JPS6261642B2 - - Google Patents
Info
- Publication number
- JPS6261642B2 JPS6261642B2 JP1898986A JP1898986A JPS6261642B2 JP S6261642 B2 JPS6261642 B2 JP S6261642B2 JP 1898986 A JP1898986 A JP 1898986A JP 1898986 A JP1898986 A JP 1898986A JP S6261642 B2 JPS6261642 B2 JP S6261642B2
- Authority
- JP
- Japan
- Prior art keywords
- furnace
- temperature
- metal wire
- blast furnace
- probe
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 229910052751 metal Inorganic materials 0.000 claims description 29
- 239000002184 metal Substances 0.000 claims description 29
- 230000008018 melting Effects 0.000 claims description 20
- 238000002844 melting Methods 0.000 claims description 20
- 239000000523 sample Substances 0.000 claims description 19
- 238000009826 distribution Methods 0.000 claims description 16
- 238000005259 measurement Methods 0.000 claims description 11
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 claims description 9
- 238000001514 detection method Methods 0.000 claims description 9
- 238000000034 method Methods 0.000 claims description 8
- 230000001681 protective effect Effects 0.000 claims description 6
- 229910052759 nickel Inorganic materials 0.000 claims description 4
- 229910000831 Steel Inorganic materials 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 239000010959 steel Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000003780 insertion Methods 0.000 description 2
- 230000037431 insertion Effects 0.000 description 2
- 239000011819 refractory material Substances 0.000 description 2
- 229910018072 Al 2 O 3 Inorganic materials 0.000 description 1
- 229910000809 Alumel Inorganic materials 0.000 description 1
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- LIXXICXIKUPJBX-UHFFFAOYSA-N [Pt].[Rh].[Pt] Chemical compound [Pt].[Rh].[Pt] LIXXICXIKUPJBX-UHFFFAOYSA-N 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 230000005496 eutectics Effects 0.000 description 1
- 239000000945 filler Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 239000006104 solid solution Substances 0.000 description 1
- 239000002344 surface layer Substances 0.000 description 1
- 238000007751 thermal spraying Methods 0.000 description 1
Landscapes
- Measuring Temperature Or Quantity Of Heat (AREA)
- Blast Furnaces (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、高炉、シヤフト炉等の操業中に炉内
装入物が荷下りする炉の炉内状況、特に高炉内の
1400〜1500℃の軟化融着帯内部形状を検知するこ
とを可能とする技術に関する。Detailed Description of the Invention (Industrial Field of Application) The present invention is intended to investigate the conditions inside a furnace where the contents of the furnace are unloaded during the operation of a blast furnace, shaft furnace, etc.
This invention relates to a technology that makes it possible to detect the internal shape of a softened cohesive zone at 1400 to 1500°C.
(従来の技術)
特公昭57−48621、実公昭60−28678、実公昭60
−28679には高炉の炉内状況把握方法とその装置
が開示されている。温度に限ると、特公昭57−
48621は、硬質保護管の長さ方向に沿つて複数の
温度感知部を形成した測定プローブを高炉内装入
原料の表層上へ半径方向に載置し、荷下りにつれ
て測定プローブを降下させながら、上記温度感知
部の到達点において温度を測定し、得られた測定
値に基づいて炉内状況を把握するものである。す
なわち垂直水平測定プローブを使用し高炉内の温
度分布を垂直、水平方向の2次元で測定してい
る。(Prior technology) Special Publication No. 57-48621, Publication No. 1986-28678, Publication No. 1986-28678, Publication No. 1987-28678, Publication No. 1987-28678
-28679 discloses a method and device for grasping the situation inside a blast furnace. As far as temperature is concerned, the
48621, a measuring probe with a plurality of temperature sensing parts formed along the length direction of a hard protective tube is placed radially on the surface layer of the raw material input into the blast furnace, and the measuring probe is lowered as the load is unloaded. The temperature is measured at the point reached by the temperature sensor, and the situation inside the furnace is determined based on the measured value. That is, a vertical and horizontal measurement probe is used to measure the temperature distribution within the blast furnace in two dimensions, vertical and horizontal.
(発明が解決しようとする問題点)
前記従来技術の垂直水平プローブは温度感知部
として熱電対を取付けて測温している。熱電対と
してはクロメル―アルメル(CA)、白金―白金ロ
ジウム(Pt―PtRk)等の各種シース熱電対があ
るが、再使用不能のため、コスト的に安価なCA
シース熱電対が用いられている。しかしCA熱電
対は正確な測温は1200℃位までしかできず、従つ
て高炉内の温度分布形状は軟化融着帯の外部まで
知り得るに留つていた。(Problems to be Solved by the Invention) The vertical and horizontal probes of the prior art measure temperature by attaching a thermocouple as a temperature sensing section. There are various sheathed thermocouples such as chromel-alumel (CA) and platinum-platinum rhodium (Pt-PtRk), but CA is less expensive because it cannot be reused.
A sheathed thermocouple is used. However, CA thermocouples can only accurately measure temperatures up to about 1200°C, and therefore the shape of the temperature distribution inside the blast furnace can only be known to the outside of the softened cohesive zone.
本発明は、0〜1200℃範囲だけでなく、1400〜
1500℃範囲の軟化融着帯の内部形状の測定を可能
とする手段を提供することを目的とする。 The present invention can be used not only in the 0-1200℃ range but also in the 1400-1400℃ range.
The purpose of this invention is to provide a means that enables measurement of the internal shape of a softened cohesive zone in the 1500°C range.
(問題点を解決するための手段、作用、実施例)
前記目的は、本発明においては、金属素線の溶
断によつて溶断位置の温度の検知を可能とするこ
とにより達成される。そのため金属素線としては
溶融温度が既知の金属を使用する。特に溶融温度
の幅のない純金属を使用することによつて正確な
測定が可能となる。素線金属としては測定温度範
囲を考慮して選択する。(Means, effects, and embodiments for solving the problems) The above object is achieved in the present invention by making it possible to detect the temperature at the melting point by cutting the metal wire. Therefore, a metal whose melting temperature is known is used as the metal wire. Particularly accurate measurement is possible by using a pure metal with a wide range of melting temperatures. The wire metal is selected in consideration of the measurement temperature range.
すなわち、本発明の高炉の炉内状況の検知方法
は、構成としては、高炉の炉内状況の検知のた
め、炉内装入物上に半径方向に載置され荷下りと
ともに降下する測定プローブとして保護シース内
に溶融温度が既知の金属素線を充填物中に埋蔵し
て折返し状に内装しプローブ内に収容し、金属素
線の閉路先端を検知管の所定位置の検知孔から露
出させその開路基端から通電状態として使用し、
金属素線の露出閉端の溶断による通電の遮断によ
り金属素線の溶断温度を以つて炉内の溶断位置の
温度と判定し、その各炉内位置のプロツトにより
当該温度分布線を得て炉内状況を検知することを
特徴とする。特に金属素線は例えば純ニツケルを
使用しその溶融温度1453℃の温度分布線を得るこ
とにより炉内の軟化融着帯の内部の把握を可能と
する。 That is, the method for detecting the inside condition of a blast furnace according to the present invention has a structure in which, in order to detect the inside condition of a blast furnace, a protective measuring probe is placed on the contents in the furnace in the radial direction and lowered as the load is unloaded. A metal wire with a known melting temperature is buried in the filling inside the sheath, folded inside the probe, and housed in the probe. Used as energized from the base end,
The melting temperature of the metal wire is determined to be the temperature at the melting point in the furnace by cutting off the current by fusing the exposed closed end of the metal wire, and the temperature distribution line is obtained by plotting each position in the furnace. It is characterized by detecting the internal situation. In particular, by using a metal wire such as pure nickel and obtaining a temperature distribution line with a melting temperature of 1453°C, it is possible to understand the inside of the softened cohesive zone in the furnace.
以下、本発明方法を第1〜6図を参照し実施例
に即して具体的に説明する。 Hereinafter, the method of the present invention will be specifically explained based on examples with reference to FIGS. 1 to 6.
本発明において使用する測温素子1の1つの基
本形を第1図に示す。 One basic form of the temperature measuring element 1 used in the present invention is shown in FIG.
金属保護シース2内に金属素線3をMgO,
Al2O3等の耐熱性、絶縁性の充填物4とともに詰
め伸線してつくる。金属素線3は保護シース内の
充填物中に折返し状に埋蔵されその一端は溶断予
定の閉路先端3aとなり、他端は通電のための開
口基端3bとなる。 The metal wire 3 is placed in the metal protective sheath 2 with MgO,
It is made by filling it with a heat-resistant and insulating filler 4 such as Al 2 O 3 and drawing it. The metal wire 3 is buried in a folded manner in the filling in the protective sheath, one end of which becomes a closed circuit tip 3a to be fused, and the other end becomes an open base end 3b for energization.
金属素線3は溶融温度が既知であり溶融温度幅
のないあるいは小さい純金属、共晶点組成合金等
を選択し、本発明の測温範囲に対しては例えば溶
融温度1453℃の純ニツケルを使用する。線径は
0.5〜2mm程度でよい。 For the metal wire 3, select a pure metal whose melting temperature is known and has no or small melting temperature range, an alloy with a eutectic point composition, etc. For example, pure nickel with a melting temperature of 1453°C is selected for the temperature measuring range of the present invention. use. The wire diameter is
Approximately 0.5 to 2 mm is sufficient.
この測温素子1の所要数を第2図に示すように
鋼管5内に収容し鋼管の長さ方向の所定の水平測
定位置に検知孔6を設け、各検知孔6から各金属
素線3の閉端3aを露出させて測定プローブ7と
する。 As shown in FIG. 2, the required number of temperature measuring elements 1 are accommodated in a steel pipe 5, and detection holes 6 are provided at predetermined horizontal measurement positions in the length direction of the steel pipe. The closed end 3a of the probe is exposed to form a measurement probe 7.
この測定プローブ7を高炉8内の頂部のすりば
ち状となつた炉内装入物9の上面に、例えば実公
昭56−28678に示す挿入装置10を使用する等し
て半径方向の姿勢として先端が炉内中心に、基端
が炉壁耐火物11の近くに位置するようにして載
置し、次の装入物の装入により埋蔵状態とし、操
業に伴う炉内装入物の荷下りとともに降下して垂
直方向の検出が可能なようにする。降下に追随す
るため各金属素線3の基端3bは接続線12に接
続され、接続線12を炉外のデツキ13上に導き
ドラム14に巻付け検出装置15により検出を実
施する。 This measuring probe 7 is placed on the upper surface of the mortar-shaped furnace contents 9 at the top of the blast furnace 8, for example by using an insertion device 10 shown in Japanese Utility Model Publication No. 56-28678, so that the tip is placed in the radial direction. It is placed in the center of the furnace with its base end located near the furnace wall refractories 11, and is placed in a buried state by charging the next charge, and is lowered as the furnace charges are unloaded during operation. to enable vertical detection. In order to follow the descent, the base end 3b of each metal wire 3 is connected to a connecting wire 12, and the connecting wire 12 is guided onto a deck 13 outside the furnace, wound around a drum 14, and detected by a detection device 15.
金属素線3の開端3bに電圧とかけると金属素
線3に電流が流れ、その閉端3aが溶断すると電
流が遮断されるので、検出装置15により断線の
起つたことを検知できる。金属素線の溶融温度
を、炉内の溶断が起つた個所の雰囲気温度と判断
する。 When a voltage is applied to the open end 3b of the metal wire 3, a current flows through the metal wire 3, and when the closed end 3a melts, the current is cut off, so that the detection device 15 can detect that a wire breakage has occurred. The melting temperature of the metal wire is determined to be the atmospheric temperature at the location in the furnace where the melting occurs.
測定プローブ7に例えば第2図に示すように高
炉内の中心、中間および周辺に該当する位置に検
知孔6を設けてそれぞれ純ニツケルの金属素線の
閉端3a,3a′および3a″を露出させてある場
合、第4図に示す3位置の高さ方向の温度分布
T,T′およびT″のもとで、素線閉端の溶断は各
温度分布線T,T′およびT″と1453℃線の交点
t,t′およびt″で起る。この溶断高さおよび該当
位置のプロツトにより第5図に示すように1453℃
の温度分布線Xを得ることができる。 For example, as shown in FIG. 2, detection holes 6 are provided in the measurement probe 7 at positions corresponding to the center, middle, and periphery of the blast furnace to expose the closed ends 3a, 3a', and 3a'' of pure nickel metal wires, respectively. In this case, under the temperature distributions T, T' and T'' in the three positions shown in Fig. 4 in the height direction, the melting of the closed end of the strand will occur as per the temperature distribution lines T, T' and T''. It occurs at the intersections t, t' and t'' of the 1453°C lines. As shown in Figure 5, the height of the melting point and the plot of the corresponding position indicate that the temperature is 1453℃.
A temperature distribution line X can be obtained.
実公昭60−28678に開示の技術によればCA熱電
対を使用して高炉内温度分布を測定して第5図に
示す室温〜1200℃の温度分布線Yが得られる。こ
の温度分布線X,Yの組合わせによつて従来1200
〜1450℃といわれている軟化融着帯の全体の形状
が明らかになる。この場合、測定プローブは第6
図に示すように各検知孔6にCA熱電対16,1
6′および16″を素線閉端3a,3a′および3
a″とともに露出させて両方の測定を行うようにす
ることができる。 According to the technique disclosed in Japanese Utility Model Publication No. 60-28678, the temperature distribution inside the blast furnace is measured using a CA thermocouple, and a temperature distribution line Y from room temperature to 1200° C. shown in FIG. 5 can be obtained. The combination of these temperature distribution lines
The overall shape of the softened cohesive zone, which is said to be at ~1450°C, becomes clear. In this case, the measuring probe is the sixth
As shown in the figure, CA thermocouples 16 and 1 are installed in each detection hole 6.
6' and 16'' to the closed wire ends 3a, 3a' and 3
can be exposed along with a″ so that both measurements are taken.
前記のように本発明方法では金属素線3は知り
度い温度域によつて金属の種類を変更する。例え
ば高炉内の軟化融着帯形状の把握には純ニツケル
が適当であるが、還元性雰囲気のもとでは炭素を
固溶することによつて溶融点温度が変化するの
で、その対策としてシースを施したりあるいは金
属素線に溶射等を施して被覆したりして使用す
る。 As described above, in the method of the present invention, the type of metal in the metal wire 3 is changed depending on the known temperature range. For example, pure nickel is suitable for determining the shape of the softened cohesive zone in a blast furnace, but in a reducing atmosphere, the melting point temperature changes due to the solid solution of carbon, so a sheath is used as a countermeasure. It is used by coating the metal wire by applying thermal spraying or the like.
(発明の効果)
一般に高炉内のガス流れは軟化融着帯形状の影
響を受けるので、高炉内ガス流れを制御するには
軟化融着帯形状を制御する必要がある。(Effects of the Invention) Generally, the gas flow in a blast furnace is affected by the shape of the softened cohesive zone, so in order to control the gas flow in the blast furnace, it is necessary to control the shape of the softened cohesive zone.
従来技術によれば軟化融着帯の外部形状は1200
℃温度分布線により測定できるようになつたがそ
の内部形状は不明であつた。本発明によれば軟化
融着帯の内部形状が1450℃温度分布線等により判
明し軟化融着帯の全体像が把握できるようにな
る。その結果、軟化融着帯形状の制御も従来より
容易行えるようになり炉内ガス流分布の制御がで
きるようになるという効果が得られる。 According to the conventional technology, the external shape of the softened cohesive zone is 1200
Although it became possible to measure the temperature using the °C temperature distribution line, its internal shape remained unknown. According to the present invention, the internal shape of the softened cohesive zone can be determined from the 1450° C. temperature distribution line, etc., and the overall image of the softened cohesive zone can be grasped. As a result, the shape of the softened cohesive zone can be controlled more easily than before, and the gas flow distribution in the furnace can be controlled.
第1図は本発明方法において使用する測温素子
の1つの基本形の縦断側面図、第2図は測定プロ
ーブの1例の側面図、第3図は測定プローブの高
炉内挿入状態をを示す炉頂部の部分の縦断側面
図、第4図は横軸に温度、縦軸に高さを取り各金
属素線閉端の溶断高さ、位置を示す図表、第5図
は高炉内の温度分布を示す図、第6図はは熱電対
と金属素線を併用する測定プローブの他例の側面
図である。
1……測温素子、2……保護シース、3……金
属素線、3a,3a′,3a″……閉路先端、3b…
…開路基端、4……充填物、5……鋼管、6……
検知孔、7……測定プローブ、8……高炉、9…
…炉内装入物、10……挿入装置、11……炉壁
耐火物、12……接続線、13……デツキ、14
……ドラム、15……検出装置、16,16′,
16″……熱電対高温端、T,T′,T″,X,Y…
…温度分布線、t,t′,t″……交点。
Fig. 1 is a vertical sectional side view of one basic type of temperature measuring element used in the method of the present invention, Fig. 2 is a side view of an example of a measuring probe, and Fig. 3 is a furnace showing the state in which the measuring probe is inserted into the blast furnace. A longitudinal cross-sectional side view of the top part, Figure 4 is a chart showing temperature on the horizontal axis and height on the vertical axis, showing the fusing height and position of the closed end of each metal wire, and Figure 5 shows the temperature distribution inside the blast furnace. FIG. 6 is a side view of another example of a measurement probe that uses both a thermocouple and a metal wire. 1... Temperature measuring element, 2... Protective sheath, 3... Metal wire, 3a, 3a', 3a''... End of closed circuit, 3b...
...Open circuit base end, 4...Filling material, 5...Steel pipe, 6...
Detection hole, 7...Measurement probe, 8...Blast furnace, 9...
... Furnace contents, 10 ... Insertion device, 11 ... Furnace wall refractories, 12 ... Connection wire, 13 ... Deck, 14
...Drum, 15...Detection device, 16, 16',
16″……Thermocouple high temperature end, T, T′, T″, X, Y…
...Temperature distribution line, t, t', t''...intersection.
Claims (1)
に半径方向に載置され荷下りとともに降下する測
定プローブとして保護シース内に溶融温度が既知
の金属素線を充填物中に埋蔵して折返し状に内装
しプローブ内に収容し、金属素線の閉路先端をプ
ローブの所定位置の検知孔から露出させその開路
基端から通電状態として使用し、金属素線の露出
閉端の溶断による通電の遮断により金属素線の溶
融温度を以つて炉内のその溶断位置の温度と判定
し、その各炉内位置のプロツトにより当該温度分
布線を得て炉内状況を検知することを特徴とする
高炉の炉内状況の検知方法。 2 前記の高炉の炉内状況のうち1400〜1500℃の
軟化融着帯の内部形状の検知のため、前記金属素
線として溶融温度が1453℃の純ニツケルを使用す
る特許請求の範囲第1項記載の高炉の炉内状況の
検知方法。[Claims] 1. In order to detect the condition inside the blast furnace, a metal wire with a known melting temperature is placed inside a protective sheath as a measurement probe that is placed radially above the contents of the furnace and lowered as the load is unloaded. The metal wire is buried in the filling, folded inside, and housed in the probe, and the closed end of the metal wire is exposed through the detection hole at a predetermined position of the probe, and the open circuit base end is used as a energized state. The melting temperature of the metal wire is determined to be the temperature at the melting point in the furnace by interrupting the current flow due to the melting of the exposed closed end, and the temperature distribution line is obtained by plotting each position in the furnace to determine the situation inside the furnace. A method for detecting the condition inside a blast furnace. 2. Claim 1, wherein pure nickel with a melting temperature of 1453°C is used as the metal wire to detect the internal shape of the softened cohesive zone at 1400 to 1500°C in the inside of the blast furnace. The described method for detecting the condition inside the blast furnace.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1898986A JPS62177111A (en) | 1986-01-30 | 1986-01-30 | Detection of condition in blast furnace |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1898986A JPS62177111A (en) | 1986-01-30 | 1986-01-30 | Detection of condition in blast furnace |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62177111A JPS62177111A (en) | 1987-08-04 |
| JPS6261642B2 true JPS6261642B2 (en) | 1987-12-22 |
Family
ID=11986983
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1898986A Granted JPS62177111A (en) | 1986-01-30 | 1986-01-30 | Detection of condition in blast furnace |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62177111A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR101225270B1 (en) | 2011-05-30 | 2013-01-22 | 현대제철 주식회사 | Method for estimating positon bordered to furnace wall of softening zone |
| KR101225273B1 (en) | 2011-05-30 | 2013-01-22 | 현대제철 주식회사 | Method for estimating thickness bordered to furnace wall of softening zone |
| CN111154935B (en) * | 2020-01-06 | 2023-05-12 | 广西柳钢东信科技有限公司 | Device and system for detecting erosion degree of molten iron runner based on cable fusing characteristics |
-
1986
- 1986-01-30 JP JP1898986A patent/JPS62177111A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62177111A (en) | 1987-08-04 |
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| EXPY | Cancellation because of completion of term |