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JPS5822888A - Electromagnetic agitator for molten metal - Google Patents

Electromagnetic agitator for molten metal

Info

Publication number
JPS5822888A
JPS5822888A JP12286681A JP12286681A JPS5822888A JP S5822888 A JPS5822888 A JP S5822888A JP 12286681 A JP12286681 A JP 12286681A JP 12286681 A JP12286681 A JP 12286681A JP S5822888 A JPS5822888 A JP S5822888A
Authority
JP
Japan
Prior art keywords
molten metal
inductor
magnetic
magnetic flux
container
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.)
Granted
Application number
JP12286681A
Other languages
Japanese (ja)
Other versions
JPS6058398B2 (en
Inventor
星加 晴雄
良一 田中
山下 隆士
大島 省三
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.)
Shinko Electric Co Ltd
Original Assignee
Shinko Electric Co Ltd
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 Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP56122866A priority Critical patent/JPS6058398B2/en
Publication of JPS5822888A publication Critical patent/JPS5822888A/en
Publication of JPS6058398B2 publication Critical patent/JPS6058398B2/en
Expired legal-status Critical Current

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  • Waste-Gas Treatment And Other Accessory Devices For Furnaces (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 この発明は容器内に蓄積されている溶融金属(以下溶湯
という)の電磁攪拌装置の機構に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a mechanism for an electromagnetic stirring device for molten metal (hereinafter referred to as molten metal) accumulated in a container.

例えば、アルミ反射炉(溶湯容器の具体的構成)におい
てはある程度の溶湯を蓄積した後は被溶解アルミ材を溶
湯中に浴せしめ、空気をしゃ断した状態(酸化防止の目
的に基づく)で溶解していく。この過程において、被溶
解アルミ材の周囲の溶湯は他の部分の溶湯に比して温度
が低く、被溶解材の溶解効率を上げるためには必然的に
攪拌作用が要求されてくる。このための手段として例え
ば反射炉の炉底部に移動磁界発生用誘導子を配置し、こ
の誘導子から生ずる移動磁界を炉内溶湯に作用させ、溶
湯に推力を与えてその攪拌作用を与えるようにする仁と
が考えられる。。
For example, in an aluminum reverberatory furnace (specific configuration of molten metal container), after a certain amount of molten metal has accumulated, the aluminum material to be melted is immersed in the molten metal and melted while cutting off air (based on the purpose of preventing oxidation). To go. In this process, the temperature of the molten metal surrounding the aluminum material to be melted is lower than that of the molten metal in other parts, and a stirring action is inevitably required to increase the efficiency of melting the material to be melted. As a means for this purpose, for example, an inductor for generating a moving magnetic field is placed at the bottom of the reverberatory furnace, and the moving magnetic field generated from this inductor is applied to the molten metal in the furnace, giving a thrust to the molten metal and stirring it. It can be thought of as Jin. .

この構成の要部は第1図に示す通りで、同図中1は反射
炉溶湯保有部で、耐火材ta を外被tb(通常磁性板
)にて囲っている。2は誘導子で、炉底部に配置され、
この誘導子2が対向する外被Ik)は磁気短絡を防止す
べく非磁性体例えばステンレス材1b’lされる。8は
アルミ溶湯、4は被溶解アルミ材である。
The main parts of this structure are as shown in FIG. 1, where 1 is a reverberatory furnace molten metal holding section, in which a refractory material ta is surrounded by an outer sheath tb (usually a magnetic plate). 2 is an inductor, placed at the bottom of the furnace,
The outer sheath Ik) facing the inductor 2 is made of a non-magnetic material, such as a stainless steel material 1b'l, to prevent magnetic short circuits. 8 is molten aluminum, and 4 is an aluminum material to be melted.

ところで、第1図中の誘導子20表面と炉内の溶湯aに
至るまでの距離Go において、次の関係式が成立つ。
By the way, the following relational expression holds true for the distance Go between the surface of the inductor 20 and the molten metal a in the furnace in FIG.

BG=Bob(−TIIGo〕・・−・・・・・川(1
ここに BG・・・・・・誘導子に最も近い溶湯面の磁
束密度BQ・・・・・・誘導子表面の磁束密度T −°
−ボールピッチ 一方、攪拌に必要な磁束密度B() は定まっており、
距離GQ  が変化しても一定以上の値を維持する必要
がある。従って距離G。が増せば(1〕式において磁束
密度BGが減少していくことから誘導子表面の磁束密度
BOを上記磁束密度B() の指灘関数的減衰の補償に
見合うだけ増さなければならない。
BG=Bob(-TIIGo)... River(1
Here, BG... Magnetic flux density on the molten metal surface closest to the inductor BQ... Magnetic flux density on the inductor surface T −°
-Ball pitch On the other hand, the magnetic flux density B() required for stirring is fixed,
Even if the distance GQ changes, it is necessary to maintain a value above a certain value. Therefore, the distance G. As the magnetic flux density BG increases in equation (1), the magnetic flux density BG decreases, so the magnetic flux density BO on the inductor surface must be increased by an amount corresponding to the compensation for the finger-like attenuation of the magnetic flux density B().

ところが、溶湯の保有に際してはある一定以王の耐火材
1aの厚さが必要とされ、これがために必要な誘導子表
面磁束密度がかなりの値に達し、ひいては誘導子2が大
型化するとともに効率の低Fが著しくなる欠点があった
。この欠点を除去するための1手段として誘導子を炉壁
内に埋設することにより上記距離G。を減少させること
も考えられるが、この構成にあっては特に高価な誘導子
への溶湯による損傷が生じやすく、誘導子の保守点検も
不可能となることがら実責に供しにくい。
However, when holding molten metal, the thickness of the refractory material 1a is required to exceed a certain level, and this requires the inductor surface magnetic flux density to reach a considerable value, which in turn increases the size of the inductor 2 and reduces efficiency. There was a drawback that the low F was extremely high. One way to eliminate this drawback is to bury the inductor in the furnace wall to reduce the distance G. Although it is conceivable to reduce this, it is difficult to put it into practical use because this configuration is particularly prone to damage to the expensive inductor by the molten metal, and maintenance and inspection of the inductor is also impossible.

この発明の目的は誘導子の各磁極に対向するコアーを溶
湯容器を形成する耐火材中に設けることにより炉壁の厚
さを充分にとって保温効果を減じることなく、誘導子の
電磁効率を向上させるこ七にある。
The purpose of this invention is to improve the electromagnetic efficiency of the inductor by providing a core facing each magnetic pole of the inductor in the refractory material that forms the molten metal container, thereby increasing the thickness of the furnace wall without reducing the heat retention effect. It's in Ko-shichi.

以下、図示する実施例について具体的に説明する。第2
図はこの発明に係る装置の要部断面図で、第1図と均等
な機械要素は同一符号にて示すものとする。同第2図に
おいて、誘導子2は外枠2a内に収納される移動磁界発
生用磁極鉄心21)  (磁極21)j、2b2.、.
2bnを備えている)とこの各磁極2b1.2b2…2
bnに対して装着されるコイル20力、ラナッている。
The illustrated embodiment will be specifically described below. Second
The figure is a sectional view of a main part of the apparatus according to the present invention, and mechanical elements equivalent to those in FIG. 1 are designated by the same reference numerals. In FIG. 2, the inductor 2 consists of moving magnetic field generating magnetic pole iron cores 21) (magnetic poles 21)j, 2b2. ,.
2bn) and each of these magnetic poles 2b1.2b2...2
The coil 20 force installed against the bn is running.

0l−Onはコアで、それぞれ上記6磁41i 2b1
〜2bn  に対銅する位置に埋設等の手段によって容
器の耐火壁内に設けられる。そしてこのコアC1〜Cn
は非磁性材rb’中より誘導子2側に突出し、誘導子各
磁極2b1〜2bnに対向している。
0l-On is the core, each of the above 6 magnets 41i 2b1
It is provided in the refractory wall of the container by means such as embedding at a position opposite to ~2bn copper. And this core C1~Cn
protrudes from the inside of the non-magnetic material rb' toward the inductor 2, and faces each of the inductor magnetic poles 2b1 to 2bn.

上記構成において、溶湯8は図示しないバーナー装置に
よって高温に維持され、この溶湯8中に浴せられた被溶
解アルミ材4は外気とのしゃ断のもとに溶湯8から熱を
奪って溶解し、これによって被溶解アルミ材4の周囲に
は溶解したばかりの他の部分の溶湯に比しかなり低温の
溶湯が分布することになる。そこで、誘導子2のコイル
2Cに対して交流電圧を印加すると、1ボールピツチを
なす磁極2bl〜2bn相互間に磁束がまたがり、電圧
位相の変化に伴って磁束が進行し、いわゆる移動磁界が
芦湯8に作用し、この溶湯8との電、磁作用により溶湯
8は推力を受けて攪拌作用がなされる。ところで、この
発明に係る。溶湯容器の耐火材中に埋設等によって保持
されるコアは耐火材に比して磁気抵抗が殆んど無視でき
る。従って、誘導子2の各磁極21) 1〜2bnより
生み出される磁束が溶湯8に達するまでの磁気抵抗は実
質的にコアC4〜Cnと溶湯8との距離G、に対応する
部分のみとなり、著しい減少がはかられる。これによっ
て上記第1式の距離GQ が距1IIG1  に減少す
るから誘導子2からの磁束、1が指数関数的な割合で有
効に溶湯8への推力増進に寄与できる。
In the above configuration, the molten metal 8 is maintained at a high temperature by a burner device (not shown), and the aluminum material 4 to be melted, which is poured into the molten metal 8, absorbs heat from the molten metal 8 and melts while being cut off from the outside air. As a result, around the aluminum material 4 to be melted, the molten metal is distributed at a considerably lower temperature than the molten metal in other parts that have just been melted. Therefore, when an AC voltage is applied to the coil 2C of the inductor 2, the magnetic flux straddles the magnetic poles 2bl to 2bn forming a one-ball pitch, and the magnetic flux advances as the voltage phase changes, causing a so-called moving magnetic field. 8, and the molten metal 8 receives a thrust due to the electric and magnetic action with the molten metal 8, and a stirring action is performed. By the way, according to this invention. The core held by embedding or the like in the refractory material of the molten metal container has almost negligible magnetic resistance compared to the refractory material. Therefore, the magnetic resistance until the magnetic flux produced by each magnetic pole 21) 1 to 2bn of the inductor 2 reaches the molten metal 8 is substantially only the portion corresponding to the distance G between the cores C4 to Cn and the molten metal 8, and is significant. A decrease is expected. As a result, the distance GQ in the first equation is reduced to the distance 1IIG1, so that the magnetic flux 1 from the inductor 2 can effectively contribute to increasing the thrust to the molten metal 8 at an exponential rate.

第3図は他の実施例を示す要部断面図で、磁気しゃ所用
非磁性体の内側にコア01〜Cn  を埋設した機構に
関するものである。かかる構成は非磁性体I L、+ 
+の厚みに対して磁気−一増加を来すものの全体の磁気
抵抗に比して非磁性体1b1の磁気抵抗はごく僅かであ
るからほぼ同等の作用を期待でき、強度的に#′i第2
図に示す構成以上のものが期待できる。
FIG. 3 is a sectional view of a main part showing another embodiment, which relates to a mechanism in which cores 01 to Cn are embedded inside a non-magnetic material for magnetic shielding. Such a configuration is a non-magnetic material IL, +
Although the magnetic resistance increases by -1 with respect to the thickness of 2
You can expect more than the configuration shown in the figure.

なお、上記説明においては反射炉中の溶湯の攪拌につい
て述べたものであるが、この電磁攪拌装置は溶湯を保有
する全ての装置に適用できることはいうまでもない。ま
た、コア01〜ら は埋設式に耐火材に設けるとはかぎ
らず、伸長自在に取付けるようにしてもよく、誘導子の
配置は容器底面部とは限らず、容器側面部としてもよい
Although the above description has been made regarding stirring of molten metal in a reverberatory furnace, it goes without saying that this electromagnetic stirring device can be applied to any device that holds molten metal. In addition, the cores 01 to 2 do not necessarily have to be installed in the refractory material in a buried manner, but may be attached in an extensible manner, and the inductor is not limited to the bottom of the container, but may be placed on the side of the container.

以上述べたようにこの発明に係る溶湯の電磁攪拌装置は
溶湯保有の容器に対して溶湯撹拌用誘導子を備える構成
において、上記誘導子の各磁極に対向する位置にコアを
、容器形成の耐火ヴ中に設けるようにしたものである。
As described above, the electromagnetic stirring device for molten metal according to the present invention has a structure in which a container holding the molten metal is provided with an inductor for stirring the molten metal, and a core is placed at a position facing each magnetic pole of the inductor to form a fireproof container. It was designed to be installed in the middle of the network.

かかる構成に基づいて、誘導子各磁極より出される磁束
が溶湯に達するまでの磁路の磁気抵抗は著しく減少され
、しかも溶湯容器の誘導子に対向する耐火壁の厚さも制
限を受けることなく高温の溶湯に対して十分の値を取る
ことができる。このことは従来、特に容器が必要とする
耐火壁を通じて溶湯に所要推力を得るために極めて大容
量の大型誘導子を用いる必要性に惇々て、この発明は同
一推力を容器内の溶湯に与えるのにごく小容量の誘導子
にて実現できる実利は大である。
Based on this configuration, the magnetic resistance of the magnetic path through which the magnetic flux emitted from each magnetic pole of the inductor reaches the molten metal is significantly reduced, and the thickness of the refractory wall facing the inductor of the molten metal container is not limited and can be used at high temperatures. can take a sufficient value for molten metal. This has traditionally been compounded by the need to use a large inductor with an extremely large capacity in order to obtain the required thrust on the molten metal through the refractory wall required by the vessel, and this invention provides the same thrust on the molten metal within the vessel. However, the practical benefits that can be achieved with a very small capacity inductor are large.

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

第1図は従来の電磁攪拌装置を備えた反射炉の要部断面
図、第2図はこの発明の実施例を示す要部詳細断面図、
第3図はこの発明の他の実施例を示す要部概略断面図で
ある。 l・・・・・・・・・・・・・・・溶湯容器  1a 
 ・・・・・・・・・・・・・・・耐火壁2・・・・・
・・・・・・・・・・誘導子   2J〜2bn・・・
・・・磁極C1〜Cn・・・コア    3・・・−・
・・・・・・・・・・・・・溶融金属出願人 神鋼電機
株式会社 代理人 弁理士 斎藤春弥 第 2  図
FIG. 1 is a sectional view of the main part of a reverberatory furnace equipped with a conventional electromagnetic stirring device, and FIG. 2 is a detailed sectional view of the main part showing an embodiment of the present invention.
FIG. 3 is a schematic sectional view of main parts showing another embodiment of the present invention. l・・・・・・・・・・・・Molten metal container 1a
・・・・・・・・・・・・・・・Fireproof wall 2・・・・・・
......Inductor 2J~2bn...
...Magnetic poles C1 to Cn...Core 3...-
・・・・・・・・・・・・Molten metal applicant Shinko Electric Co., Ltd. agent Patent attorney Haruya Saito Figure 2

Claims (1)

【特許請求の範囲】[Claims] 1溶融金属を保有する容器に対して上記溶融金属に推力
を及はし当該溶融金属を攪拌する誘導子を備える構成に
おいて、誘導子の各磁極の磁極面に対向し、当該磁極面
と溶融金属との間に存する耐火壁内に上記各J14ii
と対をなす複数のコアを設置したことを特徴とする溶融
金属の電磁攪拌装置。
1. In a configuration including an inductor that applies thrust to the molten metal and stirs the molten metal in a container holding the molten metal, the inductor faces the magnetic pole surface of each magnetic pole of the inductor, and the magnetic pole surface and the molten metal Each of the above J14ii inside the fireproof wall existing between
An electromagnetic stirring device for molten metal characterized by having a plurality of cores arranged in pairs.
JP56122866A 1981-08-04 1981-08-04 Electromagnetic stirring device for molten metal Expired JPS6058398B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56122866A JPS6058398B2 (en) 1981-08-04 1981-08-04 Electromagnetic stirring device for molten metal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56122866A JPS6058398B2 (en) 1981-08-04 1981-08-04 Electromagnetic stirring device for molten metal

Publications (2)

Publication Number Publication Date
JPS5822888A true JPS5822888A (en) 1983-02-10
JPS6058398B2 JPS6058398B2 (en) 1985-12-19

Family

ID=14846567

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56122866A Expired JPS6058398B2 (en) 1981-08-04 1981-08-04 Electromagnetic stirring device for molten metal

Country Status (1)

Country Link
JP (1) JPS6058398B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2007018241A1 (en) * 2005-08-10 2007-02-15 Central Research Institute Of Electric Power Industry Electromagnetic agitator

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4829456U (en) * 1971-08-13 1973-04-11
JPS55144477U (en) * 1979-04-03 1980-10-16

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4829456U (en) * 1971-08-13 1973-04-11
JPS55144477U (en) * 1979-04-03 1980-10-16

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2007018241A1 (en) * 2005-08-10 2007-02-15 Central Research Institute Of Electric Power Industry Electromagnetic agitator
JP2007069264A (en) * 2005-08-10 2007-03-22 Central Res Inst Of Electric Power Ind Electromagnetic stirring device
JP4648851B2 (en) * 2005-08-10 2011-03-09 財団法人電力中央研究所 Electromagnetic stirring device
US7972556B2 (en) 2005-08-10 2011-07-05 Central Research Institute Of Electric Power Industry Electromagnetic agitator

Also Published As

Publication number Publication date
JPS6058398B2 (en) 1985-12-19

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