JPS582327B2 - infrared gas burner - Google Patents
infrared gas burnerInfo
- Publication number
- JPS582327B2 JPS582327B2 JP50126677A JP12667775A JPS582327B2 JP S582327 B2 JPS582327 B2 JP S582327B2 JP 50126677 A JP50126677 A JP 50126677A JP 12667775 A JP12667775 A JP 12667775A JP S582327 B2 JPS582327 B2 JP S582327B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- infrared
- burners
- burner
- gas burner
- 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
Links
Landscapes
- Gas Burners (AREA)
Description
【発明の詳細な説明】
従来の赤外線放射面を有する赤外線ガスバーナとしては
、青砥を生成物とする耐火板に多数の円孔を設けたセラ
ミソクバーナ、金網の網目一つ一つを火孔にした金網バ
ーナ、プンセンバーナで耐火物を高温に加熱するバーナ
などが用いられていた。DETAILED DESCRIPTION OF THE INVENTION Conventional infrared gas burners having an infrared radiation surface include ceramic burners in which a large number of circular holes are provided in a refractory plate made of acetic acid as a product; Burners that heated refractories to high temperatures, such as wire mesh burners and punsen burners, were used.
上記セラミックバーナは機械的強度が弱く、赤熱するま
で時間がかかり、又赤外線発生効率も低い。The ceramic burner has low mechanical strength, takes time to become red hot, and has low infrared generation efficiency.
これはセラミック自体の熱伝導が忍いため円孔周辺は比
較的温度が高いが、円孔から離れた所は温度が低く輻射
量が少ない。This is because the heat conduction of the ceramic itself is poor, so the temperature around the hole is relatively high, but the temperature is lower in areas away from the hole, and the amount of radiation is small.
しかし高温下での腐蝕などは全くなくこの点はセラミソ
クバーナの大きな特徴と言える。However, there is no corrosion at all under high temperatures, and this can be said to be a major feature of Ceramisokuvarna.
一方金網バーナは熱伝導が良いにもかかわらず高温腐蝕
の面から温度が上げられず輻射量を犬き〈することがで
きなかった。On the other hand, although wire mesh burners have good heat conductivity, they cannot raise the temperature due to high-temperature corrosion and cannot reduce the amount of radiation.
更にブンセンバーナ方式で耐火物を加熱する方法でも均
等な赤熱が得られず輻射量はこれらのバーナの中で一番
低い欠点があった。Furthermore, even the method of heating refractories using the Bunsen burner method had the disadvantage that uniform red heat could not be obtained and the amount of radiation was the lowest among these burners.
本発明はこれら従来の欠陥を除いた赤外線ガスバーナに
関するものである。The present invention relates to an infrared gas burner that eliminates these conventional deficiencies.
以下図面をもとに本発明の一実施例について説明する。An embodiment of the present invention will be described below based on the drawings.
第1,2図に於いて、1はセラミソク等の耐火物の内容
に耐熱金属材料の酸化物、粒、繊維などを混合分散し、
多数のガス噴出孔1′を設けて平板状に構成した燃焼部
、2はその固定枠、3,4はガス供給部を構成する混合
管および空気吸引口で、ガス元栓に連通したノズル5よ
り噴出した町燃性ガスをそのエゼクター作用により空気
吸引口4より空気を吸引し混合管3において空気と混合
せしめて混合ガス化する。In Figures 1 and 2, 1 mixes and disperses oxides, grains, fibers, etc. of heat-resistant metal materials in the contents of refractory materials such as ceramics,
The combustion section is configured in a flat plate shape with a large number of gas ejection holes 1', 2 is its fixed frame, 3 and 4 are a mixing tube and air suction port that constitute the gas supply section, and a nozzle 5 that communicates with the gas main valve is used. The ejector action of the ejected combustible gas draws air through the air suction port 4 and mixes it with air in the mixing pipe 3 to form a mixed gas.
この混合ガスは燃焼部1の内側に至り噴出孔1′より噴
出すると同時に着火し、これより燃焼部1の表面温度は
上昇し、900〜1000℃の高温に達して赤熱し、強
力な赤外線を放射する。This mixed gas reaches the inside of the combustion section 1, ejects from the nozzle 1', and is ignited at the same time. From this, the surface temperature of the combustion section 1 rises, reaching a high temperature of 900 to 1000 degrees Celsius, becoming red-hot and emitting strong infrared rays. radiate.
この種の赤外線ガスバーナに於いては加熱に適した赤外
線を最も多く放射するように設計しなければならない事
は当然のことでその際の赤外線の波長は第3図に示すよ
うに2.5μ位が最も通している。It goes without saying that this type of infrared gas burner must be designed to emit the maximum amount of infrared rays suitable for heating, and the wavelength of the infrared rays in this case is approximately 2.5μ as shown in Figure 3. is the most common.
第3図において、水の層の厚さを変えた場合及びひふの
場合のそれぞれの分光透過率を示し、一般に水は赤外線
をよく吸収するため水を含有するものは、その分光特性
が水に大きく影響され水とよく似た分光特性を示す。Figure 3 shows the spectral transmittance when the thickness of the water layer is changed and when the water layer is thin. Generally speaking, water absorbs infrared rays well, so if it contains water, its spectral characteristics will be similar to that of water. It exhibits spectral properties similar to those of water.
この第3図で明らかなように、いずれに於いても0.4
〜2.5μm程度の帯域に於いて透過率が大きく、すな
わち吸収が悪いことを示している。As is clear from this Figure 3, in both cases 0.4
This shows that the transmittance is large in the band of about 2.5 μm, that is, the absorption is poor.
前述の如く、できるだけ吸収が大きな(すなわち透過率
が極力小さい)すなわち加熱に適した赤外線を最も多く
放射するような赤外線バーナが望ましく、このことから
も赤外線バーナから放射されるエネルギーが効率よく吸
収され、熱に変換されるためには2.5μm位の波長が
最も適していると言える。As mentioned above, it is desirable to use an infrared burner that has as much absorption as possible (that is, the transmittance is as low as possible), that is, it emits the most infrared rays suitable for heating, and from this point of view, the energy radiated from the infrared burner can be absorbed efficiently. It can be said that a wavelength of about 2.5 μm is most suitable for conversion into heat.
ここでその波長とバーナ輻射体温度との関係をウィーン
の変位則から求めてみると横軸に波長、縦軸に輻射体温
度を表わすと第4図のような曲線となり、加熱に適した
輻射エネルギーの波長約2.5μを得るには輻射体温度
は約900℃にすればよいことがわかる。Now, if we calculate the relationship between the wavelength and the burner radiator temperature using Wien's displacement law, we can plot the wavelength on the horizontal axis and the radiator temperature on the vertical axis, and the curve as shown in Figure 4 will be obtained, indicating the radiation suitable for heating. It can be seen that in order to obtain an energy wavelength of approximately 2.5μ, the radiator temperature should be approximately 900°C.
しかしながらこのように温度の高い輻射体は従来得られ
なかった。However, such a high-temperature radiator has not been previously available.
前述のセラミックバーナやブンセンバーナで耐火物を高
温加熱するバーナでは高々800℃程度であり、又金網
バーナでは金属の高温酸化腐蝕、逆火現象を起こすなど
から840℃以上に上げることができなかった。With the aforementioned ceramic burners and Bunsen burners, which heat refractories at high temperatures, the temperature is at most about 800°C, and with wire mesh burners, it is not possible to raise the temperature above 840°C because of high-temperature oxidation corrosion of the metal and backfire phenomenon. .
本発明の赤外線がスバーナは金網バーナの高温腐蝕、セ
ラミソクバーナ、ブンセン方式の機械的強度、熱伝導、
赤熱の不均一性などの問題をすべて一掃したものである
。The infrared rays of the present invention can improve the high-temperature corrosion of wire mesh burners, the mechanical strength of ceramic burners, the Bunsen method, thermal conductivity,
This eliminates all problems such as uneven red heat.
すなわち耐火物の内部に耐熱金属材料の酸化物、粒、繊
維などを混合分散させることにより、熱伝導がスムーズ
になり噴出孔間、噴出孔から離れたところの温度分布が
なくなり温度が均一になる。In other words, by mixing and dispersing oxides, grains, fibers, etc. of heat-resistant metal materials inside the refractory, heat conduction becomes smooth and there is no temperature distribution between the nozzles or at a distance from the nozzles, making the temperature uniform. .
又、金属材料を齢分散しているため温度上昇も速くなり
従来のセラミソクバーナでは表面温度も800℃程度で
あったのに対し本発明のバーナでは900〜950℃ま
でも充分町能である。In addition, because the metal material is dispersed in age, the temperature rises quickly, and while the surface temperature of conventional ceramic burners was around 800°C, the burner of the present invention has a sufficient temperature range of 900 to 950°C. .
機械的強度の面でも例えば金属繊維などを混合分散させ
ることにより機械的衝撃性、熱衝撃性も高めることがで
きる。In terms of mechanical strength, mechanical impact resistance and thermal impact resistance can also be improved by mixing and dispersing metal fibers.
本発明のバーナを試作し各特性を比較すれば次表の通り
である。The burner of the present invention was prototyped and its characteristics were compared as shown in the following table.
以上のように本発明のものは、耐火物の内部に成形時に
あらかじめ分散、混合しておくものであり、付着させた
タイプのものとは異なり、加熱冷却のくり返しによる剥
離や落下などは全く起らず、使用条件としてはきわめて
きびしい酸化や還元を受ける火炎の中にさらされること
もなく、バーナプレートとしての耐久性を著しく向上さ
せたものである。As described above, the material of the present invention is dispersed and mixed inside the refractory material beforehand at the time of molding, and unlike the adhesion type, there is no possibility of peeling or falling due to repeated heating and cooling. Moreover, it is not exposed to flames that undergo extremely severe oxidation and reduction under the conditions of use, and its durability as a burner plate is significantly improved.
第1図は本発明の一実施例を示す赤外線ガスバーナの断
面図、第2図は燃焼部の拡大断面図、第3図は赤外線波
長と透過率の関係を示す曲線図、第4図は赤外線波長と
輻射体温度の関係を示す曲線図である。
1・・・・・・燃焼部、1′・・・・・・ガス噴出孔。Fig. 1 is a sectional view of an infrared gas burner showing an embodiment of the present invention, Fig. 2 is an enlarged sectional view of the combustion section, Fig. 3 is a curve diagram showing the relationship between infrared wavelength and transmittance, and Fig. 4 is an infrared gas burner. It is a curve diagram showing the relationship between wavelength and radiator temperature. 1... Combustion part, 1'... Gas injection hole.
Claims (1)
部に混合分散し、多数のガス噴出孔を設けて燃焼部を形
成したことを特徴とする赤外線ガスバーナ。1. An infrared gas burner characterized in that oxides, grains, or fibers of a heat-resistant metal material are mixed and dispersed inside a refractory, and a combustion section is formed by providing a large number of gas ejection holes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50126677A JPS582327B2 (en) | 1975-10-20 | 1975-10-20 | infrared gas burner |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50126677A JPS582327B2 (en) | 1975-10-20 | 1975-10-20 | infrared gas burner |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5250037A JPS5250037A (en) | 1977-04-21 |
| JPS582327B2 true JPS582327B2 (en) | 1983-01-17 |
Family
ID=14941114
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50126677A Expired JPS582327B2 (en) | 1975-10-20 | 1975-10-20 | infrared gas burner |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS582327B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5735209A (en) * | 1980-08-12 | 1982-02-25 | Kyocera Corp | Burner plate |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4413034Y1 (en) * | 1965-12-16 | 1969-05-30 |
-
1975
- 1975-10-20 JP JP50126677A patent/JPS582327B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5250037A (en) | 1977-04-21 |
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