JPH0258724B2 - - Google Patents

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Publication number
JPH0258724B2
JPH0258724B2 JP60161355A JP16135585A JPH0258724B2 JP H0258724 B2 JPH0258724 B2 JP H0258724B2 JP 60161355 A JP60161355 A JP 60161355A JP 16135585 A JP16135585 A JP 16135585A JP H0258724 B2 JPH0258724 B2 JP H0258724B2
Authority
JP
Japan
Prior art keywords
conductor
film
copper
cupric oxide
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 - Lifetime
Application number
JP60161355A
Other languages
Japanese (ja)
Other versions
JPS6193509A (en
Inventor
Michio Takaoka
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.)
Fujikura Ltd
Original Assignee
Fujikura 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 Fujikura Ltd filed Critical Fujikura Ltd
Priority to JP16135585A priority Critical patent/JPS6193509A/en
Publication of JPS6193509A publication Critical patent/JPS6193509A/en
Publication of JPH0258724B2 publication Critical patent/JPH0258724B2/ja
Granted legal-status Critical Current

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  • Non-Insulated Conductors (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 この発明は電力ケーブルに用いられる大サイズ
導体の改良、特に分割導体の改良に関するもので
ある。 〔従来の技術〕〔発明が解決しようとする問題点〕 近年石油化学にともなうエネルギーコストの上
昇と用地の取得難から、地中送電線の低損失化と
大容量化を計る手段として高電圧化、導体の大サ
イズ化及びケーブルの冷却が採用されてきたが、
大容量化に伴なうケーブルの発生損失も増加する
ので、冷却負担の軽減、省エネルギー等の面から
も低損失化の技術開発が急務となつている。導体
についてみると、益々大サイズ化が進み、現在で
は導体断面積2000mm2の大サイズケーブルの使用が
一般化している。又、2500mm2も一部では既に使用
実績があり、数年後には3000mm2以上の大サイズケ
ーブルも実用化が予想されている。 このような導体の大サイズ化の傾向に伴い、導
体交流実効抵抗の直流抵抗に対する増加の程度が
益々大きくなり、送電容量の向上及び省エネルギ
ーの点から、大サイズ導体の交流実効抵抗(表皮
効果係数+近接効果係数)の低減が強く要求され
てきている。 この対策として多分割導体、素線絶縁などが考
えられてきた。いま導体サイズと表皮効果係数の
関係を示せば第1図のとおりであり、大サイズ化
によつて交流実効抵抗の増大の要因となる表皮効
果係数が増大するので、分割導体化による表皮効
果係数の減少が図られてきたが、これによつても
2000mm2以上の導体サイズになると、分割導体であ
つても表皮効果係数は10%を超え、無視できなく
なる。従つて2500mm2〜3000mm2以上では素線絶縁な
どの適用が交流実効抵抗の低減に効果が大きいこ
とが判つた。 ここに素線絶縁について説明すると、裸銅素線
間の接触抵抗だけでは表皮効果の低減に対して十
分な効果が得られないため、素線間を強制的に絶
縁しようとする方式で、これを分割導体に適用す
ると、半経方向に移動する電流が抑制され、かつ
セグメント内の素線は、分割導体の中心部分と外
側部分とに撚られながら転移するので、一定長進
むと、前記中心部分が外側部分となり、逆に外側
部分が中心部分に移るので、各素線のインダクタ
ンスはほぼ均一となり、同時にセグメント内電流
分布は均一化されて表皮効果が低減される。 従来は、この素線絶縁の方法としてエナメルを
コーテイングすることが考えられ、近接効果、表
皮効果に一応有効であることは認められたが、こ
のエナメルコーテイングによる素線絶縁は所定の
特性を得るためには、コーテイング材料の選定と
ともに34〜64μmという比較的肉厚の皮膜として
被覆しなければならないため、素線の仕上がり外
径が大きく、ひいてはこれを撚り合わせた導体外
径も大きくなり、例えば2500mm2のケーブル導体の
場合、エナメルの使用によつて外径が約3mm
(300mm2相当)増加し、更に各素線にエナメルコー
テイングする工程に手数がかかり、価額も高くな
る難点がある。 又ケーブル導体を接続する場合、スリーブ圧着
接続するときにエナメル皮膜を完全に除去する必
要があり、この除去作業に化学薬品を用いるため
に非常に手数がかかり、他方溶接接続の場合には
マンホール内で接続作業をするときに、エナメル
の熱分解による有害ガスを多量に発生する結果、
大掛かりな排ガス装置を必要とする等の欠点があ
る。 更にエナメル皮膜による素線絶縁では、ステン
レステープ巻および内部遮蔽層と内部の導体とが
絶縁されるため、通常のケーブルでは発生しない
異常電圧により放電が発生し、エナメル皮膜の熱
分解劣化を起こすおそれがある。 これらの理由によつて素線絶縁のエナメル化は
実用化されなかつたのである。 〔問題点を解決するための手段〕 本発明は上記の如き実情に鑑み鋭意検討の結果
なされたもので、酸化第二銅(CuO)皮膜の有す
る通常の絶縁体より低い体積抵抗率(導体と絶縁
体との中間の抵抗)に着目し、研究を重ねた結果
これを銅素線表面に形成すると、優れた素線絶縁
性能を発揮することを見出した。これを用いてケ
ーブルの分割圧縮整形より線という特殊構造に応
用することにより、従来の技術の問題点を解決
し、表皮効果、近接効果に有効なケーブル導体を
提供することに成功したものである。 ここにおいて、酸化第二銅(CuO)皮膜の体積
抵抗率はρ=104〜106Ω・cm(固有の値)であ
り、またCuO皮膜の厚さは0.3〜3.0μmより好ま
しくは0.5〜1.0μmである。 すなわち、分割導体を構成する各扇形部分であ
つて大きさが順次小さくなつていく上記各扇形部
分は酸化第二銅により互いに絶縁されていて、か
つ一定長(通常は20〜30cm)のピツチで撚り合わ
せられている。 この扇形部分は酸化第二銅の半導電抵抗を有す
る皮膜で被覆されていることによつて、銅素線同
士の接触に比べ素線間の接触抵抗が十分大きくな
るので、銅素線の長手方向抵抗が電気的に独立し
た状態となり、かつ素線が撚り線構造となつてい
る。従つて上記各扇形部分は等価的にほぼ均一な
インダクタンス分を持つことができ、又分割導体
の中心部分と外側部分とが撚られながら転移する
ので、従つて分割導体分について各扇形部分に均
一な電流が流れるので表皮効果の低減が効果的に
できる。 本発明で用いられる素線絶縁は第2図に見る如
く、各銅線12の表面に酸化第二銅皮膜14を設
けて素線絶縁された素線10を構成しており、例
えば銅素線12を300℃以上に加熱して、その表
面に酸化第二銅の皮膜14を形成するか、又は多
くの化学的手法、例えば、亜塩素酸ナトリウムと
カ性ソーダの酸化剤混合液中に銅素線を浸漬する
ことによつて表面酸化を行い、酸化第二銅皮膜1
4を形成した銅素線すなわち素線絶縁体を得るこ
とができる。 本発明における素線絶縁は酸化第二銅皮膜の固
有の抵抗値であるから、本発明の対象である上述
の構造において、すなわち104〜106Ω−cmである
から導体を構成する各銅素線間ではその電位差が
1mV程度と低いものであつて、この電圧に対し
て絶縁できるのに十分な抵抗値である。 導体に高電圧が印加されても、電位分担が微少
であるから、異常電圧、充電電流に起因する放電
の発生を防ぐことができる。 更に上記において述べた如く、本発明では酸化
第二銅皮膜を有するために放電が生じないが、従
来のエナメル皮膜による絶縁すなわちエナメル皮
膜の体積低抗率はρ'=1013〜1015Ω・cmと高く、
皮膜厚が厚く容量分布となり電圧分担が高くなる
ため、導体を構成する素線間で放電が生じて、そ
の結果導体の接触抵抗が零となり、皮膜を設けた
意味がなくなる。この結果劣化ガス(例えばOF
ケーブルの場合C2H2等)が発生し、絶縁油を劣
化させたり、同様に絶縁体を劣化させたりした
が、本発明の半導電領域の抵抗率を有する酸化第
二銅皮膜ではこのようなことは起こらない。 本発明では銅の酸化皮膜の形成手段の相違には
関係なく、厚さ約0.3μm〜3.0μmより好ましくは
0.5〜1.0μm程度の皮膜が形成され、皮膜の体積
抵抗率ρ=104〜106Ω・cmのものが得られた。 〔実施例〕 本発明ではこのような酸化第二銅皮膜を設けた
銅素線を用い、例えば第3図に見られるように、
ケーブル導体を構成するものであり、銅素線表面
の全部に酸化第二銅皮膜が形成されている。すな
わち複数本の銅素線をより合わせて圧縮整形して
セグメント20を構成しているが、このセグメン
ト20の各銅素線は酸化第二銅皮膜を有する銅素
線10よりなる。なお、図ではセグメントの数が
6ケのものが示されているがこれに限られない。 本発明における酸化第二銅皮膜を有するケーブ
ル導体は酸化第二銅が耐熱性に優れているため海
底ケーブルなどに欠くことのできない可撓ジヨイ
ントの導体同径接続ができる。 本発明で用いる酸化第二銅皮膜の素線とエナメ
ル被覆の素線とを作成し、その特性を比較試験し
たところ下表のとおりであつた。
[Industrial Field of Application] This invention relates to improvements in large-sized conductors used in power cables, and in particular to improvements in divided conductors. [Prior art] [Problem to be solved by the invention] In recent years, due to the rise in energy costs associated with petrochemical production and the difficulty in acquiring land, high voltage has been developed as a means of reducing loss and increasing capacity of underground power transmission lines. , increasing the size of the conductor and cooling the cable have been adopted,
Since the loss generated in cables increases as the capacity increases, there is an urgent need to develop technology to reduce loss from the perspective of reducing the cooling burden and saving energy. Regarding conductors, they are becoming larger and larger, and it is now common to use large cables with a conductor cross-sectional area of 2000 mm2 . In addition, 2500mm 2 cables have already been used in some areas, and large-sized cables of 3000mm 2 or larger are expected to be put into practical use in the next few years. With this trend toward larger conductor sizes, the degree of increase in conductor AC effective resistance relative to DC resistance is becoming larger and larger. + proximity effect coefficient) has been strongly demanded. As a countermeasure to this problem, multi-segmented conductors, wire insulation, etc. have been considered. The relationship between the conductor size and the skin effect coefficient is shown in Figure 1. As the size increases, the skin effect coefficient, which is a factor in increasing the AC effective resistance, increases. efforts have been made to reduce the
When the conductor size is 2000 mm 2 or more, the skin effect coefficient exceeds 10% and cannot be ignored even if the conductor is divided. Therefore, it has been found that application of wire insulation etc. is highly effective in reducing the effective AC resistance for areas over 2500 mm 2 to 3000 mm 2 . To explain strand insulation here, contact resistance between bare copper strands alone is not sufficient to reduce the skin effect, so this is a method that attempts to forcibly insulate between strands. When applied to a segmented conductor, the current moving in the semi-mechanical direction is suppressed, and the strands in the segment are twisted and transferred between the center and outer parts of the segmented conductor. Since the portion becomes the outer portion, and conversely, the outer portion moves to the center portion, the inductance of each strand becomes substantially uniform, and at the same time, the current distribution within the segment is made uniform, and the skin effect is reduced. Conventionally, enamel coating has been considered as a method of insulating wires, and it has been recognized that it is somewhat effective against the proximity effect and skin effect, but it is difficult to insulate wires with enamel coating in order to obtain the specified characteristics. In addition to selecting the coating material, it is necessary to apply a relatively thick film of 34 to 64 μm, which results in a large finished outer diameter of the strands, which in turn increases the outer diameter of the conductor that is twisted together.For example, 2500 mm. In the case of cable conductor 2 , the outer diameter is approximately 3 mm due to the use of enamel.
(equivalent to 300 mm 2 ), and the process of enamel coating each strand is time-consuming and expensive. In addition, when connecting cable conductors, it is necessary to completely remove the enamel film when connecting by crimping the sleeve, and this removal process requires chemicals, which is very time-consuming. When making connections, a large amount of harmful gas is generated due to the thermal decomposition of the enamel.
There are drawbacks such as the need for a large-scale exhaust gas system. Furthermore, with wire insulation using enamel coating, since the stainless steel tape wrapping and internal shielding layer are insulated from the internal conductor, abnormal voltage that does not occur with normal cables can cause electrical discharge, which may cause thermal decomposition deterioration of the enamel coating. There is. For these reasons, enamelling of wire insulation has not been put to practical use. [Means for Solving the Problems] The present invention was developed as a result of intensive studies in view of the above-mentioned circumstances, and the present invention has been made as a result of intensive studies in view of the above-mentioned circumstances. As a result of repeated research, we discovered that forming this on the surface of a copper wire provides excellent wire insulation performance. By applying this to the special structure of split, compressed, and stranded cables, we have succeeded in solving the problems of conventional technology and providing a cable conductor that is effective against the skin effect and proximity effect. . Here, the volume resistivity of the cupric oxide (CuO) film is ρ = 10 4 to 10 6 Ω·cm (specific value), and the thickness of the CuO film is 0.3 to 3.0 μm, preferably 0.5 to 3.0 μm. It is 1.0 μm. In other words, each of the sector-shaped parts constituting the divided conductor, whose size gradually decreases, is insulated from each other by cupric oxide, and is arranged at a pitch of a certain length (usually 20 to 30 cm). It is twisted together. Since this fan-shaped part is coated with a film of cupric oxide that has semiconducting resistance, the contact resistance between the copper wires is sufficiently large compared to the contact between copper wires, so that The directional resistance is electrically independent, and the wires have a twisted wire structure. Therefore, each of the sector-shaped parts described above can equivalently have a substantially uniform inductance, and since the center part and the outer part of the divided conductor are transferred while being twisted, the inductance of the divided conductor is uniform in each sector-shaped part. Since the current flows, the skin effect can be effectively reduced. As shown in FIG. 2, the strand insulation used in the present invention comprises a strand 10 which is insulated by providing a cupric oxide film 14 on the surface of each copper wire 12, for example, a copper strand. 12 can be heated to over 300°C to form a film 14 of cupric oxide on its surface, or by various chemical methods, such as heating copper oxide in an oxidizing agent mixture of sodium chlorite and caustic soda. Surface oxidation is performed by immersing the wire to form a cupric oxide film 1.
4 can be obtained, that is, a wire insulator. Since the wire insulation in the present invention is the inherent resistance value of the cupric oxide film, in the above-mentioned structure that is the subject of the present invention, in other words, since it is 10 4 to 10 6 Ω-cm, each copper constituting the conductor The potential difference between the wires is
It has a low resistance of about 1 mV, which is sufficient to insulate against this voltage. Even if a high voltage is applied to the conductor, the potential sharing is small, so it is possible to prevent the occurrence of discharge due to abnormal voltage or charging current. Furthermore, as mentioned above, in the present invention, since the present invention has a cupric oxide film, no discharge occurs, but the insulation by the conventional enamel film, that is, the volume resistivity of the enamel film is ρ'=10 13 to 10 15 Ω・cm high,
Since the coating thickness is thick and the capacitance is distributed, and the voltage sharing becomes high, discharge occurs between the wires that make up the conductor, and as a result, the contact resistance of the conductor becomes zero, and the provision of the coating becomes meaningless. This results in degraded gas (e.g. OF
In the case of cables, C 2 H 2, etc.) occur, which deteriorates the insulating oil and the insulator, but the cupric oxide film of the present invention, which has a resistivity in the semiconducting range, does not nothing happens. In the present invention, the thickness is preferably about 0.3 μm to 3.0 μm, regardless of the method of forming the copper oxide film.
A film with a thickness of about 0.5 to 1.0 μm was formed, and a film with a volume resistivity ρ of 10 4 to 10 6 Ω·cm was obtained. [Example] In the present invention, a copper wire provided with such a cupric oxide film is used, for example, as shown in FIG.
It constitutes the cable conductor, and a cupric oxide film is formed on the entire surface of the copper wire. That is, the segment 20 is constructed by twisting and compressing a plurality of copper wires, and each copper wire of the segment 20 is made of a copper wire 10 having a cupric oxide film. Note that although the figure shows a case where the number of segments is six, it is not limited to this. In the cable conductor having a cupric oxide film according to the present invention, since cupric oxide has excellent heat resistance, it is possible to connect conductors with the same diameter at a flexible joint, which is indispensable for submarine cables. A strand with a cupric oxide coating and an enamel-coated strand used in the present invention were prepared, and their properties were compared and tested as shown in the table below.

【表】 従つてエナメル被覆より遥かに薄く導体外径は
太くならず、エナメル被覆のように特別な塗布焼
き付け装置は必要とせず、皮膜形成手段が簡単な
ため低コストですむ。又、上述の抵抗率なので、
従来どうりの導体遮蔽構造がとれる。 次に酸化第二銅皮膜による素線絶縁導体を試作
し、交流実効抵抗を測定した。 測定法は導体に所定の電流を通電し、交流電位
差計を用いて電流、電位降下の値及び電圧と電流
の位相を実測し、交流実効抵抗を算出した。 ケーブル長は7〜8m有効測定長は約5mとし
た。ケーブルの両端末は酸化第二銅皮膜を除去し
た後、ロツドを圧縮接続し通電端子にとり付け
た。 供試導体は下表のとおりである。
[Table] Therefore, it is much thinner than enamel coating, and the outer diameter of the conductor does not increase. Unlike enamel coating, special coating and baking equipment is not required, and the film forming method is simple, resulting in low cost. Also, since the resistivity is as mentioned above,
A conventional conductor shielding structure can be used. Next, we prototyped a strand insulated conductor with a cupric oxide film and measured its effective AC resistance. The measurement method was to apply a predetermined current to the conductor, and use an AC potentiometer to measure the current, potential drop, and phase of voltage and current, and calculate the AC effective resistance. The cable length was 7 to 8 m, and the effective measurement length was approximately 5 m. After removing the cupric oxide film from both ends of the cable, the rods were compressed and attached to current-carrying terminals. The test conductors are shown in the table below.

【表】 これにより表皮効果係数を測定した結果は下記
のとおりで本発明が優れていることが判る。 ここで表皮効果係数λは交流実効抵抗rac、rac
測定温度の直流抵抗をrdcとすれば、 λ=rac−rdc/rdcより算出される。 表皮効果係数測定結果
[Table] The results of measuring the skin effect coefficient are shown below, and it can be seen that the present invention is superior. Here, the skin effect coefficient λ is the AC effective resistance r ac , r ac
If the DC resistance at the measured temperature is r dc , it is calculated from λ=r ac −r dc /r dc . Skin effect coefficient measurement results

【表】【table】

〔発明の効果〕〔Effect of the invention〕

本発明に於いて全素線に酸化第二銅皮膜を形成
してあることは部分的にこの素線を用いたものよ
りも、表皮効果近接効果を減少し、前記各種の効
果を奏するか、特にその製造上はより線構造とし
てから酸化することにより容易に製造することが
できるとともに製造コスト上も有利であり、又導
体接続時の酸化皮膜除去を行う場合素線を選別せ
ずに行い得るので、この点からも作業性の高い構
造のものということができる。 又本発明は銅素線を体積抵抗率ρ=104
106Ω・cmで皮膜厚が約0.5〜1.0μm程度のCuO皮
膜を設けたものを用いているため、分割圧縮整形
より線導体における近接効果、表皮効果を小さく
押さえることができ、かつ皮膜は薄くしかも特性
が安定しており、製造も容易で、分割圧縮整形よ
り線導体ケーブルにおける近接効果、表皮効果を
小さく押さえられ、外径、重量も大きくならな
い。又、絶縁油に対しても安定で、かつ接続に際
してはサンドブラストホーニング等機械的手段に
より容易に皮膜を除去することができるので、溶
接接続が容易である等の各種効果を奏するもので
ある。
In the present invention, by forming a cupric oxide film on all the wires, the skin effect proximity effect is reduced and the various effects described above are achieved, compared to the case where this wire is partially used. In particular, it is easy to manufacture by forming a stranded wire structure and then oxidizing it, which is also advantageous in terms of manufacturing cost.Also, when removing the oxide film when connecting conductors, it can be done without sorting the wires. Therefore, from this point of view as well, it can be said that the structure is highly workable. In addition, the present invention uses a copper wire with a volume resistivity ρ=10 4 ~
Since a CuO film with a resistance of 10 6 Ω・cm and a film thickness of approximately 0.5 to 1.0 μm is used, the proximity effect and skin effect in the wire conductor can be kept to a minimum compared to split compression shaping, and the film is It is thin, has stable characteristics, and is easy to manufacture. Proximity effects and skin effects in wire conductor cables can be kept to a minimum compared to split compression shaping, and the outer diameter and weight do not increase. In addition, it is stable against insulating oil, and the film can be easily removed by mechanical means such as sandblasting and honing during connection, resulting in various effects such as easy welding connection.

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

第1図は表皮効果係数と導体断面積の関係図、
第2図は本発明に用いられる絶縁素線の断面図、
第3図は本発明によるケーブル導体の一実施例を
示す断面図である。 10…絶縁素線、12…銅素線、14…酸化第
二銅皮膜、20…セグメント。
Figure 1 is a diagram of the relationship between skin effect coefficient and conductor cross-sectional area.
FIG. 2 is a cross-sectional view of the insulated wire used in the present invention,
FIG. 3 is a sectional view showing an embodiment of the cable conductor according to the present invention. DESCRIPTION OF SYMBOLS 10... Insulated strand, 12... Copper strand, 14... Cupric oxide film, 20... Segment.

Claims (1)

【特許請求の範囲】[Claims] 1 銅素線を撚り合わせ圧縮整形してなる分割圧
縮整形撚線導体において、前記銅素線表面の全部
にCuO皮膜が形成されていることを特徴とするケ
ーブル導体。2 銅素線を撚り合わせ圧縮整形し
てなる分割圧縮整形撚線導体の銅素線表面の全部
にCuO皮膜が形成されているケーブルにおいて、
CuO皮膜が体積抵抗率ρ=104〜106Ω・cmである
特許請求の範囲第1項記載のケーブル導体。
1. A split compression-shaped stranded wire conductor made by twisting and compressing copper strands, characterized in that a CuO film is formed on the entire surface of the copper strands. 2. In a cable in which a CuO film is formed on the entire surface of the copper wire of a divided compression-formed stranded wire conductor made by twisting and compressing copper wires,
The cable conductor according to claim 1, wherein the CuO film has a volume resistivity ρ of 10 4 to 10 6 Ω·cm.
JP16135585A 1985-07-19 1985-07-19 Cable conductor Granted JPS6193509A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16135585A JPS6193509A (en) 1985-07-19 1985-07-19 Cable conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16135585A JPS6193509A (en) 1985-07-19 1985-07-19 Cable conductor

Publications (2)

Publication Number Publication Date
JPS6193509A JPS6193509A (en) 1986-05-12
JPH0258724B2 true JPH0258724B2 (en) 1990-12-10

Family

ID=15733501

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16135585A Granted JPS6193509A (en) 1985-07-19 1985-07-19 Cable conductor

Country Status (1)

Country Link
JP (1) JPS6193509A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005166560A (en) * 2003-12-04 2005-06-23 Fujikura Ltd Cable core and transmission cable
JP4740720B2 (en) * 2005-11-09 2011-08-03 ニッタ株式会社 Elastic bearings for structures
CN102360588A (en) * 2011-09-09 2012-02-22 江苏圣安电缆有限公司 3000 mm<2> aluminum core segmental conductor

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4936520A (en) * 1972-08-10 1974-04-04

Also Published As

Publication number Publication date
JPS6193509A (en) 1986-05-12

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