JPH0447854Y2 - - Google Patents

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Publication number
JPH0447854Y2
JPH0447854Y2 JP1983200958U JP20095883U JPH0447854Y2 JP H0447854 Y2 JPH0447854 Y2 JP H0447854Y2 JP 1983200958 U JP1983200958 U JP 1983200958U JP 20095883 U JP20095883 U JP 20095883U JP H0447854 Y2 JPH0447854 Y2 JP H0447854Y2
Authority
JP
Japan
Prior art keywords
insulator
cable
semiconducting layer
layer
breakdown voltage
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
Application number
JP1983200958U
Other languages
Japanese (ja)
Other versions
JPS60112021U (en
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 filed Critical
Priority to JP20095883U priority Critical patent/JPS60112021U/en
Publication of JPS60112021U publication Critical patent/JPS60112021U/en
Application granted granted Critical
Publication of JPH0447854Y2 publication Critical patent/JPH0447854Y2/ja
Granted legal-status Critical Current

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  • Conductive Materials (AREA)
  • Organic Insulating Materials (AREA)

Description

【考案の詳細な説明】[Detailed explanation of the idea]

[産業上の利用分野] この考案は、直流用の架橋ポリエチレン電力ケ
ーブルに関するものである。 [直流ケーブル特有の問題] 直流用電力ケーブルの絶縁材料として架橋ポリ
エチレンを使用した場合、空間電荷の影響が大き
いといわれる。 空間電荷の挙動は、まだ良く解明されていない
が、高温時における直流破壊電圧特性および極性
反転破壊電圧特性の低下にも、関係があると思わ
れている。 [従来の技術と考案が解決しようとする課題] ・その1: ケーブル絶縁体中に有機半導電液を浸透させる
方法が考えられている(たとえば特開昭52−8487
号公報)。 しかし、この場合、有機半導電液が浸透してい
るのは半導電層の近くだけで、上記特開昭52−
8487号公報の添付図面から見ても、ケーブル絶縁
体の全体にわたつて有機半導電液が浸透している
ものとは考えられない。 ・その2: ケーブル絶縁体と内外半導電層との間に、それ
ぞれ、カーボン混入などにより絶縁抵抗を絶縁体
より小さく半導電層より大きく、かつその絶縁抵
抗が絶縁体側から半導電層側にかけて小さくなる
抵抗勾配を有するようにした極く薄い層(たとえ
ば0.5mm程度)を設ける、という考えもある(特
公昭50−116983号公報)。 この技術は、絶縁体と半導電層との界面および
その近傍に空間電荷が蓄積し、かつその蓄積は、
課電電圧と課電時間に密接な関係を有するという
考えに立ち、 上記界面とその近傍に空間電荷が蓄積しないよ
うにすることを狙つたものであり、 その結果、長期課電特性が改善されたことを、
報告している。 しかし、高温時における直流破壊電圧特性およ
び極性反転破壊電圧特性が改善されたという報告
は無い。 [課題を解決するための手段] 上記従来技術「その2」のように、ケーブル絶
縁体と半導電層との界面の極く薄い層だけを、カ
ーボン混入の層としたのではなくて、 ケーブル絶縁体の全体を、カーボン粒子を含有
させて、抵抗率を1012〜1016Ω・cmとした架橋ポ
リエチレンによつて形成する、という手段をと
る。 [作用] ケーブル絶縁体の全体を、カーボン粒子を含有
させて、抵抗率を1012〜1016Ω・cmとした架橋ポ
リエチレンによつて形成した場合、空間電荷がど
のような挙動をとるか、については、よく分から
ない点もあるが、下記のように、高温時における
直流破壊電圧特性および極性反転破壊電圧特性が
改善され、その結果直流電力の送電容量が増大す
ることが、実験により確認された。 [実施例 1] 「第1図」において、10はケーブル導体、以
下順次、内部半導電層20、外部半導電層40、
ケーブルシース50を設ける。これらは従来のも
のと同じである。 30は絶縁体で、上記のようにカーボン粒子入
りの架橋ポリエチレンからなる。 これは粒子径が30〜100mmのカーボン粒子を、
架橋ポリエチレンに、0.5〜15%含有させること
により、抵抗率1012〜1016Ω・cm(at90℃)の値
を実現させたものである。なおこれは、純粋の架
橋ポリエチレンにくらべてやや低い値である。 このようにすると、空間電荷の影響が抑制さ
れ、特に高温時の直流破壊電圧および極性反転破
壊電圧を向上させることができた。それは、次ぎ
の理由によるものと考えられる。従来の架橋ポリ
エチレンケーブルの場合は、半導電層の架橋ポリ
エチレン絶縁体との間の境界面の電荷移動に対す
る障壁が大きく、電荷が半導電層近傍の絶縁体中
に蓄積されてしまうための直流破壊特性が損なわ
れてしまうと考えられる。 電荷移動に対する障壁は、一般的には「仕事関
数」とも呼ばれており、半導電材料と絶縁体の様
な種類の異なるものが接触した時に、界面にある
大きさのエネルギーバリアーが存在し、その界面
を電荷担体が通過するときには、ある一定以上の
エネルギーを必要とするものである。 上記に示す直流特性低下現象を定性的に説明す
る。 半導電層と架橋ポリエチレン絶縁体との間の境
界面の電荷移動に対する障壁を「界面抵抗」と呼
び、絶縁体中の電荷移動に対する抵抗を「絶縁抵
抗」と呼ぶことにすると、通常の架橋ポリエチレ
ンケーブルは、 界面抵抗>>絶縁抵抗 であるため、絶縁体中を電極面(半導電層)に向
つて移動してきた電荷が、半導電と絶縁体界面を
なかなか通過できずに半導電層近傍の絶縁体中の
電界強度が著しく上昇し、結果的に直流破壊特性
が損なわれてしまうものと考えられる。 絶縁体中の空間電荷を早めに飛ばして直流特性
を向上させるためには、絶縁抵抗を高くするか、
界面抵抗を低くすることによつて、 界面抵抗≒絶縁抵抗の状態を作り出すのが最も
望ましいものと思われる。 しかし架橋ポリエチレンは現在考えられている
実用的な絶縁体では、最も高い絶縁抵抗を有する
絶縁体のひとつであり、絶縁抵抗をより高くする
のは困難である。 従つて本発明では、半導電層は絶縁体に多量の
カーボンを添加させて半導電としているので、同
じ様に絶縁体にカーボンを添加すれば、絶縁体全
体にわたつて、同系統の均質な材料となるので界
面抵抗が低減すると考え、絶縁体中にカーボンを
添加させたものである。 本発明は、上記の様な考えに基づくものであ
り、 界面抵抗≒絶縁抵抗 という状態が出来上がつたために、空間電荷を早
めに飛ばす、すなわち電極面(半導電層)近傍に
電極面と逆極性の空間電荷が蓄積されなくなつて
(あるいは蓄積量が著しく減少して)、その結果直
流破壊特性が向上したものと考えられる。 なお具体的数値の例を示すと次のとおりであ
る。これは、導体断面積200mm、絶縁厚2.5mmの
6.6kvCVケーブルの高温時(導体温度90℃)の特
性例である。
[Industrial Application Field] This invention relates to a cross-linked polyethylene power cable for direct current. [Problems specific to DC cables] When cross-linked polyethylene is used as an insulating material for DC power cables, it is said that the influence of space charges is large. Although the behavior of space charge is not yet well understood, it is thought to be related to the decrease in DC breakdown voltage characteristics and polarity reversal breakdown voltage characteristics at high temperatures. [Problems to be solved by conventional techniques and ideas] - Part 1: A method of infiltrating an organic semiconducting liquid into a cable insulator has been considered (for example, Japanese Patent Laid-Open No. 52-8487).
Publication No.). However, in this case, the organic semiconducting liquid penetrates only near the semiconducting layer;
Even from the attached drawings of Publication No. 8487, it cannot be considered that the organic semiconducting liquid permeates the entire cable insulator.・Part 2: Between the cable insulator and the inner and outer semiconducting layers, the insulation resistance is smaller than the insulator and greater than the semiconducting layer due to carbon inclusion, and the insulation resistance decreases from the insulator side to the semiconducting layer side. There is also an idea to provide an extremely thin layer (for example, about 0.5 mm) having a resistance gradient as follows (Japanese Patent Publication No. 116983/1983). In this technology, space charges accumulate at and near the interface between the insulator and the semiconducting layer, and the accumulation
Based on the idea that there is a close relationship between the applied voltage and the applied time, the aim is to prevent space charge from accumulating at the interface and its vicinity, and as a result, the long-term charging characteristics are improved. That thing,
Reporting. However, there is no report that DC breakdown voltage characteristics and polarity reversal breakdown voltage characteristics are improved at high temperatures. [Means for solving the problem] Instead of making only the extremely thin layer at the interface between the cable insulator and the semiconducting layer a carbon-containing layer, as in the conventional technology "Part 2" above, The entire insulator is made of crosslinked polyethylene containing carbon particles and having a resistivity of 10 12 to 10 16 Ω·cm. [Function] If the entire cable insulator is made of cross-linked polyethylene containing carbon particles and having a resistivity of 10 12 to 10 16 Ωcm, how will the space charge behave? Although there are some points that are not well understood, it has been confirmed through experiments that the DC breakdown voltage characteristics and polarity reversal breakdown voltage characteristics at high temperatures are improved, resulting in an increase in DC power transmission capacity, as described below. Ta. [Example 1] In "Fig. 1", 10 is a cable conductor, and the following are in order: an inner semiconducting layer 20, an outer semiconducting layer 40,
A cable sheath 50 is provided. These are the same as the conventional ones. 30 is an insulator, which is made of crosslinked polyethylene containing carbon particles as described above. This is carbon particles with a particle size of 30 to 100 mm,
By containing 0.5 to 15% of crosslinked polyethylene, a resistivity of 10 12 to 10 16 Ω·cm (at 90°C) is achieved. Note that this value is slightly lower than that of pure crosslinked polyethylene. In this way, the influence of space charges was suppressed, and the DC breakdown voltage and polarity reversal breakdown voltage, especially at high temperatures, could be improved. This is considered to be due to the following reasons. In the case of conventional cross-linked polyethylene cables, there is a large barrier to charge transfer at the interface between the semi-conducting layer and the cross-linked polyethylene insulator, resulting in DC breakdown due to charges being accumulated in the insulator near the semi-conducting layer. It is thought that the characteristics will be lost. The barrier to charge transfer is generally called the "work function," and when different types of materials, such as a semiconducting material and an insulator, come into contact, an energy barrier of a certain size exists at the interface. When charge carriers pass through that interface, energy above a certain level is required. The above-mentioned DC characteristic deterioration phenomenon will be qualitatively explained. If we call the barrier to charge transfer at the interface between the semiconducting layer and the cross-linked polyethylene insulator "interfacial resistance" and the resistance to charge transfer in the insulator "insulation resistance," then normal cross-linked polyethylene Since the cable has interfacial resistance>>insulation resistance, charges moving towards the electrode surface (semiconducting layer) in the insulator cannot easily pass through the interface between the semiconducting material and the insulating material, and the charges near the semiconducting layer. It is thought that the electric field strength in the insulator increases significantly, resulting in a loss of DC breakdown characteristics. In order to quickly dissipate the space charge in the insulator and improve DC characteristics, it is necessary to increase the insulation resistance or
It seems most desirable to create a condition where interfacial resistance ≒ insulation resistance by lowering the interfacial resistance. However, cross-linked polyethylene has one of the highest insulation resistances among the practical insulators currently being considered, and it is difficult to increase the insulation resistance even higher. Therefore, in the present invention, the semiconducting layer is made semiconductive by adding a large amount of carbon to the insulator, so if carbon is added to the insulator in the same way, the same type of homogeneous layer will be formed throughout the insulator. Carbon is added to the insulator because it is thought that the interfacial resistance will be reduced because it becomes a material. The present invention is based on the above-mentioned idea, and since the state of interfacial resistance≒insulation resistance has been established, the space charge is quickly dissipated, that is, the electrode surface is placed near the electrode surface (semiconductor layer). It is thought that space charges of opposite polarity are no longer accumulated (or the amount accumulated is significantly reduced), and as a result, the DC breakdown characteristics are improved. Examples of specific numerical values are as follows. This has a conductor cross section of 200mm and an insulation thickness of 2.5mm.
This is an example of the characteristics of a 6.6kvCV cable at high temperature (conductor temperature 90℃).

【表】 なお従来品というのは、カーボンを含有しない
直流ケーブルのことである。 [実施例 2] 絶縁体30を多層化し、半径方向のグレーデイ
ングをつけたものである。 すなわち、たとえば「第2図」のように、絶縁
体30を31,32,33の3層に分け、31と
33の層のカーボン含有料を大きくして抵抗率を
1013〜1014Ω・cmにし、中間の32の層の抵抗率
を1015〜1016Ω・cmとしたものである。 このようにすると、第2図に併記した電位と電
界の分布図のように、空間電荷による電界の変歪
が効果的に押えられて、いつそう直流破壊電圧お
よび極性反転破壊電圧を向上させることができる
ようになる。 なお具体的数値の例を示すと次のとおりであ
る。これは、「実施例1」の場合と同じケーブル
で、導体温度も同じく90℃の高温の場合の例であ
る(従来ケーブルの数値は「実施例1」の場合と
同じであるが、参考までに併記した。)
[Table] Conventional products refer to DC cables that do not contain carbon. [Example 2] The insulator 30 is multilayered and graded in the radial direction. That is, for example, as shown in Figure 2, the insulator 30 is divided into three layers 31, 32, and 33, and the resistivity is increased by increasing the carbon content of the layers 31 and 33.
10 13 to 10 14 Ω·cm, and the resistivity of the middle 32 layers is 10 15 to 10 16 Ω·cm. In this way, as shown in the potential and electric field distribution diagram shown in Figure 2, the distortion of the electric field due to space charges is effectively suppressed, and the DC breakdown voltage and polarity reversal breakdown voltage can be easily improved. You will be able to do this. Examples of specific numerical values are as follows. This is an example of the same cable as in "Example 1", and the conductor temperature is also as high as 90 degrees Celsius (the values for the conventional cable are the same as in "Example 1", but for reference only) )

【表】 [考案の効果] ケーブル絶縁体の全体を、カーボン粒子を含有
させて、抵抗率を1012〜1016Ω・cmとした架橋ポ
リエチレンによつて形成することにより、高温時
における直流破壊電圧特性および極性反転破壊電
圧特性が改善されることが、実験により確認され
た。この結果直流電力の送電容量の増大が図れ
る。
[Table] [Effects of the invention] By forming the entire cable insulator from cross-linked polyethylene containing carbon particles and having a resistivity of 10 12 to 10 16 Ωcm, direct current breakdown at high temperatures can be reduced. It was confirmed through experiments that the voltage characteristics and polarity reversal breakdown voltage characteristics were improved. As a result, the power transmission capacity of DC power can be increased.

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

第1図は本考案の実施例の説明図で、第2図は
別の実施例に電位、電界分布図を併記した説明
図。 10……ケーブル導体、20……外部半導電
層、30……ケーブル絶縁体、40……外部半導
電層。
FIG. 1 is an explanatory diagram of an embodiment of the present invention, and FIG. 2 is an explanatory diagram of another embodiment together with a potential and electric field distribution diagram. DESCRIPTION OF SYMBOLS 10... Cable conductor, 20... Outer semiconducting layer, 30... Cable insulator, 40... Outer semiconducting layer.

Claims (1)

【実用新案登録請求の範囲】 ケーブル導体の周りに、内部半導電層、絶縁
体、外部半導電層を順次設けてなる直流用電力ケ
ーブルにおいて、 前記絶縁体の全体にわたつて、カーボン粒子を
含有させて、抵抗率を1012〜1016Ω・cmとした架
橋ポリエチレンによつて形成したことを特徴とす
る、直流用電力ケーブル。
[Claims for Utility Model Registration] A DC power cable in which an inner semiconducting layer, an insulator, and an outer semiconducting layer are sequentially provided around a cable conductor, wherein the entire insulator contains carbon particles. A direct current power cable, characterized in that it is made of crosslinked polyethylene with a resistivity of 10 12 to 10 16 Ω·cm.
JP20095883U 1983-12-30 1983-12-30 DC power cable Granted JPS60112021U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20095883U JPS60112021U (en) 1983-12-30 1983-12-30 DC power cable

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20095883U JPS60112021U (en) 1983-12-30 1983-12-30 DC power cable

Publications (2)

Publication Number Publication Date
JPS60112021U JPS60112021U (en) 1985-07-29
JPH0447854Y2 true JPH0447854Y2 (en) 1992-11-11

Family

ID=30762294

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20095883U Granted JPS60112021U (en) 1983-12-30 1983-12-30 DC power cable

Country Status (1)

Country Link
JP (1) JPS60112021U (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50116983A (en) * 1974-02-28 1975-09-12
JPS528487A (en) * 1975-06-04 1977-01-22 Hitachi Cable Ltd D.c. use bridge polyethylene insulation cable

Also Published As

Publication number Publication date
JPS60112021U (en) 1985-07-29

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