JPH0135574B2 - - Google Patents
Info
- Publication number
- JPH0135574B2 JPH0135574B2 JP57105500A JP10550082A JPH0135574B2 JP H0135574 B2 JPH0135574 B2 JP H0135574B2 JP 57105500 A JP57105500 A JP 57105500A JP 10550082 A JP10550082 A JP 10550082A JP H0135574 B2 JPH0135574 B2 JP H0135574B2
- Authority
- JP
- Japan
- Prior art keywords
- wire
- diameter
- snow
- magnetic
- wires
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02A—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
- Y02A30/00—Adapting or protecting infrastructure or their operation
- Y02A30/14—Extreme weather resilient electric power supply systems, e.g. strengthening power lines or underground power cables
Landscapes
- Resistance Heating (AREA)
- Wire Processing (AREA)
- Insulated Conductors (AREA)
- Suspension Of Electric Lines Or Cables (AREA)
Description
この発明は架空送配電線の氷結防止のために電
線上に巻付けられる線状磁性体に関するものであ
る。
冬期に於て、寒冷地域特に北日本、或は裏日本
では、架空送・配電線に着雪、着氷を来たし、こ
れが成長してかなりの大きさとなり、径間におけ
る電線重量の増大、風圧荷重の増大を招き、電線
の弛度の増大や、過大張力による電線の破断、更
には鉄塔の倒壊などの事故を発生するに至る原因
となる場合が多い。又、着氷雪がブロツク状とな
り落下すると、架空線下を通行する人間に対する
危険がある外、架空線下が農地であつても、作物
やビニルハウス等に損傷を与えるおそれがあり、
大きな社会問題を発生するためこの問題の解決が
要望されている。
このため、これまで着雪防止対策として、一時
的な大電流送電により、導体のジユール熱により
融解する方法、或いはリング状のものを送電線に
取り付けて、着雪塊を落下せしめる方法等が行な
われているが、大電流送電は電力系統運用上制限
を受け自由には実施できず、リング状のものを取
付けても着氷雪の種類によつて効果に差があり、
更に、成長した氷雪塊を単に落下させると、その
落下地点に於て2次災害を発生するおそれがあ
り、十分な対策とは言えないものである。
一方交流送電線上に磁性体で作られたスリーブ
或いはスパイラル状に加工された線状体、テー
プ、ロツド等を巻き付け、送電々流による交流磁
界がスリーブ等を通過することによつて発生する
ヒステリシス損、渦電流損による損失熱を利用し
て融雪する方法も提案されているが、これらのス
リーブ、線、テープ、ロツドを電線上に巻き付け
ると電線重量が増加するため、なるべく軽量であ
ることが望ましく、又、着氷雪の起らない温度で
の磁性体からの発熱は、送電損失の増加となるの
で、高温時には磁気特性が低下し発熱しなくなる
キユリー点の低い材料が望ましい。
ところでキユリー点が0℃から100℃位に存在
する磁性合金としてFe−N1−C〓−Si合金等が常
温付近にキユリー点を有し、又、磁気特性も良好
で、この合金をスリーブ状に加工して電線に被せ
たり、線状或はテープ状に加工して電線に巻き付
けると、降雪時にこの磁性体が強磁性体となり、
ヒステリシス損或は渦電流損による発熱が、電線
の抵抗損による発熱とともに複合して作用し、電
線に付着した雪を融解し、高温状態では磁性体が
常磁性体となり、不必要な発熱による送電損失を
無くすことができるので雪害対策として実用上有
効な方法である。
ところが、従来からこの種の合金は熱処理条件
や加工条件が磁気特性に大きく影響し、再現性に
乏しい欠点があつた。
例えば線条体に加工する場合、通常引き抜き加
工が行なわれるが、引き抜き加工度の大小にかか
わらず、磁気特性が劣化してしまい、雪害対策と
して効果のある量を電線に取り付けると、著るし
くその重量が増加してしまい実用上使用すること
ができなくなる等の欠点がある。
本発明はこのように状況に鑑みてなされたもの
で、磁性体の周囲に高導電性金属が被覆され、か
つ歪の除去された融雪電線用線材及び磁性金属線
材の周囲に導電性金属を被覆し、所定の径まで減
径加工した後、磁性金属線材の径と曲げ径の比が
2〜9%となるようにくり返し曲げ加工を施して
残留歪をとることを特徴とする融雪電線用線材の
製造方法に存する。
磁性材料に伸線加工や圧延加工を加えると、結
晶が歪み、その歪みは外周部に至る程、加工設備
その他との摩擦が加えられるために大きくなる傾
向がある。
一般にこの残留歪が磁気特性を変化させている
ものと考えられている。そして一般にこの歪は加
熱によつて回復することが多いが、本発明で使用
される磁性金属(合金)のような場合には、加熱
による回復度は小さく、また高温に加熱すると強
度が低下してしまつたり、かつ被覆材の導電金属
と磁性材との界面に化合物層を生成し、導電性能
を阻害したり、磁気特性を変質したりするおそれ
があつた。
本発明による方法はこれらの欠点を生ずること
なしに、熱処理により残留歪を回復させ、磁気特
性を著るしく向上させることができる。
次に本発明の実施例について述べる。
実施例 1
表1に示す組成のFe−Ni系合金を真空溶解して
直径30mmのインゴツトに鋳造し、その後熱間鍜造
及び冷間鍜造を行なつて、直径10mmの線材を得
た。
This invention relates to a linear magnetic material that is wrapped around electric wires to prevent freezing of overhead power transmission and distribution lines. During the winter, snow and ice accrete on overhead transmission and distribution lines in cold regions, especially in northern Japan and the back of Japan, and this can grow to a considerable size, increasing the weight of the wires in the span and causing wind pressure loads. This often leads to an increase in the slackness of the wires, breakage of the wires due to excessive tension, and even the collapse of steel towers. In addition, if ice and snow fall in the form of blocks, not only is there a danger to people passing under the overhead lines, but even if the area under the overhead lines is agricultural land, there is a risk of damaging crops, vinyl houses, etc.
There is a demand for a solution to this problem as it causes a major social problem. For this reason, as a measure to prevent snow accumulation, methods have been used to prevent snow accumulation, such as temporarily transmitting large currents to melt the snow due to the heat generated by the conductor, or attaching ring-shaped objects to power transmission lines to cause the snow to fall. However, large current power transmission cannot be carried out freely due to power system operation restrictions, and even if ring-shaped devices are installed, the effectiveness varies depending on the type of ice and snow.
Furthermore, if the grown ice and snow blocks are simply dropped, there is a risk that secondary disasters will occur at the point where they fall, and this cannot be said to be a sufficient countermeasure. On the other hand, when a sleeve made of magnetic material, a spirally processed linear body, tape, rod, etc. is wrapped around an AC power transmission line, hysteresis loss is generated when the AC magnetic field due to the transmission current passes through the sleeve, etc. A method of melting snow using heat loss due to eddy current loss has also been proposed, but wrapping these sleeves, wires, tapes, and rods around electric wires increases the weight of the wires, so it is desirable that they be as lightweight as possible. Furthermore, since heat generated from the magnetic material at temperatures at which icing and snow does not occur increases power transmission loss, it is desirable to use a material with a low Curie point that reduces magnetic properties and does not generate heat at high temperatures. By the way, Fe-N 1 -C〓-Si alloy, etc., has a Curie point near room temperature as a magnetic alloy with a Curie point between 0℃ and 100℃, and also has good magnetic properties. When it is processed into a wire and covered with it, or processed into a wire or tape and wrapped around the wire, this magnetic material becomes a ferromagnetic material during snowfall.
Heat generation due to hysteresis loss or eddy current loss acts in combination with heat generation due to resistance loss in the wire, melting snow attached to the wire, magnetic material becomes paramagnetic in high temperature conditions, and power transmission is caused by unnecessary heat generation. This is a practically effective method as a countermeasure against snow damage because it eliminates losses. However, in the past, this type of alloy had the disadvantage that heat treatment conditions and processing conditions greatly affected the magnetic properties, resulting in poor reproducibility. For example, when processing wires into wires, drawing is usually performed, but regardless of the degree of drawing, the magnetic properties will deteriorate, and if a quantity that is effective as a snow damage countermeasure is attached to electric wires, it will cause significant damage. There are drawbacks such as an increase in weight, making it impossible to use it practically. The present invention has been made in view of the above circumstances, and provides a wire material for snow melting wires in which a highly conductive metal is coated around a magnetic material and strain is removed, and a conductive metal is coated around a magnetic metal wire material. A wire material for snow-melting electric wires, characterized in that, after the diameter is reduced to a predetermined diameter, the magnetic metal wire material is subjected to repeated bending processing so that the ratio of the diameter to the bending diameter is 2 to 9% to remove residual strain. It consists in the manufacturing method. When a magnetic material is subjected to wire drawing or rolling, the crystals become distorted, and the distortion tends to increase toward the outer periphery due to friction with processing equipment and other objects. It is generally believed that this residual strain changes the magnetic properties. In general, this strain is often recovered by heating, but in the case of magnetic metals (alloys) used in the present invention, the degree of recovery by heating is small, and the strength decreases when heated to high temperatures. In addition, there was a risk that a compound layer would be formed at the interface between the conductive metal and the magnetic material of the coating material, impeding the conductive performance or altering the magnetic properties. The method according to the present invention can recover the residual strain by heat treatment and significantly improve the magnetic properties without causing these drawbacks. Next, examples of the present invention will be described. Example 1 An Fe--Ni alloy having the composition shown in Table 1 was vacuum melted and cast into an ingot with a diameter of 30 mm, and then hot and cold forged to obtain a wire rod with a diameter of 10 mm.
【表】
これらの線材の表面の酸化スケール、油等を取
り除き清浄にした後、外径12mm肉厚0.8mmのアル
ミ管を被覆した後、直径2.6mmまで伸線加工し、
アルミニウムとその内部の磁性合金とを金属的接
着をさせた。
この線を磁性金属線材の線径r、曲げ径Rとす
るときにr/R=0.052即ち1.5%、5.2%、9.5%
の曲げ歪が合金最外部で全周に亘り加わるように
曲げ加工をくり返し施し残留歪取りを行なつたも
のを、伸線したままで曲げ加工による歪取りをし
なかつたものと比較して直流磁化測定器によつて
磁気特性を測定した。その結果は表2の通りで本
発明による複合線はその磁気特性が大幅に改良さ
れていることが判る。(いずれも測定条件は0℃、
30Oeである。)[Table] After cleaning the surface of these wires to remove oxidation scale, oil, etc., they were coated with aluminum tubes with an outer diameter of 12 mm and a wall thickness of 0.8 mm, and then wire-drawn to a diameter of 2.6 mm.
Aluminum and the magnetic alloy inside were bonded metallically. When this wire is the wire diameter r of the magnetic metal wire and the bending diameter R, r/R=0.052, that is, 1.5%, 5.2%, 9.5%
The wire was repeatedly bent so that the bending strain was applied all around the outermost part of the alloy to remove residual strain, and the wire was drawn as it was and the strain was not removed by bending. Magnetic properties were measured using a magnetization measuring device. The results are shown in Table 2, and it can be seen that the composite wire according to the present invention has significantly improved magnetic properties. (In both cases, the measurement conditions were 0℃,
It is 30Oe. )
【表】
実施例 2
Ni6.2重量%、Cr3.1重量%、Si1.0重量%残部
Fe及び不純物からなる合金を実施例1と同じ方
法によつて、直径2.6mmの合金とアルミニウムと
の複合線とし、これを表3に示す歪が合金線の最
外部に作用するようにくり返し曲げ加工を施し、
残留歪取りを行なつた。
表3から判るように曲げ歪が2%以下ではほと
んどその改良した効果が認められず、又、9%以
上では線材にうねりを生じたり、材料が破断した
りするために好ましくない。[Table] Example 2 Ni 6.2% by weight, Cr 3.1% by weight, Si 1.0% by weight balance
An alloy consisting of Fe and impurities was made into a composite wire of alloy and aluminum with a diameter of 2.6 mm by the same method as in Example 1, and this was repeatedly bent so that the strain shown in Table 3 was applied to the outermost part of the alloy wire. Processed,
Residual strain was removed. As can be seen from Table 3, when the bending strain is less than 2%, the improved effect is hardly recognized, and when it is more than 9%, it is not preferable because it causes waviness in the wire or the material breaks.
【表】
実施例 3
表1に示されたFe−Ni系合金のうち、A,B
合金及び炭素鋼を実施例1と同じ方法によりアル
ミニウムを被覆した複合線外径2.6mmを作成し、
15Oeの交番磁界中での発熱量を0℃に於て測つ
たところ1Kg当り表4の発熱を得た。[Table] Example 3 Among the Fe-Ni alloys shown in Table 1, A and B
A composite wire with an outer diameter of 2.6 mm was prepared by coating aluminum with alloy and carbon steel in the same manner as in Example 1.
When the calorific value in an alternating magnetic field of 15 Oe was measured at 0°C, the calorific value per 1 kg was obtained as shown in Table 4.
【表】
表4よりFe−Ni系合金では残留歪とり加工を
行なつたものは、行なわなかつたものに比べ発熱
量が大幅に増加していることが判る。又、炭素鋼
では残留歪とりの効果が現われず、歪とりによる
発熱量の増大はFe−Ni系合金特有のものである
ことが理解されよう。
なお、本発明の実施に当り前述したr/Rが2
%より少ない場合は歪とりが不十分で所期の発熱
量が得られず、又、9%を越えた場合には残留歪
とりは十分であるが、加工が出来なかつたり、後
加工での成形性を低下または機械的強度が低下
し、ともに実用上は好ましくないものとなり、結
局2〜9%の範囲が発熱即ち融雪効果及び強度の
加工性の面から優れているものと言える。[Table] From Table 4, it can be seen that the calorific value of Fe-Ni alloys that were subjected to residual strain relief processing was significantly increased compared to those that were not treated. In addition, it will be understood that the effect of residual strain relief does not appear in carbon steel, and the increase in heat generation due to strain relief is unique to Fe-Ni alloys. In addition, when carrying out the present invention, the above-mentioned r/R is 2.
If it is less than 9%, the strain relief is insufficient and the expected heat generation cannot be obtained, and if it exceeds 9%, the residual strain relief is sufficient, but machining may not be possible or it may be difficult to obtain the desired amount of heat in post-processing. The moldability or mechanical strength decreases, both of which are undesirable from a practical standpoint.In the end, a range of 2 to 9% can be said to be excellent in terms of heat generation, that is, snow melting effect, and strength workability.
Claims (1)
れ、かつ減径加工による残留歪の除去された融雪
電線用線材。 2 磁性金属線材の周囲に導電性金属を被覆し、
所定の径まで減径加工した後、磁性金属線材の径
と曲げ径の比が2〜9%となるようにくり返し曲
げ加工を施して残留歪をとることを特徴とする融
雪電線用線材の製造方法。[Scope of Claims] 1. A wire material for a snow-melting electric wire, in which the surface of a magnetic metal material is coated with a conductive metal, and residual strain due to diameter reduction processing is removed. 2 Coating a conductive metal around the magnetic metal wire,
Manufacture of a wire material for snow-melting electric wire, which is characterized by reducing the diameter to a predetermined diameter and then repeatedly bending the wire material so that the ratio of the diameter of the magnetic metal wire material to the bending diameter is 2 to 9% to remove residual strain. Method.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57105500A JPS58224511A (en) | 1982-06-21 | 1982-06-21 | Snow fusing wire material and method of producing same |
| GB08316146A GB2126409B (en) | 1982-06-21 | 1983-06-14 | Magnetic wire |
| CA000430437A CA1210054A (en) | 1982-06-21 | 1983-06-15 | Magnetic material wire and method of producing same |
| US06/506,013 US4525432A (en) | 1982-06-21 | 1983-06-20 | Magnetic material wire |
| US06/703,763 US4606779A (en) | 1982-06-21 | 1985-04-12 | Method of producing a magnetic material wire |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57105500A JPS58224511A (en) | 1982-06-21 | 1982-06-21 | Snow fusing wire material and method of producing same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58224511A JPS58224511A (en) | 1983-12-26 |
| JPH0135574B2 true JPH0135574B2 (en) | 1989-07-26 |
Family
ID=14409316
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57105500A Granted JPS58224511A (en) | 1982-06-21 | 1982-06-21 | Snow fusing wire material and method of producing same |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58224511A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0681404B2 (en) * | 1988-10-19 | 1994-10-12 | 株式会社フジクラ | Magnetic heating filament manufacturing method |
-
1982
- 1982-06-21 JP JP57105500A patent/JPS58224511A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58224511A (en) | 1983-12-26 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4606779A (en) | Method of producing a magnetic material wire | |
| JP3724033B2 (en) | High-strength, high-heat-resistant aluminum alloy and its manufacturing method, conductive wire and overhead wire | |
| JPH08196022A (en) | Snow melting wire | |
| JPH0135574B2 (en) | ||
| JP6461570B2 (en) | Transmission line and method for manufacturing transmission line | |
| JPH0449723B2 (en) | ||
| CA1210054A (en) | Magnetic material wire and method of producing same | |
| JP2822104B2 (en) | Magnetic material for preventing icing of overhead transmission and distribution lines | |
| JPS58223211A (en) | Linear magnetic material | |
| JPH07322457A (en) | Snow melting wire | |
| JP3428843B2 (en) | Snow melting wire | |
| JPH07161222A (en) | Snow melting member for power lines | |
| GB2126409A (en) | Magnetic wire | |
| JPH01233007A (en) | Manufacture of conjugate wire | |
| JPH0836919A (en) | Snow melting wire | |
| JPH03124211A (en) | Snow melting alloy ring | |
| JPH02193516A (en) | Snow melting alloy wire rod and its manufacture | |
| JP3166339B2 (en) | Heat-generating alloy wire for hard-to-reach ice and snow wires | |
| JPH1141768A (en) | Magnetic heating composite wire | |
| JPH02159352A (en) | Snow melting alloy wire rod and production thereof | |
| JPH06121438A (en) | Snow-melting alloy for power transmission line and its wire and ring | |
| JPH02193517A (en) | Snow melting alloy ring and its manufacture | |
| JPH01174212A (en) | Magnetic wire rod for thawing snow | |
| JPH0598396A (en) | Snow melting alloy | |
| JP3499975B2 (en) | Snow melting electric wire and method of manufacturing the same |