JPH0681404B2 - Magnetic heating filament manufacturing method - Google Patents
Magnetic heating filament manufacturing methodInfo
- Publication number
- JPH0681404B2 JPH0681404B2 JP63263347A JP26334788A JPH0681404B2 JP H0681404 B2 JPH0681404 B2 JP H0681404B2 JP 63263347 A JP63263347 A JP 63263347A JP 26334788 A JP26334788 A JP 26334788A JP H0681404 B2 JPH0681404 B2 JP H0681404B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core wire
- alloy
- wire
- heating filament
- 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 - Fee Related
Links
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- Suspension Of Electric Lines Or Cables (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は架空電線の融雪線等として使用される磁性発熱
線条体の製造方法に関し、特にその磁性発熱特性を向上
させた低磁界高発熱型の磁性発熱線条体の製造方法に関
する。Description: TECHNICAL FIELD The present invention relates to a method for manufacturing a magnetic heating filament used as a snow melting wire of an overhead wire, and particularly to a low magnetic field and high heat generation with improved magnetic heating characteristics. To a magnetic heating filament of a mold.
[従来の技術] 架空電線の融雪線として使用される磁性線条体の構造
は、第2図に示すように、強磁性の金属又は合金からな
る芯線1の周囲を導電性の金属又は合金からなる被覆層
2で被覆したものとなっている。この磁性線条体は架空
電線に対しその撚り方向と直角に近い角度をなして巻き
付けて使用する。[Prior Art] As shown in FIG. 2, the structure of a magnetic filament used as a snow-melting wire of an overhead wire is made of a conductive metal or alloy around a core wire 1 made of a ferromagnetic metal or alloy. It is coated with the coating layer 2. This magnetic filament is used by winding it around an overhead wire at an angle close to a right angle to the twisting direction.
磁性線条体の発熱の原理は、以下のようなものである。
架空電線の架線方向に交番電流を通ずると架空電線の周
囲に円輪状の交番磁界が生じる。The principle of heat generation of the magnetic filament is as follows.
When an alternating current is passed in the overhead wire direction, a ring-shaped alternating magnetic field is generated around the overhead wire.
そうすると、架空電線の周囲に巻回された磁性線条体に
おいて、空間磁場成分及び電場成分が強磁性体の芯線1
にトラップされ、周囲の漏れ磁束が強磁性体芯線1の周
囲に被着した導電性被覆層2に集中する。この集中した
磁束によって電磁誘導が起こり、導電性の金属又は合金
からなる被覆層2に渦電流が生じる。この渦電流による
Joule損失によって磁性発熱線条体が発熱し、その発熱
によって架空電線に付着した雪に対する融雪がおこる。Then, in the magnetic filaments wound around the overhead wire, the core magnetic field 1 of which the spatial magnetic field component and the electric field component are ferromagnetic
The leakage magnetic flux of the surroundings is concentrated on the conductive coating layer 2 attached to the periphery of the ferromagnetic core wire 1. Electromagnetic induction occurs due to the concentrated magnetic flux, and an eddy current is generated in the coating layer 2 made of a conductive metal or alloy. Due to this eddy current
The Joule loss causes the magnetic heating filament to generate heat, which causes snow melting on the snow that has adhered to the overhead wire.
この場合に、発熱量を左右するのは渦電流損失の大きさ
であるが、この渦電流損失を左右する要因には以下に示
す2つのものがあり、これらの要因の組合せで発熱量が
決まってくる。In this case, it is the magnitude of the eddy current loss that influences the heat generation amount. The following two factors influence the eddy current loss, and the heat generation amount is determined by the combination of these factors. Come on.
導電性被覆層2を通過する漏れ磁束密度の時間変化。The time change of the leakage magnetic flux density passing through the conductive coating layer 2.
強磁性芯線1からの距離による電磁場減衰のしかた。How to attenuate the electromagnetic field depending on the distance from the ferromagnetic core wire 1.
そして、これらの特性に大きな影響を与えるのは、中心
強磁性芯線1の透磁率である。特に、低磁界側の透磁率
がこれらの特性を左右する。The magnetic permeability of the central ferromagnetic core wire 1 has a great influence on these characteristics. In particular, the magnetic permeability on the low magnetic field side influences these characteristics.
而して、従来の線条体は太径の中心磁性体に導電性金属
を被覆し、次いでこの複合体を塑性加工により細線化し
た後、機械的に応力緩和を行って製品としていた。Thus, in the conventional filamentous body, a thick central magnetic material is coated with a conductive metal, and then this composite is thinned by plastic working, and then mechanical stress relaxation is performed to obtain a product.
[発明が解決しようとする課題] しかしながら、この従来の製造方法においては、機械的
な応力緩和では内部応力が容易には除去されないこと、
及び塑性加工により結晶方位が1方向に集中した集合組
織を形成してしまうことから、一軸磁気異方性が生じや
すい。このような磁気異方性が生じると、透磁率が著し
く低下する。通常、融雪スパイラル線は100e以下の磁界
環境では融雪の能力はなくなってしまう。[Problems to be Solved by the Invention] However, in this conventional manufacturing method, internal stress is not easily removed by mechanical stress relaxation,
Also, since the plastic working forms a texture in which the crystal orientations are concentrated in one direction, uniaxial magnetic anisotropy is likely to occur. When such magnetic anisotropy occurs, the magnetic permeability remarkably decreases. Normally, the snowmelt spiral wire loses its ability to melt in a magnetic field environment of 100e or less.
本発明はかかる問題点に鑑みてなされたものであって、
中心に配設される強磁性芯線の透磁率を向上させ、発熱
特性を改善して低磁界でも十分な融雪能力をもたせるこ
とができる磁性発熱線条体の製造方法を提供することを
目的とする。The present invention has been made in view of such problems,
It is an object of the present invention to provide a method for manufacturing a magnetic heating filament in which the magnetic permeability of a ferromagnetic core wire disposed in the center is improved, the heat generation characteristics are improved, and a sufficient snow melting ability can be provided even in a low magnetic field. .
[課題を解決するための手段] 本発明に係る磁性発熱線条体の製造方法は、強磁性の金
属又は合金を塑性加工して芯線を得、次いでこの芯線を
その再結晶温度より高い温度に加熱して再結晶化させた
後、前記芯線の周囲に導電性の金属又は合金をメッキし
て被着することを特徴とする。[Means for Solving the Problems] A method of manufacturing a magnetic heating filament according to the present invention is to plastically work a ferromagnetic metal or alloy to obtain a core wire, and then heat the core wire to a temperature higher than its recrystallization temperature. After being heated and recrystallized, a conductive metal or alloy is plated and deposited around the core wire.
[作用] 本発明においては、芯線を塑性加工した後、この芯線を
再結晶温度より高い温度に加熱して再結晶化させる。こ
れにより、塑性加工により低下していた透磁率が回復
し、十分に高い透磁率が得られる。一方、この再結晶温
度は通常の強磁性芯線材料として使用される金属又は合
金では900℃を超えるため、通常導電性被覆層として使
用されるアルミニウム合金の融点を超えてしまう。そこ
で、この被覆層は再結晶熱処理の後に芯線の周囲にメッ
キにより被着する。これにより、中心磁性体の透磁率が
著しく向上した磁性発熱線条体が得られる。[Operation] In the present invention, after the core wire is plastically worked, the core wire is heated to a temperature higher than the recrystallization temperature to be recrystallized. As a result, the magnetic permeability which has been lowered by the plastic working is recovered, and a sufficiently high magnetic permeability can be obtained. On the other hand, this recrystallization temperature exceeds 900 ° C. for a metal or alloy used as a usual ferromagnetic core wire material, and therefore exceeds the melting point of an aluminum alloy usually used as a conductive coating layer. Therefore, this coating layer is deposited by plating around the core wire after the recrystallization heat treatment. As a result, a magnetic heating filament in which the magnetic permeability of the central magnetic body is remarkably improved can be obtained.
[実施例] 以下、本発明の実施例について具体的に説明する。[Examples] Examples of the present invention will be specifically described below.
融雪線として使用される磁性発熱線条体の中心磁性体
(芯線)には、Fe,Ni,Cr,Mn又はCo等の3d遷移金属を含
有する合金、中でもFeを主成分とする合金が使用され
る。これらの合金は、伸線時の塑性加工により生じる内
部残留応力によって一軸異方性が発生し、透磁率が著し
く低下する。An alloy containing 3d transition metal such as Fe, Ni, Cr, Mn or Co is used for the central magnetic body (core wire) of the magnetic heating filament used as a snow melting wire, and an alloy mainly containing Fe is used. To be done. In these alloys, uniaxial anisotropy occurs due to internal residual stress generated by plastic working during wire drawing, resulting in a marked decrease in magnetic permeability.
第1図は横軸に磁界(0e)をとり、縦軸に磁束密度
(G)をとって市販の42合金の磁化特性を示すグラフ図
である。FIG. 1 is a graph showing the magnetization characteristics of the commercially available 42 alloy with the horizontal axis representing the magnetic field (0 e ) and the vertical axis representing the magnetic flux density (G).
第1図中、磁化特性を図示した4種の材料は、夫々伸線
加工(線径8mmから線径4mmまで)のままのもの、450℃
で焼鈍したもの、900℃で30分間溶体化処理した後水焼
入れしたもの及び900℃で30分間焼鈍したものである。In Fig. 1, the four types of materials whose magnetization characteristics are shown are those that have been drawn (drawn from wire diameter 8 mm to wire diameter 4 mm) at 450 ° C.
Those annealed at 900 ° C., solution-quenched at 900 ° C. for 30 minutes and then water-quenched, and annealed at 900 ° C. for 30 minutes.
この第1図に示された磁束密度の最大値を対応する磁界
で除算することにより透磁率が求まるが、このようにし
て求められた伸線直後の透磁率は77(CGS・EMU)と極め
て低いのに対し、900℃焼鈍後の透磁率は1000(CGS・EM
U)となり、約13倍の極めて高い透磁率が得られる。こ
れは900℃で焼鈍することにより再結晶化が進行したた
めである。これに対して、450℃の焼鈍の場合は、再結
晶化が生じないために透過率は126(CGS・EMU)と低
い。The magnetic permeability can be obtained by dividing the maximum value of the magnetic flux density shown in Fig. 1 by the corresponding magnetic field. The magnetic permeability immediately after wire drawing thus obtained is 77 (CGS / EMU). Despite being low, the magnetic permeability after annealing at 900 ℃ is 1000 (CGS / EM
U), and an extremely high magnetic permeability of about 13 times is obtained. This is because recrystallization proceeded by annealing at 900 ° C. On the other hand, in the case of annealing at 450 ° C, since recrystallization does not occur, the transmittance is as low as 126 (CGS / EMU).
従って、本発明方法においては、芯線となる強磁性の金
属又は合金をその再結晶温度以上に加熱して再結晶化さ
せる。そして、この再結晶化処理の後は、芯線に塑性加
工を加えない。Therefore, in the method of the present invention, the ferromagnetic metal or alloy serving as the core wire is recrystallized by heating it to the recrystallization temperature or higher. After the recrystallization treatment, the core wire is not subjected to plastic working.
従来の磁性発熱線条体の製造方法においては、前述の如
く、芯線となる線材の周囲に導電性被覆層となる材料を
被覆した後、この複合体を伸線加工することにより、芯
線が被覆層で被覆された磁性線条体を製造している。と
ころが、本願発明においても同様にして複合体の伸線加
工により被覆層を形成し、その後、前述の再結晶化処理
を実施しようとすると、以下に示す不都合がある。In the conventional method for producing a magnetic heating filament, as described above, the core wire is coated by coating the material for the conductive coating layer around the core wire and then drawing the composite. A magnetic filament coated with layers is produced. However, also in the present invention, if the coating layer is formed by wire drawing of the composite in the same manner and then the above-mentioned recrystallization treatment is carried out, the following problems occur.
即ち、融雪線は架空電線に巻回して使用される都合上、
融雪線(磁性発熱線条体)の導電性被覆層としては、通
常、アルミニウム合金を使用している。しかしながら、
このアルミニウム合金はその融点が前記再結晶化処理温
度(42合金の場合は例えば900℃)よりも低いため、ア
ルミニウム合金層を被着した後に、前述の再結晶化処理
を実施することはできない。このように、導電性被覆層
を被着した後に、芯線を再結晶化処理することは極めて
困難である。一方、芯線を再結晶化処理した後、アルミ
ニウム合金材を被着し、この複合体を伸線加工すること
により芯線の周囲にアルミニウム合金の被覆層を形成す
ることは、芯線に対して塑性変形を加えることになり、
透磁率の低下を招来する。That is, the snow-melting wire is used by being wound around an overhead wire,
An aluminum alloy is usually used for the conductive coating layer of the snow melting wire (magnetic heating filament). However,
Since the melting point of this aluminum alloy is lower than the recrystallization treatment temperature (for example, 900 ° C in the case of 42 alloy), the above-mentioned recrystallization treatment cannot be performed after depositing the aluminum alloy layer. Thus, it is extremely difficult to recrystallize the core wire after depositing the conductive coating layer. On the other hand, after recrystallizing the core wire, depositing an aluminum alloy material and drawing the composite to form an aluminum alloy coating layer around the core wire is a plastic deformation of the core wire. Will be added,
This causes a decrease in magnetic permeability.
そこで、本発明においては、再結晶化処理後の芯線に対
してメッキによりアルミニウム合金等の被覆層を形成す
る。このメッキ方法としては、溶融メッキ、電気メッキ
及び無電解メッキ等がある。なお、アルミニウム合金を
導電性被覆層として使用する場合には、製造コスト等を
勘案すると溶融メッキ法により被覆層を形成することが
好ましい。Therefore, in the present invention, a coating layer of aluminum alloy or the like is formed on the core wire after the recrystallization treatment by plating. Examples of this plating method include hot dipping, electroplating, and electroless plating. When an aluminum alloy is used as the conductive coating layer, it is preferable to form the coating layer by a hot dip plating method in consideration of manufacturing cost and the like.
このようにして製造された磁性発熱線条体は、芯線が42
合金であり、被覆層がアルミニウム合金であるとする
と、従来の磁性発熱線条体に比して4倍以上の発熱量を
得ることができ、100e以下の低磁界における融雪線とし
ての使用も可能である。The magnetic heating filament produced in this way has a core wire of 42
If it is an alloy and the coating layer is an aluminum alloy, it is possible to obtain more than four times as much heat generation as the conventional magnetic heating filament, and it can also be used as a snow melting wire in a low magnetic field of 100e or less. Is.
[発明の効果] 本発明によれば、磁性体芯線を再結晶化処理して塑性加
工時の異方性を除去し、透磁率を高めた後、導電性の被
覆層をメッキにより形成するから、再結晶化処理後芯線
に塑性変形を加えることなく被覆層を形成することがで
きる。[Effects of the Invention] According to the present invention, the magnetic core wire is recrystallized to remove anisotropy during plastic working to increase the magnetic permeability, and then the conductive coating layer is formed by plating. After the recrystallization treatment, the coating layer can be formed without applying plastic deformation to the core wire.
このため、本発明によれば、芯線の透磁率が高く、発熱
量が著しく増大し、低磁界においても十分な融雪効果が
得られる磁性発熱線条体を製造することができる。Therefore, according to the present invention, it is possible to manufacture a magnetic heating filament in which the magnetic permeability of the core wire is high, the amount of heat generation is significantly increased, and a sufficient snow melting effect is obtained even in a low magnetic field.
第1図は42合金の磁化特性を示すグラブ図、第2図は磁
性発熱線条体の断面を示す図である。 1;強磁性の金属又は合金の芯線、2;導電性の金属又は合
金の被覆層FIG. 1 is a grab diagram showing the magnetization characteristics of 42 alloy, and FIG. 2 is a diagram showing a cross section of a magnetic heating filament. 1; Ferromagnetic metal or alloy core wire, 2; Conductive metal or alloy coating layer
Claims (2)
を得、次いでこの芯線をその再結晶温度より高い温度に
加熱して再結晶化させた後、前記芯線の周囲に導電性の
金属又は合金をメッキして被着することを特徴とする磁
性発熱線条体の製造方法。Claim: What is claimed is: 1. A ferromagnetic metal or alloy is plastic-processed to obtain a core wire, which is then heated to a temperature higher than its recrystallization temperature to recrystallize the core wire. A method of manufacturing a magnetic heating filament, which comprises depositing a metal or an alloy by plating.
キ、電気メッキ又は無電解メッキにより前記芯線に被着
することを特徴とする請求項1に記載の磁性発熱線条体
の製造方法。2. The method for producing a magnetic heating filament according to claim 1, wherein the conductive metal or alloy is applied to the core wire by hot dipping, electroplating or electroless plating.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63263347A JPH0681404B2 (en) | 1988-10-19 | 1988-10-19 | Magnetic heating filament manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63263347A JPH0681404B2 (en) | 1988-10-19 | 1988-10-19 | Magnetic heating filament manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02111215A JPH02111215A (en) | 1990-04-24 |
| JPH0681404B2 true JPH0681404B2 (en) | 1994-10-12 |
Family
ID=17388210
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63263347A Expired - Fee Related JPH0681404B2 (en) | 1988-10-19 | 1988-10-19 | Magnetic heating filament manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0681404B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS59806A (en) * | 1982-06-28 | 1984-01-06 | 株式会社フジクラ | Magnetic material |
| JPS58223211A (en) * | 1982-06-21 | 1983-12-24 | 株式会社フジクラ | Linear magnetic material |
| JPS58224511A (en) * | 1982-06-21 | 1983-12-26 | 株式会社フジクラ | Snow fusing wire material and method of producing same |
-
1988
- 1988-10-19 JP JP63263347A patent/JPH0681404B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02111215A (en) | 1990-04-24 |
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|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |