TWI329677B - - Google Patents

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TWI329677B
TWI329677B TW095140218A TW95140218A TWI329677B TW I329677 B TWI329677 B TW I329677B TW 095140218 A TW095140218 A TW 095140218A TW 95140218 A TW95140218 A TW 95140218A TW I329677 B TWI329677 B TW I329677B
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Taiwan
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gas
layer
combustion
concentration
fuel
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TW095140218A
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Chinese (zh)
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TW200722529A (en
Inventor
Oyama Nobuyuki
Sato Hideaki
Machida Satoshi
Takeda Kanji
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Jfe Steel Corp
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    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22BPRODUCTION AND REFINING OF METALS; PRETREATMENT OF RAW MATERIALS
    • C22B1/00Preliminary treatment of ores or scrap
    • C22B1/14Agglomerating; Briquetting; Binding; Granulating
    • C22B1/16Sintering; Agglomerating
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22BPRODUCTION AND REFINING OF METALS; PRETREATMENT OF RAW MATERIALS
    • C22B1/00Preliminary treatment of ores or scrap
    • C22B1/14Agglomerating; Briquetting; Binding; Granulating
    • C22B1/16Sintering; Agglomerating
    • C22B1/20Sintering; Agglomerating in sintering machines with movable grates
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22BPRODUCTION AND REFINING OF METALS; PRETREATMENT OF RAW MATERIALS
    • C22B1/00Preliminary treatment of ores or scrap
    • C22B1/14Agglomerating; Briquetting; Binding; Granulating
    • C22B1/16Sintering; Agglomerating
    • C22B1/20Sintering; Agglomerating in sintering machines with movable grates
    • C22B1/205Sintering; Agglomerating in sintering machines with movable grates regulation of the sintering process
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F27FURNACES; KILNS; OVENS; RETORTS
    • F27BFURNACES, KILNS, OVENS, OR RETORTS IN GENERAL; OPEN SINTERING OR LIKE APPARATUS
    • F27B21/00Open or uncovered sintering apparatus; Other heat-treatment apparatus of like construction
    • F27B21/06Endless-strand sintering machines
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F27FURNACES; KILNS; OVENS; RETORTS
    • F27DDETAILS OR ACCESSORIES OF FURNACES, KILNS, OVENS, OR RETORTS, IN SO FAR AS THEY ARE OF KINDS OCCURRING IN MORE THAN ONE KIND OF FURNACE
    • F27D3/00Charging; Discharging; Manipulation of charge
    • F27D3/10Charging directly from hoppers or shoots

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  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Mechanical Engineering (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Geology (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Manufacturing & Machinery (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • Materials Engineering (AREA)
  • Environmental & Geological Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • General Engineering & Computer Science (AREA)
  • Manufacture And Refinement Of Metals (AREA)

Description

1329677 九、發明說明: 【發明所屬之技術領域】 本發明係關於使用下方吸引式之型帶式 lioyd,DL)燒結機來製造高爐原料用燒結礦之;法、wl/ht - 該方法所使用之燒結機。 、以及 - 【先前技術】 _作為高爐製生鐵法之主要原料之燒結礦,—般經由圖i _所不之步驟而製造。原料為鐵粉礦石、製鐵所内之回收 粉、燒結礦筛下粉、石灰石以及白雲石等含Ca〇原料、生 石灰等之造粒助劑、焦炭粉或者無煙炭等。石灰石及白雲 石等含CaO原料,以下稱作r Ca〇系副原料」。該等原料 自各漏斗1…於運輸機上以特定比例剪下。將所剪下之原 料利用圓筒混合機2等,一面添加適量之水,一面進行混 合,繼而造粒,形成平均直徑具有3. 〇 mm〜6 〇 之模 擬粒子之燒結原料。所形成之燒結原料於回轉爐3中進行 φ乾燥。乾燥後之燒結原料自配置於燒結機上之接料桶4、 5,經由筒式給料機6及剪切槽7而裝入到無端移動式燒 結機台車8上,形成亦稱作燒結床之裝入層9。裝入層之 ..厚度(两度)為400 mm〜800 mm左右。其後,利用設置於 -裝入層9上方之點火爐10來對該裝入層中之炭材點火。 該裝入層中之炭材經由配設於台車8下方之風箱π而吸 引至下方,由此依序燃燒,並且上述燒結原料利用此時所 產生之燃燒熱而燃燒、炫融’生成燒結塊。其後,所獲得 之燒結塊粉碎後經粒化’成為由5. 〇 mm以上之塊狀物所 312/發明說明書(補件)/96-01/95140218 5 1329677 構成之成品燒結礦而回收。 於上述製造過程中,首先,利用點火爐1〇對裝,入層之 表面進行點火。裝入層中之炭材依自該裝入層頂部吸引至 下層部之吸引氣體的作用而燃燒,並且該燃燒隨著台車8 -之移動而逐漸向下層且前方行進。與該燃燒之行進同時, .該裝入層中之燒結原料粒子之水分,雖因炭材之燃燒所產 生之熱量而蒸發,卻會被吸引至下方,並濃縮於仍未升溫 鲁之下層濕潤帶之燒結原料中。當該水分濃度增大至一定程 度以上岬,由於水分會填補吸引氣體之流路(即原料粒子 間之空隙),故通氣阻力增大。再者,於燒結化反應中所 必要之溶融部分,通氣阻力亦增大。 燒結礦之生產量(t/hr)通常由燒結生產性(t/hr · m2)x 燒結機面積(m2)來決定。即,生產量之變化取決於燒結機 之機寬及機長、原料堆積層之厚度(裝入層厚度)、燒結原 料之體積密度、燒結(燃燒)時間、良率等。為了增加該燒 φ結礦之生產量,認為以下方法有效,即:改善裝入層之通 氣性(壓損),以縮短燒結時間之方法;或者提高粉碎前燒 結塊之冷延強度以使良率提高之方法等。 . 圖2係表示裝入層内之壓損與溫度之分佈圖。圖2之溫 '度分佈曲線表示於裝入層中移動之燃燒(火焰)前線,位於 該裝入層之厚度方向之台車上約4〇〇 mm之位置時之情 況。此時之壓損分佈於濕潤帶約為6〇% ,於燃燒熔融二 為 40% 〇 圖3係表示燒結礦高生產時與低生產時,裴入層内之溫 312/發明說明書(補件)/96-01/95140218 6 1329677 度:佈圖。溫度保持在原料粒子開始熔融之丨2〇(rc以上 的同’皿區域保持時間,於低生產時用t丨表示,於重視生產 ί1生之鬲生產時用h表示。於高生產時,必須提高台車速 度,故此時之高溫區域保持時間t2短於低生產時之高溫區 -=保持時間tl。由於保持於高溫之時間變短,使燒成不充 .二’導致燒結礦之冷延強度降低,引起良率降低。因此, 為為了提升咼強度燒結礦之生產量,有效的是,利用某 籲,方法來提高燒結塊之強度,即提高燒結礦之冷延強度, 實現良率之維持、提高。再者,對於燒結礦冷延強度,使 用 SI(Shatter Index,碎裂指數)、TI(TumMer Index, 轉鼓指數)。 圖4(a)表示燒結機台車上裝入層之燒結行進原理,圖 400表示裝入層内燒結過程之溫度分佈加以 P ern)圖4(c)表示燒結塊之良率分佈。根據圖4(b) 可知,,入層上部(燒結層)與下層部相比,溫度難以上 籲升,且高溫區域保持時間變短。因此,於該裝入層上邙, 燃燒炫融反應(燒結化反應)不充分,如_ 4(c)所曰示由 於燒結塊之強度降低,故呈現良率並未提高,生產性降低 . 之傾向。 - 習知,已提出有用以使裝入層上部保持高溫之方法。 =專=開昭48-刪2號公報揭示有於點火爐正 後方吹入向湲度可辦'性教I#之枯供 時,…,、二曰 吹入可燃性氣體 時亚未削減厌材莖,故燒結層内形成超過1380 溫,因此無法獲得充分之冷延強度提高、良率增加之改: 312/發明說明書(補件)/96-01/95140218 7 1329677 效果。又,於點火爐正後方以〇分鐘至2分鐘之時間吹入 可燃性氣體,係點燃可燃性氣體引起大火災之危險高,缺 乏實用性之技術’並未達到實用化地步。 又,曰本專利特開昭55 — 18585號公報揭示有如下技 術:為了使燒結原料之裝入層内達到高溫,而於該裝入層 -上方配設排煙罩,通過該排煙罩將空氣與焦爐氣體之混合 •氣體吹入到點火爐正後方之位置處。燒結層内之溫度成: 超過1350 C之尚溫,故無法獲得上述吹入效果,並且可 •燃性混合氣體被點燃,具有大火災之危險,因此並未得到 實用化。 更進一步,日本專利特開平5一 31 1257號公報揭示有將 低融點溶劑與炭材或者可燃性氣體同時於點火爐正後方 之位置處吹入之技術。該方法亦係由於在表面殘留有火焰 之狀態下吹入可燃性氣體而引起大火災之危險高同時由 於燒結帶之寬度未;i夠厚(約15随以下),故無法充分發 •揮效果。更進-步’由於存在大量低融點溶劑,故於上層 部會引起過剩熔融現象,以堵塞空氣流路之氣孔。由於^ 氣性惡化,導致生產性降低,故該項技術亦至今未 .用化。 如上所述’迄今為止所提出之習知技術均未得到實用 化’因此迫切«對經濟上成立之吹人條件進行探索。 於燒結礦U質調整中’重要的是,調整燃燒時之 到達溫度及高溫區域係持時間等,燒結礦之品質依該等= 整而決L該方面’日本專利特開昭仏—刪2號公 312/發明說明書(補件V96*01/95140218 以if =不之方法係使氣體燃料於裝入層之表面燃燒’ 術。/燒結步騾之前半部分中該裝入層上部溫度之技 維二’該方法存在如下問題:氣體燃料濃度高,因而 山鉍ϋ之二氣(氧氣)量不充分,有可能造成燒結原料之 ΐ材(焦炭)之燃燒降低,而導致無法實現燒結礦品質之改 二又」日本專利特開昭55— 18585號公報+所揭示之方 麻〜糸:置排煙罩以供給燃燒以氣與可燃性氣體,由此 :侍更'溫度之方法,然而該方法亦會造成熱量不充分。 二ΐΤ法亦存在下述問題:於高溫帶區域,焦炭燃燒所 m _氣因用於吹入可燃性氣體之燃燒而消耗,故焦炭之 燃燒緩慢,導致燒結時間延長。 更進一步,日本專利特開平5一 31 1257號公報中所揭示 2方法存在如下問題:由於使空氣(氧氣)量增加,並且混 :有低融㈣材及炭材,故雖然可燃性氣體及焦炭之燃燒 ^度增加,但由於低融點熔材及粉體一同吹入故燃燒用 空氣之通氣性降低。 【發明内容】 A本發明之目的在於提供燒結礦之製造方法以及用以實 鈀該方法之燒結機,上述燒結礦之製造方法係於下方吸引 式,結機之操料’纟未使裝入層全體之通氣性惡化,而 以高良率製造高強度之燒結礦。 為了達成上述目的,本發明提供具有以下步驟之燒結礦 之製造方法。 裝入步驟,於循環移動之台車上,裝入含有粉礦石及炭 3127發明說明書(補件)/96-01/95140218 9 1329677 材之燒結原料,使於台車上形成含有炭材之裝入層; 點火步驟,於點火爐中對裝入層表面之炭材進行點火; 燒成步驟,通過配置於台車下之風箱而吸引空氣,使裝 入層中之炭材燃燒,並且利用所產生之燃燒熱而生成燒結 塊;以及 乳體燃料燃燒步驟’自裝人層之上方供給稀釋成燃燒下 限濃度以下之氣體燃料’使上述氣體燃料於裝入層内燃 燒。 上述氣體燃料燃燒步驟較佳為,包含下述動作:自裝入 層之上方供給稀釋成燃燒下限濃度以下之氣體燃料,使上 述氣體燃料於裝人層内燃燒,且調整裝人層内之最高到達 /皿f、或裝入層内之高溫區域保持時間、或者裝入層内之 最向到達溫度與高溫區域保持時間。 以如下態樣來實施上述裝入層内之最高到達溫度之調 整較佳。 (A) 自裝人層之上方供給稀釋成燃燒下限濃度以下之氣 體燃料,且調整裝入層内之最高到達溫度。 (B) 自裝人層之上方供給稀釋成燃燒下限漢度以下之氣 體燃料’且調整燒結原料中之炭材量,藉此而調整裝入層 内之最高到達溫度。 (C)自裝入層之上方供給稀釋成燃燒下限濃度以下之氣 體燃料’且調整氣體燃料之供給量,調整最高到達温度。 自裝^層之上方供給稀釋成燃燒下限濃度以下之氣 ’調燒結原料中之炭材量與氣體燃料之供給量,1329677 IX. Description of the Invention: [Technical Field of the Invention] The present invention relates to a sinter of a blast furnace raw material using a suction type belt type lioyd, DL) sintering machine; method, wl/ht - used in the method Sintering machine. And - [Prior Art] _ Sinter, which is the main raw material of the blast furnace-made pig iron method, is generally manufactured through the steps of Figure i. The raw materials are iron powder ore, recycled powder in iron ore, sinter ore sieve powder, limestone, dolomite and other granulation aids such as Ca-containing raw materials, lime, etc., coke powder or smokeless charcoal. CaO-containing raw materials such as limestone and dolomite are hereinafter referred to as r Ca〇-based auxiliary materials. The raw materials are cut from the respective funnels 1 on a conveyor at a specific ratio. The raw material to be cut is mixed with a proper amount of water by a cylindrical mixer 2 or the like, and then granulated to form a sintered raw material having a mean diameter of 3. 〇 mm to 6 〇. The sintered raw material formed is dried in the rotary kiln 3 by φ. The dried sintering raw material is loaded into the endless moving sintering machine trolley 8 from the receiving buckets 4 and 5 disposed on the sintering machine via the drum feeder 6 and the shearing tank 7, forming a so-called sintering bed. Load layer 9. The thickness of the layer (two degrees) is about 400 mm to 800 mm. Thereafter, the carbonaceous material in the packed bed is ignited by means of an ignition furnace 10 disposed above the loading layer 9. The carbon material in the charging layer is sucked to the lower side via a bellows π disposed under the bogie 8, thereby sequentially burning, and the sintered raw material is burned and smelted by the combustion heat generated at this time. Piece. Thereafter, the obtained agglomerate is pulverized and recovered by granulation & into a finished sinter composed of a mass of 5. 〇 mm or more 312 / invention specification (supplement) / 96-01 / 95140218 5 1329677. In the above manufacturing process, first, the surface of the layer is ignited by the ignition furnace. The charcoal charged in the layer is burned by the action of the attracting gas attracted to the lower portion from the top of the packed layer, and the combustion gradually proceeds to the lower layer and travels forward as the trolley 8 moves. At the same time as the progress of the combustion, the moisture of the sintered raw material particles in the charged layer evaporates due to the heat generated by the combustion of the carbon material, but is attracted to the lower side and is concentrated to be wetted under the temperature In the sintering raw materials. When the water concentration is increased to a certain extent or more, since the water fills the flow path of the suction gas (i.e., the gap between the raw material particles), the ventilation resistance increases. Further, the venting resistance is also increased in the molten portion necessary for the sinter reaction. The production of sinter (t/hr) is usually determined by the sintering productivity (t/hr · m2) x sintering machine area (m2). That is, the variation in the amount of production depends on the machine width and length of the sintering machine, the thickness of the raw material accumulation layer (loading layer thickness), the bulk density of the sintered raw material, the sintering (combustion) time, the yield, and the like. In order to increase the production amount of the sintered φ ore, the following method is considered to be effective, that is, to improve the air permeability (pressure loss) of the packed layer to shorten the sintering time; or to increase the cold rolling strength of the sintered block before the crushing to make the good The method of increasing the rate, etc. Figure 2 is a graph showing the distribution of pressure loss and temperature in the packed layer. The temperature profile of Fig. 2 shows the combustion (flame) front line moving in the loading layer, which is about 4 mm on the trolley in the thickness direction of the loading layer. At this time, the pressure loss is distributed in the wet zone of about 6〇%, and the combustion melt is 40%. Figure 3 shows the temperature of the intrusion layer when the sintered ore is produced at low production and low production. ) /96-01/95140218 6 1329677 degrees: layout. The temperature is maintained at the beginning of the melting of the raw material particles 2 〇 (the same period of the rc above the holding period of the dish, expressed as t 低 in low production, expressed in h when the production is important.) In high production, it must be Increasing the speed of the trolley, so the high temperature zone holding time t2 at this time is shorter than the high temperature zone during low production -= holding time t1. Since the time of keeping at high temperature becomes shorter, the firing is not charged. The second 'causes the cold casting strength of the sintered ore. Lowering, causing a decrease in yield. Therefore, in order to increase the production capacity of strontium ore, it is effective to use a certain method to increase the strength of the sintered block, that is, to increase the cold rolling strength of the sintered ore and to maintain the yield. Further, for the sinter cold rolling strength, SI (Shatter Index) and TI (TumMer Index) are used. Figure 4 (a) shows the sintering progress of the loading layer on the sintering machine trolley. Principle, Fig. 400 shows the temperature distribution of the sintering process in the packed layer, and Fig. 4(c) shows the yield distribution of the sintered block. As can be seen from Fig. 4(b), the upper portion of the layer (sintered layer) is harder to rise in temperature than the lower layer portion, and the high temperature region holding time is shortened. Therefore, on the packed layer, the combustion-spinning reaction (sintering reaction) is insufficient, as shown by _ 4 (c), since the strength of the sintered block is lowered, the yield is not improved and the productivity is lowered. The tendency. - Conventionally, a method has been proposed which is useful for maintaining the upper portion of the packed layer at a high temperature. =Special = Kai Zhao 48-Deleted No. 2 bulletin reveals that when the front of the ignition furnace is blown into the dryness of the 'sexual teaching I#, ..., the second is blown into the flammable gas. The material stem, so the formation of more than 1380 temperature in the sintered layer, so can not obtain sufficient cold expansion strength, yield improvement: 312 / invention manual (supplement) / 96-01/95140218 7 1329677 effect. Further, the inflammable gas is blown in the rear side of the ignition furnace for 〇 minute to 2 minutes, and the igniting of the flammable gas causes a high risk of a large fire, and the technique lacking in practicality has not reached the practical level. Further, Japanese Laid-Open Patent Publication No. Sho 55-18585 discloses a technique in which a hood is disposed above the loading layer in order to achieve a high temperature in the charging layer of the sintering raw material, and the hood is passed through the hood. Mixing air with coke oven gas • The gas is blown into the rear of the ignition furnace. The temperature in the sintered layer is such that the temperature exceeds 1350 C, so that the above-described blowing effect is not obtained, and the combustible gas mixture is ignited, which is dangerous to a large fire, and thus has not been put into practical use. Further, Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. In this method, the risk of a large fire is caused by blowing a flammable gas in a state where a flame remains on the surface, and the width of the sintered belt is not high; i is thick enough (about 15 or less), so that the effect cannot be fully generated. . Further advancement - Because there are a large number of low melting point solvents, excessive melting occurs in the upper layer to block the pores of the air flow path. Due to the deterioration of the gas, the productivity is reduced, so the technology has not been used yet. As described above, the conventional techniques proposed so far have not been put into practical use. Therefore, it is urgent to explore the conditions for the economic establishment. In the U-quality adjustment of sinter, it is important to adjust the temperature at which the combustion reaches the temperature and the holding time of the high-temperature region. The quality of the sinter is determined by the same factor. The Japanese patent special opening-- No. 312 / invention specification (supplement V96*01/95140218 is to use the if = no method to make the gaseous fuel burn on the surface of the loading layer.) / The upper part of the sintering step in the first half of the sintering step The second method of this method has the following problems: the gas fuel concentration is high, and thus the amount of the second gas (oxygen) of the hawthorn is insufficient, which may cause the combustion of the coffin (coke) of the sintering raw material to be lowered, thereby failing to achieve the quality of the sintered ore. Japanese Patent Laid-Open No. 55-18585* discloses a square 糸~糸: a flue hood is provided to supply combustion with gas and flammable gas, thereby: a method of serving more 'temperature, however The method also causes insufficient heat. The second method also has the following problem: in the high temperature zone, the coke combustion m _ gas is consumed by the combustion of the flammable gas, so the combustion of the coke is slow, resulting in sintering time. Extend. In the method disclosed in Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. The combustion degree is increased, but the aeration property of the combustion air is lowered because the low melting point molten material and the powder are blown together. [Invention] The present invention aims to provide a method for producing sintered ore and a method for realizing palladium. In the sintering machine, the method for producing the sintered ore is a lower suction type, and the material of the junction is not deteriorated, and the high-yield sintered ore is produced at a high yield. The invention provides a method for manufacturing a sintered ore having the following steps: loading step, in a trolley for circulating movement, containing a sintering raw material containing a powder ore and a charcoal 3127 invention specification (supplement)/96-01/95140218 9 1329677 a charging layer containing a carbon material formed on the trolley; an ignition step of igniting the carbon material charged on the surface of the layer in the ignition furnace; a firing step through the bellows disposed under the trolley Attracting air, burning the carbon material in the layer, and generating the agglomerate by using the generated heat of combustion; and the step of burning the fuel in the milk fuel step to supply the gas fuel diluted to the lower limit of the lower combustion concentration The gaseous fuel is combusted in the charging layer. The gas fuel burning step preferably includes an operation of supplying a gaseous fuel diluted to a lower concentration of combustion below the loading layer to cause the gaseous fuel to be in the loading layer. Burning, and adjusting the highest arrival/dish f in the loading layer, or the high temperature region holding time in the loading layer, or the maximum reaching temperature and the high temperature region holding time in the loading layer. The adjustment of the highest reaching temperature in the in-layer is preferred. (A) The gaseous fuel diluted to the lower limit of the combustion lower limit is supplied above the self-assembled layer, and the highest reaching temperature in the packed layer is adjusted. (B) The gas fuel diluted to the lower limit of the combustion limit is supplied above the self-assembled layer, and the amount of the carbon material in the sintered raw material is adjusted, thereby adjusting the maximum reaching temperature in the charged layer. (C) The gas fuel diluted to the lower limit of the combustion lower limit is supplied from above the charging layer and the supply amount of the gaseous fuel is adjusted to adjust the maximum reaching temperature. Supplying the amount of carbon in the sintering raw material and the amount of gaseous fuel supplied to the gas below the concentration below the lower limit of the combustion concentration.

312/發明說明書(補件)/96-0丨/95140218 L 1329677 藉此調整上述最高到達溫度。 # 2 1 9述(A) (D)中,較理想為,將上述最高到達溫度調 整為 1205°c 〜135(Tc。 以如下態樣來實施上诚驴 思 _ 呔裝入層内之尚溫區域保持時間 <調整較佳。 =自裝入層之上方供給稀釋成燃燒下限濃度以下之氣 …、料’調整裝人層内之高溫區域保持時間。 自裝人層之上方供給稀釋錢燒下限濃度以下之氣 之Γ/,且根據燒結原料中之炭材量來調整上述氣體燃料 /辰又’並且調整|人層内之高溫區域保持時間。 述氣體燃料燃燒步驟較佳為,包含以如下態樣來 調整燃燒、溶融帶之形態。 許=自裝人層之上方供給稀釋成燃燒下限濃度以下之氣 體燃料,調整燃燒、熔融帶之形態。 二I自裝入層之上方供給稀釋成燃燒下限濃度以下之氣 之二長燃燒、熔融帶之高溫保持時間,調整燒結礦 之冷延強度。 自裝入層之上方供給稀釋成燃燒下限濃度以下之氣 以使至少其一部分以維持未燃燒之狀態而到達上 述裝入層中之燃燒、熔融帶,調整燃燒、熔融帶之形離。 ’調節燃燒、炫融帶域之高度方向之厚度及/或台 卓移動方向之寬度。 =步’關於氣體燃料之供給位置,較佳為,以如下 態樣來實施上述氣體燃料燃燒步驟。 312/發明說明書(補件)/96_〇丨/95丨4〇2】8 11 1329677 (a) 自裝入層之上方供給稀釋成燃燒下限濃度以下之氣 體燃料’使上述氣體燃料於裝入層内燃燒,且調整上述氣 體燃料對裝入層之供給位置。 (b) 於點火爐後之位置處,自裝入層之上方供給稀釋成 燃燒下限濃度以下之氣體燃料,使上述氣體燃料於裝入層 内燃燒。 (c) 於燃燒、炫融帶之厚度為15 mm以上之區域中,供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 •於裝入層内燃燒。 (d) 於燃燒前線到達表層下1〇〇 mm之位置後,供給稀釋 成燃燒下限濃度以下之氣體燃料,使上述氣體燃料於裝入 層内燃燒。更佳為,於燃燒前線到達表層下200 mm之位 置後’供給具有燃燒下限濃度以下之氣體燃料。 (e) 於該裝入層之兩側壁附近,供給稀釋成燃燒下限濃 度以下之氣體燃料,使上述氣體燃料於裝入層内燃燒。 •⑴於燒結機長度方向上,自裝入詹之上方供給稀釋成 燃燒下限濃度以下之氣體燃料’使上述氣體燃料於裝入層 内燃燒’且調整燒結礦之冷延強度。 .上述氣體燃料較佳為,濃度稀釋成燃燒下限濃度之75% 、下 、上之可燃性氣體。更佳為,濃度稀釋成舞燒 下限濃度之咖以下且2%以上之可燃性氣體,尤 ^稀釋成燃燒下限濃度之25%以下且2%以上之可燃性氣 上述氣體燃料較佳為,選自由高爐氣體、焦爐氣體、高 312/發明說明書(補件)/96-〇1/9514〇218 I329677 爐與焦爐混合氣體、丙烷氣體、天然氣以及甲烷氣體所組 成之群組中之至少一種氣體。 更進一步’本發明提供燒結機,其具備循環移動之台 車、配設於上述台車之下方之吸引用風箱、用以向台車上 供給燒結原料上之原料供給裝置、以及用以對燒結原料中 之厌材進行點火之點火爐,該燒結機之特徵在於:於上述 點火爐之下游側’配設有氣體燃料供給裝置,用以自裝入 _層之上方,將濃度已稀釋成燃燒下限濃度以下之氣體燃料 吹入到該裝入層中。 上述氣體燃料供給裝置較佳為’於點火爐下游側之燒結 機之機長方向上,至少配設一個以上。 上述氣體燃料供給裝置更佳為,於台車行進方向上,配 °又於自燃燒前線行進至表層下方之階段直至燒結完成之 間之位置處。 又,上述氣體燃料供給裝置較理想為,配設於側壁附近。 【實施方式】 本發月之燒、纟σ礦之製造方法具有裝入步驟、點火步驟、 燒成步驟以及氣體燃料燃燒步驟。上述裝入步驟包含下述 於循環移動之台車上裝人含有㈣石與炭材之燒結 使於台車上形成含有炭材之裝人層。上述點火步驟 點火爐t對裝人層表面之炭材進行點火之動作。上 二燒成步驟包含下述動作··通過配置於台車 ^空氣’使裝人層中之炭材燃燒,並且利 熱而生錢結塊。上述氣體燃料燃燒步错自裝入層之:方 312/發明說明書(補件)/96-01/95140218 13 供給稀釋成燃燒下限濃产 a /晨度M下之氣體燃料,使上述氣體燃 科於裝入層内婵燒。兮裔聛 ”,、現Μ乳體燃料燃燒步驟係本發明之特徵 二ίΐ'ΐ體燃料燃燒步驟中,上述氣體燃料較佳為,使 他二刀之3有濃度已稀釋至大氣中常溫下燃燒下限 展度之75%以下之可揪备μ ^ ”,、11軋體。上述氣體燃料更佳為,使312 / Invention Manual (supplement) / 96-0 / 95140218 L 1329677 Thereby to adjust the above maximum temperature. # 2 1 9 In (A) (D), it is preferable to adjust the above-mentioned maximum arrival temperature to 1205 ° c to 135 (Tc. The implementation is as follows: The temperature zone holding time < adjustment is better. = The gas is diluted to the lower limit of the combustion lower limit concentration from above the loading layer. The material 'adjusts the high temperature zone holding time in the loading layer. The dilution money is supplied above the manned layer. Burning the gas below the lower limit concentration, and adjusting the gas fuel according to the amount of the carbon material in the sintering raw material and adjusting the high temperature region holding time in the human layer. The gas fuel burning step preferably includes The shape of the combustion and the melting zone is adjusted in the following manner: 1. The gas fuel diluted to the lower limit of the combustion lower limit is supplied above the self-assembled layer to adjust the shape of the combustion and the melting zone. The second combustion of the gas below the lower limit of combustion concentration, the high temperature retention time of the molten zone, and the cold rolling strength of the sintered ore are adjusted. The gas diluted below the lower limit of combustion is supplied from above the packed bed to make at least a part thereof The combustion and melting zone in the above-mentioned charging layer are maintained in an unburned state, and the combustion and the melting zone are separated. 'Adjusting the thickness of the burning and the melting zone in the height direction and/or the width of the movement direction of the table. = Step ' Regarding the supply position of the gaseous fuel, it is preferred to carry out the above-described gas fuel combustion step in the following manner. 312 / Invention specification (supplement) / 96_〇丨/95丨4〇2] 8 11 1329677 (a) supplying a gaseous fuel diluted to a lower concentration below the combustion concentration from above the charging layer, causing the gaseous fuel to be burned in the charging layer, and adjusting the supply position of the gaseous fuel to the charging layer. (b) In the ignition furnace At the rear position, the gaseous fuel diluted to the lower limit of the combustion lower concentration is supplied from above the charging layer to cause the gaseous fuel to be burned in the charging layer. (c) In the region where the thickness of the burning zone is 15 mm or more. In the middle, the gas fuel diluted to the lower limit of the combustion lower concentration is supplied to cause the gas fuel to be burned in the charging layer. (d) After the combustion front reaches the position below the surface layer of 1 〇〇 mm, the supply is diluted to the lower combustion concentration. The gaseous fuel is used to cause the gaseous fuel to be burned in the charging layer. More preferably, after the combustion front reaches a position 200 mm below the surface layer, a gaseous fuel having a concentration lower than the lower limit of combustion is supplied. (e) at the loading layer In the vicinity of the two side walls, the gaseous fuel diluted to the lower limit of the combustion lower concentration is supplied to cause the gaseous fuel to be burned in the charging layer. (1) In the longitudinal direction of the sintering machine, it is supplied to the upper portion of the lower limit of combustion to be diluted below the lower limit of combustion. The gaseous fuel 'burns the gaseous fuel in the charging layer' and adjusts the cold rolling strength of the sintered ore. The gas fuel is preferably diluted to a concentration of 75% of the lower limit of combustion, and the lower and upper flammable gas. Preferably, the flammable gas which is diluted to a concentration lower than the concentration of the lower limit of the dance, and which is 2% or more, is diluted to 25% or less and 2% or more of the lower limit of the combustion concentration, and the gaseous fuel is preferably selected from the group consisting of Blast Furnace Gas, Coke Oven Gas, High 312/Invention Manual (Supplement)/96-〇1/9514〇218 I329677 Furnace and coke oven mixed gas, propane gas, natural gas and methane gas At least one gas of the group. Further, the present invention provides a sintering machine including a cycle moving trolley, a suction bellows disposed below the trolley, a raw material supply device for supplying a sintering raw material to the trolley, and a material for sintering the raw material. An ignition furnace for igniting, wherein the sintering machine is characterized in that: a gas fuel supply device is disposed on the downstream side of the ignition furnace for self-loading above the layer, and the concentration is diluted to a lower combustion concentration The following gaseous fuel is blown into the loading layer. Preferably, the gas fuel supply device is disposed at least one or more in the direction of the length of the sintering machine on the downstream side of the ignition furnace. More preferably, the gas fuel supply device is disposed at a position in the traveling direction of the trolley from a stage from the front of the combustion to a stage below the surface layer until the completion of sintering. Further, it is preferable that the gas fuel supply device is disposed in the vicinity of the side wall. [Embodiment] The manufacturing method of the sinter and 纟σ ore of the present month has a charging step, an igniting step, a firing step, and a gas fuel burning step. The above-described loading step includes the following sintering of the (four) stone and the carbon material on the trolley which is cyclically moved to form a charging layer containing the carbon material on the trolley. In the above ignition step, the ignition furnace t ignites the carbon material on the surface of the charging layer. The second firing step includes the following operations: • The carbon material in the charging layer is burned by being placed in the trolley ^air, and the money is agglomerated by heat. The gas fuel combustion step is self-loaded into the layer: side 312 / invention specification (supplement) / 96-01 / 95140218 13 supply of gas fuel diluted to a lower combustion limit and a / morning M, so that the gas burning Simmer in the loading layer.兮 聛 , , , , Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ Μ ΐ ΐ ΐ ΐ ΐ ΐ ΐ ΐ ΐ ΐ ΐ The sintered lower limit of 75% of the combustion can be prepared for μ ^ ”, 11 rolling bodies. The above gaseous fuel is better, so that

用稀釋至60%以下之可•揪科$ μ L 了燃性虱體,尤佳為,使用濃度稀釋 /。以下之可燃性氣體。之所以使用稀釋至燃燒下限濃 a、下之75%以下之可燃性氣體較佳,其理由具有下述兩 個。 U)向襄人詹上部供給上述氣體燃料,有時可能導致爆 ί*生燃燒’故至少於常溫下’即使存在火種,仍處於不會 燃燒之狀態。 & (b)於燒結機上(裝入層並未完全燃燒,以維持未燃 燒=狀態而到達位於燒結機下游側之電氣集塵器等時,亦 籲;儿全不可月匕在電氣集I器放電下燃燒之狀態,即於燃燒 下限濃度以下之條件下進行。 再者,如下所述,該氣體燃料必須使用濃度稀釋後者, 以便不會導致燒結原料中總炭材(固體燃料+氣體燃料) -之燃燒所須之空氣(氧氣)不足而引起燃燒不足。上述氣體 燃料較佳為’濃度稀釋成燃燒下限濃度之2%以上之可燃 生氣體。若濃度為2%以上,則燒結礦之強度與良率將進 步得到改善。又’根據炭材量(固體燃料)而調整氣體燃 料之濃度。更進一步,如下所述,藉由稀釋氣體燃料而可 312/^Μ*(Μίφ)/96.〇1/9514〇21 14 1329677 調整於裝人層中特定區域位置之燃燒。 ^本發明之燒結礦之製造方法中在對 f後’將稀釋後之氣體燃料供給至裝入層。儘; 、:正後方之位置處供給稀釋氣體燃料 ^燃燒,對燒結層並未造成任何影響。較佳為,於;入 形成燒結塊層後,將稀釋後之氣體 ^ 裴入層。右有形成燒結塊層,則可於任音位置 f供給稀釋後之氣體燃料。之所以於形成燒結塊層:後供 給稀釋後之氣體燃料,其理由如下。 思曰之後供 1裝人層之上部仍未生成燒結塊之狀態下供給該 现體⑽,則於職人層上具有產生爆炸性職之危險。 b)乳體燃料之供給係以有必要提高良率之部分為對 °即’有效的是供給至欲使燒結礦強度提高之部分。 為了調整裝入層最高到達溫度或者高溫區域保持時間 之任-方,較佳為,上述燃燒、熔融帶之厚度於滿足下述 之條件下進行稀釋氣體燃料之供給:至少為15觸以上, 較佳為20 mm以上,更佳為30 mm以上。若未達15 mm, 則隨著通過燒結層(燒結塊)所吸弓丨的大氣(大氣與氣體燃 料之混合氣體)之冷卻,即使供給氣體燃料,亦不會使燃 燒、熔融帶之厚度擴大,故氣體燃料供給之效果不充分。 若於上述燃燒、熔融帶之厚度為15随以上、較佳為2〇麵 以上、更佳為30 mm以上之階段,對上述氣體燃料進行稀 釋並供給,則燃燒、熔融帶之厚度將大範圍擴大,且高溫 區域保持時間延長。 M2/發0月說明書(補件)解〇1/9514〇2 i 8 15 1329677 再者,上述燃燒、熔融帶之厚度例如可使用附帶透明石 英製固之丑型管狀试驗鋼來確認,有利於決定上述稀釋氣 體燃料的供給位置。 又,較佳為,於燃燒前線下降至表層下方,且燃燒、熔 融帶下降至距離表層l〇〇 mm以上、較佳為2〇〇随以上之 位置處,進行上述稀釋後之氣體燃料之供給。即,較佳為, 以中、下層部區域為對象而供給稀釋後之氣體燃料。例 如,使稀釋氣體燃料於上述裝入層中生成燒結塊後之裝入 層中之中、下層部,即燃燒前線自表層移動100 mm後之 I1白(以於未燃燒之狀態下到達該區域之方式)開始燃 燒,以此方式供給稀釋氣體燃料。其理由在於,若於下降 100 _、以上之位置,則受到通過燒結層所吸引之大氣造 j之冷部影響減輕,使燃燒、熔融帶之厚度擴大。更佳為, "下降2 0 0 mm以上,則受到大氣造成之冷卻影響解除, 使燃燒、·溶融帶之厚度擴大至30· α上。又,更佳為, 於良率下降顯著之側壁附近之寬度方向(於直行於台車行 進方向之f向)的兩端部,進行上述供給。 再者氣體燃料供給裝置亦依燒結機之規模而不同,例 如’於氣體燃料供給量為l,_m3/h〜5,G00m3(標準)/h、 約1.5萬噸/日,且機具 且機長為90 m之燒結機規模時,氣體燃 …、父佳為,配置於點火爐下游側之約5m以後之 位置處。 於本發明之製造方法中 較佳為,自於台車移動方 312/發明說明書(補件)/96叫/9514〇 上述稀釋氣體燃料之供給位置 向之點火爐出料側生成燒結塊 1329677 後、所謂燃燒前線行進至表層下方之位置(例如,於表層 下100腿以上’較佳為約⑽ΠΠΠ以下,產生氣體燃料; 燒之位置)直至燒結完成之間之i個位置以上之任音位 置。即’如上所述,此係指於燃燒前線移至裝入層之i層 下方之階段開始供給該氣體燃料,並且係指由於氣體燃料 之燃燒於裝入層内部發生,而且逐漸移至更下層,故無爆 炸危險,可進行安全之燒結操作。 料於製造方法中’向裝入層中供給稀釋氣體燃 '、日 所生成之燒結塊之再加熱。π,該氣體燃料 之供給具有如下意義:由於原本高溫區域保持時間短而容 易造成熱f不足,故針對燒結礦之冷延強度低之燒結塊, 與向該部分供給固體燃料相比,供給反應性高之氣體燃 料’可實現燃燒、熔融帶之再生及擴大,填補容易造成敎 量不足之該部分之燃燒熱。 … 又’於本發明之燒結礦之製造方法中,較佳為,使自點 火後之裝人層上部所供給之上述氣體燃料之至少一部 以維持未燃燒之狀態而吸引(導人)至燃燒、熔融帶,並且 置燃燒,以此方式供給。此係由於認為氣體燃料 Ό效果’即向裝入層中吹入氣體燃料之效果,不舒 響裝入層上部,而且使其影響厚度方向之 : ,融帶更加有效。其原因在於,若於易造成熱量不=高 :£域保持時間不足)之裝入層之上層部進行 供給,則將提供充分之燃燒熱,且可改善該部分之品質(燒 、.口強度)。而且,若使氣體燃料供給作用波及至中層部以 312/發明翻書(補件)/96-Gl/9514G218 17 / :之::帶:形等= 在果原本之燃燒、熔融帶上方形成再燃 大,可於不提高最高^達^/帶域之上下方向之寬度擴 持時間之延長,並且J 下,實現高溫區域保 結果引起穿入声人妒 台車速度而實現充分燒結。其 丨起穿入層全體之燒結塊之品質改善(冷延強度提 ^。’進—步使成品燒結礦之品質(冷延強度)與生產性提 於本發明中,第1转 係根據其供给之2 上述稀釋氣體燃料之供給, 整上:::用、效果影響裝入層中某處之觀點來調 ::供給位置,而且第2特徵為:根據固體燃料之量,於 以下:與上述燃料之供給-同,將裝入層内 ν達/皿度及尚溫區域保持時間調整為某種程度。 給至梦=轉μ,&佳為’當將上述稀釋氣體燃料供 、:、、:3入曰中時’不僅調整其供給之位置,而且調整燃 、二、=融帶本身之形態,進一步調整燃燒、熔融帶之最高 到達溫度及/或高溫區域保持時間。 ° 一般而言’隨著台車之移動,燃燒(火焰)前線逐漸 方且則方(下游側)擴大之過程中,點火後之裝入層之 燒、熔融帶之位置如圖4(a)所示而變化。而且,如圖4(b”) 所示,於燒結層内之燒結過程中之受熱歷程,於上層 層、下層各不相同,如圖所示,於上層至下層之間:古田 區域保持時間(約12〇(rc以上)大不相同。其結果,= 層形成如® 4(c)所示之良率分佈。即,表層部(上層 良率低’而於中層、下層方向上形成高良率分佈。‘此, 312/發明說明書(補件)/96·01/95140218 lg 1329677 f根據本發明方法,當供給上述氣體燃料時,燃燒、熔融 τ會向上下方向之厚度或範圍等擴大之方向上變化,其反 映出成品燒結礦之品質提高。而且,由於形成高良率分佈 之中層、下層可進一步調整高溫區域保持時間,故可 率更加提高。 藉由調整上述氣體燃料之供給位置,而可調整燃燒、熔 融帶之形態,即該帶域之高度方向之厚度及/或台'車移動 方向之寬度,並且可調整最高到達溫度及高溫區域保持時 間。該等調整使本發明之效果更進一步顯著,通過燃燒、 熔嘁帶之上下方向厚度之擴大及最高到達溫度、高溫區域 保持時間之調整,常可實現充分之燒成,因而有助於有效 提高成品燒結礦之冷延強度。 …又’於本發明中,向裴入層中供給上述氣體燃料,亦可 說係為了調整成品燒結礦全體之冷延強度。關於該方面, 吹入上述氣體燃料之目的原本在於提高燒結塊、更進一步 |燒、,Ό礦之冷延強度,尤其係通過氣體燃料供給位置之調 整、燒結原料滯留於燃燒、溶融帶之時間等高溫區域保持 時間之調整、以及最高到達溫度之調整,來使燒結礦之冷 延強度(shatter index,SI)達到75%以上至85%左右,較 佳為80%以上’更佳為90%以上。 該強度標準於本發明中較佳為,於考慮燒結原料令之炭 材量後(於使投入熱量固定之條件下),尤其可藉由調整上 述氣體燃料之濃度、供給量、吹入位置、以及吹入範圍而 廉價實現。再者’提高燒結礦之冷延強度於另一方面,有 312/發明說明書(補件)/96-01/95140218 , „ 1329677 時會導致通氣阻力增大及生產性降低,故於本發明中,上 述問題藉由調整最高到達溫度及高溫區域保持時間而消 除,結果使燒結礦之冷延強度提高。再者,當為利用實機 燒結機所製造之燒結礦時,上述冷延強度s丨值表示較鍋 試驗值更高10%〜15%之SI值。 於本發明之製造方法中,對台車移動方向上之上述氣體 燃料供給位置之調整,係以如何設置自裝入層中所生成之 鲁燒結塊至濕潤帶之間任意帶之燒結礦之冷延強度為基 準。為了該調整,本發明中較佳為,根據燒結原料中之炭 材1(固體燃料)來調整氣體燃料供給裝置之規模(大 小)、數夏、位置(離點火爐之距離)、氣體濃度,由此不 僅主要調整燃燒、熔融帶之大小(上下方向以及台車移動 方向之寬度),而且亦調整高溫到達溫度、高溫區域保持 時間,藉此,調整裝入層中所生成之燒結塊之強度。 =本發明之上述製造法中,氣體燃料之較佳構成為:使 _用高爐氣體、焦爐氣體、高爐與焦爐混合氣體、丙烷氣體、 天氣或甲烷、或者該等之混合氣體中之任一者。上述氣 體均3有燃燒成分,將其利用空氣等進行稀釋,用作濃度 '為燃燒下限濃度之約75%以下之氣體燃料。再者,氣體^ -料之稀釋除利用$氣以夕卜亦可利用惰性氣體進行稀釋: $性氣體與氧氣、惰減體與空氣、以及^氣與氧氣之也 合進行稀釋。 ’ 當實施本發明之燒結礦之製造方法時使用燒結機, 。燒結機係如下所述之下方吸引式DL(型帶式)燒結機: 312/發_ 明書(補件)/96-01/95140218 20 1329677 裝入層而循環移動之台車下方配設 =用風柏,於該台車上具備原料供給裝置,於該裝置 二ΓΓ向下游侧具備點火爐,並且於上述點火爐之 :二配設有氣體燃料供給裳置,用以自裝入層之上方 裝入層中吹入濃度稀釋成燃燒下限濃度以下之氣 明中,上述氣體燃料供給裝置之配設較佳為,以沿 者“機之寬度方向橫跨台車兩侧壁之方式而配設。上述 ,=料供給裝置之構成較料,配設有供給稀釋後之氣 體燃料之吹人排煙罩’或者於吹人排煙罩内,配設有供給 亂體燃料或者稀釋後之氣體燃料之吹入管,該吹入管呈狹 縫狀或者將吹入喷嘴排列設置成板狀。 再者,於點火爐下游侧且燃燒熔融帶於裝入層中行進過 程中之台車行進方向上之任意位置處,配設有一個以上之 上述氣體燃料供給裝置,並且向裝入層中供給上述氣體燃 #料較佳為,於對該裝入層甲之炭材進行點火後之位置處進 行供給。即,於點火爐之下游側、燃燒前線行進至表層下 方以後之任意位置處,配設有一個或者數個該裝置,且根 '擄調整作為目標之成品燒結礦之冷延強度之觀點,而調整 大小、位置、及數量❶又,較佳為:該氣體燃料供給裝置 配設於兩側壁附近之低良率部之位置處;上述氣體燃料使 用濃度稀釋成燃燒下限濃度之75%以下且2%以上之可燃 性氣體,更進一步,使用濃度稀釋成燃燒下限濃度之6〇% 以下且2%以上之可燃性氣體。 312/發明說明書(補件)/96-01/95140218 21 丄似677 由*以上4明’根據本發明,對於下方吸引式燒結機之操 作’藉由自裝人層之上方使用稀釋後之氣體燃料,而可使 其於作為裝入層内之目標之位置處燃燒,且於此情況下, 藉由調整稀釋氣體燃料之供給位置及燃燒時之最高到達 溫度、高溫區域保持時間,而可進行如下操作:不僅提高 易&成燃燒不足且燒結礦之冷延強度易降低的裝入層上 4之^ο、、Ό礦強度,而且提高裝入層之中層以下任意部分之 •,結礦強度。並且,於本發明中,可不使裝人層全體之通 氣性惡化,尤其通過調整於燃燒、熔融帶之反應,例如調 整該帶上下方向上之厚度及台車移動方向之寬度,來調整 任意位置處燒結塊之強度,故可良率佳且霉保高生產性地 製造燒結礦全體冷延強度高之成品燒結礦。並且,若使用 本發明之燒結機,可穩定進行上述燒結機之操作。 圖5表示本發明的燒結礦之製造裝置之一實施形態。本 發明並非僅限定於該例示之形態。用以吹人高爐氣體與焦 鲁爐氣體之混纟氣體(Μ氣體)等氣體燃料之氣體燃料供給裝 置(排煙罩)12 ’於點火爐1G之台車移動方向之下游侧裝 入層之上邊,僅配設有丨台。該氣體燃料供給裝置12包 -含使數個管狀氣體吹入喷嘴12a向下且於機寬方向上排 '列有數個之結構。上述數個管狀氣體吹入喷嘴12a以下述 方式而配設:、經由氣體燃料供給裝置12巾自未圖示之侧 壁上方覆蓋裝入層。自氣體燃料供給裝置12所供給之上 述Μ氣體,自裝入層之上方經由生成於表層之燒結塊,利 用台車8下方之風箱u之吸引力而吸引至裝入層之深部 312/發明說明書(補件)/96-01/95140218 „ ^29677 當以提高圖4(c)所示之良率低達_之區域 之良革為目的時,較佳為,將上述噴嘴 ^ 車兩側壁附近之位置處供給大量氣體燃料。-成可向台 使料供給裝412所供給之氣體燃料,例如可 氣體)、體.尚爐氣體(Β氣體)、焦爐氣體(c .2)、4氣體與焦爐氣體之混合氣體(Μ氣體)、丙院 3、天然氣(LNG)或甲烷、或者該等混 ::燃料亦可於另外獨立於點火爐,。之配管系統之:;二 =。X,亦可以如下方式構成··在與點火爐用燃.料配 用之配管上’尤其與稀釋氣體導人管共同配設, 乳體燃料之濃度稀釋調整為燃燒下限濃度以下後,將其連 接於通向點火爐10之氣體供給管(未圖示)之延長上:、 下表1表示本發明中所使用之各種氣體燃料各自之燃 燒下限濃度、以及吹入濃度上限(75%、6〇%、2 俨 濃度例。 孔體 瞻例如,對於丙烷氣體,燃燒下限濃度為2 2體積%,稀 釋成75%之吹入氣體濃度上限為1:7體積%,稀釋成6〇% 之吹入氣體濃度上限為1.3體積%,稀釋成25%之吹入氣 ‘體濃度為〇. 4體積%。該吹入效果開始顯現之濃度,即, -稀釋後之吹入氣體濃度下限為0.05體積%。因此,較佳範 圍如下所述。 較佳範圍(1) : 2. 2體積%〜〇. 〇5體積% 較佳範圍(2) : 1.7體積%〜〇. 〇5體積% 較佳範圍(3): 1.3體積%〜〇. 〇5體積% 312/發明說明書(補件)/96-01/95140218 23 1329677 .較佳範圍⑷:0.4體·〜〇〇5體積% 於C氣體中,燃燒下限 之吹入氣體濃度上限為3 8 :二5'體積%’稀釋成75% ^ ^ L山 .8體積%,稀釋成60%之吹入氣 體濃度上限為3.0體積%,鞴锩劣9以 心人入轧 0 9 r^〇/ ^ 稀釋成25%之吹入氣體濃度為Use a dilution of 60% or less of the 揪 揪 $ μ μ μ $ 了 了 了 了 了 了 了 。 。 。 。 。 。 。 。 。 。 The following flammable gases. The reason why it is preferable to use a flammable gas diluted to a lower limit of the combustion lower limit and 75% or less is the following two reasons. U) Supplying the above-mentioned gaseous fuel to the upper part of the monk, sometimes causing the explosion to burn, so at least at normal temperature, even if there is a kind of fire, it is still in a state of not burning. & (b) On the sintering machine (when the loading layer is not completely burned to maintain the unburned = state and reaches the electric dust collector located on the downstream side of the sintering machine, etc. The state of combustion under the discharge of the I, that is, under the condition of the lower limit of the combustion limit. Further, as described below, the gaseous fuel must be diluted with the concentration so as not to cause the total carbon in the sintered raw material (solid fuel + gas) Fuel) - The air (oxygen) required for combustion is insufficient to cause insufficient combustion. The gas fuel is preferably a combustible gas whose concentration is diluted to 2% or more of the lower limit of combustion concentration. If the concentration is 2% or more, the sintered ore is sintered. The strength and yield will be improved. In addition, the concentration of the gaseous fuel will be adjusted according to the amount of carbon (solid fuel). Further, as described below, by diluting the gaseous fuel, it can be 312/^Μ*(Μίφ)/ 96. 〇 1/9514 〇 21 14 1329677 Adjusting the combustion at a specific area in the loading layer. ^ In the manufacturing method of the sinter of the present invention, the diluted gaseous fuel is supplied to the charging layer after f. ; : The supply of the dilute gas fuel at the position directly behind is not affected by the sintered layer. Preferably, after the formation of the sintered block layer, the diluted gas is poured into the layer. In the layer, the diluted gaseous fuel can be supplied at the arbitrary sound position f. The reason why the sintered agglomerate layer is formed after the dilution of the gaseous fuel is as follows is as follows: After the thinking, the upper portion of the 1 human layer is still not sintered. The supply of the present body (10) in the state of the block has the risk of exploding on the employee's level. b) The supply of the milk fuel is based on the necessity to increase the yield. The part of the sinter strength improvement. In order to adjust the maximum temperature of the loading layer or the holding time of the high temperature region, it is preferable that the thickness of the combustion and the melting zone be supplied to the diluted gaseous fuel under the following conditions: at least 15 touches or more. Preferably, it is 20 mm or more, more preferably 30 mm or more. If it is less than 15 mm, the thickness of the combustion and melting zone will not increase even if the gaseous fuel is supplied by the atmosphere (the mixture of the atmosphere and the gaseous fuel) which is sucked by the sintered layer (agglomerate). Therefore, the effect of gas fuel supply is insufficient. When the thickness of the combustion and the melting zone is 15 or more, preferably 2 〇 or more, and more preferably 30 mm or more, the gas fuel is diluted and supplied, and the thickness of the combustion and the melting zone is wide. Expanded, and the high temperature area stays longer. M2/0 month manual (supplement) solution 1/9514〇2 i 8 15 1329677 Furthermore, the thickness of the above-mentioned combustion and melting zone can be confirmed, for example, by using an ugly tubular test steel with transparent quartz. The supply position of the above diluted gaseous fuel is determined. Further, it is preferable that the gas line is supplied to the lower portion of the surface layer before the combustion, and the combustion and the melting zone are lowered to a distance of more than 10 mm from the surface layer, preferably 2 Å or more, to supply the diluted gaseous fuel. . That is, it is preferable to supply the diluted gaseous fuel to the middle and lower layer regions. For example, the diluted gas fuel is placed in the loading layer after the agglomerate is formed in the above-mentioned charging layer, and the lower layer portion, that is, the I1 white after the burning front line moves 100 mm from the surface layer (to reach the region in an unburned state). In this way, combustion is started, and the diluted gaseous fuel is supplied in this manner. The reason for this is that if the position is lowered by 100 _ or more, the influence of the cold portion which is attracted by the sintered layer is reduced, and the thickness of the combustion and the melting zone is increased. More preferably, if the temperature drops by more than 200 mm, the cooling effect caused by the atmosphere is released, and the thickness of the combustion and melting zone is increased to 30·α. Further, it is more preferable that the supply is performed at both end portions in the width direction (in the f direction straight ahead in the traveling direction of the carriage) in the vicinity of the side wall where the yield is significantly lowered. Furthermore, the gas fuel supply device also differs depending on the scale of the sintering machine, for example, 'the gas fuel supply amount is l, _m3/h~5, G00m3 (standard)/h, about 15,000 tons/day, and the machine tool has a length of At the scale of the 90 m sintering machine, the gas is burned, and the father is placed at a position about 5 m after the downstream side of the ignition furnace. Preferably, in the manufacturing method of the present invention, after the trolley moving portion 312 / invention specification (supplement) / 96 call / 9514 〇 the supply position of the diluted gaseous fuel is generated to generate a sintered block 1329677 to the discharge side of the ignition furnace, The position where the front line of the combustion travels to the lower surface of the surface layer (for example, at least 100 legs or more below the surface layer is preferably about (10) , or less, and the gas fuel is generated; the burning position) is at any position above the i position between the completion of sintering. That is, as described above, this refers to the supply of the gaseous fuel at the stage where the combustion front is moved below the i-layer of the charging layer, and refers to the occurrence of combustion of the gaseous fuel inside the charging layer, and gradually moves to the lower layer. Therefore, there is no danger of explosion, and a safe sintering operation can be performed. In the manufacturing method, the reheating of the agglomerates generated by the "diluted gas burning into the packed bed" and the daily generation is carried out. π, the supply of the gaseous fuel has the following meaning: since the original high temperature region has a short holding time and is likely to cause insufficient heat f, the sintering block having a low cold rolling strength for the sintered ore is supplied to the solid fuel in comparison with the supply of the solid fuel to the portion. The high-gas gas fuel can realize the regeneration and expansion of combustion and melting zone, and fills in the combustion heat of this part which is easy to cause insufficient amount of enthalpy. In the method for producing a sintered ore according to the present invention, it is preferable that at least one portion of the gaseous fuel supplied from the upper portion of the charging layer after the ignition is sucked (introduced) to maintain the unburned state. It is burned, melted, and burned, and supplied in this manner. This is because the effect of the gas fuel enthalpy is considered to be the effect of blowing the gaseous fuel into the charging layer, which does not relax the upper portion of the layer and affects the thickness direction: the melting band is more effective. The reason is that if the supply is performed on the upper layer of the loading layer which is likely to cause heat not to be high: the retention time of the domain is insufficient, sufficient combustion heat is supplied, and the quality of the portion (burning, mouth strength) can be improved. ). Further, if the gas fuel supply action is applied to the middle portion to 312/inventive book (supplement)/96-Gl/9514G218 17 / ::: belt: shape, etc. = re-ignition is formed above the original burning and melting zone Large, can not increase the maximum length of the ^ / ^ band above the width of the extension of the extension of the time, and J, the realization of the high temperature area to ensure that the speed of the sound of the people into the trolley to achieve full sintering. It improves the quality of the agglomerate of the entire penetration layer (cold strength is improved.) The quality of the finished sinter (cold strength) and productivity are improved in the present invention, and the first transformation system is based on Supply 2 The supply of the above-mentioned dilute gas fuel is adjusted as follows: the use position and the effect of affecting somewhere in the layer: the supply position, and the second characteristic is: according to the amount of solid fuel, the following: The supply of the above-mentioned fuel is the same, and the holding time of the ν up/dish and the temperature range in the loading layer is adjusted to some extent. To the dream = turn μ, & good is 'When the above diluted gas fuel is supplied,: ,: 3 when entering the raft, 'not only adjust the position of the supply, but also adjust the shape of the fuel, the second, the fusion zone itself, and further adjust the maximum temperature of the combustion, the melting zone and/or the holding time of the high temperature zone.言 'With the movement of the trolley, the burning (flame) front line gradually increases and the square (downstream side) expands. The position of the burning and melting zone of the charged layer after ignition changes as shown in Fig. 4(a). And, as shown in Figure 4(b)), in sintering The heating process in the sintering process is different in the upper layer and the lower layer, as shown in the figure, between the upper layer and the lower layer: the Gutian area retention time (about 12 〇 (rc or more) is very different. The result, = The layer forms a yield distribution as shown in ® 4(c), that is, the surface layer portion (lower layer yield is lower) and a high yield distribution is formed in the middle layer and the lower layer direction. 'This, 312/invention specification (supplement)/96 01/95140218 lg 1329677 f According to the method of the present invention, when the gaseous fuel is supplied, the combustion and melting τ change in the direction in which the thickness or range of the upward and downward directions is expanded, which reflects the improvement in the quality of the finished sintered ore. Since the middle layer and the lower layer of the high-yield distribution can further adjust the holding time of the high-temperature region, the rate can be further improved. By adjusting the supply position of the gas fuel, the shape of the combustion and the melting zone can be adjusted, that is, the height direction of the band. The thickness and/or the width of the moving direction of the table, and the maximum reaching temperature and the holding time of the high temperature region can be adjusted. These adjustments make the effect of the present invention even more remarkable. The expansion of the upper and lower thickness of the burning and melting zone and the adjustment of the maximum temperature and the holding time of the high temperature region can often achieve sufficient firing, thereby contributing to the effective improvement of the cold rolling strength of the finished sintered ore. In the invention, the supply of the gaseous fuel to the intrusion layer may be performed to adjust the cold rolling strength of the entire sintered ore. In this respect, the purpose of injecting the gaseous fuel is to increase the sintered mass and further burn, The cold rolling strength of the antimony ore, especially the adjustment of the gas fuel supply position, the retention time of the high temperature region such as the time when the sintering raw material stays in the combustion, the melting zone, and the adjustment of the maximum reaching temperature, so as to cool the sintered ore. The shatter index (SI) is about 75% or more to about 85%, preferably 80% or more, and more preferably 90% or more. In the present invention, it is preferable to adjust the concentration of the gaseous fuel, the supply amount, the blowing position, and the like, in consideration of the amount of the carbon material to be sintered (in the case where the input heat is fixed). And it is cheap to implement by blowing in the range. Furthermore, 'increasing the cold rolling strength of the sintered ore, on the other hand, has 312/invention specification (supplement)/96-01/95140218, „1329677, which causes an increase in ventilation resistance and a decrease in productivity, so in the present invention The above problem is eliminated by adjusting the maximum reaching temperature and the holding time of the high temperature region, and as a result, the cold rolling strength of the sintered ore is improved. Further, when the sintered ore produced by the actual sintering machine is used, the above-mentioned cold rolling strength 丨The value indicates an SI value that is 10% to 15% higher than the pot test value. In the manufacturing method of the present invention, the adjustment of the gas fuel supply position in the moving direction of the trolley is generated by how to set the self-loading layer. For the adjustment, in the present invention, it is preferred to adjust the gaseous fuel supply device according to the carbon material 1 (solid fuel) in the sintering raw material. The size (size), the number of summers, the position (distance from the ignition furnace), and the gas concentration, thereby not only mainly adjusting the size of the combustion and the melting zone (the vertical direction and the width of the trolley moving direction), but The high temperature reaching temperature and the high temperature region holding time are also adjusted, thereby adjusting the strength of the sintered block formed in the charged layer. In the above manufacturing method of the present invention, the gas fuel is preferably configured to: use blast furnace gas, Any one of a coke oven gas, a mixed gas of a blast furnace and a coke oven, propane gas, weather or methane, or a mixed gas thereof. The gas 3 has a combustion component, and is diluted with air or the like to be used as a concentration' It is a gaseous fuel that burns less than about 75% of the lower concentration. Further, the dilution of the gas can be diluted with an inert gas by using: gas: gas and oxygen, inertia and air, and ^Gas and oxygen are also combined for dilution. 'When the method of manufacturing the sintered ore of the present invention is carried out, a sintering machine is used. The sintering machine is a lower suction type DL (belt type) sintering machine as described below: 312/发_ Mingshu (supplement)/96-01/95140218 20 1329677 Underneath the trolley that is loaded into the layer and circulated and moved = Use the cypress, the raw material supply device is provided on the trolley, and the ignition furnace is provided on the downstream side of the device , and And in the above-mentioned ignition furnace: two gas fuel supply skirts are arranged for loading the gas into the layer above the loading layer and diluting into a concentration lower than the lower limit of combustion concentration, the gas fuel supply device Preferably, it is disposed so as to straddle the two side walls of the trolley along the width direction of the machine. In the above, the composition of the material supply device is relatively good, and a blower hood for supplying the diluted gaseous fuel is disposed or disposed in the blower hood, and is provided with a chaotic fuel or a diluted gaseous fuel. The tube is blown, and the blowing tube has a slit shape or the blowing nozzles are arranged in a plate shape. Further, at any position on the downstream side of the ignition furnace and in the traveling direction of the trolley during the traveling of the combustion melting zone in the loading layer, one or more of the above-mentioned gaseous fuel supply devices are disposed, and the above-mentioned gas supply means is supplied to the loading layer Preferably, the gas fuel is supplied at a position after the carbon material charged in the layer is ignited. That is, at the downstream side of the ignition furnace and at any position after the combustion front line travels below the surface layer, one or several devices are disposed, and the root '掳 adjusts the viewpoint of the cold rolling strength of the target sintered ore. Preferably, the gas fuel supply device is disposed at a position of a low-yield portion near the two side walls; and the gas fuel is diluted to a concentration lower than 75% of the lower limit of combustion and 2 More than or equal to flammable gas, the flammable gas is diluted to a concentration lower than or equal to 6% by mass and 2% or more. 312 / invention specification (supplement) / 96-01 / 95140218 21 丄 677 from * above 4 'in accordance with the present invention, for the operation of the lower suction sintering machine' by using the diluted gas above the self-installed layer The fuel can be burned at a position as a target in the charging layer, and in this case, by adjusting the supply position of the diluted gaseous fuel, the maximum reaching temperature at the time of combustion, and the holding time of the high temperature region, The following operations: not only improve the easy & burn-in and the chilled strength of the sinter is easy to reduce the strength of the loading layer on the loading layer, and increase the strength of the layer below the layer, the ore strength. Further, in the present invention, it is possible to improve the air permeability of the entire manned layer, and to adjust the position of the belt in the vertical direction and the width of the moving direction of the trolley, for example, by adjusting the reaction of the combustion and the melting zone, for example, by adjusting the width of the belt in the vertical direction of the belt. Since the strength of the agglomerate is good, the finished sintered ore having a high cold rolling strength of the sintered ore can be produced with good yield and high productivity. Further, if the sintering machine of the present invention is used, the operation of the above sintering machine can be stably performed. Fig. 5 shows an embodiment of the apparatus for producing a sintered ore according to the present invention. The invention is not limited to the illustrated embodiment. A gas fuel supply device (exhaust hood) 12' for blowing a gaseous fuel such as a blast furnace gas and a coke oven gas (gas) gas is placed on the downstream side of the moving direction of the ignition furnace 1G. It is only equipped with a balcony. The gas fuel supply device 12 includes a structure in which a plurality of tubular gases are blown into the nozzle 12a downward and arranged in the machine width direction. The plurality of tubular gas injection nozzles 12a are disposed so as to cover the charging layer from above the side wall (not shown) via the gas fuel supply device 12. The helium gas supplied from the gas fuel supply device 12 is sucked from the upper portion of the loading layer through the agglomerates formed on the surface layer to the deep portion 312 of the loading layer by the suction force of the bellows under the trolley 8 (supplement)/96-01/95140218 „ ^29677 When it is intended to improve the quality of the area shown in Figure 4(c), it is preferable to use the above nozzles near the two side walls of the vehicle. A large amount of gaseous fuel is supplied at a position. - a gaseous fuel that can be supplied to the stage supply 412, such as a gas, a gas, a gas, a coke oven gas (c. 2), a gas, and a gas. The mixed gas of coke oven gas (helium gas), propylene compound 3, natural gas (LNG) or methane, or the like: the fuel may be separately independent of the ignition furnace, the piping system:; two =. X, It can also be configured as follows: • It is disposed in conjunction with a diluent gas guide tube in a pipe for use with a fuel for ignition furnace, and the concentration of the emulsion fuel is adjusted to be equal to or lower than the lower limit of combustion concentration, and then connected thereto. The extension of the gas supply pipe (not shown) to the ignition furnace 10: Table 1 below shows the lower limit of the combustion limit and the upper limit of the blowing concentration of each of the various gaseous fuels used in the present invention (75%, 6〇%, 2俨 concentration). For example, for propane gas, the lower limit of combustion is 2 2 vol%, the upper limit of the blown gas concentration diluted to 75% is 1:7 vol%, the upper limit of the blown gas concentration diluted to 6 〇% is 1.3 vol%, and the blown gas concentration diluted to 25% is 4. 4% by volume. The concentration at which the blowing effect starts to appear, that is, the lower limit of the blowing gas concentration after dilution is 0.05% by volume. Therefore, the preferred range is as follows. Preferred range (1): 2. 2体积%~〇. 〇5 vol% preferred range (2): 1.7 vol%~〇. 〇5 vol% preferred range (3): 1.3 vol%~〇. 〇5 vol% 312/invention manual (supplement) ) /96-01/95140218 23 1329677. Preferred range (4): 0.4 body · ~ 〇〇 5 vol% In the C gas, the lower limit of the blowing gas concentration of the lower limit of combustion is 3 8 : 2 5 vol% 'diluted to 75 % ^ ^ L Shan. 8 vol%, diluted to 60% of the upper limit of the blown gas concentration is 3.0 vol%, 鞴锩9 in person Rolling 0 9 r^〇/ ^ diluted to 25% of the blowing gas concentration is

〇:9體…。該吹人效㈣始顯現H 吹入氣體濃度下限為〇.24體 P稀釋後之 述。 *髖積%。因此,較佳範圍如下所〇: 9 body... The blowing effect (4) begins to show that the lower limit of the H blowing gas concentration is 〇.24 body P after dilution. * Hip volume%. Therefore, the preferred range is as follows

車父佳範圍⑴:5· 0體積%〜〇. 24體積% 較佳範圍(2) : 3. 8體積%〜〇· 24體積% 杈佳範圍(3) : 3· 0體積%〜〇· 24體積% 較佳範圍(4) : 0.9體積%〜〇 24體積% 一於二中,燃燒下限濃度為4 8體積%,稀釋成驗 二二:度上限為3· 6體積%,稀釋成_之吹入氣體 駚又限為2.9體積%,稀釋成25%之吹入氣體濃度為〇.9车佳佳 range (1): 5 · 0 vol% ~ 〇. 24 vol% preferred range (2): 3. 8 vol% ~ 〇 · 24 vol% 杈 better range (3): 3 · 0 vol% ~ 〇 24 vol%, preferably range (4): 0.9 vol% to 〇24 vol%, in the second, the lower limit of combustion concentration is 48 vol%, diluted to the second two: the upper limit is 3.6 vol%, diluted to _ The gas enthalpy is limited to 2.9% by volume, and the concentration of the blown gas diluted to 25% is 〇.9

體積%。稀釋後之吹人氣體濃度下限為體積%。因此, 較佳範圍如下所述。 較佳範圍(1) : 4.8體積%〜〇·丨體積% 較佳範圍(2) : 3.6體積如〜匕:^體積% 較佳範圍(3) : 2. 9體積%〜〇. 1體積% 較佳範圍(4) : 0.9體積%〜〇·ι體積% 於高爐氣體中’燃燒下限濃度為4〇 ()體積%,稀釋成 75%之人入氣體辰度上限為3〇. 〇體積%,稀釋成之吹 入氣體濃度上限為24.〇體積%’稀釋成25%之吹入氣體濃 度為7. 6體積%。稀釋後之吹入氣體濃度下限為〇24體積 312/發明說明書(補件)/96-〇1/9514〇218 %。因此,較佳範圍如下所述。 較佳範圍(1):40.0體積%〜125體積% 較佳範圍(2): 30.〇體積%〜125體積% 較佳範圍(3) : 24.0體積%〜125體積% 較佳範圍(4) : 了^體積^〜^託體積% ,次’表2表示作為C氣體、lng、B|l體之燃燒成分 之虱CO、曱烷、乙烷、丙烷之含有量及發埶量。 表1 ”、 氣體 -丙烷 ^-- 燃燒下限濃度 %、相對於空氣 (爆炸下限、 2.2 - 1 吹入濃度上限 %、相對於空氣 (75%) 〇 吹入濃度上限 %、相對於空氣 (60%) IV 吹入濃度 %、相對於空氣 (25?0 j火溫度 空氣—、°c Μ. __甲烷 co i艚 4.0 ' 5.0 1 O c 〇 3.8 1· 0 〇 Γ 0Α) ϋ· 4 0.8 Ο ' -5282i5M _580 〜Μη βΚΛ - .焦爐i艏 -J.NG Γ 5.0 4.8 9.4 3.8 3.6 r 7.5 3.0 2 ο ^.3 -0.9 Π π b5U〜7Rn _ 6t>8〜674 約630 冋爐煎.俄 _ 40.0 — 30.0 20 υ, y Γ5 i5*68(i~~ nsunm 表2volume%. The lower limit of the blown gas concentration after dilution is vol%. Therefore, the preferred range is as follows. Preferred range (1): 4.8 vol% to 〇·丨 volume% Preferred range (2): 3.6 volume such as 匕: 体积 vol% preferred range (3): 2. 9 vol% to 〇. 1 vol% Preferred range (4): 0.9% by volume to 〇·ι% by volume The lower limit of combustion in the blast furnace gas is 4〇()% by volume, and the upper limit of the gas entering the dilution to 75% is 3〇. 〇% by volume 6体积百分比。 The blown gas concentration was 7.6% by volume. The lower limit of the blown gas concentration after dilution is 〇24 volume 312/invention specification (supplement)/96-〇1/9514〇218%. Therefore, the preferred range is as follows. Preferred range (1): 40.0% by volume to 125% by volume Preferred range (2): 30. 〇% by volume to 125% by volume Preferred range (3): 24.0% by volume to 125% by volume Preferred range (4) : ^ volume ^ ~ ^ tray volume %, time 'Table 2 shows the content of CO, decane, ethane, propane and hair sputum as combustion components of C gas, lng, B|l body. Table 1 ”, Gas-propane^-- Lower limit of combustion concentration %, relative to air (lower limit of explosion, upper limit of 2.2 - 1 blowing concentration, relative to air (75%) 〇 blown in upper concentration %, relative to air (60 %) IV blown in %, relative to air (25?0 j fire temperature air-, °c Μ. __methane co i艚4.0 ' 5.0 1 O c 〇3.8 1· 0 〇Γ 0Α) ϋ· 4 0.8 Ο ' -5282i5M _580 ~Μη βΚΛ - .Coke oven i艏-J.NG Γ 5.0 4.8 9.4 3.8 3.6 r 7.5 3.0 2 ο ^.3 -0.9 Π π b5U~7Rn _ 6t>8~674 About 630 煎. Russia _ 40.0 — 30.0 20 υ, y Γ 5 i5*68 (i~~ nsunm Table 2

, ~-~~~~^~~~^~~=_·__=_L —— ητ~ 以下’就作為本發明之燒結礦之製造方法的開發契機 實驗進行說明❶ 該實驗係使用圖6所示之實驗裝置,即附帶透明石英 ®之豎型管狀試驗鋦(150 x400 mmH),使用高爐氣體 與焦爐氧體之混合氣體(Μ氣體)作為所使用之氣體燃料, 並且使用與申請人公司之燒結工廠中所使用之原料相同 之燒結原料,即表3所示之燒結原料,於下方吸引壓力為 25 312/發明說明書(補件)/96-〇1/9514〇218 1329677 11.8 Kpa之固定條件下所進行之操作例。此處之例為, 上述Μ氣體之燃燒成分之濃度利用空氣而稀釋,使^於 0. 5體積%〜15體積%之範圍内變動。再者,用於該實:之 Μ氣體之燃燒下限濃度為12體積%。 表 - 原料種類 比例(哲县叱、 羅布河鐵破(Robe River) 1 J ν Β Μ. 7〇 J _ 豆石礙(Yandi) 2Γ~8 _ 卡拉加斯礦(Cara ias) 42 0 石灰石 16.6 矽石 2 7 焦炭粉 4. 7, ~-~~~~^~~~^~~=____=_L —— ητ~ The following is described as an opportunity to develop the method for producing a sintered ore according to the present invention. The experimental device shown is a vertical tubular test crucible (150 x 400 mmH) with clear quartz®, using a mixture of blast furnace gas and coke oven oxygen (helium gas) as the gaseous fuel used, and used with the applicant company. The sintering raw materials of the same raw materials used in the sintering plant, that is, the sintering raw materials shown in Table 3, have a lower suction pressure of 25 312 / invention specification (supplement) / 96-〇1/9514〇218 1329677 11.8 Kpa fixed An example of the operation performed under the conditions. In the example, the concentration of the combustion component of the helium gas is diluted with air to vary within a range of 0.5% by volume to 15% by volume. Further, the lower limit of combustion concentration of the helium gas used for the real thing was 12% by volume. Table - Proportion of raw materials (Robe River) 1 J ν Β Μ. 7〇J _ Yanshi 2Γ~8 _ Cara ias 42 0 Limestone 16.6矽石 2 7 Coke powder 4. 7

情況’尤其表示燃燒前線隨著移動而下降之狀況。由圖6 可知,當於試驗鍋内原料堆積層中,吹入含有超過燃燒下 限濃度(12體積%)之15體積%之μ氣體的氣體燃料時,氣 體燃料立即於裝入層表面開始燃燒,而並未到達裝入層之 下層,故吹入效果小。與其相對,根據本發明,當使用由 空氣稀釋至作為上述氣體燃料之燃燒下限濃度即12體積 %的75%以下之3體積%為止之氣體燃料時,其不會於原料 堆積層表面燃燒,而到達裝入層内深處,即燃燒、熔融帶 相备區域。其結果,相對於在大氣中燒結時之燃燒帶(亦 稱作燃燒、熔融帶)之厚度為7〇 mm,本例中可使燃燒帶 之厚度擴大至150 mm,即2倍以上。即,燃燒帶之厚度 擴大無非就是實現高溫區域保持時間之延長。 而且,於該試驗鍋之實驗中,當燃燒前線隨著實機燒結 機之台車移動而行進時,燃燒帶之下降速度(其倒數為燒 312/發明說明書(補件)/96·〇1/95μ〇218 26 1329677 f時間)依稀釋氣體燃料之供給而加快,並且與增加焦户 :時及吹入高溫空氣時同樣,可使燃燒帶上下方向之厚 J二:上所述’當向燒結原料之裝入層中適當吹入稀釋 乳體燃料時,與f知之使用固體燃料、液體燃料、未 .,釋^可燃性氣體時相比較,可知該燃燒帶寬度之擴大效 •顯著,且燃燒前線之下降速度亦與大氣燒結時幾乎無變 -化,以相同速度而行進。 圖7(a)圖7(d)係歸納有上述實驗之燒結鋼試驗結果 者。根據該結果,按照本發明,當向原料裝入層令適當吹 入稀釋後之Μ氣體時,儘管燒結時間幾乎未變化,但良率 有若干提>高(圖7(a)),且燒結生產性亦增加(圖7(b))。 而且,對咼爐之操作成績有大影響之冷延強度管理指標之 碎裂強度(si)亦改善10%以上(圖7(c)),還原粉化特性 (RDI)亦改善 8%(圖 7(d))。 於本發明中,供給至裝入層中之上述氣體燃料係使用稀 籲釋後之氣體,以下就其稀釋程度加以說明。表4表示高爐 氣體、焦爐氣體以及二者之混合氣體(M氣體)、丙烷、曱 烧、天然氟之燃燒下限以及燃燒上限。例如,具有上述燃 燒極限之軋體若於裝入層内未燃燒而通向排風機,則將於 •中途之電氣集塵機等處產生爆炸或燃燒之危險。因此,發 明者4试行錯誤之結果可確認,使用無上述危險之極限、 即濃度稀釋成燃燒下限以下之氣體燃料,且為了進一步提 向安全性’而使用濃度進一步為該燃燒下限濃度之75%以 下之氣體燃料後’於多次實驗中未產生任何問題。 312/發明說明書(補件)/96-01/95140218 27 1329677 例如,高爐氣體燃燒之範圍如表4所示,於大氣中常溫 下,燃燒下限為40體積%(即,未達4〇體積%時未燃燒), 又其燃燒上限為71體積%。此係指若超過71體積%,則 高爐氣體之濃度過濃’此時又變為未燃燒之狀態。以下根 據圖式,說明該數值之依據。 表4 €爐氣雜 _燒下限 4〇 η ___燃燒上限 焦爐IL雜 Λ- 71 混合氣镀(Μ氣艚、 0 · u Γ27η 22 ~12~ 之一例。關 ,圖中高爐氣體中所含之燃燒成分(可燃性氣體)及其他 inert gas .惰性氣體)成分之比例,將仏與⑽以及⑺ 與N2進行組合而研究如下。 (1) H2與C〇2」分之組合時’(惰性氣體可燃性氣 體)之比為 3.5/20.0=5.7。 因此’求出該燃燒極限圖由主_ m 触、 Γ ΰ中表不(惰性氣體)/(可燃性氣 體)之比的橫轴之盘5 7夕a & ^ ΙΑ ^ . 轴相父的Η2 + C〇2曲線之相交部 分(燃燒極限)。下限為 u ^ _π 马32體積/g ’上限為64體積%。即, H=之燃燒極限之下限為32體積%,上限為64體積❶ JL f :、方面’剩餘燃燒成分即「CO與N2」之組合時, G月f生氣體)/ (可燃性氣體) L 札餒)之比為53.5/23.0= 2.3,故同 樣地’可自該圖’根據橫軸? •七山 相軸2. 3與CO+Nz之曲線之交點而 求出下限為44體積%,上限盍 ^ & .^ 上限為74體積%。因此,該情況之 燃燒極限之下限為44體藉。/ , 篮積% ’上限為74體積%。 312/發明說明書(補件)/96_〇1/9514〇218 28 1329677 更進一步,含有兩燃燒成分之高爐氣體的燃燒下限可由 下式而求出。 燃燒下限=100/(23. 5/32 + 76. 5/44)与 40% 又’若該式中應用上述(1)、(2)之上限值,則可求出燃 燒上限。以此方式’可求出高爐氣體之燃燒下限以及燃燒 上限。 又’於本發明中,著眼於氣體燃料之燃燒下限之另一理 由如下所述。圖9係表示於大氣中常溫下,氣體燃料之燃 •燒成分(燃燒氣體)濃度與溫度之關係者。(參照C〇rona社 燃燒便覽)。而燃燒極限雖可以上述方式而求出,但該燃 燒極限具有溫度依存性,列舉一例:儘管常溫下燃燒下限 值(圖中相當於燃燒氣體濃度)約為4〇體積%,但下述情況 已為人所知:於200°C區域中變化為26體積%〜27體積%, 於1 000°C區域中變為數體積%,於12〇〇°c區域中未達i體 積%時,亦燃燒。 φ 由此可知,供給至裝入層之氣體燃料之濃度(燃燒成分 之含有量),若稀釋至較常溫之燃燒下限更低之安全區域 後再進行供給’則為安全,且只要預先調整好該稀釋氣體 -之濃度,則於裝入層内厚度方向(溫度分佈)上之燃燒位置 調整之自由度亦變高。 並且亦已知,雖然氣體燃料燃燒時如上所述,具有溫度 依存性’例如,環境溫度愈高,燃燒範圍愈廣,於燒結機 之燃燒、熔融帶附近之溫度場内經常發生燃燒,但於位於 燒結機下游側的電氣集塵機内等200°C左右之溫度場内, 312/發明說明書(補件)/96-01/95140218 29 ;只明之較佳實施例中所示之濃度下,則不燃燒。 、、=’當製造燒結礦時,供給至燒結原料之裝人層中之 ^述孔體燃料藉由台車τ之風箱而吸引,並且於因該裝入 ft固體燃料(焦炭粉)之燃燒而形成之燃燒、熔融帶之高 • 區域内燃燒。因此’氣體燃料供給時,在使向裝入層投 熱1固定之條件下,調整上述氣體燃料之濃度及供給 里等貝]可調整(減少)燒結原料中之焦炭粉量。又,氣體 料之/辰度調整係指冑整成使該t體燃料之燃燒於裝入 ’層中之預期位置(濃度區域)處進行。 於上述意義中,所謂以習知技術為基礎之裝入層中之燃 燒、溶融帶’係指僅固體燃料(焦炭粉)燃燒之帶域,而於 本卷明中,可指除該焦炭粉以外,進一步使氣體燃料亦一 同使丄之帶域。因此,本發明中,上述氣體燃料之濃度及 ,給量Y其他供給條件,係以含有焦炭粉作為燃料之一部 分為前提,當使與其之關係適當變化時,可對最高到達溫 籲度及/或高溫區域保持時間進行所期望之調整,以此使燒 結塊之強度提高。 於本發明方法中,使用稀釋後之氣體燃料之又一理由在 .於,通過調整上述燒結、熔融帶之形態來調整燒結塊之強 •度、良率。此係由於在調整使該燒結塊於高溫帶(燃燒、 熔融帶)保持多長時間,以及使其到達多高溫度之後,可 使該稀釋氣體燃料有效發揮作用。換言之,上述氣體燃料 之使用’係指調整使燒結原料之高溫區域保持時間變長, 且最高到達溫度適當變高。並且,該調整係指根據燒結原 312/發明說明書(補件)/96*〇ι/95140218 30 1329677 料中之固體燃料量(焦炭粉量),使用稀釋調整後不會於燃 燒環境中產生助燃性氣體(空氣或者氧氣)之過量或者不' 足之上述氣體燃料。此情況於習知技術中,與燒結原料之 固體燃料量無關,且未對可燃性氣體進行濃度調整即吹 入,故導致與固體燃料量及可燃性氣體量相當之助燃性氣 體(氧氣)之不足,因而引起燃燒不良,或者相反,產生部 分過度燃燒而導致強度不均勻。即,本發明係對氣體燃料 之濃度稀釋調整後而使用,故可避免上述問題。 其次,揭示對於每一種類氣體燃料進行稀釋後供給之稀 釋氣體燃料之影響。圖丨〇係表示習知燒結法(未吹入氣體 燃料)與使用濃度稀釋成燃燒下限以下之氣體燃料的本發 明燒結法之比較實驗之條件及結果。未進行稀釋氣體燃料 吹入之習知燒結法中,使用5%的焦炭粉為例,而根據本 發明之稀釋氣體燃料之吹入例中,吹入相當於〇 8%焦炭 粉之稀釋氣體燃料,為了使總熱量固^,而將焦炭粉添加 量設為4.2質量%。於稀釋氣體燃料使用例中,均看到碎 裂強度、成品良率、生產性之提I再者,於稀釋氣體燃 料使用例中,碎裂強度、成品良率等提高之理由可認為係 由於燃燒狀況所顯示之燃燒、熔融帶之擴大所引起,且已 知出現尚溫區域保持時間延長之結果。 圖11係表示使用丙烷氣體與(:氣體作為氣體燃料時之 吹入氣體濃度之影響圖,其係表示稀釋氣體燃料之濃度與 碎裂強度(a)、良率⑻、燒結時間(c)、生產性⑷之關係 圖。由該圖可明白’於丙院氣體時,將其用作稀釋氣體燃 31j 4〇2 j g :夺為了提向碎裂強度而添加。。5體積驗產生效果, 確二:亦出現幾乎同樣之改善效果。丙烧氣體所產生之明 ^效果係自〇. i體積%開始,較佳為〇. 2體積%,換 异、c軋體’則藉由添加〇24體積%而產生The situation 'is especially indicative of the situation in which the front of the combustion drops as it moves. As can be seen from Fig. 6, when a gaseous fuel containing 15% by volume of μ gas exceeding the lower limit of combustion concentration (12% by volume) is blown into the raw material accumulation layer in the test pot, the gaseous fuel immediately starts to burn on the surface of the packed bed. It does not reach the lower layer of the loading layer, so the blowing effect is small. On the other hand, according to the present invention, when a gaseous fuel which is diluted with air to a lower limit of the combustion limit of the gas fuel, that is, 75% by volume or less, which is 75% by volume or less, is used, it does not burn on the surface of the raw material accumulation layer. It reaches the depth in the loading layer, that is, the burning and melting zone. As a result, the thickness of the combustion zone (also referred to as combustion, melting zone) at the time of sintering in the atmosphere is 7 〇 mm, and in this example, the thickness of the combustion zone can be expanded to 150 mm, that is, twice or more. That is, the enlargement of the thickness of the combustion zone is nothing more than an extension of the holding time of the high temperature region. Moreover, in the experiment of the test pot, when the combustion front line travels with the trolley of the actual sintering machine, the descending speed of the combustion belt (the reciprocal number is burned 312 / invention specification (supplement) / 96 · 〇 1 / 95 μ 〇218 26 1329677 f time) is accelerated by the supply of dilute gas fuel, and as in the case of increasing coke: time and blowing high temperature air, the thickness of the combustion zone can be increased in the up and down direction. When the diluted emulsion fuel is appropriately blown into the charging layer, it is known that the width of the burning belt is enlarged and significant, and the combustion front line is compared with the case where the solid fuel, the liquid fuel, and the flammable gas are used. The descending speed is also almost unchanged from the sintering of the atmosphere, and travels at the same speed. Fig. 7(a) and Fig. 7(d) summarize the results of the test for the sintered steel of the above experiment. According to the results, according to the present invention, when the raw material is charged into the layer to appropriately blow the diluted helium gas, although the sintering time hardly changes, the yield is somewhat higher (Fig. 7(a)), and Sintering productivity is also increased (Fig. 7(b)). Moreover, the fracture strength (si) of the cold-strength strength management index, which has a great influence on the operation performance of the furnace, is also improved by more than 10% (Fig. 7(c)), and the reduction pulverization property (RDI) is also improved by 8% (Fig. 7). 7(d)). In the present invention, the gas fuel supplied to the packed bed is a gas which is diluted and released, and the degree of dilution will be described below. Table 4 shows the lower limit of combustion of the blast furnace gas, the coke oven gas, and a mixture of the two (M gas), propane, smoldering, natural fluorine, and the upper limit of combustion. For example, if the rolling body having the above-described burning limit is not combusted in the charging layer and is led to the exhaust fan, there is a risk of explosion or burning at the electric dust collector or the like in the middle. Therefore, as a result of the trial error of the inventors 4, it was confirmed that the gas fuel having the limit of the above-mentioned danger, that is, the concentration is diluted to the lower limit of the combustion, and the use concentration is further increased to 75% of the lower limit of the combustion in order to further improve the safety. The following gaseous fuels did not cause any problems in many experiments. 312/Invention Manual (Supplement)/96-01/95140218 27 1329677 For example, the range of combustion of blast furnace gas is as shown in Table 4. At normal temperature in the atmosphere, the lower limit of combustion is 40% by volume (ie, less than 4% by volume) When it is not burned, the upper limit of combustion is 71% by volume. This means that if it exceeds 71% by volume, the concentration of the blast furnace gas is too rich, and it becomes unburned again. The basis for this value is explained below based on the schema. Table 4: Furnace gas miscellaneous _ burning lower limit 4〇η ___ combustion upper limit coke oven IL miscellaneous - 71 mixed gas plating (Μ gas 艚, 0 · u Γ27η 22 ~ 12~ one example. Off, in the blast furnace gas The ratio of the combustion component (flammable gas) and other inert gas components contained in the combination of (10) and (7) and N2 was studied as follows. (1) The ratio of the combination of H2 and C〇2"' (inert gas flammable gas) is 3.5/20.0 = 5.7. Therefore, 'the combustion limit map is obtained from the main axis _ m touch, Γ 表 in the ratio of (inert gas) / (flammable gas) on the horizontal axis of the disk 5 7 a & ^ ΙΑ ^ . The intersection of the Η2 + C〇2 curve (combustion limit). The lower limit is u ^ _π The horse 32 volume / g ' upper limit is 64% by volume. That is, the lower limit of the combustion limit of H = 32% by volume, the upper limit is 64 volumes ❶ JL f :, in the case of the combination of "CO and N2" as the remaining combustion component, G gas (g gas) / (flammable gas) The ratio of L Sapporo is 53.5/23.0 = 2.3, so the same 'from the figure' is based on the horizontal axis? • The intersection of the seven mountain phase axis 2.3 and the curve of CO+Nz is 44% by volume, and the upper limit is 74 ^ & . . . The upper limit is 74% by volume. Therefore, the lower limit of the combustion limit for this case is 44. / , The basket %' upper limit is 74% by volume. 312/Invention Manual (Supplement)/96_〇1/9514〇218 28 1329677 Further, the lower limit of combustion of the blast furnace gas containing two combustion components can be obtained by the following formula. The lower limit of combustion is 100/(23.5/32 + 76. 5/44) and 40%. If the above upper limits of (1) and (2) are applied, the upper limit of combustion can be determined. In this way, the lower limit of combustion of the blast furnace gas and the upper limit of combustion can be obtained. Further, in the present invention, another reason for focusing on the lower limit of combustion of the gaseous fuel is as follows. Fig. 9 is a graph showing the relationship between the concentration of the combustion component (combustion gas) of the gaseous fuel and the temperature at normal temperature in the atmosphere. (Refer to the C〇rona Society Burning Guide). While the combustion limit can be obtained by the above-described method, the combustion limit has a temperature dependency. For example, although the lower limit of combustion at a normal temperature (corresponding to the concentration of the combustion gas in the drawing) is about 4% by volume, the following case is obtained. It is known that it varies from 26% by volume to 27% by volume in the region of 200 ° C, becomes several vol% in the region of 1 000 ° C, and does not reach i vol % in the region of 12 〇〇 ° c. combustion. φ It can be seen that the concentration of the gaseous fuel supplied to the packed bed (the content of the combustion component) is safe if it is diluted to a safe area lower than the lower limit of combustion at normal temperature, and is safely adjusted as before. The concentration of the diluent gas is also increased in the degree of freedom in the combustion position adjustment in the thickness direction (temperature distribution) in the layer. It is also known that although the gas fuel is burned as described above, it has temperature dependence. For example, the higher the ambient temperature, the wider the combustion range, and the combustion often occurs in the temperature field near the combustion and melting zone of the sintering machine. In the temperature range of about 200 ° C in the electric dust collector on the downstream side of the sintering machine, 312 / invention specification (supplement) / 96-01 / 95140218 29; at the concentration shown in the preferred embodiment, it does not burn. , when the sintered ore is produced, the pore fuel supplied to the charging layer of the sintering raw material is attracted by the bellows of the trolley τ, and is burned by the ft solid fuel (coke powder) The resulting combustion, the high melting zone • burning in the area. Therefore, at the time of the supply of the gaseous fuel, the amount of the coke powder in the sintered raw material can be adjusted (reduced) by adjusting the concentration of the gaseous fuel and the supply of the gas to the charged layer. Further, the gas/length adjustment means that the t-fuel is burned at a desired position (concentration region) in the charged layer. In the above sense, the combustion, melting zone in the loading layer based on the prior art refers to the zone in which only the solid fuel (coke powder) is burned, and in the present disclosure, the coke powder may be excluded. In addition, the gas fuel is further brought together by the gas. Therefore, in the present invention, the concentration of the gaseous fuel and the other supply conditions of the feed amount Y are based on the premise that the coke powder is contained as a part of the fuel, and when the relationship is appropriately changed, the highest temperature and/or the temperature can be reached. Or the high temperature zone is maintained for the desired adjustment to increase the strength of the agglomerate. Another reason for using the diluted gaseous fuel in the method of the present invention is to adjust the strength and yield of the agglomerate by adjusting the form of the sintering and the melting zone. This is because the dilute gas fuel can effectively function by adjusting how long the agglomerate is held in the high temperature zone (combustion, melting zone) and how high it is reached. In other words, the use of the above gas fuel means that the high temperature region holding time of the sintering raw material is adjusted to be long, and the highest reaching temperature is appropriately increased. Moreover, the adjustment refers to the amount of solid fuel (coke powder amount) in the raw material of the raw material 312/invention specification (supplement)/96*〇ι/95140218 30 1329677, which does not generate combustion-supporting in the combustion environment after dilution adjustment. Excessive or non-sufficient gas (air or oxygen). In this case, in the prior art, the amount of solid fuel of the sintered raw material is not related, and the concentration of the combustible gas is not adjusted, that is, the combustion-supporting gas (oxygen) corresponding to the amount of the solid fuel and the amount of the combustible gas is caused. Insufficient, resulting in poor combustion, or conversely, partial overburning resulting in uneven strength. That is, the present invention is used after the concentration adjustment of the gaseous fuel is diluted, so that the above problems can be avoided. Next, the effect of the diluted gaseous fuel supplied for dilution of each type of gaseous fuel is disclosed. The figure shows the conditions and results of a comparative experiment of the conventional sintering method (not blown into a gaseous fuel) and the sintering method of the present invention using a gas fuel diluted to a lower combustion limit or lower. In the conventional sintering method in which the dilution gas fuel is not blown, 5% of the coke powder is used as an example, and in the blowing example of the diluted gas fuel according to the present invention, the diluted gas fuel equivalent to 〇 8% of the coke powder is blown. In order to fix the total amount of heat, the amount of coke powder added was set to 4.2% by mass. In the case of dilute gas fuel use, the crack strength, the yield of the finished product, and the productivity are also observed. In the case of the use of the diluted gas fuel, the reason for the improvement of the fracture strength and the yield of the finished product is considered to be due to The combustion is indicated by the combustion condition, and the expansion of the melting zone is caused, and it is known that the temperature retention time is prolonged. Figure 11 is a graph showing the effect of the concentration of the blown gas when propane gas and (the gas is used as the gaseous fuel), which indicates the concentration of the diluted gaseous fuel and the fracture strength (a), the yield (8), the sintering time (c), The relationship diagram of productivity (4). It can be understood from the figure that when it is used in the gas of the hospital, it is used as a diluent gas to burn 31j 4〇2 jg: it is added to increase the fracture strength. 5 volume test produces effect, indeed Second: there is almost the same improvement effect. The effect produced by the C-burning gas is from the 〇. i volume% starts, preferably 〇. 2 vol%, the change, the c-rolling body' by adding 〇24 5% by volume

^體㈣以上,明叙改善效果為1〇體積%以上。因此為 丙烧氣體時’至少為G. 〇5體積%以上,較佳為Q. }體積 /°以上’更佳為〇.2體㈣上。另-方面,為C氣體時, 至J為0.24體積%以上’較佳為〇. 5體積%以上,更佳為 1. 〇體積%以上,上限為燃燒下限濃度之75%以下。再者, 當為丙烷氣體時,添加〇·4體積%時效果大致飽和,此時 之氣體濃度相當於燃燒下限濃度之25%。^ Body (4) or more, the improvement effect is more than 1% by volume. Therefore, when it is a propane gas, it is at least G. 〇 5 vol% or more, preferably Q. } volume / ° or more ‘more preferably 〇. 2 body (4). On the other hand, in the case of C gas, it is preferably 0.24 vol% or more to J. 5% by volume or more, more preferably 1. 〇 vol% or more, and the upper limit is 75% or less of the lower limit of combustion concentration. Further, in the case of propane gas, the effect is substantially saturated when 〇·4% by volume is added, and the gas concentration at this time corresponds to 25% of the lower limit of combustion.

曰其次,根據本發明之方法,考慮到燒結原料中之炭材 量,來説明供給上述氣體燃料而製造之燒結礦之冷延強度 與還原粉化特性(RDI)。根據「礦物工學」(今井秀喜、武 内壽久禰、藤木良規編,1976年,175,朝倉書店),將 燒結反應之示意圖歸納為如圖12所示。又,表5中顯示 有燒結過私中所生成之各種礦物之拉伸強度(冷延強度) 與被還原性之值。由圖12可明白,於燒結過程中,在1200 °C時開始生成融液,且生成於燒結礦之構成礦物中強度最 咼、被還原性亦較咼之鐵酸舞。當溫度進一步升高而超過 約1380°C時’分解成冷延強度與被還原性最低之非晶質 石夕酸鹽(石夕酸妈)、與易還原粉化之二次赤鐵礦。因此,為 了提高燒結礦之冷延強度以及改善RDI,能否使鐵酸鈣不 分解而可穩定地持續生成,成為課題。 312/發明說明書(補件)脚-〇1/95140218 32 1329677Next, according to the method of the present invention, the cold rolling strength and the reduction pulverization property (RDI) of the sintered ore produced by supplying the above gaseous fuel will be described in consideration of the amount of the carbon material in the sintering raw material. According to "Polyline Engineering" (Imai Hideki, Takeuchi Shoujiu, Fujiki Ryo, 1976, 175, Asakura Bookstore), the schematic diagram of the sintering reaction is summarized as shown in Fig. 12. Further, Table 5 shows the values of tensile strength (cold strength) and reducibility of various minerals formed during sintering. As can be seen from Fig. 12, in the sintering process, the melt is started to be formed at 1200 ° C, and the ferrite which is the strongest in the constituent minerals of the sintered ore and which is less reducible is formed. When the temperature is further increased and exceeds about 1380 ° C, it is decomposed into a non-amorphous austenitic acid salt of the cold strength and the lowest reducibility, and a secondary hematite which is easily reduced and pulverized. Therefore, in order to improve the cold rolling strength of the sintered ore and improve the RDI, it is possible to stably form the calcium ferrite without decomposing it. 312/Invention manual (supplement) foot-〇1/95140218 32 1329677

拉伸強度 (MPa) 被還原性 赤鐵礦 49 磁鐵礦 58 ^__ 鐵酸鈣 102 矽酸鈣 19 — *1 〇 — 礦之還原粉化起點的二次赤鐵礦之析出動作,如圖ΐ3所 示進行說明。根據該說明,成為礦物合成試驗之結果、還 原粉化之起點之骸晶狀二次赤鐵礦,為了於升溫至Μ叫.π + Liq.區域並冷卻後析出,經由狀態圖上(2)路徑而非 路徑來製造燒結礦,藉此可抑制還原粉化性。因此,為了 製造低RDI燒結礦與高強度燒結礦,重要的是,於12〇〇 °c (鐵酸鈣之固相線溫度)與約138(rc (轉移溫度)之範圍 内,以何種方式來實現於裝入層内長時間保持之溫度記錄 圖(heatpattern)。因而可知,利用氣體燃料之供給而調 整所添加之炭材量的裝入層最高到達溫度為,超過12〇〇 C而未達138(TC,較佳為1 20 5°C〜135(TC之範圍内。 繼而,發明者等為獲知燃燒帶之寬度與稀釋燃料氣體之 關係,而使用附帶透明石英製窗之豎形管狀試驗鍋進行試 驗將利用燒結機冷卻器之廢氣而稀釋之丙燒氣體,自該 鍋之上方吹入到燒結原料之裝入層中。於該實驗中所使用 之燒結原料為申請人公司所使用之一般性原料,吸引壓力 固定為1200 mmihO。於該實驗中,吹入丙烷氣體之濃度係 稀釋成0. 5體積%及2. 5體積%者。再者,進行投入熱量換 算時,大致相當於吹入05體積%的丙烷氣體,且添加 312/發明說明書(補件)/96-01/95140218 33 1329677 質量%的焦炭粉。 圖14係表示該實驗之丙烷氣體吹入時,燃燒帶之觀察 結果之照片。如該圖所示,對於濃度稀釋成2 5體積%之 丙烷氣體,在吹入後隨即於原料裝入層上燃燒,氣體燃料 並未進入裝人層内,故無效果。與其相對,若使用濃度稀 釋程度相對於空氣為0.5體積%之丙烷氣體,則不會於裝 入層上部燃燒,而進入該裝入層内部,且於該裝入層内迅 速燃燒。其結果,相比於大氣條件下燒結時之燃燒帶上下 方向寬度約為70 mm,當以此方式吹入稀釋丙烧氣體時, 燃燒帶之寬度(即’相當於高溫區域保持時間)擴大至 _,為2倍以上。 士因而可知,於丙烷之濃度為燃燒下限濃度體積蚁理 =’相對於空氣)之1/5 gp 〇5體積%時,亦發現燃燒帶 擴ί效果。相反亦得知,於本發明之氣體燃料吹入 内之燃燒調整。燃枓,則難以進行裝入層 於該實驗中’亦有就燃燒帶之下降速度(其 =區域保持時間)進行檢討,其結果為,於僅增 者於吹人高溫空氣時,下降速度大為降低, 降低,而於使用稀釋後之氣體燃料時,則由於 二=之使用例相比’燃燒速度顯著加快,故燃燒帶 繼而與大乱燒結之情況下幾乎看不出差異。Tensile strength (MPa) Reduced hematite 49 Magnetite 58 ^__ Calcium ferrite 102 Calcium citrate 19 — *1 〇 — The precipitation of secondary hematite from the origin of reduction of the ore of the mine, as shown in the figure The description is shown in ΐ3. According to the description, the twin-shaped hematite, which is the result of the mineral synthesis test and the starting point of the reduction pulverization, is heated to the Μ.π + Liq. region and is cooled and precipitated, via the state diagram (2). The path is formed instead of the path to produce a sintered ore, whereby the reduction pulverizability can be suppressed. Therefore, in order to produce low RDI sinter and high-strength sinter, it is important to be in the range of 12 ° ° C (solid phase temperature of calcium ferrite) and about 138 (rc (transfer temperature)). The method realizes a heat pattern which is maintained in the loading layer for a long time. Therefore, it can be seen that the maximum reaching temperature of the charging layer for adjusting the amount of the added carbon material by the supply of the gaseous fuel is more than 12 〇〇C. It is less than 138 (TC, preferably 1 20 5 ° C to 135 (in the range of TC. Then, the inventor, etc., knows the relationship between the width of the combustion zone and the diluted fuel gas, and uses a vertical window with a transparent quartz window) The tubular test pot was tested and the acrylic gas diluted by the exhaust gas of the sintering machine cooler was blown from above the pot into the charging layer of the sintering raw material. The sintering raw material used in the experiment was the applicant company. The volume of the propane gas is diluted to 0.5% by volume and 2.5% by volume. In addition, when the input heat is converted, the pressure is approximately 1200 mmih. Equivalent to blowing into the 05 body % of propane gas, and 312/invention specification (supplement)/96-01/95140218 33 1329677% by mass of coke powder is added. Fig. 14 is a photograph showing the observation result of the combustion zone when the propane gas is blown in the experiment. As shown in the figure, the propane gas diluted to a concentration of 25 vol% is burned on the raw material charging layer immediately after the blowing, and the gaseous fuel does not enter the charging layer, so there is no effect. When propane gas having a concentration dilution of 0.5% by volume with respect to air is used, it does not burn in the upper portion of the packed bed, but enters the inside of the packed layer and rapidly burns in the packed layer. As a result, compared with the atmosphere Under the condition, the width of the burning belt in the vertical direction is about 70 mm. When the diluted propane gas is blown in this way, the width of the burning belt (that is, 'corresponding to the holding time of the high temperature region) is expanded to _, which is twice or more. Therefore, it can be seen that when the concentration of propane is 1/5 gp 〇 5 vol% of the lower limit of combustion concentration ant = 'relative to air), the effect of expanding the combustion zone is also found. On the contrary, the gas of the present invention is also known. Fuel blowing In-burn combustion adjustment. Burning, it is difficult to carry out the loading layer in the experiment. 'There is also a review of the falling speed of the burning zone (it = zone holding time). As a result, only the increase in blowing high temperature air When the dilute gas fuel is used, the combustion rate is significantly accelerated, so that the combustion belt is almost indistinguishable from the large-scale sintering. .

㈣而,發明者我稀釋氣體燃料之吹人位置之影響進行 312/發明說明書(補件V96-01/9514021S 34 丄/ s亥貫驗之方法如表6所示。每私 ★ κ驗NO· 1係燒結原料中添 加5質量%焦炭之現狀之基礎 、' 好 哫怿件,貫驗No. 2係使焦炭粉 之比例下降1質量%設為4質量 人物 負里%並取而代之吹入〇· 5體 積究丙燒氣體之投入埶蚩囡金玫从 . 新曰 …里固疋條件;實驗NO. 3係添加有 2㈣焦炭粉之條件;實驗紙4係以驗證與保熱爐(日 本專利特開昭60 - 155626號公報)之差異為目的而吹入 450°C的高溫氣體之條件。 NO. 2 NO. 3 NO. 4 NO.(4) However, the inventor of my dilute gas fuel blows the position of the impact of the 312 / invention manual (supplement V96-01/9514021S 34 丄 / s Hai inspection method as shown in Table 6. Every private ★ κ test NO · The basis of the current situation of adding 5 mass% of coke to the 1st sintering raw material, 'good condition, the inspection No. 2 system reduces the proportion of coke powder by 1% by mass to 4% of the number of people, and instead blows it into the 〇· 5 volume of C-burning gas input 埶蚩囡金玫从. New 曰...Ligu 疋 conditions; experimental NO. 3 series added 2 (four) coke powder conditions; experimental paper 4 series to verify and heat furnace (Japanese patent special The condition of blowing a high-temperature gas of 450 ° C for the purpose of the difference of Kai-Sho 60 - 155626. NO. 2 NO. 3 NO. 4 NO.

--二,▼,—、mm A4了,只里J ~^^1_度(相對於空氣,體積 JiA爐(吹入 45(ΓΓ 埶)a.、 圖15係表示其結果者,其係使用騎成⑽ (C氣體)作為氣體燃料之例。該圖係表示進行氣體燃料之 吹)時,其吹入位置與成品燒結礦碎裂強度及成品良率之 關係之調査結果。稀釋氣體燃料之吹入位置設為,距離裝 入層表面100 mrn〜200 mm之位置、200 mm〜3〇〇 mm之位 置、以及300 mm〜400 mm之位置。由該圖所示結果可知, 於吹入位置為1〇〇 mm〜2〇〇 mm時,圖中明亮(白色)顯示 之燃燒、炫融帶移動至100 mm位置後,自上述試驗銷之 上方供給稀釋氣體燃料,而在位於100 mm〜2〇〇 mm期間, 於燃燒、溶融帶使稀釋氣體燃料燃燒。而且同樣地,於 200 mm〜300 mm位置處,自燃燒、熔融帶到達2〇〇 mm位 置之階段開始’自試驗鍋上方供給稀釋氣體燃料,繼而於 300 mm〜400 mm之位置亦同樣地,自燃燒、熔融帶到達 312/發明說明書(補件)/96-01/95140218 35 1329677 300 mm位置之階段開始’供給稀釋氣體燃料。再者,為 供參考’亦顯示有習知法之未進行稀釋氣體燃料之吹入 日守’上述各層位置之燃燒、熔融帶。 又’試驗鋼之燃燒用空氣之供給與通常之燒結操作相 同,係自上方流向下方,故添加氣體燃料時,係以使氣體 燃料達到# $濃度之方式而向該燃燒用$氣中添加並且 供給。 如圖15中明亮(白色)顯示,燃燒、熔融帶於1〇〇咖〜 200 mm區域,僅較習知法稍厚些許。於2〇〇咖〜3〇〇咖 區域,燃燒、熔融帶之厚度與習知法相比明顯增加,而於 300 mm〜400 mm區域,與習知法相比亦具有明確差異。 由於上述情況,故稀釋氣體燃料吹入效果較佳為,於距 離裝入層表面200 mm以下之區域的燒結機台車上之燃 燒、熔融帶部分,進行氣體燃料之供給,且亦可實現氣體 燃料使㈣本之降低H對於離裝人層表面未達獅 _之區域,即便未強行供給氣體燃料,但由於供給至200 随以下之區域時,燒結礦之碎裂強度大幅度上升,故亦 可使成品燒結礦之良率全體提高。 圖16係示意化表示距離裝入層表面2〇〇miB$止之上層 部與200 πππ以下之中、下層部之燃燒狀況。該圖所干二 前頭A表示燒結之行進方向(燃料方向),圖16( 層部(< 為止)之焦炭粉與氣體燃料之燃燒位^ 此時,由於焦聽之職所形叙燃燒帶於裝^之 肩本狭窄,該线粉職帶與錢燃燒帶㈣^氣體燃 312/發明說明書(補件)/96-01/95140218 36--Two, ▼, —, mm A4, only J ~ ^ ^ 1 _ degrees (relative to air, volume JiA furnace (blowing into 45 (ΓΓ 埶) a., Figure 15 shows the result, its system An example of the use of riding (10) (C gas) as a gaseous fuel. This figure shows the investigation result of the relationship between the blowing position and the sintered crushing strength of the finished product and the yield of the finished product when the gas fuel is blown. The blowing position is set to a position of 100 mrn to 200 mm from the surface of the loading layer, a position of 200 mm to 3 mm, and a position of 300 mm to 400 mm. From the results shown in the figure, it is known that the blowing is performed. When the position is 1〇〇mm~2〇〇mm, the bright (white) light in the figure shows that the burning and the smelting belt move to the position of 100 mm, and the diluted gas fuel is supplied from above the test pin, and is located at 100 mm~ During the period of 2 〇〇mm, the dilute gas fuel is burned in the burning and melting zone, and similarly, at the position of 200 mm to 300 mm, the self-combustion and melting zone reach the position of 2 〇〇mm, and the supply from the test pot is started. Dilute the gaseous fuel, and then in the same position from 300 mm to 400 mm Self-combustion, melting zone arrival 312 / invention specification (supplement) / 96-01/95140218 35 1329677 300 mm position starting stage 'supply of dilute gas fuel. Again, for reference' also shows that there is no conventional method The dilute gas fuel is blown into the fire and the melting zone of the above-mentioned layers. The supply of the combustion air of the test steel is the same as the normal sintering operation, and flows downward from the top. Therefore, when the gaseous fuel is added, The gas fuel is added to the combustion gas in a manner that reaches the concentration of #. As shown in Fig. 15, the bright (white) shows that the combustion and melting are in the area of 1 〇〇 to 200 mm, which is only slightly smaller than the conventional method. Thicker. In the area of 2 〇〇 ~ 〇〇 〇〇 , , , , , , 燃烧 〜 〜 〜 〜 〜 〜 〜 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧 燃烧In this case, it is preferable that the dilution gas fuel is blown into the combustion and melting zone portion of the sintering machine trolley in a region of 200 mm or less from the surface of the charging layer, and the gas fuel can be supplied. The body fuel makes (4) the reduction of H. For the area where the surface of the unloading layer is not up to the lion, even if the gas fuel is not forcibly supplied, the fragmentation strength of the sinter is greatly increased due to the supply to the area below 200. It is also possible to improve the overall yield of the finished sintered ore. Fig. 16 is a schematic representation showing the combustion of the upper layer portion and the lower layer portion of the layer above the surface of the layer 2 〇〇miB$ and the lower layer portion. The front head A indicates the direction of travel of the sintering (fuel direction), and Fig. 16 (the burning position of the coke powder and the gas fuel in the layer (<>>) ^ At this time, the burning belt is shaped as the shoulder of the burning belt Ben narrow, the line of powder belt and money burning belt (four) ^ gas burning 312 / invention manual (supplement) / 96-01/95140218 36

荦it·占相互接⑨’故形成於該圖右側戶斤揭示之溫度圖 區域:者:於該溫度分佈中,將焦炭粉(固體燃料)之燃燒 :域矣:為衫線部分,將於其上方燃燒之氣體燃料之溫度 I為非影線部分。根據該圖可知,於裝入層上部, ':厌與氣體燃料同時期燃燒(二者相互接近而燃 二A u圖中Τ”Τ2所表示之期間之高溫區域保持時間 12_)如圖所示變得狹窄。即,形成影線部 Τ之焦厌燃燒區域為稍許擴大程度之溫度分佈。如 2襄入層中供給上述氣體燃料較佳為於燃燒、炼融帶之 2成為15mm以上後進行供給,上述情況與當原先之高 =域保持時間範圍狹窄時,氣體燃料之吹人效果低之情 與致3方面,圖16(b)為對中層、下層部分供給氣 •料之情況’於中層、下層區域,隨著燃燒帶自上層移 向下方’裳人層之溫度亦上升,使燃燒帶寬度擴大,於較 圖16(a)之情況更偏離之位置處燃燒。其結果形成圖iwb) 右侧所示之溫度分佈。即,氣體燃料之燃燒點遠離影線所 示之固體燃料(焦炭)之燃燒點’故所合成之溫度分佈曲線 形成基部大之溫度分佈。因此,I、I所表示之固體姆料 與氣體燃料之燃燒所產生之高溫區域保持時間得到延 長,因而使所獲得之燒結礦之碎裂強度提高。 再者,於圖16(b)之例中,用以調整高溫區域保持時間 之氣體燃料之著火溫度,較佳為4〇〇〇c〜8〇〇c>c ,更佳著 火溫度為50(TC〜700〇C,其理由為,若使著火溫度未達 400 C,則無法擴大高溫區域,而僅使低溫區域分佈擴大, 312/發明說明書(補件)/96-01 /95140218 37 面若超過8 〇 〇 C,則過於接近固體燃料烬燒$ ㈣域__,使高㈣域料時間之延長效果 其次,說明供給稀釋氣體燃料而調整裝入層中最高到達 =層内溫度)之方法之一例。圖1?係示意性表示燒結 二内-度分佈之情況。該圖係以於習知燒結法之溫度分 加5質量%固體燃料(焦炭粉)為基準,來說明本 X 凡結法0例如,於添加5質量%焦炭之燒結摔作中, 將習知燒結法用曲線a表示…般而言,4了^作: 域保持時間’有效的是增加焦炭粉之使用量,例=二 不用虛線a表示添加有1〇質量%的焦炭粉之情況 層厚所表示之高溫區域保持時間自(〇_A)擴大至⑶― B)’但是最高溫度亦㈣13_上升至約m代 c,故無法獲得低Rdi且高強度之燒結礦。 上述情況於根據本發明法之燒結操作方法中,一 將焦炭t之使用量控制於4·2質量%,另一方面由於吹i 稀釋C軋體’故最高到達溫度可抑制纟127(TC,同時, 由於高溫區域保持時間擴大至(0-0,故可充分實現尹: 目的’即於習知法中無法實現之製造低RDI、高強度= 石廣0 ' ° 總之’習知燒結法係著眼於調整高溫區域保持時 局溫度中任—方之操作方法。而本發明: 使用量(例如,㈣於4·2„%)之基礎上,= 溫度崎〜135(TC)進行調整,另一方面,亦係;= 入稀釋乳體燃料而調整高溫區域保持時間之操作方^。^ 312/發明說明書(補件)/96·01/95ΐ4〇2ΐ8 38 1329677 者,圖16之曲線d係表示僅將固體燃料使用量降至4 2 質量%之例’其最高到達溫度亦低’高溫區域保持時間亦 圖18中,作為習知燒結法,呈現有使用有5質量%的声 炭粉之例;作為本發明之適合例,呈現有共同吹入使用量 為4.2質焦炭粉與濃度為2.0體積%稀釋仁氣體之例。 根據該圖之熱圖像可知’於習知法+,為了維持高溫區域荦it·occupies 9', so it is formed in the temperature map area revealed by the right side of the figure: in this temperature distribution, the burning of coke powder (solid fuel): domain 矣: part of the shirt line, will The temperature I of the gaseous fuel burned above it is a non-hatched portion. According to the figure, in the upper part of the loading layer, the temperature of the high temperature region during the period of time indicated by the combustion of the gaseous fuel (the two are close to each other and burned in the second figure) is as shown in the figure. In other words, the burnt-down region in which the hatching portion is formed is a slightly expanded temperature distribution. For example, it is preferable to supply the gas fuel to the combustion layer and the smelting zone 2 to be 15 mm or more. Supply, the above situation is the same as when the original high = domain holding time range is narrow, the gas fuel blowing effect is low, and Figure 3 (b) is the case of supplying gas and material to the middle and lower parts. In the middle layer and the lower layer, as the combustion zone moves from the upper layer to the lower side, the temperature of the layer is also increased, so that the width of the burning zone is enlarged, and it burns at a position further deviated from the case of Fig. 16(a). The result is iwb. The temperature distribution shown on the right side, that is, the burning point of the gaseous fuel away from the burning point of the solid fuel (coke) shown by the hatching, so the temperature distribution curve synthesized forms a large temperature distribution at the base. Therefore, I, I Solid solid The holding time of the high temperature region generated by the combustion of the material and the gaseous fuel is prolonged, thereby increasing the fracture strength of the obtained sintered ore. Furthermore, in the example of Fig. 16(b), the holding time of the high temperature region is adjusted. The ignition temperature of the gaseous fuel is preferably 4〇〇〇c~8〇〇c>c, and the ignition temperature is 50 (TC~700〇C). The reason is that if the ignition temperature is less than 400 C, it cannot be Expanding the high temperature region, and only expanding the distribution of the low temperature region, if the surface exceeds 8 〇〇C, it is too close to the solid fuel to burn the $ (four) domain __, making it high (4) Effect of prolonging the domain material time Next, an example of a method of supplying the diluted gas fuel to adjust the highest arrival in the packed layer = the temperature in the layer) is shown. Fig. 1 is a schematic view showing the case of sintering the internal-degree distribution. Based on the temperature of the conventional sintering method and adding 5% by mass of solid fuel (coke powder) as a reference, the description of the X method is as follows. For example, in the sintering of 5% by mass of coke, the conventional sintering method is used. Expressed by curve a... In general, 4 works: When the domain is maintained 'It is effective to increase the amount of coke powder used. For example, the absence of the dotted line a indicates that the coke powder is added in an amount of 1% by mass. The high-temperature region retention time indicated by the layer thickness is expanded from (〇_A) to (3)-B) 'But the maximum temperature is also (4) 13_ rises to about m generation c, so low-Rdi and high-strength sinter can not be obtained. In the above case, in the sintering operation method according to the method of the present invention, the amount of coke t used is controlled to 4· 2% by mass, on the other hand, because of the dilution of the C-rolled body by blowing i, the maximum temperature reached can suppress 纟127 (TC, and at the same time, since the holding time of the high-temperature region is expanded to (0-0, the Yin can be fully realized) In the conventional method, it is impossible to manufacture low RDI, high strength = Shi Guang 0 ' ° In short, the conventional sintering method focuses on adjusting the high temperature region to maintain the current temperature. However, the present invention: the amount of use (for example, (4) on the basis of 4·2%), = temperature s 135 (TC) for adjustment, on the other hand, is also; = into the diluted milk fuel to adjust the high temperature region to maintain The operation of the time ^ ^ 312 / invention manual (supplement) / 96 · 01 / 95 ΐ 4 〇 2 ΐ 8 38 1329677, the curve d of Figure 16 shows the example of only reducing the amount of solid fuel used to 42% by mass The highest reaching temperature is also low. The high temperature region holding time is also shown in Fig. 18. As a conventional sintering method, there is an example in which 5% by mass of the sonic powder is used. As a suitable example of the present invention, a common blowing amount is used. 4.2 Example of a coke powder and a concentration of 2.0% by volume of diluted lean gas. According to the thermal image of the figure, it is known that in the conventional method, in order to maintain a high temperature region

保持時間,而產生超過1400Ϊ之燃燒狀況。另一方面, t將焦炭粉之使用量控制於4. 2質量%,且吹入濃产2體 版C氣體時,剛。C之區域消失,形成下述狀;:最 向到達溫度可控· 1350〇C以下,同時可實現高溫區域 保持時間之延長。 圖19係表示於投入熱量固定條件時,吹入稀釋後之丙 2氣體而引起之裝入層内溫度(a)、廢氣溫度(5)、通過風 量(c)、以及廢氣組成(d)之經時變化。此處,裝入層内溫 #度為使用傳熱裝置所測定之值,該傳熱裝置係於上^試^ 鍋中,在距離爐條高度2〇〇 mm(裝入層厚為6〇〇 mm)之位 置處裝入。又,於試驗鍋之圓周方向,於中心部與距離壁 .5 mm之兩個部位進行測定。根據該等圖可確認,藉由吹 •入稀釋後之丙烷氣體,使加熱至12051:以上之燒結原料 之熔融,間(以下稱作「高溫區域保持時間」)增加2倍以 上:但最高到達溫度並未上升。又,藉由吹入稀釋後之丙 燒乳體,使廢氣中氧濃度降低,故可推測,氧有助於燃燒 反應效率提高。 312/^^0^#(^{φ)/96.〇 1/95 J40218 39 1329677 又,圖20表示吹入稀釋後之丙烷(〇· 5體積%)時與僅増 加焦炭量(10質量%)時裝入層内溫度(^)、(a,)與廢氣濃 度(b) ' (b’)之經時變化之對比。根據該等圖式,當使焦 厌粉之使用比例倍增時,12〇〇eC以上之高溫區域保持時間 與吹入濃度稀釋成〇. 5體積%之丙烷氣體時大致相等,但 最高到達溫度超過1 3501。又,可確認,由於增加焦炭 也之里,使廢氣中C〇2濃度自20體積%大幅上升至25體積 %,且CO濃度亦增加,焦炭粉有助於燃燒之比例降低。 圖21係對上述試驗中之各種特性試驗結果進行歸納 者。由該圖可明白,燒結時間因吹入稀釋後之丙烷氣體而 有右干延長,但良率及碎裂強度、生產率均得到改善,並 且還原粉化性(RDI)及被還原性亦均大為改善,故可確 認’藉由使稀釋氣體燃料之吹入適當化,除了可改善生產 率及良率之外,還可使燒結礦高品質化。 與此相對,於僅使焦炭粉增加至1 〇質量%之情況下,不 馨僅燒、’·σ時間延長,而且最南到達溫度亦上升到必要溫度以 上’反而生成大量低強度之非晶質矽酸鹽,造成碎裂強度 與良率均大幅降低。又,於45(TC保熱爐之例中,碎裂強 .度與良率之改善效果小,與迄今為止之商業設備之結果大 致一致。 根據以上說明可知,當使用稀釋後之氣體燃料時,該氣 體於裝入層内燃燒,使該層内之燃燒帶擴大,同時由於燒 結原料t焦炭之燃燒熱與稀釋後之丙烷氣體的燃燒熱之 相乘作用,而形成寬燃燒帶。其結果,使最高燃燒到達溫 312/發明說明書(補件)/96_〇 1/95140218 40 丄:529677 度不會過高’且另-方面’對於高溫區域保持時間,因所 供給之稀釋氣體之燃燒而得到延長。 其次’發明者等係針對吹人稀釋後之氣體燃料而對成品 燒結礦之被還原性、冷延強度等所造成之影響,與習知法 (5質量%,10質量%之焦炭、吹入熱風)對比而進行調査。 所測疋之項目為成品燒結礦中之礦物組成比例(影響冷延 強度,被還原性)' 外觀比重(影響冷延強度)、0 5咖以 下之氣孔徑分佈(影響被還原性)。 首先,圖22表示藉由粉末X射線繞射法而定量化之成 品燒結礦中礦物相之組成比例之調查結果。根據該圖可認 為,當使投入熱量固定(焦炭4質量% +丙烷〇5體積%), 且固體燃料與稀釋丙烷氣體併用時,穩定生成鐵酸鈣,此 可認為致使被還原性提高及冷延強度增加。 圖23係表不成品燒結礦之外觀比重之測定結果,且圖 23表不壓汞儀測定之〇· 5 mm以下的氣孔徑分佈之測定結 果。根據圖22,藉由吹入稀釋後之丙烷氣體,而自造粒 粒子外側進行加熱,其結果可促進熔融液流動,降低〇 5 mm以上之氣孔率(外觀比重),故可認為此係冷延強度提 咼之重要原因。又,根據圖24可認為,以投入熱量固定 之方式吹入稀釋丙烷氣體可使燒結原料粒子中之熱源減 少,因此容易殘留對被還原性造成影響之來自礦石的5〇〇 A m以下之微細氣孔,故可進行高被還原性燒結礦之製造。 圖25係表示僅使用焦炭時(a)與一併吹入稀釋氣體燃 料時(b)之燒結動作之示意圖。如該圖所示,於習知之僅 312/發明說明書(補件)/96-0丨/95140218 1329677 結中,相對於利用焦炭粉燃燒而自模擬粒子 …於本發明之焦炭+氣體燃料之併用方法 利用氣體燃料之燃燒而自模擬粒子外部進行加 …、’故容易殘留礦石内 ϋ 内之铋細軋孔,故可推察,與RDI低 相比,ns —RI亦可推移至較高位。 - 圖26表示吹入稀釋後氣 ^ 巩體燃枓時’燒結礦之氣孔構 思圖。如該圖所示,為了提高燒結礦之生產 2疋,促進影響良率及冷延強度之。.5_〜5随氣孔 便,、數里減;,並使影響通氣性之5咖以 上之虱孔比例增加。又可知,為古 Μ ,χ . 馮了獒间燒結礦之被還原 权佳為,形成大量殘留有主要存在於鐵礦石内 Γ以下之微細氣孔的氣孔構造。根據本發明,可認為藉 由吹入稀釋後之氣體燃料, ‘、”曰 構造。 』按近理想之燒結礦之氣孔 二表:把握可維持必要冷延強度之極限焦炭比 (所明極限焦厌比’係指碎裂強度達到與不使用稀釋後之 ==時之最大料7_等之焦炭比。)之試驗結果。 如S玄圖所示,由於吹入稀釋徭 0/、 + 柿枰设之丙烷氣體(濃度0.5體積 =使用以獲得與現狀相同之冷延強度(碎裂強度⑽之 焦厌比如圖27⑷所示,可自5質量%降低至3質量%(約 ,/小又’如圖27(b)、(c)所示而可明白,用以獲 得73%之良率及ΐ·86之生產率之隹户 降低至3.5質量%。 4之焦-比,分別自5㈣ 根據以上說明而可明白’本發明係於燃燒、溶融帶隨著 312/發明說明書(補件)/96-01/95140218 42 台車之行進而自裝入層之表声 量,適當將豨鏗4 A _ a 下層期間,根據炭材 可發揮撟大η 燃料選擇適當位置後供給,藉此 實現心;:層内之燃燒、炫融帶功能之作用,以此可 1現&結礦質量之改善、生產性之提高。 (貫施例) 之H二1.進行燒結鍋試驗,該試驗使用圖6所示 (H 5體2焦爐氣體(C氣體)作為稀釋後之氣體燃料 〆i體積小且將原料中之炭材(焦炭)量設為5質量 :於圖Γ广與f述實驗條件⑽37段落)相同。其結果顯 乡 。如该圖所示可知’當根據本發明法而使用稀 C氣體時’若提高該c氣體之濃度,則燃燒帶寬度 β者K大且良率及生產率提高,並且冷延強度 得到改善。 (2) 只%例2 .在與實施例1相同之條件下進行試驗。 其結果顯示於® 29。如該圖所示可知,當根據本發明法 而使用已稀釋之丙烷氣體(〇 〇2〜〇 5體積%)時,若提高 該C氣體之濃度,則燃燒帶寬度顯著擴大,且良率及生產 率提高,並且冷延強度(SI)亦得到改善。 (3) 實施例3 :該實施例係使用圖6所示之試驗鍋,與 未吹入稀釋氣體之例進行對比,將利用冷卻器廢氣而稀釋 之焦爐氣體(C氣體)自該鍋之上方吹入到表7所示之燒結 原料(包含回收礦20質量%)之裝入層中。 於該實施例中,燒結層中包含4. 8質量%〜5. 0質量%焦 炭粉(計劃外數),作為本發明之適合例,係將濃度為j. 〇 312/發明說明書(補件)/96-01/95140218 43 1329677 〜2·0體積%(相對於空氣)之c氣體於吸引壓力12〇〇 mmAq(差壓1 000 Aq)之條件下,吹入距離裝入層表面1〇〇 〜400 mm(整個厚度6〇〇 mm,差厚為於最下層積層回收礦 200顏)之位置處。再者,關於上述吹入位置,當讪燒結 機之全長為80 m時,若將其應用於整個高度6〇〇 mm,則 试驗NO. 2之吹入位置1〇〇〜2〇〇 mm,相當於如下例:在 80(m)xl00 〜200/600(mm) = 13. 3(m)〜26. 6(m)之位置 處,設置長度為13. 3m之稀釋氣體吹入排煙罩12而進行 燒結機之操作。因此,試驗NO. 2之吹入位置2〇〇〜goo mm 之例相當於下述情況··在燒結機台車上之點火爐後方約 26.7〜39.7 mm之位置處,仍設置長度為133 ^之稀釋 氣體吹入排煙罩12,以進行氣體吹入。Hold time and produce more than 1400 燃烧 of burning. On the other hand, t is used to control the amount of the coke powder to be used in an amount of 2.2% by mass, and is blown into a concentrated 2-body C gas. The area of C disappears and forms the following shape: The temperature of the most reachable temperature is controlled below 1350 〇C, and the holding time of the high temperature area can be extended. Figure 19 is a diagram showing the in-layer temperature (a), the exhaust gas temperature (5), the passing air volume (c), and the exhaust gas composition (d) caused by blowing the diluted C 2 gas when the heat is fixed. Change over time. Here, the inner temperature of the loading layer is the value measured by using the heat transfer device, and the heat transfer device is placed in the upper test pot at a height of 2 mm from the height of the grate (the thickness of the layer is 6 装入). Load at the position of 〇mm). Further, in the circumferential direction of the test pot, measurement was performed at two points of the center portion and the distance wall of .5 mm. According to the above-mentioned figures, it is confirmed that by blowing the diluted propane gas, the melting of the sintering raw material heated to 12051: or more is increased by two times or more (hereinafter referred to as "high temperature region holding time"): but the highest is reached. The temperature did not rise. Further, by blowing the diluted propylene emulsion to lower the oxygen concentration in the exhaust gas, it is presumed that oxygen contributes to an improvement in combustion reaction efficiency. 312/^^0^#(^{φ)/96.〇1/95 J40218 39 1329677 Further, Fig. 20 shows the amount of coke (10% by mass) when propane is diluted (〇·5 vol%) When compared with the time-dependent changes in the temperature (^), (a,) and the exhaust gas concentration (b) ' (b'). According to the drawings, when the proportion of use of the coke powder is multiplied, the holding time of the high temperature region of 12 〇〇eC or more is diluted with the blowing concentration to be 〇. 5 vol% of the propane gas is substantially equal, but the highest reaching temperature exceeds 1 3501. Further, it was confirmed that the concentration of C〇2 in the exhaust gas was greatly increased from 20% by volume to 25% by volume, and the CO concentration was also increased, and the proportion of the coke powder contributing to the combustion was lowered. Fig. 21 is a summary of the results of various characteristic tests in the above test. As can be seen from the figure, the sintering time is extended by the right dryness by blowing the diluted propane gas, but the yield and the fracture strength and productivity are improved, and the reduction pulverization (RDI) and the reducibility are also large. In order to improve, it has been confirmed that by optimizing the blowing of the diluent gas fuel, in addition to improving productivity and yield, the sintered ore can be made of higher quality. On the other hand, in the case where only the coke powder is increased to 1 〇 mass%, the igniting only burns, the '· σ time is prolonged, and the southernmost reaching temperature also rises above the necessary temperature', which generates a large amount of low-intensity amorphous. The bismuth citrate causes a significant decrease in the strength and yield of the fracture. Moreover, in the case of 45 (TC heat preservation furnace, the improvement effect of the crack strength and the yield is small, which is substantially consistent with the results of the commercial equipment hitherto. According to the above description, when the diluted gaseous fuel is used, The gas is burned in the charging layer to expand the combustion zone in the layer, and a wide burning zone is formed by the combustion heat of the sintering raw material t coke and the heat of combustion of the diluted propane gas. , so that the highest combustion reaches the temperature 312 / invention manual (supplement) / 96_〇 1 / 95140218 40 丄: 529677 degrees will not be too high 'and the other side' for the high temperature area to maintain time, due to the combustion of the supplied dilution gas In the second place, the inventors and the like have an effect on the reduction and cold strength of the sintered ore of the finished product against the gas fuel diluted by the inventor, and the conventional method (5 mass%, 10 mass%) The coke and the hot air are compared and investigated. The measured project is the proportion of minerals in the finished sinter (affecting the cold rolling strength, being reduced) 'appearance specific gravity (affecting the cold rolling strength), below 0 5 coffee gas Pore size distribution (affecting the reduction property) First, Fig. 22 shows the results of investigation of the composition ratio of the mineral phase in the finished sintered ore quantification by the powder X-ray diffraction method. According to the figure, when the input heat is fixed (Coke 4% by mass + propane 〇 5 vol%), and when the solid fuel is used in combination with the diluted propane gas, calcium ferrite is stably formed, which is considered to cause an increase in the reductive property and an increase in the chilling strength. The measurement result of the specific gravity of the ore, and the measurement result of the pore diameter distribution of 〇·5 mm or less measured by the mercury intrusion meter is shown in Fig. 23. According to Fig. 22, the self-granulating particles are blown by blowing the diluted propane gas. The outside is heated, and as a result, the flow of the melt is promoted, and the porosity (appearance specific gravity) of 〇5 mm or more is lowered, so that it is considered to be an important cause of the cooling strength of the crucible. Further, according to Fig. 24, it is considered that the heat is input. By blowing the diluted propane gas in a fixed manner, the heat source in the sintered raw material particles can be reduced, so that fine pores of 5 Å or less or less from the ore which are affected by the reducing property are likely to remain. Therefore, the production of the highly reduced sintered ore can be carried out. Fig. 25 is a schematic view showing the sintering operation of (b) when only the coke is used and the diluent gas is blown together (b). Known only 312 / invention specification (supplement) / 96-0 / 95140218 1329677 in the knot, compared to the use of coke powder combustion from the simulation of particles ... in the coke + gas fuel of the present invention combined with the use of gaseous fuel combustion The outside of the simulated particles is added..., so it is easy to leave the fine-rolled holes in the inner ore of the ore, so it can be inferred that the ns-RI can be shifted to a higher position than the low RDI. - Figure 26 shows the blown into the diluted gas. ^ The idea of the stomata of the sinter in the burning of the body. As shown in the figure, in order to improve the production of sinter, it will promote the influence of the yield and the strength of the cold. .5_~5 is reduced with stomata, and several times, and the proportion of pupils above 5 coffees affecting ventilation is increased. It is also known that the ancient Μ, χ. Feng 獒 獒 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 烧结 。 。 。 According to the present invention, it can be considered that by diluting the diluted gaseous fuel, the ', 曰 structure. 』 According to the ideal sinter stomata two tables: grasp the limit coke ratio that can maintain the necessary cold strength (the limit limit The ratio of the ratio of the crushing strength to the coke ratio of the maximum material 7_ when the diluted == is not used. As shown in the S diagram, the dilution is 徭0/, + persimmon. Propane gas (concentration: 0.5 volume = used to obtain the same cold rolling strength as the current situation (the cracking strength (10) of the caribody is as shown in Fig. 27 (4), which can be reduced from 5 mass% to 3 mass% (about, / small As shown in Fig. 27(b) and (c), it can be understood that the households with a productivity of 73% and a productivity of ΐ86 are reduced to 3.5% by mass. The coke-ratio of 4, respectively, from 5 (four) As can be understood from the above description, the present invention relates to the amount of sound that is self-loaded into the layer along with the progress of the combustion and melting zone along with the 312/invention specification (supplement)/96-01/95140218 42 trolley, and appropriately 豨铿4 A _ a During the lower layer, according to the carbon material, the fuel can be supplied at an appropriate position after the fuel is selected, thereby achieving the heart; : The function of combustion and smelting zone function in the layer, which can improve the quality of the ore and improve the productivity. (Example) H 2 1. Perform the sintering pot test. 6 (H 5 body 2 coke oven gas (C gas) as a diluted gaseous fuel 〆i volume is small and the amount of carbon material (coke) in the raw material is set to 5 mass: in the experimental conditions (10) Section 37) is the same. The result is obvious. As shown in the figure, 'When using a rare C gas according to the method of the present invention', if the concentration of the c gas is increased, the width K of the combustion zone is large, and the yield and productivity are high. Increased and the cold strength was improved. (2) Only % Example 2. The test was carried out under the same conditions as in Example 1. The results are shown in ® 29. As shown in the figure, it is known to be used according to the method of the present invention. When the dilute propane gas (〇〇2 to 〇5 vol%) is increased, the concentration of the C gas is increased, the width of the combustion zone is remarkably enlarged, the yield and productivity are improved, and the cold rolling strength (SI) is also improved. (3) Example 3: This example uses the test pot shown in Fig. 6 with and without blowing In the case of the dilution gas, the coke oven gas (C gas) diluted with the cooler exhaust gas was blown from above the pot into the charging layer of the sintering raw material (including 20% by mass of the recovered ore) shown in Table 7. In the embodiment, the sintered layer contains 4.8 mass% to 5. 0 mass% of coke powder (planned number), as a suitable example of the present invention, the concentration is j. 〇 312 / invention specification ( Replenishment)/96-01/95140218 43 1329677 ~2·0% by volume (relative to air) c gas is blown into the surface of the loading layer under the conditions of suction pressure 12〇〇mmAq (differential pressure 1 000 Aq) 1〇〇~400 mm (the whole thickness is 6〇〇mm, the difference thickness is the 200th color of the bottom layer of the recovered layer). Further, regarding the above-described blowing position, when the entire length of the sinter sintering machine is 80 m, if it is applied to the entire height of 6 〇〇 mm, the blowing position of the test No. 2 is 1 〇〇 2 2 mm. , the equivalent of the following example: at a position of 80 (m) xl00 ~ 200 / 600 (mm) = 13. 3 (m) ~ 26. 6 (m), set the length of 13. 3m of the dilution gas into the exhaust The cover 12 is operated by a sintering machine. Therefore, the case where the blowing position of the test No. 2 is 2〇〇~goo mm is equivalent to the following case: • At a position of about 26.7 to 39.7 mm behind the ignition furnace on the sintering machine trolley, the length is still set to 133 ^ The diluent gas is blown into the fume hood 12 to perform gas injection.

312/發明說明書(補件)胸1/95140218 1329677 卜< 卜 33. 76 33. 76 Cv3 οά 1. 52 CS3 od CD S (4.8) C氣體 <=> 03 300-400 mm Ο 1000 CO 33. 76 CO CO CO 呀 οα <ΝΪ 1. 52 oo od O a S (4.8) c氣體 〇> csi 200-300 mm <=> 1000 LO CO CO CO CD CO CO 2.24 1 1. 52 <>a od C=5 o s (4.8) c氣體 〇 03 100-200 mm Ο 寸 1000 呀 CD CO CO CO CO CO 2.24 1. 52 od o s (4.9) c氣體 〇 f—^ 300-400 mm ο 1000 CO ◦ 卜 co CO <X) CO CO (Nl 〇〇· :1. 52 oa 卜 od CD s (4.9) c氣體 〇 200~300 mm CD 〇> ο <=> 03 CO CO CO CO CO CO 03 CO 1. 52 8.72 Q C3 G> CO (4.9) c氣體 ◦ 100-200 mm ◦ 1000 CO CO CO CD CO CO 2.24 1 οα LO 8.72 | O o (5.0) 無(基本) 1 1 <=> 1000 'No. 條件 '^ 豆石破 Yandi (-8 mm) 卡拉加斯破Carajas(-8 mm) 石夕石(-1 mm) 生石灰 石灰石(-3 mm) 回收礦 焦炭(-3 mm) 吹入氣體 濃度(體積%,相對於空氣) 供給位置(設表面為0 mm) 層厚(mm) 差壓(mmAq) 備考 噼S晚名玉 (辑 »w S呀 81SHS6/o.96/ff藥)_恶藏盔靡/Ζΐε 1329677 表8係表示該實施例(NO. 1〜NO. 7)之實施結果。根據該 實施結果可判斷,關於燒結礦之冷延強度(SI強度)及良 率,表示本發明之適合例所示之NO. 2〜NO. 7均高於作為 比較例之NO. 1,尤其在吹入位置位於裝入層中段之例 (NO. 3,4,6,7)中,改善效果顯著。又已知,與降低焦 '炭量以提高吹入氣體量之濃度相比,於固定焦炭量(4. 8 質量%)之基礎上,將吹入氣體濃度調整為1體積%時,生 產性變高。又已知,關於燒結礦之品質,最有效為下述吹 籲入方法:其與還原率(RI)、還原粉化率(RDI)—同,影響 吹入位置200〜300 mm之裝入層之中段。312/Invention Manual (supplement) chest 1/95140218 1329677 卜< Bu 33. 76 33. 76 Cv3 οά 1. 52 CS3 od CD S (4.8) C gas <=> 03 300-400 mm Ο 1000 CO 33. 76 CO CO CO 呀οα <ΝΪ 1. 52 oo od O a S (4.8) c gas 〇> csi 200-300 mm <=> 1000 LO CO CO CO CD CO CO 2.24 1 1. 52 <>a od C=5 os (4.8) c gas 〇03 100-200 mm Ο inch 1000 yeah CD CO CO CO CO CO 2.24 1. 52 od os (4.9) c gas 〇f—^ 300-400 mm ο 1000 CO ◦ 卜 co CO <X) CO CO (Nl 〇〇· : 1. 52 oa 卜 CD s (4.9) c gas 〇 200~300 mm CD 〇> ο <=> 03 CO CO CO CO CO CO 03 CO 1. 52 8.72 Q C3 G> CO (4.9) c gas ◦ 100-200 mm ◦ 1000 CO CO CO CD CO CO 2.24 1 οα LO 8.72 | O o (5.0) None (Basic) 1 1 <=> 1000 'No. Conditions'^ Bean stone broken Yandi (-8 mm) Caragas broken Carajas (-8 mm) Shi Xishi (-1 mm) Quicklime limestone (-3 mm) Reclaimed coke (- 3 mm) Injected gas concentration (% by volume, relative to air) Supply position (with surface 0 mm) Layer thickness (mm) Differential pressure (mmAq) ) 备 晚 晚 晚 晚 ( 辑 辑 w w w w w w w w w w w w w w w 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1329677 Table 8 shows the implementation results of this example (NO. 1 ~ NO. 7) According to the results of the implementation, it is judged that the cold rolling strength (SI strength) and the yield of the sintered ore are NO. 2 to NO. 7 which are suitable examples of the present invention are higher than the NO. 1, which is a comparative example. In the case where the blowing position is located in the middle section of the loading layer (NO. 3, 4, 6, 7), the improvement effect is remarkable. It is also known that, compared with the concentration of reducing the amount of charcoal to increase the amount of the blown gas, In addition to the fixed coke amount (4.8% by mass), when the blowing gas concentration is adjusted to 1% by volume, productivity is high. It is also known that, regarding the quality of sintered ore, the most effective method is the following blowing method: it has the same reduction rate (RI) and reduction pulverization rate (RDI), and affects the loading layer of the blowing position of 200 to 300 mm. Middle section.

312/發明說明書(補件)/96-01/95H0218 46 卜 C^> f* H 卜· <Τ3 CO 1.84 12.1 1.71 CO CO 0¾ CO CO 10.9 卜 D—’ | 73.8 I | 75.5 | CO cd 1 ι.6δ 1 1230 η 1270 L〇 1320 1 76.6 1 30.0 | 59.6 | LO σί CD 7.24 13.0 1.84 12.1 r-< r—< oo σ> o CNI CO CO czJ to 卜· f—< 73.5 L〇 1—< ι 1 卜 1230 1270 § 1320 ο 77.7 30.9 59.7 LT5 σ> L〇 7.04 卜 oi 1.80 11.8 1.67 ΙΛ 03 σ5 s CO 10.4 CO 卜· | 69.3 1 69.9 14.8 5 1230 1270 LD 1320 g 74.4 29.9 59.7 CT5 oo 7.20 12.7 1.80 11.8 1.67 1 05 CO C<l CO 10.5 CO 卜*’ 72.9 r- <J> CO τ*Η 1240 1280 m 1330 g 76.3 32.2 59.6 LTD 03 co 〇o CO 12.7 1.80 11.8 £ cn oo <NI CO 10.3 CO 卜· CO 72.6 CO 1240 1280 § 1330 s 寸 LO OO 30.8 59.7 10.1 OJ 6.93 12.7 1.80 11.8 1.67 00 01 另 CO 10.5 ς〇 c-_ 70.3 C=> cJ 03 L〇 r—H s 1240 1280 LO 寸 1330 g oo 31.6 59.0 CO CJ5 CO 12.7 1.80 11. δ 1.68 OO CO oo oa c=! L〇 卜* i 68.9 71.2 ' 15.9 1 [1.59 1250 1290 ir> 1360 § 67.4 29.3 59.5 OO ai _______ 實施 No. --. 原料水分(%) 裝入濕量(wet · kg) 裝入濕密度(wet · ton/m3) 裝入乾量(dry · kg) | k 8 點火前風壓(mmifcO) 廢氣溫度(°c) 燒成量(kg) 成品量(kg) SI強度(%) 成品良率(%) 1 燒結時間(分鐘) 1 1 •Η ¥ 最高到達溫度(°C) 高溫區域保持時間(>1200°C)(秒) ' 最高到達溫度(°C) 高溫區域保持時間(>1200°C)(秒) 最高到遠溫度(°C) 高溫區域保持時間(>1200°C)(秒) 還原率(RI) 還原粉化率(RDI) T.Fe(%) Fe0(%) 100〜200 C g c c ) 5 <1 C C C ? — 結果 位置 ^ 81SH s6/s-96/ff}紫)修盔恶Kagl/tNl ε 1329677 (4)實施例4 :該實施例係用以說明將本發明之燒結礦 之製造方法應用於日產i萬噸規模之DL型燒結機之例。 所使用之DL:^結機之機長為自點火爐至排礦部為止之卯 m。於該燒結機之點火爐後方約3〇1〇之位置處,設置有長 度(台車移動方向)為15 m、大小覆蓋整個機寬之氣體吹 入排煙罩,並且使用焦爐氣體(c氣體)作為氣體燃料。= .其不以該燒結機之原料裝入層之上層部分為目標,而在與 距離燃燒、熔融帶之存在位置3〇〇 mm相當之位置處,供 給有由常溫之空氣稀釋成濃度2體積%之c氣體,上述燃 燒、熔融帶係於裝入層層厚為6〇〇 mm(除回收礦厚度 则1以外)之條件下,行進至相當於距離裝入層厚度方向之 表層200 mm處。該吹入C氣體藉由調整燒結機台車下方 之風箱之吸引負壓,而通過燒結層到達上述位置,於燃 燒、熔融帶燃燒。再者,上述氣體吹入排煙罩内因大氣壓 而稍為正壓,由此使與上述風箱之吸引負壓平衡。此時C •氣體使用量為3, 000 m3 (標準狀態)/h。 該燒結機之操作、結果,使轉鼓強度全體較通常操作時 提高約3%,RDI亦較通常操作水平改善約3%,RI較通常 -操作時改善約4%。且生產率增加〇.03 t/hr · y。 【圖式簡單說明】 圖1係燒結製程之說明圖。 圖2係燒結層内之壓損與溫度分佈圖。 圖3係高生產時與低生產時之溫度分佈圖。 圖4(a)、(b)、(c)係燒結機内之溫度分佈與良率分佈 312/發明說明書(補件)/96-01/95140218 48 U29677 圖。 圖5係本發明產生之氣體燃料吹入製造之說明圖。 圖6係表示本电明方法之實驗結果的試驗銷内燃燒溶 融帶之推移圖(照片)。 圖7(a)至(d)係燒結鍋試驗結果之比較圖表。 圖8係氣體燃料燃燒極限之計算方法之說明圖。 圖9係表示燃燒之溫度依存性之說明圖。 圖係氣體燃料吹入時氣體種類之影響示意圖。 圖11(a)至(d)係表示吹入氣體濃度與碎裂強度、良率、 燒結時間、生產之關係之說明圖。 圖12係燒結反應之示意圖。 圖13係骸晶狀二次赤鐵礦之生成過程之示意圖。 圖14係吹入稀釋丙烷時燃燒極限之觀察圖(照片)。 圖15係表示吹入位置之影響之圖。 圖16(a)、(b)係表示吹入位置之影響之圖。 圖Π係燒結時層内溫度分佈之說明圖。 圖18係檢驗吹入位置之影響之結果的說明圖。 圖19係吹入稀釋丙烷時裝入層溫度(&)、廢氣溫度 (b)、通過風量(c)、廢氣組成(d)之經時變化圖。 圖20係稀釋丙烷吹入時與僅焦炭量增加時裝入層内 温度(a)、(a’)及廢氣溫度(b)、(b’)之經時變化圖。 圖21係表示各種吹入條件下之燒結特性試驗詰果圖。 圖22係表示各種吹人條件下,礦物組成比例之變化之 比較圖。 312/發明說明書(補件)/96-01/95140218 49 1329677 圖23係表示成品燒結礦之外觀比重之變化圖。 圖2 4係成品燒結礦中〇. 5 mm以下之氣孔徑分佈圖表。 圖25係僅使用焦炭時(a)與氣體吹入時(b)燒結動作之 不思圖。 圖26係稀釋氣體吹入時氣孔構造之示意圖。 圖27(a)、(b)、(c)係把握可維持冷延強度之極限焦炭 比之實驗結果圖。312/Invention Manual (supplement)/96-01/95H0218 46 Bu C^> f* H Bu· <Τ3 CO 1.84 12.1 1.71 CO CO 03⁄4 CO CO 10.9 Bu D—' | 73.8 I | 75.5 | CO cd 1 ι.6δ 1 1230 η 1270 L〇1320 1 76.6 1 30.0 | 59.6 | LO σί CD 7.24 13.0 1.84 12.1 r-<r-< oo σ> o CNI CO CO czJ to 卜· f—<73.5 L 〇1—< ι 1 Bu 1230 1270 § 1320 ο 77.7 30.9 59.7 LT5 σ> L〇7.04 卜 oi 1.80 11.8 1.67 ΙΛ 03 σ5 s CO 10.4 CO 卜 · | 69.3 1 69.9 14.8 5 1230 1270 LD 1320 g 74.4 29.9 59.7 CT5 oo 7.20 12.7 1.80 11.8 1.67 1 05 CO C<l CO 10.5 CO Bu*' 72.9 r- <J> CO τ*Η 1240 1280 m 1330 g 76.3 32.2 59.6 LTD 03 co 〇o CO 12.7 1.80 11.8 £ cn oo <NI CO 10.3 CO Bu·CO 72.6 CO 1240 1280 § 1330 s inch LO OO 30.8 59.7 10.1 OJ 6.93 12.7 1.80 11.8 1.67 00 01 Additional CO 10.5 ς〇c-_ 70.3 C=> cJ 03 L〇r-H s 1240 1280 LO inch 1330 g oo 31.6 59.0 CO CJ5 CO 12.7 1.80 11. δ 1.68 OO CO oo oa c=! L〇卜* i 68.9 71.2 ' 15.9 1 [1.59 1250 1290 ir> 1360 § 67.4 29.3 59.5 OO ai _______ Implementation No. --. Raw material moisture (%) Loading moisture (wet · kg) Loading wet density (wet · ton/m3) Loading dry weight (dry · kg) | k 8 Pre-ignition wind Pressure (mmifcO) Exhaust gas temperature (°c) Burning amount (kg) Finished product (kg) SI strength (%) Finished product yield (%) 1 Sintering time (minutes) 1 1 •Η ¥ Maximum reaching temperature (°C) High temperature zone hold time (>1200°C) (seconds) 'Maximum reach temperature (°C) High zone hold time (>1200°C) (seconds) Highest to far temperature (°C) High temperature zone hold time (&gt ; 1200 ° C) (seconds) reduction rate (RI) reduction pulverization rate (RDI) T.Fe (%) Fe0 (%) 100~200 C gcc ) 5 <1 CCC ? - result position ^ 81SH s6/s -96/ff}Purple) Helmet Kagl/tNl ε 1329677 (4) Example 4: This example is used to illustrate the application of the sinter manufacturing method of the present invention to a DL type sintering machine of a scale of 10,000 tons per day. An example. The DL used: The length of the machine is from the ignition furnace to the mine discharge. At a position about 3〇1〇 behind the ignition furnace of the sintering machine, a gas blowing hood having a length (tray moving direction) of 15 m and covering the entire width of the machine is provided, and coke oven gas (c gas) is used. ) as a gaseous fuel. = It does not target the upper layer of the raw material of the sintering machine, but is diluted with a normal temperature air to a concentration of 2 at a position equivalent to a distance of 3 〇〇mm from the burning and melting zone. % c gas, the above-mentioned combustion and melting zone is carried out under the condition that the layer thickness is 6 〇〇mm (except for the thickness of the recovered ore), and travels to a surface 200 mm away from the surface layer in the thickness direction of the loading layer. . The blown C gas is adjusted to the above-mentioned position by the sintering layer by adjusting the suction negative pressure of the bellows under the sintering machine trolley, and is burned in the combustion and melting zone. Further, the gas is blown into the fume hood to be slightly positively pressurized by the atmospheric pressure, thereby balancing the suction negative pressure with the bellows. At this time, C • gas usage is 3,000 m3 (standard state) / h. The operation of the sintering machine, as a result, increased the drum strength by about 3% as compared with the usual operation, the RDI was improved by about 3% compared with the usual operation level, and the RI was improved by about 4% compared with the usual - operation. And productivity increased by 03.03 t/hr · y. [Simple description of the drawing] Fig. 1 is an explanatory diagram of the sintering process. Figure 2 is a graph of pressure loss and temperature distribution in a sintered layer. Figure 3 is a graph of temperature distribution at high production and low production. Figure 4 (a), (b), (c) is the temperature distribution and yield distribution in the sintering machine 312 / invention specification (supplement) / 96-01/95140218 48 U29677 figure. Fig. 5 is an explanatory view showing the manufacture of a gaseous fuel blow-in produced by the present invention. Fig. 6 is a transition view (photograph) showing the combustion melting zone in the test pin of the experimental result of the present invention. Figures 7(a) to (d) are comparative charts of the results of the sintering pot test. Fig. 8 is an explanatory diagram of a calculation method of a gas fuel combustion limit. Fig. 9 is an explanatory view showing the temperature dependence of combustion. The figure is a schematic diagram of the influence of the gas type when the gaseous fuel is blown. 11(a) to 11(d) are explanatory views showing the relationship between the concentration of the blown gas and the fracture strength, the yield, the sintering time, and the production. Figure 12 is a schematic illustration of a sintering reaction. Figure 13 is a schematic illustration of the formation process of twin crystalline hematite. Fig. 14 is a view (photograph) of the burning limit when the diluted propane is blown. Fig. 15 is a view showing the influence of the blowing position. Fig. 16 (a) and (b) are views showing the influence of the blowing position. Figure 说明 is an explanatory diagram of the temperature distribution in the layer during sintering. Fig. 18 is an explanatory diagram showing the result of examining the influence of the blowing position. Fig. 19 is a graph showing the change with time of the layer temperature (&), the exhaust gas temperature (b), the passing air volume (c), and the exhaust gas composition (d) when the diluted propane is blown. Fig. 20 is a graph showing the change with time in the temperature (a), (a') and the temperature (b) of the exhaust gas when the amount of the coke is increased during the blowing of the diluted propane. Fig. 21 is a graph showing the results of a test for sintering characteristics under various blowing conditions. Fig. 22 is a graph showing a comparison of changes in the composition ratio of minerals under various blowing conditions. 312/Invention Manual (Supplement)/96-01/95140218 49 1329677 Figure 23 is a graph showing the change in the apparent specific gravity of the finished sintered ore. Figure 2 shows the pore size distribution chart of 〇. 5 mm or less in the finished sinter. Fig. 25 is a view showing the case where only coke is used (a) and when the gas is blown (b). Fig. 26 is a schematic view showing the configuration of the pores when the diluent gas is blown. Fig. 27 (a), (b), and (c) are graphs showing experimental results of the limit coke ratio at which the cold rolling strength can be maintained.

圖28係表示實施例1之結果圖(照片)。 圖29係表示實施例2之結果圖(照片)。 【主要元件符號說明】 1 原料漏斗 2 圓筒混合機 3 回轉爐 4 ' 5 接料桶 6 筒式給料機 7 切割槽 8 台車 9 裝入層 10 點火爐 11 風箱 12 氣體燃料供給裝置(排煙罩) 12a 氣體吹入喷嘴 312/發明說明書(補件)/96-01/95140218 50Fig. 28 is a view showing the result (photograph) of Example 1. Fig. 29 is a view showing the result (photograph) of Example 2. [Explanation of main component symbols] 1 Raw material funnel 2 Cylinder mixer 3 Rotary furnace 4 ' 5 Feeding tank 6 Cartridge feeder 7 Cutting trough 8 Pallet 9 Loading layer 10 Ignition furnace 11 Bellows 12 Gas fuel supply device (row Hood) 12a gas injection nozzle 312 / invention manual (supplement) / 96-01/95140218 50

Claims (1)

1 曰拉旮浍頁 APR 2 7 2010 替換本 1329677 ^ 1 十、申請專利範圍: 1. 一種燒結礦之製造方法,包含下述步驟: 裝入步驟,於循環移動之台車上,裝入包含粉礦石與炭 材之燒結原料,使於台車上形成含有炭材之裝入層; 點火步驟,於點火爐中對裝入層表面之炭材進行點火; 燒成步驟,通過配置於台車下之風箱而吸引空氣,使裝 入層中之炭材燃燒,並且利用所產生之燃燒熱而生成燒結 0塊;以及 氣體燃料燃燒步驟,自裝入層之上方供給稀釋成燃燒下 限濃度以下之氣體燃料,使上述氣體燃料於裝入層内燃 燒, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方 .供給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃 料於裝入層内燃燒,且調整裝入層内之最高到達溫度、裝 入層内之高溫區域保持時間、或者裝入層内之最高到達溫 籲度與高溫區域保持時間。 2. 如申請專利範圍第1項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 ' 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 • 於裝入層内燃燒,且調整裝入層内之最高到達溫度。 3. 如申請專利範圍第2項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 於裝入層内燃燒,且藉由調整燒結原料中之炭材量而調整 95140218 51 1329677 料叫日修正観 裝入層内之最高到達溫度。 4. 如申請專利範圍第3項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 於裝入層内燃燒,且藉由調整燒結原料中之炭材量,而將 上述最高到達溫度調整為1205°C〜1 350°C。1 曰拉旮浍 page APR 2 7 2010 Replacement 1329677 ^ 1 10, the scope of application: 1. A method of manufacturing sinter, comprising the following steps: loading step, on the trolley for circulating movement, containing powder The sintering material of the ore and the carbon material is used to form a charging layer containing the carbon material on the trolley; the ignition step is to ignite the carbon material on the surface of the layer in the ignition furnace; the firing step is performed by the wind disposed under the trolley The box attracts air, burns the carbon material in the layer, and generates the sintered 0 piece by using the generated heat of combustion; and the gas fuel burning step, supplies the gas fuel diluted below the lower limit of combustion concentration from above the charged layer The gas fuel is combusted in the charging layer, and the gas fuel burning step includes an operation of supplying a gaseous fuel diluted to a lower concentration of combustion below the self-loading layer to cause the gaseous fuel to burn in the charging layer. And adjusting the highest reaching temperature in the loading layer, the high temperature region holding time in the loading layer, or the highest reaching temperature and temperature in the loading layer Domain hold time. 2. The method for producing a sintered ore according to the first aspect of the invention, wherein the gas fuel burning step comprises the operation of: supplying a gas fuel that is diluted to a lower concentration of a lower combustion limit than a gas layer above the charging layer; Fuel • Burns in the loading zone and adjusts the maximum temperature reached in the loading zone. 3. The method for producing a sintered ore according to the second aspect of the invention, wherein the gas fuel burning step includes the operation of supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer, and the gaseous fuel is The inner layer is burned in the layer, and the maximum temperature reached in the layer is adjusted by adjusting the amount of the carbon material in the sintered raw material by adjusting the amount of the carbon material in the sintered raw material. 4. The method for producing a sintered ore according to claim 3, wherein the gas fuel burning step includes an operation of supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer to cause the gaseous fuel to be The inside of the layer is burned, and the above-mentioned maximum reaching temperature is adjusted to 1205 ° C to 1 350 ° C by adjusting the amount of the carbon material in the sintering raw material. 5. 如申請專利範圍第2項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 於裝入層内燃燒,且藉由調整氣體燃料之供給量,而將上 述最高到達溫度調整為1205°C〜1350°C。 6. 如申請專利範圍第2項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 於裝入層内燃燒,且藉由調整燒結原料甲之炭材量與氣體 燃料之供給量,而將上述最高到達溫度調整為1205°C〜 1350。。。 7. 如申請專利範圍第1項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 於裝入層内燃燒,且調整裝入層内之高溫區域保持時間。 8. 如申請專利範圍第7項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體燃料 95140218 52 1329677 -βΗ月/日1 於裝入層内燃燒,且根據燒結原料4之炭4 t來.铜整上述 氣體燃料之濃度,並且調整裝入層内之嵩溫區域保持時 間。 9.如申請專利範圍第1項之燒結礦之製造方法,其中, 上述氣體燃料燃燒步驟包含下述動作:自裝入層之上方供 給稀釋成燃燒下限濃度以下之氣體燃料,使稀釋成燃燒下 ' 限濃度以下之氣體燃料燃燒,以使至少其一部分以維持未 |燃燒之狀態而到達上述裝入層中之燃燒、炫融帶。 1 〇.如申請專利範圍第1項之燒結礦之製造方法,其 中,上述氣體燃料燃燒步驟包含下述動作:自裝入層之上 方供給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體 燃料於裝入層内燃燒,以調整燃燒、熔融帶之形態。 11.如申請專利範圍第10項之燒結礦之製造方法,其 中,上述燃燒、熔融.帶之形態調整係指調節該帶域之高度 方向之厚度及/或台車移動方向之寬度。 • 12.如申請專利範圍第1項之燒結礦之製造方法,其 中,上述氣體燃料燃燒步驟包含下述動作:自裝入層之上 方供給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體 • 燃料於裝入層内燃燒,以延長燃燒、熔融帶之高溫保持時 . 間,調整燒結礦之冷延強度。 13.如申請專利範圍第1項之燒結礦之製造方法,其 中,上述氣體燃料燃燒步驟包含下逑動作:自裝入層之上 方供給稀釋成燃燒下限濃度以下之氣體燃料,使上述氣體 燃料於裝入層内燃燒,且調整上述氣體燃料對裝入層之供 95140218 53 1329677 給位置 14.如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:於點火爐後之 位置處’自裝入層之上方供給稀釋成燃燒下限濃度以下之 氣體燃料,使上述氣體燃料於裝入層内燃燒。 15 ·如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:自於裝入層之5. The method for producing a sintered ore according to the second aspect of the invention, wherein the gas fuel combustion step comprises the operation of supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer to cause the gaseous fuel to be The inside of the layer is burned, and the above-mentioned maximum reaching temperature is adjusted to 1205 ° C to 1350 ° C by adjusting the supply amount of the gaseous fuel. 6. The method for producing a sintered ore according to the second aspect of the invention, wherein the gas fuel burning step comprises the operation of supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer, and the gaseous fuel is The inner layer is burned in the layer, and the maximum reaching temperature is adjusted to 1205 ° C to 1350 by adjusting the amount of the carbon material of the sintered raw material A and the supply amount of the gaseous fuel. . . 7. The method for producing a sintered ore according to claim 1, wherein the gas fuel burning step includes the operation of supplying a gaseous fuel diluted to a lower limit of combustion concentration or higher from above the charging layer to cause the gaseous fuel to be The inner layer is burned in the layer and the high temperature region within the packed layer is adjusted to maintain time. 8. The method for producing a sintered ore according to claim 7, wherein the gas fuel burning step includes the operation of supplying a gaseous fuel diluted to a lower limit of combustion concentration or higher from above the charging layer to make the gaseous fuel 95140218 52 1329677 - βΗ月/日 1 is burned in the charging layer, and according to the carbon 4 4 of the sintering raw material 4, the concentration of the above gaseous fuel is adjusted, and the temperature in the temperature region of the charging layer is adjusted. 9. The method for producing a sintered ore according to claim 1, wherein the gas fuel burning step comprises the operation of supplying a gaseous fuel diluted to a lower concentration of combustion below the charged layer to be diluted into a combustion. The gaseous fuel below the concentration limit is burned so that at least a portion thereof reaches the combustion and smelting zone in the above-mentioned packed layer while maintaining the state of not being burned. The method for producing a sintered ore according to the first aspect of the invention, wherein the gas fuel burning step comprises the operation of supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer to make the gaseous fuel It is burned in the packed layer to adjust the form of combustion and melting zone. 11. The method of producing a sintered ore according to claim 10, wherein the shape of the burning and melting zone is adjusted to adjust the thickness of the zone in the height direction and/or the width of the trolley moving direction. 12. The method for producing a sintered ore according to claim 1, wherein the gas fuel burning step comprises the operation of supplying a gas fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer to make the gas The fuel is burned in the packed bed to prolong the combustion and the high temperature retention of the molten zone to adjust the cold rolling strength of the sintered ore. 13. The method of producing a sintered ore according to claim 1, wherein the gas fuel burning step comprises a squatting operation: supplying a gaseous fuel diluted to a lower concentration of a lower combustion concentration from above the charging layer, so that the gaseous fuel is The method of manufacturing the sintered ore of the first aspect of the present invention, wherein the gas fuel burning step comprises the following actions: : The gaseous fuel diluted to a lower concentration of the lower combustion concentration is supplied above the self-loading layer at a position after the ignition furnace, and the gaseous fuel is burned in the charging layer. 15. The method of manufacturing a sintered ore according to claim 1, wherein the step of burning the gas fuel comprises the following actions: from loading the layer 表層部生成燒結塊起直至燒結完成之期間,供給稀釋成燃 k下限濃度以下之氣體燃料’使上述氣體燃料於裝入層内 燃燒。 16.如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:於燃燒、熔融 π之厚度為15 mm以上之區域中,供給稀釋成燃燒下限濃 度以下之氣體燃料,使上述氣體燃料於裝入層内燃燒。 17·如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:於燃燒前線達 到表層下1 〇〇 mm之位置後,供給豨釋成燃燒下限濃度以 下之氣體燃料’使上述氣體燃料於裝入層内燃燒。 18.如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:於該裝入層之 兩側壁附近’供給稀釋成燃燒下限濃度以下之氣體燃料, 使上述氣體燃料於裝入層内燃燒。 19·如申請專利範圍第1項之燒結礦之製造方法,其 令’上述氣體燃料燃燒步驟包含下述動作:於燒結機長度 95140218 54 IJ29677 |---------— 方向上’自裝入層之上 氣體燃料’使上述氣體 礦之冷延強度。 月’修正替換頁丨 方供給稀釋成燃燒下限濃度以下之 燃料於燒結層内燃燒,且調整燒結 如申請專利範圍第】項之燒結 豆 t,上述氣體燃料係濃产豨 '、 …上之可燃性1:成燃燒下限濃度之75%以下 21. 如二請專利範圍第9項之燒結礦之製造方法,其 ’。上述軋體燃料係濃度稀釋成燃燒下限濃度之60%以下 且2%以上之可燃性氣體。 22. 如申請專利範圍第1()項之燒結礦之製造方法,其 令’上述氣體燃料係濃度稀釋成燃燒下限濃度之25%以下 且2%以上之可燃性氣體。 23. 如申請專利範圍第1項之燒結礦之製造方法,其 令,上述氣體燃料係選自由高爐氣體、焦爐氣體、高爐與 焦爐混合氣體、丙烧氣體、天然氣以及曱貌氣體所組成之 群組中之至少一種氣體。 24.種燒結機,係具備循環移動之台車、配設於上述 台車之下方之吸引用風m向台車上供給燒結原料之 原料供給裝置、以及用以對燒結原料中之炭材進行點火之 點火爐,其特徵在於:於上述點火爐之下游側,配設有氣 體燃料供給裝置,用以自裝人層之上方,將濃度已稀釋成 燃燒下限濃度以下之氣體燃料吹入到該襄入層中, 上述氣體燃料供給裝置供給有濃度稀釋成燃燒下限濃 度之75%以下且2%以上之可燃性氣體。 95140218 55 1329677 . . .......... 日修正替換莨 25. 如申請專利範圍第24項之燒結機,,上述氣體 燃料供給裝置係於點火爐下游側之燒結機之機長方向 上,至少配設有一個以上。 26. 如申請專利範圍第24項之燒結機,其中,上述氣體 燃料供給裝置於台車行進方向上,配設於自燃燒前線行進 至表層下方之階段直至燒結完成之間之位置處。 ' 27.如申請專利範圍第24項之燒結機,其中,上述氣體 #燃料供給裝置配設於側壁附近。 28.如申請專利範圍第24項之燒結機,其中,上述氣體 燃料供給裝置供給有濃度稀釋成燃燒下限濃度之60%以下 且2%以上之可燃性氣體。 - 29.如申請專利範圍第28項之燒結機,其中,上述氣體 . 燃料供給裝置供給有濃度稀釋成燃燒下限濃度之25%以下 且2%以上之可燃性氣體。The surface portion is formed into a sintered block until the completion of sintering, and the gaseous fuel is supplied to be diluted to a lower concentration of the lower limit of combustion, and the gaseous fuel is burned in the packed bed. 16. The method for producing a sintered ore according to claim 1, wherein the step of burning the gas fuel comprises the following operation: in a region where the thickness of the combustion and melting π is 15 mm or more, the supply is diluted to a lower concentration of combustion. The gaseous fuel below burns the gaseous fuel in the charging layer. 17. The method of manufacturing a sintered ore according to claim 1, wherein the step of burning the gas fuel comprises the following action: after the front line of the combustion reaches a position of 1 〇〇 mm below the surface layer, the supply is released into a lower combustion concentration. The following gaseous fuel 'burns the above gaseous fuel in the charging layer. 18. The method of manufacturing a sintered ore according to claim 1, wherein the step of burning the gas fuel comprises the step of: supplying a gaseous fuel diluted to a lower concentration of combustion below a lower side wall of the packed layer, The gaseous fuel is burned in the charging layer. 19. The method of manufacturing a sintered ore according to claim 1, wherein the step of burning the gas fuel comprises the following actions: in the length of the sintering machine 95140218 54 IJ29677 |----------direction The gaseous fuel above the self-loading layer 'cools the strength of the gas ore described above. The monthly 'correction replacement page' is supplied with a fuel diluted below the lower combustion limit concentration to be burned in the sintered layer, and the sintering is adjusted as in the case of the patented scope of the sintered bean t, and the gas fuel system is rich in flammable 、', ... Sex 1: It is less than 75% of the lower limit of the combustion concentration. 21. The manufacturing method of the sinter of the ninth patent scope is as follows. The rolling body fuel is diluted to a concentration of 60% or less of the lower limit of combustion and 2% or more of the combustible gas. 22. The method for producing a sintered ore according to the first aspect of the invention, wherein the gas fuel system is diluted to a concentration of 25% or less and 2% or more of the combustible gas. 23. The method of manufacturing a sintered ore according to claim 1, wherein the gaseous fuel is selected from the group consisting of blast furnace gas, coke oven gas, blast furnace and coke oven mixed gas, propane gas, natural gas, and sulphur gas. At least one gas in the group. 24. A sintering machine comprising: a trolley for circulating movement; a raw material supply device for supplying a sintering raw material to a trolley disposed below the trolley; and a point for igniting the carbon material in the sintering raw material The furnace is characterized in that: on the downstream side of the ignition furnace, a gas fuel supply device is disposed for blowing a gas fuel whose concentration has been diluted to a lower concentration of combustion below the self-installation layer to the intrusion layer In the gas fuel supply device, the combustible gas having a concentration diluted to 75% or less and 2% or more of the lower limit of the combustion concentration is supplied. 95140218 55 1329677 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . At least one or more are provided. 26. The sintering machine of claim 24, wherein the gas fuel supply device is disposed in a traveling direction of the bogie at a position from the front of the combustion front to a lower portion of the surface layer until the completion of sintering. 27. The sintering machine of claim 24, wherein the gas #fuel supply device is disposed adjacent to the side wall. The sintering machine according to claim 24, wherein the gas fuel supply device supplies a combustible gas having a concentration diluted to 60% or less and 2% or more of a lower limit of combustion concentration. The sintering machine according to claim 28, wherein the fuel supply device supplies a combustible gas having a concentration diluted to 25% or less and 2% or more of a lower limit of combustion concentration. 95140218 5695140218 56
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