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JPS5910495B2 - How to detect sintered layer depth - Google Patents
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JPS5910495B2 - How to detect sintered layer depth - Google Patents

How to detect sintered layer depth

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Publication number
JPS5910495B2
JPS5910495B2 JP4934177A JP4934177A JPS5910495B2 JP S5910495 B2 JPS5910495 B2 JP S5910495B2 JP 4934177 A JP4934177 A JP 4934177A JP 4934177 A JP4934177 A JP 4934177A JP S5910495 B2 JPS5910495 B2 JP S5910495B2
Authority
JP
Japan
Prior art keywords
sintered
layer
sintered layer
magnetic detection
magnetic
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
Application number
JP4934177A
Other languages
Japanese (ja)
Other versions
JPS53135386A (en
Inventor
義博 藤井
清太 上川
健二 田村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP4934177A priority Critical patent/JPS5910495B2/en
Publication of JPS53135386A publication Critical patent/JPS53135386A/en
Publication of JPS5910495B2 publication Critical patent/JPS5910495B2/en
Expired legal-status Critical Current

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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】 本発明は鉄鉱石を無端の移動火格子を用いて焼結鉱に製
造する際に用いられる方法であつて、焼結層深度もしく
は焼結層深度プロフィールをオンラインで検出する方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention is a method for producing sintered ore from iron ore using an endless moving grate, in which the sinter layer depth or sinter layer depth profile is detected online. Regarding how to.

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D
L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, powdered iron ore, lime, and coke are kneaded with an appropriate moisture content, and the sintering raw materials are turned into pseudo-granules using moving grate-type sintering equipment. (Usually D
Dwight Lloyd type sintering equipment known as L sintering equipment is used, and this equipment will be described 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
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、粉化しに
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 iron ore sintering method using the endless moving grate described above, in order to obtain high quality sintered ore that has sufficient crushing strength even at high temperatures, is difficult to powder, and maintains high air permeability,
It is necessary to constantly monitor whether firing is progressing properly according to standards 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。
For example, in DL sintering equipment, if the pallet movement speed is too fast, sintering will be insufficient.

つまリベット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粉化指数が悪化する
、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
態においてペット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適値も変化する。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
来は排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1個もしくは2個以上の磁気
検出端をパレツトの幅方向およびもしくは長さ方向に移
動せしめつつ、焼成の進行に応じて変化する磁気偏倚量
を検出し該磁気偏倚量から焼結層深度もしくは焼結層深
度プロフイールを検出することを特徴とする焼結層深度
の検出方法、および前記方法をさらに改良した方法即ち
、無端の移動火格子を用いる鉄鉱石の焼結に用いられる
方法であつて、点火後の焼結原料表層に近接して1個も
しくは2個以上の磁気検出端を測定間隔保持手段を介し
てパレツトの幅方向およびもしくは長さ方向に移動せし
めつつ、焼成の進行に応じて変化する磁気偏倚量を検出
し該磁気偏倚量から焼結層深度もしくは焼結層深度プロ
フイールを検出することを特徴とする焼結層深度の検出
方法にある。以下本発明を図面を用いて詳細に説明する
Since sufficient sintering reaction does not proceed to the lower layer of the tab rivet, the yield decreases and the resulting product has low drop 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 powdering 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 PET changes depending on the state of different raw material compositions, so the pallet moving speed should be adjusted accordingly. The optimal value of also changes. 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 ore discharge area was 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. In other words, the progress of firing and whether the firing speed is suitable or not can be directly monitored online.
Currently, there is no means to provide effective information for firing control. Therefore, the present inventors researched a method of directly detecting the progress of sintering, and as a result, developed the method of the present invention. A method used in which one or more magnetic detection ends are moved in the width direction and/or length direction of the pallet close to the surface layer of the sintered raw material after ignition, and changes are made as the firing progresses. A method for detecting the depth of a sintered layer, characterized in that the amount of magnetic deviation is detected, and the depth of the sintered layer or the depth profile of the sintered layer is detected from the amount of magnetic deviation, and a method further improved from the above method, that is, an endless method. A method used for sintering iron ore using a moving grate, in which one or more magnetic detection ends are placed close to the surface layer of the sintered raw material after ignition, and the width of the pallet is measured through a measuring interval holding means. Sintering characterized by detecting the amount of magnetic deviation that changes according to the progress of firing while moving in the direction and/or length direction, and detecting the sintered layer depth or the sintered layer depth profile from the amount of magnetic deviation. This is in the layer depth detection method. 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はバレツト、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1〜5w!/mの速度で移動せしめられる。パ
レツト2上の焼晴原料の層厚は30〜50α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。前記焼結帯8は通常2
0〜3011a!/1!11t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、焼成進度とはバレツトの移動方向つまり長さ方
向または幅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 shows a schematic diagram of the sintering equipment, in which 1 is a sprocket wheel, 2 is a bullet, 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. For convenience of explanation, a part of the pallet 2 is omitted and not shown, but the pallet 2 usually has a sprocket wheel 1 of 1 to 5w! It is moved at a speed of /m. The layer thickness of the sintered raw material on the pallet 2 is about 30 to 50α, and after the sintered raw material is ignited on the surface layer in the ignition furnace 5, it is sucked and aerated downward in the wind box 10 provided at the bottom of the pallet 2. Firing is performed. The sintered zone 8 is usually 2
0~3011a! /1!Moves downward at a speed of 11t,
The ore is controlled to reach the lowest layer in the ore discharge section 11. In the present invention, the speed at which the combustion zone 8 moves downward from the surface layer is referred to as the sintering speed, and the sintering progress refers to the depth of the sintered layer at any position in the bullet's moving direction, that is, the length or width direction.

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。さらにパレツト内の燃焼原料について該パレ
ツトの幅方向および長さ方向の焼結層深度つまり焼結層
厚を表面を基準とし燃焼帯との境界面までの深さで表示
し、該境界面の形状をもつてプロフイールと称する。゛
ただし焼成が完了した際は前記焼結層厚は床敷層までの
深さとなる。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即ち長さ方向および/もしく
は幅方向における燃焼層プロフイールを検出し、それが
過去の操作研究から実証的に知られている焼結層プロフ
イルつまり基準焼結層プロフイールと一致しているか否
かを比較することによつて知ることができる。この点に
ついて、さらに詳細に説明する。
Further, the distance from the surface of the combustion zone 8 at an arbitrary position is referred to as the combustion zone depth. Furthermore, the sintered layer depth, that is, the sintered layer thickness, of the combusted raw material in the pallet in the width and length directions of the pallet is displayed as the depth from the surface to the interface with the combustion zone, and the shape of the interface is shown. is referred to as a profile. However, when the firing is completed, the thickness of the sintered layer is the same as the bedding layer. Now, whether or not the firing is being carried out satisfactorily is determined by detecting the combustion layer profile in the moving direction of the pallet, that is, the length direction and/or the width direction. It can be determined whether the layer profile matches the reference sintered layer profile or not by comparing it with the reference sintered layer profile. 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る第2
図のように表わすことができる。
The second diagram schematically shows the progress of firing 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は燃暁帯、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−N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仙の
距離は燃焼帯8の厚さを示すことになる。
In the figure, 7 is the unsintered layer, 8 is the combustion zone, and 9 is the 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-N is determined. If the intersections of the upper edge 13a and the lower edge 13b of the diagonally shaded portion 13 and the vertical plane 14 are B and B', respectively, the distance between B and B indicates the thickness of the combustion zone 8.

而して前記未焼結層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。ところで焼詰鉱
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℃付近のキユリー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 unsintered 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 burnt 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 magnetic permeability up to 400°C, but at the Curie point near 800°C, magnetic permeability changes significantly. 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即ち焼結層深度を知るこ
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 sintered layer. Hereinafter, a method for determining the sintered layer depth using the magnetic detection end will be described in detail.

第20図は常温の焼結鉱よりなる充填層46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46の表層46aから50詣の測定
間隔を用いて近接させた磁気検出端である。
FIG. 20 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 46 made of sintered ore at room temperature, for example, in units of 5011. The magnetic detection end is placed close to the surface layer 46a of the filling layer 46 using a measurement interval of 50 degrees.

第21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(M7IL)
、縦軸が磁気検出端の出力(MV)を示す。第21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47
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。ただし Z:焼結層深度 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、
焼結鉱層厚即ち焼結層深度を知ることが可能になる。
Figure 21 is a graph comparing the output of the magnetic detection end with the layer thickness changed, and the horizontal axis is the sintered ore layer thickness (M7IL).
, the vertical axis indicates the output (MV) of the magnetic detection end. As is clear from Fig. 21, as the layer thickness of the sintered ore increases, the curve 47
The output VMM of the magnetic detection end, represented by , increases in proportion to the depth of the sintered layer, as shown in equation (1) below. However, like Z: sintered layer depth, 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, the magnetic detection end By measuring the output
It becomes possible to know the sintered ore layer thickness, that is, the sintered layer depth.

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。
Next, the theoretical formula for the output of the magnetic detection end is as follows (2
) is shown in the formula.

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, the temperature within the sintered layer 9 on the pallet is not constant as shown in FIG. 3, 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21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℃のキユーリーポイント
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22図に従つて説明する。第22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100w!Lll5OmlL,2
OOll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
22図においてたとえば線分48は焼結層内温度が80
0℃の界面における焼結層深度と磁気検出端出力の関係
を表わし、同様に線分49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49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22図で説明すると磁気検出端出力が
30mVのときの焼結層深度は縦軸30mを通る水平な
線と線分49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16511)として求められる。本
発明者等の研究結果によれば第22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
より近く設定されることが検出精度の点から好ましいこ
とである。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または測定効果の大小によつて磁気
検出端の測定位置もしくは走査位置を決めるべきである
。本発明において焼結原料表層に近接して磁気検出端を
設けるとは前述の意味において用いるものであり、また
焼結原料層の焼結層深度のプロフィールを求めるとは前
述のようにパレツトの幅方向および/もしくは長さ方向
において焼結層の燃焼帯との境界面の形状を求める即ち
連続的な境界面の形状を求めることを云うものである。
さらに燃焼帯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と截然と区分したものでは
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。
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 21, 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 approximately 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 the method will be explained with reference to FIG. 22. Fig. 22 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 firing depth changes. Although not shown, the depth within the sintered raw material layer immediately below the magnetic detection end is 100W! Lll5OmlL,2
A thermocouple was inserted at the position of OOll and the temperature inside the sintered layer was 300℃, 400℃, 500℃...
・・・・Corresponding to the magnetic detection end output at 800℃,
This diagram illustrates 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. In FIG. 22, for example, line segment 48 indicates that the internal temperature of the sintered layer is 80.
The line segment 49 represents the relationship between the sintered layer depth at the interface at 0° C. and the magnetic sensing end output, and similarly, the line segment 49 represents the relationship between the sintered layer depth at the interface at a temperature of 700° C. and the magnetic sensing end output. 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 operational experience or other parameters. 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 49 and the magnetic detection end output. In other words, to explain with Fig. 22, the sintered layer depth when the magnetic detection end output is 30 mV is the intersection point q of the horizontal line drawn from the intersection p of the horizontal line passing through the vertical axis 30 m and the line segment 49 and the horizontal axis.
(16511 in this example). According to the research results of the present inventors, it has been confirmed that the relational expression of the line segments shown in Fig. 22 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, i.e. sintering. Layer depth can be detected at any time and location as a comprehensive comparison of independent points, ie, 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 to set it closer to the surface layer of the sintered raw material. However, due to differences in the function of the magnetic detection end itself, the presence or absence of equipment that causes magnetic changes in the measurement field, differences in the physical properties of the object to be measured, the amount and layer thickness of the object to be measured, or the magnitude of the measurement effect. Therefore, the measurement position or scanning position of the magnetic detection end should be determined. In the present invention, providing a magnetic detection end close to the surface layer of the sintered raw material is used in the above-mentioned meaning, and determining the profile of the sintered layer depth of the sintered raw material layer refers to the width of the pallet as described above. This means determining the shape of the interface between the sintered layer and the combustion zone in the direction and/or length direction, that is, determining the shape of the continuous interface.
Furthermore, since the magnetic permeability changes significantly in each part of the combustion zone, the sintered layer in the present invention is not clearly separated from the combustion zone 8 as shown as the sintered layer 9 in FIG. It should be understood that this refers to a layer in which a significant change in magnetic permeability has occurred when based on the sintered raw material of .

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. Now, in the present invention, as mentioned above, a 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, but in particular, the present inventor invented and applied for a patent application. It is more appropriate to use the principle of the magnetic detection end filed in Japanese Patent Application No. 100995/1982, 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。第5図に示す磁気検出端は磁
心をM,,M2のように二分割し、これに両者が差動に
働らくように反転した巻線を行なつたものである。
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. The magnetic detection terminal shown in FIG. 5 has a magnetic core divided into two parts M, , M2, and reversed windings are applied to the two parts so that they act differentially.

而して2個のスイツチングトランジスタTrl,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ん侶前後の発振が生ずる。このとき磁心M,,
M2のいずれか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
2はその出力端子を示し、Eは電源で、Rl,R,は調
整抵抗を示すが、差動巻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P1〜P,以降の
巻線においてP1〜P3以降の結線とP,〜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。
Therefore, two switching transistors Trl and Tr2
When excited, in this example, oscillations of around 40 degrees occur due to the nonlinearity of the magnetic cores M1 and M2. At this time, the magnetic core M,,
If an increase or decrease in the magnetic substance, that is, a change in the firing progress described above in the present invention occurs in the vicinity of either one of M2, the magnetic oscillation will be distorted because it is generated by the built-in excitation magnet G1, and a DC component proportional to the amount of distorted magnetism will occur. is output. Tl,T
2 shows the output terminal, E is the power supply, and Rl and R are the adjustment resistors, but some parts of the circuit such as the differential winding are omitted for convenience to avoid complication, and the connection terminals P1 to P, In the subsequent windings, the connections after P1 to P3 and the connections after P, -P, and after are the same. 6 and 7 respectively show the output waveform in a magnetically balanced state and the output waveform in a magnetically unbalanced state at the magnetic detection end described above, and in the embodiment of the present inventors, the period T .

はほぼ25μ8eCであつた。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。
was approximately 25μ8eC. 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.

図において16は磁気検出端で、図示していない移動走
行装置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。
In the figure, reference numeral 16 denotes a magnetic detection end, which is installed so as to face the vicinity of the surface 9a of the sintered layer 9 via a fixing device 50 that is detachable from a beam 51 attached to a moving traveling device (not shown). .

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MO,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5
2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ど磁気検出
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1個以上又は複数個パレツトの幅方
向およびもしくは長さ方向に移動せしめて用いることが
出来る。
Ml and M2 are the aforementioned two-divided magnetic cores, and G1 is an exciting magnet. The magnetic cores MO, M2, excitation magnet G1, etc. are made of non-magnetic material, for example stainless steel case 5.
2, which is shown in longitudinal section 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, as shown in FIG. It is possible to use one or more magnetic detection ends 16 by moving them in the width direction and/or length direction of the pallet.

即ち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結
層プロフイールと比較するかあるいは検出値の変化を比
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が焼結層の表層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
接触転動する車輪の如き接触式のものを採用してもさし
つかえない。而して第9図に示す実施例の装置を用い、
DL焼結精備において該装置をパ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00、縦軸は磁気検出端出力(MV)
で、曲線25は磁気検出端出力、点線で示す曲線26は
焼成速度を20m1/7!i!t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
ツド内温度測定、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。
In other words, the firing progress at the measurement location is detected in advance by actually taking samples, etc., and compared with a set reference sintered layer profile at that location, or by comparing changes in detected values, the suitability of firing is determined. You can know.
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. A distance meter of, for example, an air micrometer type or an optical type attached to the sintered layer detects a change in distance to 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 preset and stored reference measurement interval, and sends a correction command via a conductive wire 23 to a magnetic detection end lifting device 24, such as a barometric pressure, hydraulic pressure, or balance type. , and operates so that the magnetic detection end 16 always maintains a set measurement interval with the surface layer 9a of the sintered layer. The distance detecting end 17 is shown as a non-contact type, but a contact type such as a wheel that rolls in contact with the surface of the sintered raw material may also be used. Then, using the apparatus of the embodiment shown in FIG.
The graph in Figure 10 shows an example in which the magnetic detection end output is determined as the firing depth changes while the device is moved at the same speed as the pallet movement speed in DL sintering equipment, and then compared with the theoretically determined firing progress. Shown below. In the figure, the horizontal axis is the pallet movement distance 00, and the vertical axis is the magnetic detection end output (MV).
Curve 25 is the magnetic detection end output, and curve 26 shown by a dotted line is the firing speed of 20m1/7! i! The change in firing depth calculated theoretically as t is the curve 26. It has been confirmed that this curve 26 approximates the actual value based on research such as bed temperature measurements in actual equipment and cross-sectional temperature distribution in the ore discharge area. It is something that 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;
It is clear that the firing progress can be accurately estimated from

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俊唄u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。
Figure 11 shows a case where the movement of pallets was stopped and sintering work was carried out (this is a typical situation in terms of operating conditions, and corresponds to a temporary stoppage of pallet movement due to equipment failure).

)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T,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T2までの時間は約10分間であり、焼結層の厚さは
約40?であつた。前述のような結果から本発明者等は
、1個もしくは2個以上つまり複数個の磁気検出端によ
つてパレツトの幅方向およびもしくは長さ方向の走査を
行ない焼結層深度もしくは焼結層深度のプロフイールを
検出することを創案したものである。
Curve 27 shows the output of the magnetic detection end obtained at time T, when the movement of the pallet stopped and firing progressed at time T. 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, it is approximately 10m from the ignition furnace.
The measurement was performed at a position close to the moving direction, the time from time t1 to time T2 was about 10 minutes, and the thickness of the sintered layer was about 40 mm. It was hot. Based on the above results, the present inventors conducted scanning in the width direction and/or length direction of the pallet using one or more magnetic detection ends, that is, a plurality of magnetic detection ends, to determine the sintered layer depth or the sintered layer depth. It was invented to detect the profiles of people.

第12図、第13図はパレツトの概路上面図で磁気検出
端16をパレツトの幅方向に移動せしめつつ走査する状
況を説明したものである。図に示すように磁気検出端を
16a,16b,16cのように移動せしめると該測定
位置ごとに焼結層深度28a,28b,28cが得られ
、これを連続的に測定すると幅方向における焼結層深度
プロフイール29が得られる。第14図、第15図は同
様にしてパレツトの長さ方向における走査によつて焼結
層深度プロフイールを求めた実施例を示すものであり、
このようにして任意位置における焼結層深度や焼結層深
度プロフイールを求めうる。第13図、第14図におい
て16d〜16zは測定位置を示すもので、点で示す2
8d〜28zは該測定位置での焼結層深度を表示し、曲
線30はパレツト長さ方向での焼結層深度プロフイール
を示す。本発明では第12図〜第14図のように測定位
置を決めての測定ではなく連続的測定を技術的範囲とす
るものである。次に第16図において、パレツト長さ方
向の走査を行うのに用いた実施例装置を示す。
FIGS. 12 and 13 are schematic top views of the pallet and illustrate the situation in which the magnetic detection end 16 is moved in the width direction of the pallet while scanning. As shown in the figure, when the magnetic detection end is moved like 16a, 16b, and 16c, the sintered layer depths 28a, 28b, and 28c are obtained for each measurement position, and when these are continuously measured, the sintered layer depth in the width direction is A layer depth profile 29 is obtained. FIGS. 14 and 15 show examples in which the sintered layer depth profile was similarly determined by scanning in the length direction of the pallet.
In this way, the sintered layer depth and sintered layer depth profile at any position can be determined. In Figs. 13 and 14, 16d to 16z indicate measurement positions, and 2
8d to 28z indicate the sintered layer depth at the measurement location, and curve 30 shows the sintered layer depth profile along the length of the pallet. In the present invention, the technical scope of the present invention is continuous measurement rather than measurement at fixed measurement positions as shown in FIGS. 12 to 14. Next, FIG. 16 shows an embodiment of the apparatus used to scan the pallet in the longitudinal direction.

図において31は天井構成ビームで、32,32″は軌
条33,33警支持する支持ビームでパレツト2の長さ
方向に伸びており、天井構成ビーム31に固定されてい
る。
In the figure, reference numeral 31 denotes a ceiling beam, and 32 and 32'' support beams supporting rails 33 and 33, which extend in the length direction of the pallet 2 and are fixed to the ceiling beam 31.

架台34は軸受台35,35″、車輪36,36′を介
して軌条33,33′11.に走行自在に乗載されてい
る。37は走行用電動機で、ピニオン38、駆動軸39
、ギヤー装置40,40″を介して前記車輪36,36
′を回動する。
The frame 34 is mounted on rails 33, 33'11 through bearing stands 35, 35'' and wheels 36, 36' so that it can run freely. 37 is an electric motor for running, which has a pinion 38 and a drive shaft 39.
, the wheels 36, 36 via gear devices 40, 40''
Rotate '.

16,16牡支持ロツド41,41′、保持装置42,
47を介して架台34に装置された磁気検出端である。
16, 16 male support rods 41, 41', holding device 42,
This is a magnetic detection end installed on the pedestal 34 via 47.

43,4ざは作業床を示し、44はパレツト2に装入さ
れた焼結原料を表示したものである。
43 and 4 indicate the work floor, and 44 indicates the sintering raw materials charged to the pallet 2.

前記装置でパレツト2の長さ方向の走査を行なうと前述
の第15図に示したような長さ方向の焼結層深度プロフ
イールを二個得ることが出来る。而してそれぞれQ暁結
層深度プロフイールを比較するとパレツトの両側におけ
る焼成のバランスを適確に知ることが可能であるのみな
らず長さ方向における焼成の適、不適を迅速に検出する
ことが可能となる。第16図において走行用電動機37
の制御機構や磁気検出端16,16″の信号処理装置は
省略して図示していないが、それは局知の無線遠隔制御
あるいは押釦式スイツチによる導電線を使用した制御な
ど、目的を逸脱しない範囲で、いずれの制御装置を用い
てもさしつかえない。
When the pallet 2 is scanned in the longitudinal direction with the above-mentioned apparatus, two longitudinal sintered layer depth profiles as shown in FIG. 15 can be obtained. By comparing the respective Q-shape formation depth profiles, it is possible not only to accurately know the balance of firing on both sides of the pallet, but also to quickly detect whether firing is appropriate or not in the length direction. becomes. In FIG. 16, the traveling electric motor 37
The control mechanism and the signal processing device of the magnetic detection ends 16, 16'' are not shown in the figure, but they may be controlled by a wireless remote control or a push button switch using a conductive wire, within the range that does not deviate from the purpose. Therefore, any control device may be used.

また信号処理装置は周知の電子回路を適宜採用して構成
することが出来る。第16図においてはパレツトの長さ
方向の走査例を示したが、これに限定されるものではな
く、パレツトの幅方向あるいは幅方向と長さ方向の走査
を適宜組合せて採用することが可能であり、第17図〜
第19図におけるパレツト概路上面図において、矢印4
5a〜45pで示すように、位置をかえて単独もしくは
グルーブとして走査を行なうと得られる焼結層深度およ
びもしくはそのプロフイールは極めて精度の高いものと
なり、操業制御に有効な情報を与え、前記焼結層深度プ
ロフイールについて経験的もしくは理論的に求められて
いる基準焼結層深度プロフイールど比較してその差が大
きいときはすみやかに各種の制御要因たとえば、火格子
の移動速度、焼結原料の装入量、装入分布、焼結原料の
配合、ウインドボツクスダン Sパ一開度、点火強度、
焼結原料の含有水分などを適宜操作して操業を適正化す
ることを可能ならしめる。
Further, the signal processing device can be constructed by appropriately employing known electronic circuits. Although FIG. 16 shows an example of scanning in the length direction of the pallet, the scanning is not limited to this, but scanning in the width direction of the pallet or a combination of width and length directions can be adopted as appropriate. Yes, Figure 17~
In the schematic top view of the palette in FIG.
As shown in 5a to 45p, the depth of the sintered layer and/or its profile obtained by changing the position and scanning alone or as a group becomes extremely accurate, providing information useful for operational control, and If the layer depth profile differs significantly from the standard sintered layer depth profile determined empirically or theoretically, various control factors such as the moving speed of the grate and the charging of sintering raw materials should be immediately adjusted. quantity, charging distribution, sintering raw material composition, wind box opening degree, ignition strength,
It is possible to optimize the operation by appropriately controlling the moisture content of the sintering raw material.

本発明は前述のように、オンラインにおいて焼成の適否
を知るための重要な情報を与えるのみならず、逆に制御
要因を変更した場合それが焼成にどのような影響を与え
るかその相関関係を知るための重要な検索手段を与える
ものである。
As mentioned above, the present invention not only provides important information online for determining whether firing is appropriate, but also provides information on how changing control factors affects firing. This provides an important means of searching for information.

【図面の簡単な説明】[Brief explanation of the drawing]

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磁気検
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、第13図、第14図、第15図は本発明にか
かる走査検出要領説明図、第16図は本発明の方法を実
施するために用いた装置の概略構成説明図、第17図、
第18図、第19図は本発明にかかる走査軌跡説明図、
第20図は磁気検出端の出力調査要領を示す概念図、第
21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22図は磁気検出端出力ど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、16,16′
−・・・・・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・・・・・・距離調節制御装置、
24・・・・・・磁気検出端昇降装置、31・・・・・
・天井構成ビーム、32,37・・・・・・支持ビーム
、33,33′・・・・・・軌条、34・・・・・・架
台、37・・・・・・走行用電動機。
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. FIG. 5 is a schematic diagram of the magnetic detection end circuit configuration used to implement the method according to the present invention, and FIGS. 6 and 7 are graphs showing the relationship between the output and the magnetic detection end output. Output waveform and schematic diagram showing output waveform in magnetic unbalance state, No. 8
Figure 9 is a schematic explanatory diagram of the schematic configuration and operation procedure of different magnetic detection ends used to carry out the method of the present invention, and Figure 10 is a proportional relationship between the firing progress and the output of the magnetic detection end. The graph shown in Fig. 11 shows the case where the magnetic detection end is fixed,
A graph showing the magnetic detection end output obtained when firing was performed with the pallet stopped moving. 12, 13, 14, and 15 are explanatory diagrams of the scanning detection procedure according to the present invention, FIG. 16 is an explanatory diagram of the schematic configuration of the apparatus used to carry out the method of the present invention, and figure,
FIG. 18 and FIG. 19 are explanatory diagrams of the scanning locus according to the present invention,
Figure 20 is a conceptual diagram showing how to investigate the output of the magnetic detection end, Figure 21 is a graph showing the relationship between the sintered ore layer thickness and the output of the magnetic detection end, and Figure 22 is the relationship between the output of the magnetic detection end and the sintered layer temperature. It is a graph showing a relationship. 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, 16'
-... Magnetic detection end, 17... Distance detection end, 18... Level holding device, 19...
Support rod, 20... Support beam, 21, 23...
... Conductive wire, 22 ... Distance adjustment control device,
24... Magnetic detection end lifting device, 31...
- Ceiling component beam, 32, 37... support beam, 33, 33'... rail, 34... frame, 37... electric motor for traveling.

Claims (1)

【特許請求の範囲】 1 無端の移動火格子を用いる鉄鉱石の焼結に用いられ
る方法であつて、点火後の焼結原料表層に近接して1個
もしくは2個以上の磁気検出端をパレットの幅方向およ
び/もしくは長さ方向に移動せしめつつ、焼成の進行に
応じて変化する磁気偏倚量を検出し該磁気偏倚量から焼
結層深度もしくは焼結層深度プロフィールを検出するこ
とを特徴とする焼結層深度の検出方法。 2 無端の移動火格子を用いる鉄鉱石の焼結に用いられ
る方法であつて、点火後の焼結原料表層に近接して1個
もしくは2個以上の磁気検出端を測定間隔保持手段を介
してパレットの幅方向および/もしくは長さ方向に移動
せしめつつ、焼成の進行に応じて変化する磁気偏倚量を
検出し該磁気偏倚量から焼結層深度もしくは焼結層深度
プロフィールを検出することを特徴とする焼結層深度の
検出方法。
[Claims] 1. A method used for sintering iron ore using an endless moving grate, in which one or more magnetic detection ends are placed on a pallet close to the surface layer of the sintered raw material after ignition. The sintered layer depth or the sintered layer depth profile is detected from the magnetic deviation amount by detecting the amount of magnetic deviation that changes as the firing progresses while moving it in the width direction and/or length direction. Detection method of sintered layer depth. 2. A method used for sintering iron ore using an endless moving grate, in which one or more magnetic detection ends are placed close to the surface layer of the sintered raw material after ignition via a measurement interval holding means. While moving the pallet in the width direction and/or length direction, the amount of magnetic deviation that changes as firing progresses is detected, and the sintered layer depth or sintered layer depth profile is detected from the amount of magnetic deviation. A method for detecting the depth of the sintered layer.
JP4934177A 1977-04-28 1977-04-28 How to detect sintered layer depth Expired JPS5910495B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4934177A JPS5910495B2 (en) 1977-04-28 1977-04-28 How to detect sintered layer depth

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4934177A JPS5910495B2 (en) 1977-04-28 1977-04-28 How to detect sintered layer depth

Publications (2)

Publication Number Publication Date
JPS53135386A JPS53135386A (en) 1978-11-25
JPS5910495B2 true JPS5910495B2 (en) 1984-03-09

Family

ID=12828289

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4934177A Expired JPS5910495B2 (en) 1977-04-28 1977-04-28 How to detect sintered layer depth

Country Status (1)

Country Link
JP (1) JPS5910495B2 (en)

Also Published As

Publication number Publication date
JPS53135386A (en) 1978-11-25

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