JPS5910497B2 - Sintered layer depth detection method - Google Patents
Sintered layer depth detection methodInfo
- Publication number
- JPS5910497B2 JPS5910497B2 JP4934377A JP4934377A JPS5910497B2 JP S5910497 B2 JPS5910497 B2 JP S5910497B2 JP 4934377 A JP4934377 A JP 4934377A JP 4934377 A JP4934377 A JP 4934377A JP S5910497 B2 JPS5910497 B2 JP S5910497B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- sintered
- detection end
- magnetic detection
- sintered layer
- 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
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- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
- Manufacture And Refinement Of Metals (AREA)
Description
【発明の詳細な説明】
本発明は主として鉄鉱石の焼結手段において用いられる
焼結層の深度検出方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates primarily to a method for detecting the depth of a sintered layer used in a means for sintering iron ore.
周知の通り、近代の鉄冶金においては、鉄鉱石、石灰、
コークスの粉粒体を適当な水分配合のもとに混錬し、擬
似粒塊とした焼結原料を移動火格子型の焼結設備(通常
DL焼結設備として知られているドワイトロイド式焼結
設備が賞用されており本発明の実施例としても前記設備
を用いて説明する。As is well known, in modern iron metallurgy, iron ore, lime,
Coke powder is kneaded with an appropriate moisture content, and the sintering raw material is turned into pseudo-granules using a moving grate type sintering equipment (Dwight Lloyd type sintering equipment, commonly known as DL sintering equipment). The present invention will be described using this equipment as an embodiment of the present invention.
)を用いて焼結鉱としたものが主要原料として使用され
ている。前述の無端の移動火格子を用いる鉄鉱石の焼結
手段においては、高温でも充分な潰裂強度を持ち、紛化
しにくく、高い通気性が保てる高品質の焼結鉱を得るた
め、焼成が基準通り適確に進行しているかどうかを常に
監視し、焼成制御を適切に実施せねばならない。) is used as sintered ore as the main raw material. In the above-mentioned method of sintering iron ore using an endless moving grate, sintering is the standard in order to obtain high-quality sintered ore that has sufficient crushing strength even at high temperatures, is difficult to atomize, and maintains high air permeability. It is necessary to constantly monitor whether the process is progressing properly and to appropriately control firing.
例を上げるとDL焼結設備ではパレットの移動速度が早
過ぎると焼成が不充分となる、つまりベッド下層部まで
充分な焼結反応が進行し、ないため歩留りが低下し、得
られた製品は落下強度の低いものとなる。逆にパレット
の移動速度が遅過ぎると焼結反応は充分であるが酸化が
進みすぎて還元紛化指数が悪化する、つまり生産性は著
しく低下してしまう。前述のように適切な焼成を行なう
ための一条件としてのパレットの移動速度のみをとつて
も、それぞれ異なつた原料配合の状態において、ベッド
の通気性が変化するためそれに応じて、パレットの移動
速度の最高値も変化する。即ち通常の操業では、原料配
合、含水率、原料充填度等が絶えず変動するため、それ
に応じてパレットの移動速度を変更する必要がある。つ
まり焼成速度を過去の技術経験から求めた値に保つこと
が要求される訳であるが前記焼成速度を定めるための指
標として適当なものがないため、従来は非鉱部でのシン
ターケーク破断面の観察結果たとえば燃焼帯の形状、厚
さ、輝度などにより判断したり、ストランド後半の排ガ
ス温度分布が一定になるように操業するなどの方法が採
用されていた。即ちオンラインで焼成の進度および焼成
速度の適、不適を直接的に監視し、焼成制御のための有
効な情報を提供する手段は見当らないのが現状であつた
。そこで本発明者等は焼成の進度を直接的に検出する方
法を研究した結果、本発明の方法を開発したもので、本
発明の要旨は、無端の移動火格子を用いる鉄鉱石の焼結
手段に用いられる方法であつて、点火後の焼結原料表層
に近接して磁気検出端を設け、焼成の進行に応じて変化
する磁気偏倚量を検出し、該磁界偏倚量から、焼結層深
度を求める焼結層深度検出方法および前記の方法をさら
に進展させた方法即ち、無端の移動火格子を用いる鉄鉱
石の焼結手段に用いられる方法であつて、点火後の焼結
原料表層に近接して、測定間隔保持手段を介して磁気検
出端を設け、焼成の進行に応じて変化する磁気偏倚量を
検出し、該磁界偏倚量から焼結層深度を求めることを特
徴とする焼結層深度検出方法にある。For example, in DL sintering equipment, if the moving speed of the pallet is too fast, sintering will be insufficient.In other words, the sintering reaction will not progress to the lower layer of the bed, resulting in a lower yield and lower product yield. It has low fall strength. On the other hand, if the moving speed of the pallet is too slow, the sintering reaction will be sufficient, but oxidation will proceed too much and the reduction atomization index will deteriorate, that is, the productivity will drop significantly. As mentioned above, even if we consider only the pallet moving speed as one of the conditions for proper firing, the air permeability of the bed changes with different raw material compositions, so the pallet moving speed must be adjusted accordingly. The maximum value of will also change. That is, in normal operation, the raw material composition, moisture content, raw material filling degree, etc. constantly change, so it is necessary to change the pallet moving speed accordingly. In other words, it is required to maintain the firing rate at a value determined from past technical experience, but since there is no suitable index for determining the firing rate, conventionally the sinter cake fracture surface in the non-mine area was used. Methods were adopted, such as making judgments based on observation results such as the shape, thickness, and brightness of the combustion zone, and operating so that the exhaust gas temperature distribution in the latter half of the strand was constant. That is, currently there is no means to directly monitor the progress of firing and the suitability or unsuitability of the firing speed online and to provide effective information for firing control. As a result of research into a method for directly detecting the progress of sintering, the present inventors developed the method of the present invention.The gist of the present invention is a means for sintering iron ore using an endless moving grate. A method used for A method for detecting the depth of the sintered layer to determine the depth of the sintered layer, and a method that is a further development of the above-mentioned method, that is, a method used for iron ore sintering means using an endless moving grate. A sintered layer characterized in that a magnetic detection end is provided via a measurement interval holding means to detect the amount of magnetic deviation that changes as firing progresses, and the depth of the sintered layer is determined from the amount of magnetic field deviation. It's in the depth detection method.
以下本発明を図面を用いて詳細に説明する。The present invention will be explained in detail below using the drawings.
第1図は本発明を実施するために用いられた周知のDL
焼結設備の概略構成図を示すもので、1はスプロケツト
ホイール、2はパレツト、3は床敷鉱供給装置、5は点
火炉、6は床敷層、7は未焼結層、8は焼成進行中の層
つまり燃焼帯、9は焼成が完了した層つまり焼結層を示
す。而して説明の便宜上、パレツト2の一部は省略し図
示していないが該パレツト2は通常スプロケツトホイー
ル1で1〜5m/Wtの速度で移動せしめられる。パレ
ツト2上の焼結原料の層厚は30〜50(m程度であり
、焼結原料は点火炉5で表層に点火されたのち、パレツ
ト2の下部に設けられたウインドボツクス10で下方に
吸引通気され焼成が行なわれる。前記燃焼帯8は通常2
0〜3011/駆の速度で下方に移動し、排鉱部11で
最下層に達するように制御される。本発明では燃焼帯8
が表層から下方に向う進行速度を焼成速度と云い、焼成
進度とはパレツトの移動方向における任意位置での焼結
層深度を指すものとする。Figure 1 shows a well-known DL used to implement the present invention.
This figure shows a schematic diagram of the sintering equipment, in which 1 is a sprocket wheel, 2 is a pallet, 3 is a bedding ore supply device, 5 is an ignition furnace, 6 is a bedding layer, 7 is an unsintered layer, and 8 is a bedding layer. 9 indicates a layer in which firing is in progress, that is, a combustion zone, and 9 indicates a layer in which firing has been completed, that is, a sintered layer. Although a part of the pallet 2 is omitted and not shown for convenience of explanation, the pallet 2 is normally moved by the sprocket wheel 1 at a speed of 1 to 5 m/Wt. The layer thickness of the sintered raw material on the pallet 2 is about 30 to 50 m (approximately 30 to 50 m), and after the sintered raw material is ignited on the surface layer in the ignition furnace 5, it is sucked downward in the wind box 10 provided at the bottom of the pallet 2. The combustion zone 8 is usually 2
It moves downward at a speed of 0 to 3011/drive and is controlled to reach the lowest layer at the ore discharge section 11. In the present invention, combustion zone 8
The speed at which the sintered layer advances downward from the surface layer is called the firing speed, and the firing progress refers to the depth of the sintered layer at any position in the direction of movement of the pallet.
また任意位置での燃焼帯8の表層からの距離を燃焼帯深
度と云う。さて、焼成が良好に行なわれているか否かは
前記パレツトの移動方向における焼結層深度を検出し、
それが過去の操業研究から実証的に知られている焼結層
深度つまり基準焼結層深度と一致しているかあるいは独
立した複数点で計測した前述の焼結層深度の相互を比較
することによつて知ることが出来る。Further, the distance from the surface of the combustion zone 8 at an arbitrary position is referred to as the combustion zone depth. Now, whether or not the firing is being performed well is determined by detecting the depth of the sintered layer in the moving direction of the pallet.
The sintered layer depth that is empirically known from past operational research, that is, the reference sintered layer depth, or the aforementioned sintered layer depths measured at multiple independent points can be compared with each other. You can find out by looking at it.
この点について、さらに詳細に説明する。This point will be explained in more detail.
点火炉から排鉱部までの焼成進度を模式的に示すと第2
図のように表わすことができる。The second diagram shows the firing progress from the ignition furnace to the ore discharge section.
It can be expressed as shown in the figure.
図において7は未焼結層で、8は燃焼帯、9は完全に焼
成が完了した焼結層を示す、さてパレツトの移動方向に
おいて任意の点をとり、鉛直方向A−A″における燃焼
帯8を示す斜線部分13の上縁13aと下縁13bと鉛
直面14との交点をそれぞれB,B′とするとB−B′
間の距離は燃焼帯8の厚さを示すことになる。In the figure, 7 is an unsintered layer, 8 is a combustion zone, and 9 is a sintered layer that has been completely fired. Now, by taking an arbitrary point in the moving direction of the pallet, the combustion zone in the vertical direction A-A'' is determined. If the intersections of the upper edge 13a and the lower edge 13b of the diagonally shaded portion 13 indicating 8 with the vertical plane 14 are B and B', respectively, then B-B'
The distance between them will indicate the thickness of the combustion zone 8.
而して前記未燃焼層7、燃焼帯8、焼結層9の温度分布
を鉛直面14に沿つて概略図示すると第3図に示すよう
になる。第3図は横軸に温度(℃)をとり、縦軸に前記
未燃焼層7、燃焼帯8、焼結層9の分布つまり焼結原料
の厚さ方向の分布をとつたものである。ところで焼結鉱
の磁気特性を調査すると第4図に示すように、温度変化
にともなつてその磁気特性が変化する、図において横軸
に温度(℃)をとり縦軸に透磁率をとると曲線15に示
すように400℃までは透磁率にさほどの変化は見られ
ないが、800℃付近のキユリ△ポイント点において透
磁率は大幅に変化する。そこで透磁率の変化に比例して
、出力が変化するマグネツトメータ一即ち磁気検出端を
用いた場合その出力変化は曲線15と近似したものとな
る。The temperature distribution of the unburned layer 7, combustion zone 8, and sintered layer 9 is schematically illustrated along the vertical plane 14 as shown in FIG. In FIG. 3, the horizontal axis represents temperature (° C.), and the vertical axis represents the distribution of the unburned layer 7, combustion zone 8, and sintered layer 9, that is, the distribution of the sintered raw material in the thickness direction. By the way, when we investigate the magnetic properties of sintered ore, we find that the magnetic properties change as the temperature changes, as shown in Figure 4. In the figure, the horizontal axis represents temperature (°C) and the vertical axis represents magnetic permeability. As shown in curve 15, there is not much change in the magnetic permeability up to 400°C, but the magnetic permeability changes significantly at the Kyuri Δ point near 800°C. Therefore, when a magnetometer, that is, a magnetic detection end whose output changes in proportion to the change in magnetic permeability, is used, the output change approximates the curve 15.
そこで焼結層の表層近傍から鉛直方向における焼結層の
磁気特性を測定すれば焼成進度すなわち結晶層深度を知
ることが可能になる。以下、磁気検出端により焼結層深
度を求める方法について詳細に説明する。Therefore, by measuring the magnetic properties of the sintered layer in the vertical direction from near the surface of the sintered layer, it becomes possible to know the firing progress, that is, the depth of the crystal layer. Hereinafter, a method for determining the sintered layer depth using the magnetic detection end will be described in detail.
第12図は常温の焼結鉱よりなる充填層28の層厚を任
意厚さたとえば5011単位で任意に増減できる装置を
用いて磁気検出端の出力を調査する実験の概念図であり
、16は前記充填層28の表層28aから501!lの
測定間隔を用いて近接させた磁気検出端である。FIG. 12 is a conceptual diagram of an experiment in which the output of the magnetic detection end is investigated using a device that can arbitrarily increase or decrease the layer thickness of the packed layer 28 made of sintered ore at room temperature by an arbitrary thickness, for example, in units of 5011. 501 from the surface layer 28a of the filling layer 28! The magnetic detection ends are placed close to each other using a measurement interval of l.
第13図は層厚を変化させ前記磁気検出端の出力との対
比を行なつたグラフで、横軸が焼結鉱層厚(11)、縦
軸が磁気検出端の出力(MV)を示す。第13図より明
らかなように焼結鉱の層厚の増大に伴つて曲線29で示
す磁気検出端の出力VMMは下記(1)式に示すように
焼結層深度に比例して増加する。同様に実際焼結設備の
焼結層の層厚は三次元の広がりを持つが磁気検出端出力
との関係をあられす検量線を作成しておけば、磁気検出
端出力を測定することによつて、焼結鉱層即ち焼結層深
度を知ることが可能になる。次に前記磁気検出端の出力
に関する理論式を下記の(2)式に示す。FIG. 13 is a graph in which the layer thickness is varied and compared with the output of the magnetic detection end, where the horizontal axis shows the sintered ore layer thickness (11) and the vertical axis shows the output (MV) of the magnetic detection end. As is clear from FIG. 13, as the layer thickness of the sintered ore increases, the output VMM of the magnetic detection end shown by the curve 29 increases in proportion to the depth of the sintered layer, as shown in equation (1) below. Similarly, the layer thickness of the sintered layer in actual sintering equipment has a three-dimensional spread, but if you create a calibration curve that shows the relationship with the magnetic detection end output, you can easily measure the magnetic detection end output. Therefore, it becomes possible to know the sintered ore layer, that is, the depth of the sintered layer. Next, a theoretical equation regarding the output of the magnetic detection end is shown in equation (2) below.
ところで、パレツト上の焼結層9内の温度は第3図に示
すごとく、一定ではなく層高方向で温度分布をもつてい
る。By the way, as shown in FIG. 3, the temperature within the sintered layer 9 on the pallet is not constant but has a temperature distribution in the layer height direction.
ここでもし焼結層内の温度がたとえ温度分布をもつてい
たとしても層内の温度が400℃以下の温度であれば、
第4図および第13図に示す関係から明らかなように磁
気検出端の出力は温度に無関係に、焼結層の深度のみに
よつて決定されるとみなして良い。しかし第4図に示す
ように、磁気検出端は約800℃のキユリーポイント以
下の温度範囲で検出力を有するものの、400℃以上の
高温域では出力が低下するため、温度補正を行なうこと
によつて800℃以下の温度範囲にある焼結層厚を検出
することが好ましい。そこで本発明者等は、磁気検出端
の出力と焼結層内の温度パターンとの相関を詳細に調査
することにより、焼結層表層から任意の温度面までの焼
結層深度を正しく推定する方法を創案した。その方法の
一例を第14図に従つて説明する。Here, even if the temperature inside the sintered layer has a temperature distribution, if the temperature inside the layer is below 400℃,
As is clear from the relationships shown in FIGS. 4 and 13, the output of the magnetic detection end can be considered to be determined only by the depth of the sintered layer, regardless of temperature. However, as shown in Figure 4, although the magnetic detection end has detection power in the temperature range below the Curie point of about 800°C, the output decreases in the high temperature range of 400°C or higher, so temperature correction is required. Therefore, it is preferable to detect the sintered layer thickness within a temperature range of 800° C. or lower. Therefore, the present inventors will accurately estimate the depth of the sintered layer from the surface layer of the sintered layer to an arbitrary temperature surface by investigating in detail the correlation between the output of the magnetic detection end and the temperature pattern within the sintered layer. invented a method. An example of this method will be explained with reference to FIG.
第14図は後述の第9図に示す実施例の磁気検出端装置
をDL焼結設備において、パレツトの移動速度と等しい
速度で移動せしめ、焼成深度変化に伴なう磁気検出端出
力を連続して求める際に、図示していないが、前記磁気
検出端の直下付近の焼結原料層内の深さ100U115
0U120011の位置に熱電対を挿入して同時に連続
し、焼結層内の温度が300℃、400℃、500℃・
・・・・・・・・800℃のときの磁気検出端出力を対
応させ、焼結層表層からの距離(深さ)と磁気検出端出
力および焼結層内温度との三者の関係を図示したもので
ある。第14図においてたとえば線分30は焼結層内温
度が800℃の界面における焼結層深度ど磁気検出端出
力の関係を表わし、同様に線分31は温度が700℃の
界面の焼結層深度と磁気検出端出力の関係を示す、従つ
て焼結層下端面の温度を測定するか、あるいは該温度が
操業経験や他のパラメーターからほぼ推定できる条件下
では容易に焼結層深度を知ることが可能となる。仮に前
記焼結層下端面の温度が700℃であつたとすれば、焼
結層深度を線分31と磁気検出端出力との関係からたや
すく推定できる。つまり第14図で説明すると磁気検出
端出力が30mのときの、焼結層深度は縦軸30mVを
通る水平な線と線分31の交点Pからおろした垂線と横
軸の交点qの深度(この例では1651!)として求め
られる。本発明者等の研究結果によれば第14図に示す
線分の関係式は、各種の異なつた操業条件下でもほぼ類
似していることが確認されており、あらかじめ該線分の
関係式を求めておくことによつて、磁気検出端出力から
焼結層深度を精度よく推定することができる。換言する
と焼結原料が点火されたのち焼成が進行し焼結鉱に変化
する状況や表層からどの位の深さまで焼結鉱に変化した
か、つまり焼結層の鉛直方向での厚さ即ち焼結層深度を
任意の時刻および位置で、独立した複数点の総合的ノ
な比較即ち焼結パターンとして、あるいは各測定点の経
時的変動としても検出することができる。また磁気検出
端は前述のような磁気特性を検出するものであるため焼
結原料の表層により近く設置されることが検出精度の点
から好ましいことであτ る。しかしながら、磁気検出
端そのものの機能の差異や測定の場における磁気変化を
ひきおこす設備などの有無、あるいは被測定物体の物理
的性状や被測定物体の量や層厚などの違いによつて磁気
検出端の測定位置を決めるべきである。本発明にOおい
て焼結原料表層に近接して磁気検出端を設けることは前
述の意味において用いるものであり、また焼結層深度を
求めるとは前述のようにパレツトの移動方向において任
意位置で、焼結層の厚さを検出することや焼成の進行に
ともなう焼結層の厚さ変化などを必要に応じて検出する
ことを云うものである。さらに燃焼帯以上の各部分にお
いて透磁率が著しく変化するので本発明における焼結層
とは第2図において焼結層9として示すように燃焼帯8
と截然と区別したものではなく、むしろ焼成前の焼結原
料を基準とした場合、透磁率に著しい変化が生じた層を
指すものと理解されるべきである。Fig. 14 shows the magnetic detection end device of the embodiment shown in Fig. 9, which will be described later, being moved at a speed equal to the moving speed of the pallet in DL sintering equipment, and the magnetic detection end output as the sintering depth changes. Although not shown in the figure, when calculating the
Thermocouples are inserted in the 0U120011 position and connected simultaneously, and the temperature inside the sintered layer is 300℃, 400℃, 500℃・
......The relationship between the distance (depth) from the surface layer of the sintered layer, the output of the magnetic detection end, and the temperature inside the sintered layer was determined by matching the output of the magnetic detection end at 800℃. This is what is illustrated. In FIG. 14, for example, line segment 30 represents the relationship between the sintered layer depth and the magnetic detection end output at the interface where the internal temperature of the sintered layer is 800°C, and similarly, line segment 31 represents the relationship between the sintered layer depth and the magnetic detection end output at the interface where the internal temperature of the sintered layer is 700°C. It shows the relationship between the depth and the output of the magnetic detection end, and therefore the depth of the sintered layer can be easily determined by measuring the temperature at the lower end of the sintered layer, or under conditions where the temperature can be approximately estimated from operating experience or other parameters. becomes possible. If the temperature of the lower end surface of the sintered layer is 700° C., the depth of the sintered layer can be easily estimated from the relationship between the line segment 31 and the magnetic detection end output. In other words, to explain with reference to FIG. 14, when the magnetic detection end output is 30 m, the sintered layer depth is the depth ( In this example, it is calculated as 1651!). According to the research results of the present inventors, it has been confirmed that the relational expression of the line segments shown in Fig. 14 is almost similar under various different operating conditions. By determining this in advance, the sintered layer depth can be accurately estimated from the magnetic detection end output. In other words, the conditions in which the sintering raw material is ignited, the sintering progresses and it changes to sintered ore, and the depth from the surface layer to which it changes to sintered ore, that is, the vertical thickness of the sintered layer, that is, the sintered ore. Determine the formation depth at any time and position by comprehensively measuring multiple independent points.
It can be detected as a comparison, that is, a sintering pattern, or as a variation over time of each measurement point. Furthermore, since the magnetic detection end detects the above-mentioned magnetic properties, it is preferable from the viewpoint of detection accuracy that it be installed closer to the surface layer of the sintered raw material. However, due to differences in the functions of the magnetic detection end itself, the presence or absence of equipment that causes magnetic changes in the measurement field, or differences in the physical properties of the object to be measured, the amount and layer thickness of the object to be measured, etc. The measurement position should be determined. In the present invention, the provision of a magnetic detection end close to the surface layer of the sintered raw material is used in the above-mentioned meaning, and the determination of the sintered layer depth is used at any position in the moving direction of the pallet as described above. This refers to detecting the thickness of the sintered layer and detecting changes in the thickness of the sintered layer as the firing progresses, as necessary. Furthermore, since the magnetic permeability changes significantly in each part above the combustion zone, the sintered layer in the present invention refers to the combustion zone 8 as shown as the sintered layer 9 in FIG.
Rather, it should be understood that it refers to a layer in which a significant change in magnetic permeability has occurred when based on the sintered raw material before firing.
而して通常は焼結鉱に転化した層と考えてよい。次に本
発明において用いられる磁気検出端の詳細について説明
する。さて本発明では前述のように焼結原料表層に近接
して透磁率の変化を検出するような機能を有するもので
あれば周知の磁気検出端を使用できるが、特に本発明者
が創案し特願昭50−100995号として出願した磁
気検出端の原理を利用したものが、より適当であり、第
5図において本発明の目的に適した前記磁気検出端の一
実施例を説明する。Therefore, it can usually be considered to be a layer that has been converted to sintered ore. Next, details of the magnetic detection end used in the present invention will be explained. In the present invention, as described above, any well-known magnetic detection end can be used as long as it has the function of detecting changes in magnetic permeability in close proximity to the surface layer of the sintered raw material. It is more appropriate to utilize the principle of the magnetic detection end filed in Japanese Patent Application No. 100995/1983, and an embodiment of the magnetic detection end suitable for the purpose of the present invention will be described in FIG.
前述のようにDL焼結設備のような鉄構造物で構成され
た設備内で磁気検出端を開放状態で使用するには、固定
構造物やクレーンのような移動構造物等による磁気的な
影響を消去して焼結原料の前記磁気特性の変化のみを取
り出す工夫が必要になる。As mentioned above, in order to use the magnetic detection end in an open state in equipment composed of iron structures such as DL sintering equipment, magnetic influences from fixed structures and moving structures such as cranes must be avoided. It is necessary to devise a method to eliminate only the change in the magnetic properties of the sintered raw material.
第5図に示す磁気検出端は磁心をMl,M2のように二
分割し、これ乳両者が差動に働らくように反転した巻線
を行なつたものである。The magnetic detection end shown in FIG. 5 has a magnetic core divided into two parts M1 and M2, and windings are reversed so that the two parts act differentially.
而して2個のスイツチングトランジスタTr,,Tr2
で励磁すると、この例では磁心Ml,M2の非線形性に
より40腫前後の発振が生ずる、このとぎ磁心M,,M
2のいずれが一方の近傍において磁性物質の増減即ち本
発明における前述の焼成進度の変化が生ずれば、内蔵し
た励磁磁石G1により発生するため磁気発振に歪が生じ
歪磁気量に比例した直流成分が出力される。Tl,T,
はその出力端子を示し、Eは電源で、R,,R2は調整
抵抗を示すが、差動回線など回路の一部は複雑化をさけ
るため便・宜上省略しており接続端子P,〜P7以降の
巻線においてP1〜P3以降の結線とP5〜P,以降の
結線は同一である。而して第6図、第7図は前述の磁気
検出端における磁気平衡状態の出力波形および磁気不平
衡状態での出力波形をそれぞれ示すものであり、本発明
者等の実施例では周期T。はほぼ)25μSecであつ
た。Therefore, two switching transistors Tr, Tr2
In this example, oscillations of around 40 mm occur due to the nonlinearity of the magnetic cores Ml, M2.
If any of the above causes an increase or decrease in the magnetic substance in the vicinity of one of them, that is, a change in the firing progress described above in the present invention, distortion will occur in the magnetic oscillation due to the built-in excitation magnet G1, resulting in a direct current component proportional to the amount of distorted magnetism. is output. Tl, T,
indicates the output terminal, E is the power supply, and R, , R2 are the adjustment resistors, but some parts of the circuit such as the differential line are omitted for convenience and convenience to avoid complication, and the connection terminals P, ~ In the windings after P7, the connections after P1 to P3 are the same as the connections after P5 to P and after. 6 and 7 respectively show the output waveform in a magnetically balanced state and the output waveform in a magnetically unbalanced state at the above-mentioned magnetic detection terminal, and in the embodiment of the present inventors, the period T. (approximately) 25 μSec.
またレベルのずれ1。が直流成分となる。次に第8図に
本発明の方法を実施するための装置の一実施例にかかる
概要図を示す。図において16は磁気検出端で、図示し
ていない支持柱に取付けられたビーム51に着脱自在な
固定装置50を介して焼結層9の表面9aの近傍に対向
するように設備されている。Ml,M2は前述の二分割
された磁心で、G1は励磁磁石である。磁心Ml,M2
および励磁磁石G1などは非磁性体からなるたとえばス
テンレススチールのケース52に収容されるが、図では
縦断面図で示してある。パレツト2の上下振動がすくな
く、かつ、焼結原料の層厚が安定しており、結果として
焼結層9の表面9aと磁気検出端16間の距離変動が極
めて少ない場合は第8図のように磁気検出端16をこの
ように固定して用いることが出来る。即ち固定した測定
場所での焼成進度をあらかじめ実際にサンプル採取など
によつて検出し設定した当該場所での基準焼成進度と比
較することによつて焼成の適、不適を知ることが出来る
。次に第9図において測定間隙保持手段を介して磁気検
出端を設けた本発明にかかる他の実施例を示す。第9図
において17は磁気検出端16と焼結層9の表面9aと
の離隔距離即ち測定間隔をほぼ一定にするためのレベル
保持装置18の距離検出端で支持桿19を介して支持ビ
ーム20に装着されたたとえば空気マイクロメーター方
式、光学方式の距離計であつて、焼結層の表面9aとの
距離変化を検出し信号を導電線21によつて距離調節制
御装置22に伝達する。該距離調節制御装置22は磁気
検出端16について、あらかじめ設定記憶されている基
準測定間隔と比較し、修正指令を導電線23を介してた
とえば気圧、液圧あるいは天秤式等の磁気検出端昇降装
置24に与え、常に磁気検出端16が焼結層の表面9a
と設定された測定間隔を保つように作動する。前記距離
検出端17は非接触式のものを示したが、焼結原料の表
面と接触転動する車輪を用いて直接測定間隔を保つよう
に構成した接触式のものを採用してもさしつかえない。
而して第9図に示す実施例0装置を用い、DL焼結設備
において該装置をバレツトの移動速度と等しい速度で移
動せしめつつ焼成深度変化にともなう磁気検出端出力を
求め、ついで理論的に求めた焼成進度と比較した例を第
10図のグラフに示す。図において横軸はパレツト移動
距離(m)、縦軸は磁気検出端出力(MV)で、曲線2
5は磁気検出端出力、点線で示す曲線26は焼成速度を
2011/Mmとして理論的に求めた焼成深度変化をあ
られす。該曲線26は実際設備でのベツト内温度測定、
排鉱部における断面温度分布などの研究から実際値に近
似していることが確しかめられているものである。曲線
25における波状の振動は、この例では4m間隔でウイ
ンドボツクスを支承する建家の鉄骨製のビームが存在し
ていたために生じたもので、曲線25から焼成進度を正
確に推定できることは明らかである。Also, the level difference is 1. becomes the DC component. Next, FIG. 8 shows a schematic diagram of an embodiment of an apparatus for carrying out the method of the present invention. In the figure, reference numeral 16 denotes a magnetic detection end, which is installed so as to face near the surface 9a of the sintered layer 9 via a fixing device 50 which is detachably attached to a beam 51 attached to a support column (not shown). Ml and M2 are the aforementioned two-divided magnetic cores, and G1 is an exciting magnet. Magnetic core Ml, M2
The excitation magnet G1 and the like are housed in a case 52 made of a non-magnetic material, for example stainless steel, which is shown in a longitudinal cross-sectional view in the figure. If the vertical vibration of the pallet 2 is small and the layer thickness of the sintered raw material is stable, and as a result, the distance variation between the surface 9a of the sintered layer 9 and the magnetic detection end 16 is extremely small, the result will be as shown in FIG. The magnetic detection end 16 can be fixed in this way and used. That is, it is possible to know whether firing is appropriate or not by detecting the firing progress at a fixed measurement location in advance by actually taking samples and comparing it with a set standard firing progress at that location. Next, FIG. 9 shows another embodiment of the present invention in which a magnetic detection end is provided via a measurement gap holding means. In FIG. 9, reference numeral 17 denotes a distance detection end of a level holding device 18 for keeping the separation distance between the magnetic detection end 16 and the surface 9a of the sintered layer 9, that is, the measurement interval, approximately constant. For example, a distance meter of an air micrometer type or an optical type is attached to the sintered layer and detects a change in distance from the surface 9a of the sintered layer, and transmits a signal to the distance adjustment control device 22 via a conductive wire 21. The distance adjustment control device 22 compares the magnetic detection end 16 with a reference measurement interval set and stored in advance, and sends a correction command via a conductive wire 23 to a magnetic detection end lifting device such as an air pressure, hydraulic pressure, or balance type. 24, and the magnetic detection end 16 is always on the surface 9a of the sintered layer.
It operates to maintain the set measurement interval. Although the distance detecting end 17 is shown as a non-contact type, it is also possible to use a contact type that uses wheels that roll in contact with the surface of the sintered raw material to maintain a direct measurement interval. .
Using the apparatus of Example 0 shown in FIG. 9, while moving the apparatus at a speed equal to the moving speed of the bullet in the DL sintering equipment, the output of the magnetic detection end as the sintering depth changes is determined, and then theoretically An example of comparison with the determined firing progress is shown in the graph of FIG. In the figure, the horizontal axis is the pallet movement distance (m), the vertical axis is the magnetic detection end output (MV), and the curve 2
5 is the magnetic detection end output, and a curve 26 shown by a dotted line shows the firing depth change theoretically determined by assuming the firing rate as 2011/Mm. The curve 26 is the temperature measurement inside the bed in actual equipment.
It has been confirmed through research on the cross-sectional temperature distribution in the ore discharge area that it approximates the actual value. In this example, the wave-like vibrations in curve 25 were caused by the presence of steel beams of the building that supported the wind boxes at 4 m intervals, and it is clear that the firing progress can be accurately estimated from curve 25. be.
第11図はパレツトの移動をとめて焼結作業を行なつた
際(これは操業の状態から云えば変則的なもので、設備
故障によるパレツト移動の一時停止がこれに当る。)に
得られた磁気検出端の出力を曲線27で示すもので、時
刻t1においてパレツトの移動が停止し焼成が進行した
ものである。時刻T2において出力は飽和し焼結が完了
したことを示している。この例では時刻T3で検出を終
了せしめたが、時刻T2ですべてが焼結層となつている
ことがサンプリングの結果確認され、曲線27は検出時
点における焼成進度を示すものとして取扱えることが明
らかになつた。この実施例では点火炉から約10m移動
方向に寄つた位置での測定であり、時刻t1から時刻T
2までの時間は約10分間であり、焼結層の厚さは約4
0c!nであつた。以上詳細に説明したように本発明の
方法によればオンラインで暁成状況を確実に検出するこ
とが可能となるので、生産性の向上や省エネルギー)品
質改善を目的とする操業方法の改善に資するところ極め
て大である。Figure 11 shows the results obtained when sintering work is carried out with the movement of pallets stopped (this is an irregular situation in terms of operational conditions, and involves a temporary stoppage of pallet movement due to equipment failure). The output of the magnetic detection end is shown by a curve 27, which indicates that the movement of the pallet stopped at time t1 and firing progressed. At time T2, the output is saturated, indicating that sintering is complete. In this example, detection ended at time T3, but the sampling results confirmed that the entire layer had become a sintered layer at time T2, and it is clear that curve 27 can be treated as indicating the firing progress at the time of detection. It became. In this example, the measurement is performed at a position approximately 10 m away from the ignition furnace in the moving direction, and from time t1 to time T
The time to 2 is about 10 minutes, and the thickness of the sintered layer is about 4
0c! It was n. As explained in detail above, according to the method of the present invention, it is possible to reliably detect the dawning state online, which contributes to improving operational methods for the purpose of improving productivity, energy saving, and quality. It is extremely large.
第1図はDL焼結設備の概略説明図、第2図は焼成進度
を説明する模式図、第3図は焼結原料の厚さ方向におけ
る温度分布説明図、第4図は温度と透磁率および検出端
出力との関係を示すグラフ、第5図は本発明にかかる方
法を実施するために用いられた磁気検出端回路構成概要
図、第6図、第7図は磁気平衡状態での出力波形および
磁気不平衡状態での出力波形を示す概路線図、第8図、
第9図は本発明の方法を実施するために用いられた、そ
れぞれ異なつた磁気検出端の概略構成と作動要領の概要
説明図、第10図は焼成進度と磁気検出端出力との比例
関係を示すグラフ、第11図は磁気検出端を固定し、パ
レツトの移動をとめて焼成を行なつた際に得られた磁気
検出端出力を示すグラフ、第12図は磁気検出端の出力
調査要領を示す概念図、第13図は焼結鉱層厚と磁気検
出端出力の関係を示すグラフ、第14図は磁気検出端出
力と焼結層温度との関係を表わすグラフである。
1・・・・・・スプロケツトホイール、2・・・・・・
パレツト、3・・・・・床敷層供給装置、4・・・・・
・焼結原料供給装置、5・・・・・・点火炉、6・・・
・・・床敷層、7・・・・・・未焼結層、8・・・・・
・燃焼帯、9・・・・・・焼結層、10・・・・・・ウ
インドボツクス、16・・・・・・磁気検出端、17・
・・・・・距離検出端、18・・・・・・レベル保持装
置、19・・・・・・支持桿、20・・・・・・支持ビ
ーム、21,23・・・・・・導電線、22・・・・・
・距離調節匍脚装置、24・・・・・・磁気検出端昇降
装置。Figure 1 is a schematic diagram of the DL sintering equipment, Figure 2 is a schematic diagram to explain the firing progress, Figure 3 is a diagram to explain temperature distribution in the thickness direction of the sintering raw material, and Figure 4 is temperature and magnetic permeability. Figure 5 is a schematic diagram of the configuration of the magnetic detection terminal circuit used to implement the method according to the present invention, and Figures 6 and 7 are the output in a magnetically balanced state. A schematic diagram showing waveforms and output waveforms in a magnetically unbalanced state, FIG.
Fig. 9 is a schematic explanatory diagram of the schematic configuration and operation procedure of different magnetic detection terminals used to carry out the method of the present invention, and Fig. 10 shows the proportional relationship between the firing progress and the output of the magnetic detection terminal. The graph shown in Figure 11 is a graph showing the magnetic detection end output obtained when firing was performed with the magnetic detection end fixed and the pallet stopped moving, and Figure 12 shows the procedure for investigating the output of the magnetic detection end. 13 is a graph showing the relationship between the sintered ore layer thickness and the magnetic detection end output, and FIG. 14 is a graph showing the relationship between the magnetic detection end output and the sintered layer temperature. 1... Sprocket wheel, 2...
Pallet, 3...Bedding layer supply device, 4...
・Sintering raw material supply device, 5... Ignition furnace, 6...
...Bedding layer, 7...Unsintered layer, 8...
- Combustion zone, 9... Sintered layer, 10... Wind box, 16... Magnetic detection end, 17.
... Distance detection end, 18 ... Level holding device, 19 ... Support rod, 20 ... Support beam, 21, 23 ... Conductive Line, 22...
- Distance adjustment pedestal device, 24...Magnetic detection end lifting device.
Claims (1)
られる方法であつて、点火後の焼結原料表層に近接して
磁気検出端を設け、焼成の進行に応じて変化する磁気偏
倚量を検出し、該磁界偏倚量から焼結層深度を求めるこ
とを特徴とする焼結層深度検出方法。 2 無端の移動火格子を用いる鉄鉱石の焼結手段に用い
られる方法であつて、点火後の焼結原料表層に近接して
測定間隔保持手段を介して磁気検出端を設け、焼成の進
行に応じて変化する磁気偏倚量を検出し、該磁界偏倚量
から焼結層深度を求めることを特徴とする焼結層深度検
出方法。[Claims] 1. A method used for sintering iron ore using an endless moving grate, in which a magnetic detection end is provided close to the surface layer of the sintered raw material after ignition, and the method A method for detecting the depth of a sintered layer, the method comprising: detecting the amount of magnetic deviation that changes depending on the amount of magnetic field deviation; and determining the depth of the sintered layer from the amount of magnetic deviation. 2. A method used for sintering iron ore using an endless moving grate, in which a magnetic detection end is provided close to the surface layer of the sintered raw material after ignition via a measuring interval holding means, and the method is used to monitor the progress of sintering. A method for detecting the depth of a sintered layer, characterized by detecting the amount of magnetic deviation that changes accordingly, and determining the depth of the sintered layer from the amount of magnetic field deviation.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4934377A JPS5910497B2 (en) | 1977-04-28 | 1977-04-28 | Sintered layer depth detection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4934377A JPS5910497B2 (en) | 1977-04-28 | 1977-04-28 | Sintered layer depth detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53135388A JPS53135388A (en) | 1978-11-25 |
| JPS5910497B2 true JPS5910497B2 (en) | 1984-03-09 |
Family
ID=12828347
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4934377A Expired JPS5910497B2 (en) | 1977-04-28 | 1977-04-28 | Sintered layer depth detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5910497B2 (en) |
-
1977
- 1977-04-28 JP JP4934377A patent/JPS5910497B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53135388A (en) | 1978-11-25 |
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