JPH0134503Y2 - - Google Patents
Info
- Publication number
- JPH0134503Y2 JPH0134503Y2 JP10144783U JP10144783U JPH0134503Y2 JP H0134503 Y2 JPH0134503 Y2 JP H0134503Y2 JP 10144783 U JP10144783 U JP 10144783U JP 10144783 U JP10144783 U JP 10144783U JP H0134503 Y2 JPH0134503 Y2 JP H0134503Y2
- Authority
- JP
- Japan
- Prior art keywords
- power transmission
- ferromagnetic
- transmission line
- metal wire
- wire
- 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
- 230000005540 biological transmission Effects 0.000 claims description 28
- 230000005291 magnetic effect Effects 0.000 claims description 24
- 229910052751 metal Inorganic materials 0.000 claims description 24
- 239000002184 metal Substances 0.000 claims description 24
- 230000005294 ferromagnetic effect Effects 0.000 claims description 22
- 230000020169 heat generation Effects 0.000 claims description 17
- 239000004020 conductor Substances 0.000 claims description 4
- 239000003302 ferromagnetic material Substances 0.000 description 11
- 239000000463 material Substances 0.000 description 10
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 6
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 229910052742 iron Inorganic materials 0.000 description 3
- 230000005415 magnetization Effects 0.000 description 3
- 229910000838 Al alloy Inorganic materials 0.000 description 2
- 230000008018 melting Effects 0.000 description 2
- 238000002844 melting Methods 0.000 description 2
- 239000007769 metal material Substances 0.000 description 2
- 229910052759 nickel Inorganic materials 0.000 description 2
- 230000002265 prevention Effects 0.000 description 2
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000007797 corrosion Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 230000005298 paramagnetic effect Effects 0.000 description 1
- 239000002907 paramagnetic material Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910002059 quaternary alloy Inorganic materials 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
Landscapes
- Insulated Conductors (AREA)
- Suspension Of Electric Lines Or Cables (AREA)
Description
【考案の詳細な説明】
この考案は、着雪を防止することのできる架空
送電線に関するものである。[Detailed Description of the Invention] This invention relates to an overhead power transmission line that can prevent snow accumulation.
一般に、降雪量の多い地域では、架空送電線に
も雪が付着するが、その着雪量が多くなると送電
線の重量が増大し、その結果送電線に大きな張力
が発生して断線事故その他の種々の不都合を招く
おそれが生じる。従来、送電線の着雪を防止する
ために、通電時の許容発熱温度以下の温度におい
て磁気変態により強磁性体に変わる磁性金属線
(これを今低キユリー金属線と称する)を送電線
に螺旋状に巻き付け、降雪があるような低い気温
では低キユリー金属線が強磁性体となることに伴
う発熱現象によつて融雪を行うことがなされてい
る。しかし、低キユリー材は、低温時に強磁性体
となつたとしても、鉄などの強磁性体より磁化率
が小さく、このため、充分な発熱量を得る上で効
率的でない。また、低キユリー材は高価なため、
通常線径の細いものを用いるが、径が細いと、送
電線の断面を非円形形状に崩してカルマン渦の発
生を防止し風騒音を低減するという効果は生じな
い。 In general, in areas with heavy snowfall, snow adheres to overhead power lines, but when the amount of snow increases, the weight of the power lines increases, resulting in large tension on the lines, which can lead to disconnection accidents and other problems. This may cause inconvenience. Conventionally, in order to prevent snow from accumulating on power transmission lines, magnetic metal wires (now referred to as low Curie metal wires), which turn into ferromagnetic materials through magnetic transformation at temperatures below the allowable heat generation temperature when energized, were spirally attached to power transmission lines. At low temperatures such as snowfall, the low-Kyrie metal wire becomes ferromagnetic and generates heat, which melts the snow. However, even if a low-Kyrie material becomes ferromagnetic at low temperatures, it has a lower magnetic susceptibility than a ferromagnetic material such as iron, and is therefore not efficient in obtaining a sufficient amount of heat. In addition, since low-Kyuri materials are expensive,
Normally, wires with a small diameter are used, but if the diameter is small, the cross section of the power transmission line will be broken into a non-circular shape, preventing the generation of Karman vortices and reducing wind noise.
この考案は上記事情に鑑みてなされたもので、
充分な融雪効果を持ち、かつ、風騒音の防止をも
図ることのできる架空送電線を得ることを目的と
するものである。 This idea was made in view of the above circumstances,
The object of the present invention is to obtain an overhead power transmission line that has a sufficient snow melting effect and can also prevent wind noise.
以下、本考案の一実施例を図面を参照して説明
する。 An embodiment of the present invention will be described below with reference to the drawings.
第1図に示す如く本考案の架空送電線は、裸撚
線導体1の外周に線条体2を螺旋状に巻き付けて
なるものであるが、特にこの線条体2を自己径d
の百倍以下の長さの強磁性金属線材3と通電時の
送電線の許容発熱温度以下の温度で強磁性を帯び
る磁性金属線材4とを直列接続してなるものにて
形成している。 As shown in FIG. 1, the overhead power transmission line of the present invention has a wire body 2 spirally wound around the outer periphery of a bare stranded wire conductor 1.
It is formed by connecting in series a ferromagnetic metal wire 3 having a length of 100 times or less, and a magnetic metal wire 4 that becomes ferromagnetic at a temperature below the allowable heat generation temperature of the power transmission line when energized.
なお、上記線条体2は、例えば第2図に断面図
を示す如くその外周にアルミニウム合金の被覆2
aを形成したもの等を用いるのが好ましい。アル
ミニウム合金で被覆した場合には、裸撚線導体1
の表面との間で電蝕が生じるのを防止することが
できる。 Note that the above-mentioned filament body 2 has an aluminum alloy coating 2 on its outer periphery, as shown in the cross-sectional view in FIG. 2, for example.
It is preferable to use a material in which a is formed. When coated with aluminum alloy, bare stranded conductor 1
It is possible to prevent electrolytic corrosion from occurring between the surface of the
また、磁性金属線材4として、すなわち、通電
時の送電線の許容発熱温度以下の温度で強磁性を
帯びる適当な材料の例として、150℃以下の温度
において強磁性を帯びる鉄60wt%、ニツケル
36wt%、クロム3wt%、およびシリコン1wt%か
らなる四元合金や、90℃以下の温度において強磁
性を帯びる鉄53.5wt%、ニツケル37wt%、クロ
ム9wt%、およびシリコン0.5wt%からなる四元
合金等を上げることができる。 In addition, as the magnetic metal wire 4, examples of suitable materials that become ferromagnetic at temperatures below the allowable heat generation temperature of power transmission lines when energized include 60wt% iron, which becomes ferromagnetic at temperatures below 150°C, and nickel.
A quaternary alloy consisting of 53.5 wt% iron, 37 wt% nickel, 9 wt% chromium, and 0.5 wt% silicon that becomes ferromagnetic at temperatures below 90°C. Alloys, etc. can be raised.
次に作用について説明する。 Next, the effect will be explained.
通電時の送電線の許容発熱温度以下の温度、例
えば降雪時の気温状況では、磁性金属線材4は強
磁性状態を示している。したがつて、このとき線
条体2は磁気的に全長にわたつて一連続の強磁性
体となつており、その強磁性体としての連続した
長さが自己径の百倍を越えるため磁気回路が実質
的に閉じたものとなる。なおここで、強磁性体の
発熱を促すには、一般にその磁気回路が閉じたも
の、つまり強磁性体が閉ループを形成しなければ
ならないものであるが、しかし閉ループを形成し
ない場合でも強磁性金属線材の長さLが、その径
dとの間にL≧100dなる関係にあれば実質的に
磁気回路が閉じたのと同様の状態となることが実
験的に確かめられているものである。したがつ
て、送電線を流れる交流電流によつて線条体2に
渦電流が生じ、かつ、磁気ヒステリシス現象が生
じ、このため渦電流損、およびヒステリシス損が
生じて線条体2が発熱する。この発熱により送電
線に付着した雪を融かして、送電線への着雪を防
ぐことができる。 At a temperature below the permissible heat generation temperature of the power transmission line when energized, for example when it is snowing, the magnetic metal wire 4 exhibits a ferromagnetic state. Therefore, at this time, the filament 2 is magnetically a continuous ferromagnetic material over its entire length, and since the continuous length of the ferromagnetic material exceeds 100 times its own diameter, the magnetic circuit is It is essentially closed. Note that in order to promote heat generation in a ferromagnetic material, generally the magnetic circuit must be closed, that is, the ferromagnetic material must form a closed loop, but even if a ferromagnetic material does not form a closed loop, It has been experimentally confirmed that if the length L of the wire meets the relationship L≧100d with the diameter d, a state substantially similar to that of a closed magnetic circuit will occur. Therefore, the alternating current flowing through the power transmission line generates eddy currents in the filamentary body 2, and magnetic hysteresis occurs, which causes eddy current loss and hysteresis loss, causing the filamentous body 2 to generate heat. . This heat generation can melt snow adhering to power transmission lines and prevent snow from accumulating on power transmission lines.
また、送電線の許容発熱温度以上の温度におい
ては、前記磁性金属線材4は常磁性体となる。す
なわち、このとき線条体2は、全長にわたつて強
磁性状態を示すものではなく、直列に介在された
磁性金属線材4によつて強磁性金属線材3がその
自己径の百倍以下の適宜長さに磁気的に分断され
たものとなる。磁性を利用した発熱を得るには、
前述の如く電流源のまわりで強磁性体の磁気回路
が閉じているか、または強磁性金属線材の長さL
がその径dの百倍以上でなければならないので、
もはや磁気回路が開いているこの状態において
は、強磁性金属線材3にも発熱現象は生じない。
このため、送電線を無用に加熱し、軟化させるこ
とがない。 Further, at a temperature equal to or higher than the allowable heat generation temperature of the power transmission line, the magnetic metal wire 4 becomes a paramagnetic material. In other words, at this time, the filament 2 does not exhibit a ferromagnetic state over its entire length, but the ferromagnetic metal wire 3 has an appropriate length of 100 times or less its own diameter due to the magnetic metal wire 4 interposed in series. It becomes magnetically divided. To generate heat using magnetism,
As mentioned above, the magnetic circuit of the ferromagnetic material is closed around the current source, or the length L of the ferromagnetic metal wire is
must be at least 100 times its diameter d, so
In this state where the magnetic circuit is no longer open, no heat generation phenomenon occurs in the ferromagnetic metal wire 3 either.
Therefore, the power transmission line will not be unnecessarily heated and softened.
また、上述の線状体2は、送電線の許容発熱温
度以下の温度で強磁性体に変わる磁性金属材料
(すなわち低キユリー材)4を全長にわたつて用
いたものと比べて、より望ましい発熱特性を持
つ。すなわち、実施例における低キユリー材4、
および強磁性金属線材3の磁化特性は第3図に示
す如くで、強磁性金属線材3の磁化率〔実線(イ)〕
は、低キユリー材4の磁化率〔破線(ロ)〕よりも大
である。このため、低キユリー材4と強磁性金属
線材3とを直列接続してなる線条体2が全長にわ
たつて強磁性体となつた時の発熱量は、この線条
体2がすべて低キユリー材4で形成されている場
合の発熱量よりも遥かに大である。なお、第3図
においてt0は送電線の許容最高発熱温度を示す。 In addition, the above-mentioned linear body 2 has a more desirable heat generation property compared to one in which a magnetic metal material (i.e., a low Curie material) 4 that turns into a ferromagnetic material at a temperature below the allowable heat generation temperature of the power transmission line is used over the entire length. have characteristics. That is, the low Curie material 4 in the example,
The magnetization characteristics of the ferromagnetic metal wire 3 are as shown in FIG. 3, and the magnetic susceptibility of the ferromagnetic metal wire 3 [solid line (A)]
is larger than the magnetic susceptibility of the low Curie material 4 [broken line (b)]. Therefore, the amount of heat generated when the filament 2, which is made by connecting the low-Kyuri material 4 and the ferromagnetic metal wire 3 in series, becomes a ferromagnetic material over the entire length is that the filament 2 is all low-Kyuri. This is much larger than the amount of heat generated when it is made of material 4. In addition, in FIG. 3, t 0 indicates the maximum allowable heat generation temperature of the power transmission line.
また、送電線の断面外周形状を実質的に非円形
形状に崩してカルマン渦の発生を阻害するように
線条体2の径を選定すれば、風騒音レベルの低減
を図ることができる。 Further, by selecting the diameter of the filament 2 so as to substantially break the cross-sectional outer peripheral shape of the power transmission line into a non-circular shape and inhibit the generation of Karman vortices, it is possible to reduce the wind noise level.
以上説明したように本考案の架空送電線は、外
周に螺旋巻きされた線条体が、自己径の百倍以下
の長さの強磁性金属線材と通電時の送電線の許容
発熱温度以下の温度で強磁性を帯びる磁性金属線
材とを直列接続してなるものにて形成されている
ので、降雪時等の低温状態では線条体全体が磁気
的に一連続の強磁性体となつて、つまり実質的に
磁気回路が閉じて通電に伴う発熱現象を生じるこ
とにより送電線への着雪を効果的に防止し、ま
た、送電線の許容発熱温度以上の温度においては
磁性金属線材が常磁性体となると共に各強磁性金
属線材が磁気的にそれぞれの長さに分断されて磁
気回路が開いた状態となるので線条体全体として
全く発熱現象が生じず、したがつて、送電線を無
用に加熱せず、送電ロス、送電線の軟化等の不都
合が生じない。そして、上述の発熱特性が磁性金
属材(低キユリー材)を一部に使用するのみで得
られるので、線条体を、したがつて着雪防止装置
を安価に提供でき、さらにその発熱特性は、降雪
時などには高い磁化特性を持つ強磁性金属線材が
有効に働いて充分な発熱をするもので、融雪の効
果が高い。また、線条体の径を太くして風騒音防
止の効果を持たせることもできる等種々の優れた
効果を奏するものである。 As explained above, the overhead power transmission line of the present invention has a ferromagnetic metal wire with a length of 100 times or less than its own diameter, and a wire body spirally wound around the outer periphery, and a temperature that is below the allowable heat generation temperature of the power transmission line when energized. Since it is formed by connecting in series a magnetic metal wire that is ferromagnetic, in low temperature conditions such as during snowfall, the entire wire becomes a continuous ferromagnetic material, that is, The magnetic circuit essentially closes and generates heat due to energization, effectively preventing snow from accumulating on power transmission lines, and magnetic metal wire becomes paramagnetic at temperatures above the allowable heat generation temperature of power transmission lines. At the same time, each ferromagnetic metal wire is magnetically divided into its own lengths and the magnetic circuit is opened, so that no heat generation occurs in the wire as a whole, thus making the power transmission line unnecessary. There is no heating, and there are no inconveniences such as power transmission loss or softening of power transmission lines. Furthermore, since the above-mentioned heat generation properties can be obtained by only partially using a magnetic metal material (low-Kyuri material), it is possible to provide the striated body and therefore the snow accretion prevention device at a low cost, and furthermore, its heat generation properties are During snowfall, the ferromagnetic metal wire with high magnetization properties works effectively and generates sufficient heat, making it highly effective at melting snow. In addition, the diameter of the filament can be increased to provide a wind noise prevention effect, and various other excellent effects can be achieved.
図面は本考案の一実施例を示すもので、第1図
は架空送電線の側面図、第2図は第1図における
線条体の他の実施例を示す断面図、第3図は磁化
特性図である。
1……裸撚線導体、2……線条体、3……強磁
性金属線材、4……磁性金属線材。
The drawings show one embodiment of the present invention, in which Fig. 1 is a side view of an overhead power transmission line, Fig. 2 is a sectional view showing another embodiment of the wire body in Fig. 1, and Fig. 3 is a magnetization It is a characteristic diagram. DESCRIPTION OF SYMBOLS 1... Bare stranded wire conductor, 2... Wire body, 3... Ferromagnetic metal wire, 4... Magnetic metal wire.
Claims (1)
架空送電線において、前記線条体2が、自己径の
百倍以下の長さの強磁性金属線材3と通電時の送
電線の許容発熱温度以下の温度で強磁性を帯びる
磁性金属線材4とを直列接続してなるものにて形
成されていることを特徴とする架空送電線。 In an overhead power transmission line in which a wire body 2 is spirally wound around the outer periphery of a bare stranded wire conductor 1, the wire body 2 is connected to a ferromagnetic metal wire 3 having a length of 100 times or less than its own diameter and the power transmission line tolerance when energized. An overhead power transmission line characterized in that it is formed by connecting in series a magnetic metal wire 4 that becomes ferromagnetic at a temperature below the heat generation temperature.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10144783U JPS6011616U (en) | 1983-06-30 | 1983-06-30 | overhead power lines |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10144783U JPS6011616U (en) | 1983-06-30 | 1983-06-30 | overhead power lines |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6011616U JPS6011616U (en) | 1985-01-26 |
| JPH0134503Y2 true JPH0134503Y2 (en) | 1989-10-20 |
Family
ID=30239551
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10144783U Granted JPS6011616U (en) | 1983-06-30 | 1983-06-30 | overhead power lines |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6011616U (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62147316U (en) * | 1986-03-11 | 1987-09-17 |
-
1983
- 1983-06-30 JP JP10144783U patent/JPS6011616U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6011616U (en) | 1985-01-26 |
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