient heat exchange cannot be performed unless the heat storage material is made longer, causing a problem that the heat storage material becomes larger. Therefore, a heat storage body composed of an aggregate in which a plurality of honeycomb structures divided in the flow direction (flow channel direction) are stacked is formed, and the crack coefficient S of each honeycomb structure is smaller than a predetermined value. The cross-sectional area of the thin tube that becomes the temperature gradient may be determined by calculating for each honeycomb structure. Considering these, in the case of the honeycomb-shaped regenerator, the cross-sectional area of the narrow tube of each honeycomb structure should be selected so as to increase on the high temperature side (combustion side) and gradually decrease on the low temperature side (anti-combustion side). It will be good.
【0016】このような観点からなされ、課題を解決す
るための手段によって、上記目的を達成したものであ
る。請求項1によれば、燃焼用空気が通過する多数の細
管が設けられた蓄熱体が少なくとも2個以上のハニカム
構造体からなり、且つ、前記燃焼用空気が送り込まれる
方向に前記ハニカム構造体が積層され、前記蓄熱体を積
層形成するハニカム構造体の細管の断面積が燃焼側ハニ
カム構造体の細管の断面積に対して反燃焼側ハニカム構
造体の細管の断面積を狭くすることにより、蓄熱効果を
高めるとともに蓄熱式バーナ用蓄熱体の温度勾配を小さ
くして割れを防止するものである。The above objects have been achieved by means for solving the problems which have been made from such a viewpoint. According to claim 1, the heat storage body provided with a large number of thin tubes through which the combustion air passes is formed of at least two or more honeycomb structures, and the honeycomb structure is formed in a direction in which the combustion air is sent. The heat storage is performed by reducing the cross-sectional area of the thin tubes of the honeycomb structure that are stacked and forming the heat storage body by laminating the cross-sectional area of the thin tubes of the anti-combustion honeycomb structure with respect to the cross-sectional area of the thin tubes of the combustion honeycomb structure. The effect is to enhance the effect and to reduce the temperature gradient of the regenerator for the regenerative burner to prevent cracking.
【0017】また、請求項2によれば、隣り合うハニカ
ム構造体の間に気体が通過可能なスペーサが設置され、
隣り合うハニカム構造体間に間隙があることを特徴とす
る蓄熱式バーナ用蓄熱体であり、ハニカム構造体間で流
路が不連続となって流動抵抗が増大するのを防止するも
のであり、燃焼効率を悪化させることがない。According to the second aspect, a spacer through which gas can pass is provided between adjacent honeycomb structures,
A regenerator for a regenerative burner characterized by having a gap between adjacent honeycomb structures, which prevents a flow path from being discontinuous between the honeycomb structures and increasing flow resistance, There is no deterioration in combustion efficiency.
【0018】更に、請求項3によれば、ハニカム構造体
の積層構造からなる蓄熱式バーナ用蓄熱体において、燃
焼側のハニカム構造体の材質をセラミックスとし、反燃
焼側のハニカム構造体の材料を金属とすることによっ
て、加熱炉の熱効率を高めることができるとともに、蓄
熱体の割れの発生を防止することができる。また、ハニ
カム構造体に比熱の高い金属を用いることにより蓄熱率
を高めることができる。According to a third aspect of the present invention, in the heat storage element for a regenerative burner having a laminated structure of honeycomb structures, the material of the honeycomb structure on the combustion side is ceramics, and the material of the honeycomb structure on the non-combustion side is ceramics. By using metal, the thermal efficiency of the heating furnace can be increased, and the occurrence of cracks in the heat storage body can be prevented. Further, the heat storage rate can be increased by using a metal having a high specific heat for the honeycomb structure.
【0019】[0019]
【実施例】以下、本発明の実施例を図面に基づいて説明
する。図1は、本発明に係る蓄熱式バーナ用蓄熱体の一
実施例を示す一部切欠斜視図である。この蓄熱式バーナ
用蓄熱体は、図3のような加熱炉に使用される蓄熱体で
あり、加熱炉3の各バーナに設けられる。図1におい
て、1はセラミックスからなるハニカム構造体を燃焼空
気の流路方向に三個積層した形状のハニカム状蓄熱体で
あり、ハニカム状蓄熱体1は第1乃至第3のハニカム構
造体1a,1b,1cの集合体から形成されている。こ
れらのハニカム構造体1a,1b,1cには、燃焼空気
や燃焼排ガスが通過する多数の細管3a,3b,3cが
それぞれ形成されている。Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a partially cutaway perspective view showing one embodiment of a heat storage body for a heat storage type burner according to the present invention. This regenerator for a regenerative burner is a regenerator used for a heating furnace as shown in FIG. 3 and is provided in each burner of the heating furnace 3. In FIG. 1, reference numeral 1 denotes a honeycomb-shaped heat storage body having a shape in which three honeycomb structures made of ceramics are stacked in a flow direction of combustion air, and the honeycomb-shaped heat storage body 1 includes first to third honeycomb structures 1a, 1b and 1c. A large number of small tubes 3a, 3b, 3c through which combustion air and combustion exhaust gas pass are formed in the honeycomb structures 1a, 1b, 1c, respectively.
【0020】各ハニカム構造体について説明すると、第
1のハニカム構造体1aは、バーナ側(燃焼側)に設け
られる。第1のハニカム構造体1aは、多数の細管3a
が形成され、その流路断面形状は正方形であり、細管3
aのピッチP1は4mmである。第2のハニカム構造体
1bは、多数の細管3bが形成され、その流路断面形状
は正方形であり、そのピッチP2は3mmである。第3
のハニカム構造体1cは反燃焼側に設けられる。第3の
ハニカム構造体1cには多数の細管3cが形成され、そ
の流路断面形状は正方形であり、そのピッチP3は2m
mである。各ハニカム構造体に設けられた細管3a,3
b,3cの流路断面積は、ハニカム構造体1aが最も燃
焼側に位置するので最も広く形成され、燃焼側から遠ざ
かる毎に順次狭く形成されている。これらのハニカム構
造体1a,1b,1cの外観寸法は同一である。Describing each honeycomb structure, the first honeycomb structure 1a is provided on the burner side (combustion side). The first honeycomb structure 1a includes a large number of thin tubes 3a.
Are formed, and the cross-sectional shape of the channel is square.
The pitch P1 of a is 4 mm. In the second honeycomb structure 1b, a large number of thin tubes 3b are formed, the cross-sectional shape of the flow channel is square, and the pitch P2 is 3 mm. Third
Is provided on the anti-combustion side. A large number of thin tubes 3c are formed in the third honeycomb structure 1c, the cross-sectional shape of the channels is square, and the pitch P3 is 2 m.
m. Narrow tubes 3a, 3 provided in each honeycomb structure
The flow channel cross-sectional areas b and 3c are formed to be the widest since the honeycomb structure 1a is located closest to the combustion side, and are gradually narrowed as the distance from the combustion side increases. The external dimensions of these honeycomb structures 1a, 1b, 1c are the same.
【0021】2はスペーサである。スペーサ2は、第1
のハニカム構造体1aと第2のハニカム構造体1b及び
第2のハニカム構造体1bと第3のハニカム構造体1c
の間にそれぞれ設けられる。スペーサ2によって隣り合
うハニカム構造体を隔てる距離は、ハニカム構造体の細
管の水力直径以上にすることにより細管3a,3b,3
cを通過する流体の流動抵抗を増加させることはない。
また、スペーサ2を挟みハニカム構造体1a,1b,1
cを集合したハニカム状蓄熱体の外形寸法は従来の蓄熱
体と同一とする。Reference numeral 2 denotes a spacer. The spacer 2 is a first
Honeycomb structure 1a and second honeycomb structure 1b, and second honeycomb structure 1b and third honeycomb structure 1c
Between them. The distance separating the adjacent honeycomb structures by the spacer 2 is set to be equal to or more than the hydraulic diameter of the thin tubes of the honeycomb structure, so that the thin tubes 3a, 3b, 3
It does not increase the flow resistance of the fluid passing through c.
Further, the honeycomb structures 1a, 1b, 1
The external dimensions of the honeycomb-shaped regenerator in which c are collected are the same as those of the conventional regenerator.
【0022】次に、図3に示すような加熱炉に、上記実
施例のハニカム状蓄熱体を使用した場合のハニカム状蓄
熱体の温度分布について説明する。ハニカム状蓄熱体1
の燃焼空気の入側と出側の温度条件を図4の条件と同一
にしてハニカム状蓄熱体内部温度分布を測定した。図5
の縦軸は温度を示し、横軸はハニカム状蓄熱体の温度測
定位置を示している。図5のA,B,C,Dはドットで
示したハニカム状蓄熱体の温度測定位置を示し、測定位
置Aは燃焼側であり、測定位置Dは反燃焼側である。Next, the temperature distribution of the honeycomb regenerator when the honeycomb regenerator of the above embodiment is used in a heating furnace as shown in FIG. 3 will be described. Honeycomb regenerator 1
The internal temperature distribution of the honeycomb-shaped regenerator was measured by setting the temperature conditions of the combustion air inlet and outlet sides to the same as those in FIG. FIG.
The vertical axis indicates the temperature, and the horizontal axis indicates the temperature measurement position of the honeycomb-shaped regenerator. A, B, C, and D in FIG. 5 indicate the temperature measurement positions of the honeycomb-shaped regenerator indicated by dots, where the measurement position A is on the combustion side and the measurement position D is on the anti-combustion side.
【0023】その温度分布の測定結果、図5に示す温度
分布となった。図5の温度分布では、ハニカム状蓄熱体
1のB点,C点の温度が図4の温度分布と比較して上昇
していることが判る。すなわち、図1のハニカム状蓄熱
体1は従来の蓄熱体と比較して蓄熱効果が高まったこと
を示している。また、ハニカム状蓄熱体1の流動抵抗に
ついても従来と同等であった。また、従来の蓄熱体では
高温側に割れが発生したが、高温側のハニカム構造体の
流路方向の温度勾配が従来よりも緩慢であるので、使用
期間内では蓄熱体の割れは発生せず長期使用に耐え得る
ものであることが判明した。As a result of measuring the temperature distribution, the temperature distribution shown in FIG. 5 was obtained. In the temperature distribution of FIG. 5, it can be seen that the temperatures at points B and C of the honeycomb-shaped heat storage body 1 are higher than those in the temperature distribution of FIG. That is, it is shown that the honeycomb-shaped heat storage body 1 of FIG. 1 has a higher heat storage effect than the conventional heat storage body. Also, the flow resistance of the honeycomb-shaped heat storage body 1 was equivalent to the conventional one. In addition, cracks occurred on the high-temperature side in the conventional heat storage body, but the temperature gradient in the flow path direction of the honeycomb structure on the high-temperature side was slower than in the past. It turned out that it can withstand long-term use.
【0024】次に、本発明に係る蓄熱式バーナ蓄熱体の
他の実施例について、図2の一部切欠斜視図に基づいて
説明する。同図において、1はハニカム構造の集合体か
らなるハニカム蓄熱体1であり、ハニカム構造体1dの
材質がセラミックからなり、ハニカム構造体1eの材質
が金属としたものである。3d,3eは燃焼空気や燃焼
排ガスが通過する細管である。ハニカム構造体1dが加
熱炉のバーナ側(燃焼側)であり、ハニカム構造体1e
が燃焼空気の流入側または燃焼排気ガスの流出側(反燃
焼側)である。また、ハニカム構造体1dの細管3dの
流路断面積はハニカム構造体1eの細管3eの流路断面
積より広い。また、ハニカム構造体1dの材質は、高温
側(燃焼側)がセラミックであり、低温側(反燃焼側)
が金属である。2はスペーサである。スペーサ2で形成
される間隙は図1の実施例と同様に設定すればよい。ハ
ニカム構造体1d,1eの外観寸法は同一である。ま
た、低温側をより比熱の高い金属を用いることによっ
て、蓄熱効果を高めたものである。Next, another embodiment of the regenerative burner regenerator according to the present invention will be described with reference to a partially cutaway perspective view of FIG. In FIG. 1, reference numeral 1 denotes a honeycomb heat storage body 1 formed of an aggregate having a honeycomb structure. The material of a honeycomb structure 1 d is made of ceramic, and the material of a honeycomb structure 1 e is metal. 3d and 3e are thin tubes through which combustion air and combustion exhaust gas pass. The honeycomb structure 1d is on the burner side (combustion side) of the heating furnace, and the honeycomb structure 1e
Is the combustion air inflow side or the combustion exhaust gas outflow side (anti-combustion side). Further, the flow channel cross-sectional area of the thin tube 3d of the honeycomb structure 1d is larger than the flow channel cross-sectional area of the thin tube 3e of the honeycomb structure 1e. The material of the honeycomb structure 1d is ceramic on the high temperature side (combustion side) and low temperature side (anti-combustion side).
Is a metal. 2 is a spacer. The gap formed by the spacer 2 may be set in the same manner as in the embodiment of FIG. The external dimensions of the honeycomb structures 1d and 1e are the same. The heat storage effect is enhanced by using a metal having a higher specific heat on the low temperature side.
【0025】上記実施例のように、本発明の蓄熱式バー
ナ蓄熱体は、ハニカム構造体の集合体からなるハニカム
状蓄熱体であり、燃焼側のハニカム構造体の流路断面積
を反燃焼側のハニカム構造体の流路断面積よりも広くし
たものである。換言すれば、高温側のハニカム構造体の
熱交換を小さくし、低温側の熱交換を大きくすることに
よって、蓄熱効果及び熱回収効率を維持し、且つ、ハニ
カム状蓄熱体の割れの発生を解消したものである。無
論、ハニカム状蓄熱体の細管の流路断面形状は、実施例
では方形であるが、この実施例に限定することなく、長
方形、三角形、或いは六角形等であってもよいことは明
らかである。As in the above embodiment, the regenerative burner regenerator according to the present invention is a honeycomb regenerator composed of an aggregate of honeycomb structures. Is wider than the cross-sectional area of the flow channel of the honeycomb structure. In other words, by reducing the heat exchange of the honeycomb structure on the high-temperature side and increasing the heat exchange on the low-temperature side, the heat storage effect and the heat recovery efficiency are maintained, and the occurrence of cracks in the honeycomb-shaped heat storage body is eliminated. It was done. Needless to say, the cross-sectional shape of the flow passage of the thin tube of the honeycomb-shaped heat storage body is rectangular in the embodiment, but it is apparent that the shape is not limited to this embodiment and may be rectangular, triangular, hexagonal, or the like. .
【0026】[0026]
【発明の効果】上述のように、本発明によれば、蓄熱体
の割れが防止できるとともに、熱交換効率を低下させる
ことなく、蓄熱式バーナを長期に安定して運転すること
ができる利点がある。従って、従来のように、蓄熱体が
割れて、蓄熱体流路が一部拡大して、蓄熱体出側燃焼ガ
ス温度が上昇し排ガス熱損失が増加し熱効率が悪化する
ことがなくなる利点がある。また、従来の蓄熱体では、
出側燃焼ガス温度の上昇等を監視しながら、蓄熱体の割
れを判定して蓄熱体を交換したり、数ケ月毎に定期的に
蓄熱体の交換を行っていたために、蓄熱体交換による設
備停止期間の生産機会の損失、蓄熱体交換費用がかかる
欠点があったが、本発明によれば、蓄熱体の交換頻度を
低減することができるので、設備の計画定期修理時期以
上に交換頻度を延長できる利点があり管理コストを低減
できる利点がある。As described above, according to the present invention, it is possible to prevent the heat storage body from cracking and to operate the regenerative burner stably for a long time without lowering the heat exchange efficiency. is there. Therefore, unlike the related art, there is an advantage that the heat storage body is not broken, the heat storage body flow path is partially expanded, the temperature of the combustion gas at the side of the heat storage body increases, the heat loss of the exhaust gas increases, and the heat efficiency does not deteriorate. . Also, in the conventional heat storage,
While monitoring the rise of the outlet combustion gas temperature, etc., it was determined that the heat storage material was cracked, and the heat storage material was replaced, or the heat storage material was replaced regularly every few months. Although there were drawbacks such as loss of production opportunities during the suspension period and heat storage unit replacement costs, according to the present invention, it is possible to reduce the frequency of replacement of the heat storage units. There is the advantage that it can be extended and the management cost can be reduced.
【0027】従って、本発明によれば、設備停止期間の
生産損失がなくなり、且つ、蓄熱体交換費用が従来の約
1/3程度に削減された。また、蓄熱体の点検、交換の
理由は、蓄熱体の割れではなく、燃焼ガスやガス中の蓄
熱体の化学反応による蓄熱体の劣化の点検や、ダストが
蓄熱体を閉塞して圧損が上昇する場合に清掃するために
限られ、作業工数を低減できる利点がある。Therefore, according to the present invention, there is no production loss during the equipment downtime, and the cost of exchanging the heat storage material is reduced to about 1/3 of the conventional cost. In addition, the reason for the inspection and replacement of the heat storage element is not cracking of the heat storage element, but inspection of deterioration of the heat storage element due to the chemical reaction of the combustion gas or the heat storage element in the gas, and dust blocking the heat storage element and increasing the pressure loss. In this case, there is an advantage that the number of work steps can be reduced only when cleaning is performed.
【図1】本発明の蓄熱式バーナ用蓄熱体の一実施例を示
す一部切欠斜視図である。FIG. 1 is a partially cutaway perspective view showing one embodiment of a heat storage body for a heat storage type burner of the present invention.
【図2】本発明の蓄熱式バーナ用蓄熱体の他の実施例を
示す一部切欠斜視図である。FIG. 2 is a partially cutaway perspective view showing another embodiment of the heat storage body for a heat storage type burner of the present invention.
【図3】蓄熱式バーナの概要を示す図である。FIG. 3 is a diagram showing an outline of a regenerative burner.
【図4】従来の蓄熱体の温度分布を示す図である。FIG. 4 is a diagram showing a temperature distribution of a conventional heat storage body.
【図5】本発明の蓄熱式バーナ用蓄熱体の温度分布を示
す図である。FIG. 5 is a diagram showing a temperature distribution of a heat storage body for a heat storage type burner of the present invention.
1 ハニカム状蓄熱体 1a〜1e ハニカム構造体 2 スペーサ 3a〜3e 細管 DESCRIPTION OF SYMBOLS 1 Honeycomb heat storage body 1a-1e Honeycomb structure 2 Spacer 3a-3e Thin tube
フロントページの続き (72)発明者 森 功 東京都千代田区丸の内一丁目1番2号 日本鋼管株式会社内 (72)発明者 田中 良一 神奈川県横浜市鶴見区尻手二丁目1番53 号 日本ファーネス工業株式会社内 (72)発明者 松尾 護 神奈川県横浜市鶴見区尻手二丁目1番53 号 日本ファーネス工業株式会社内会社 内 (58)調査した分野(Int.Cl.7,DB名) F28D 17/02 F28D 20/00 F28D 19/04 Continued on the front page. (72) Isao Mori, 1-2-1, Marunouchi, Chiyoda-ku, Tokyo Nippon Kokan Co., Ltd. (72) Ryoichi Tanaka 2-53, Shirate, Tsurumi-ku, Yokohama, Kanagawa, Japan Nihon Furnace Industries (72) Inventor: Mamoru Matsuo 2-53-1, Shirite, Tsurumi-ku, Yokohama-shi, Kanagawa Prefecture In-house company of Japan Furnace Industries Co., Ltd. (58) Field surveyed (Int. Cl. 7 , DB name) F28D 17 / 02 F28D 20/00 F28D 19/04
Claims (3)
過する多数の細管が設けられた蓄熱体が少なくとも2個
以上のハニカム構造体からなり、且つ、前記燃焼用空気
が送り込まれる方向に前記ハニカム構造体が積層され、
前記蓄熱体を積層形成するハニカム構造体の細管の断面
積が燃焼側ハニカム構造体の細管の断面積に対して反燃
焼側ハニカム構造体の細管の断面積を狭くしたことを特
徴とする蓄熱式バーナ用蓄熱体。1. A regenerator for a regenerative burner, wherein at least two or more honeycomb structures are provided with a plurality of thin tubes through which combustion air and exhaust gas for fuel alternately flow while changing the flow direction. And, the honeycomb structure is stacked in a direction in which the combustion air is sent,
The heat storage type wherein the cross-sectional area of the thin tube of the honeycomb structure in which the heat storage body is formed in a lamination is made smaller in cross-sectional area of the thin tube of the anti-combustion side honeycomb structure with respect to the cross-sectional area of the thin tube of the combustion side honeycomb structure. Thermal storage for burner.
して間隙を設けたことを特徴とする請求項1に記載の蓄
熱式バーナ用蓄熱体。2. The heat storage element for a regenerative burner according to claim 1, wherein a spacer is arranged between said honeycomb structures to provide a gap.
蓄熱体において、燃焼側ハニカム構造体の材質がセラミ
ックスであり、反燃焼側ハニカム構造体の材質が金属か
らなることを特徴とする請求項1または2に記載の蓄熱
式バーナ用蓄熱体。3. The heat storage body having a laminated structure of the honeycomb structures, wherein a material of the combustion-side honeycomb structure is ceramics, and a material of the non-combustion-side honeycomb structure is metal. Or the regenerator for a regenerative burner according to 2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP04946295A JP3260580B2 (en) | 1995-03-09 | 1995-03-09 | Thermal storage for thermal storage burners |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP04946295A JP3260580B2 (en) | 1995-03-09 | 1995-03-09 | Thermal storage for thermal storage burners |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08247671A JPH08247671A (en) | 1996-09-27 |
| JP3260580B2 true JP3260580B2 (en) | 2002-02-25 |
Family
ID=12831818
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP04946295A Expired - Fee Related JP3260580B2 (en) | 1995-03-09 | 1995-03-09 | Thermal storage for thermal storage burners |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3260580B2 (en) |
Families Citing this family (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5966431B2 (en) * | 2012-02-28 | 2016-08-10 | Jfeスチール株式会社 | Radiant tube burner |
| AU2013280611A1 (en) * | 2012-06-29 | 2015-02-05 | Saint-Gobain Ceramics & Plastics. Inc. | Low void fraction thermal storage articles and methods |
| JP5946853B2 (en) * | 2014-03-18 | 2016-07-06 | 東京窯業株式会社 | Honeycomb structure |
| JP6194068B2 (en) | 2015-08-05 | 2017-09-06 | 東京窯業株式会社 | Thermal storage |
| JP6952461B2 (en) * | 2016-12-15 | 2021-10-20 | 大阪瓦斯株式会社 | Heat storage burner and heating furnace |
| CN107525274B (en) * | 2017-10-17 | 2023-05-16 | 临沂市欧科节能技术有限公司 | Method for improving energy conservation and stability of gas boiler |
| CN111854494A (en) * | 2020-06-26 | 2020-10-30 | 苏州诺瑞达新材料科技有限公司 | A high-efficiency, long-life, low-coking and low-clogging regenerator |
| JP7646471B2 (en) * | 2021-06-17 | 2025-03-17 | 株式会社東芝 | Thermal storage power generation system and power generation control system |
| JP7517490B1 (en) * | 2023-02-07 | 2024-07-17 | 三菱マテリアル株式会社 | Wire mesh laminated porous body and porous body-containing pipe |
| JP7517488B1 (en) * | 2023-02-07 | 2024-07-17 | 三菱マテリアル株式会社 | Wire mesh laminated porous body and porous body-containing pipe |
-
1995
- 1995-03-09 JP JP04946295A patent/JP3260580B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH08247671A (en) | 1996-09-27 |
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