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JPH0520180B2 - - Google Patents
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JPH0520180B2 - - Google Patents

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Publication number
JPH0520180B2
JPH0520180B2 JP60019035A JP1903585A JPH0520180B2 JP H0520180 B2 JPH0520180 B2 JP H0520180B2 JP 60019035 A JP60019035 A JP 60019035A JP 1903585 A JP1903585 A JP 1903585A JP H0520180 B2 JPH0520180 B2 JP H0520180B2
Authority
JP
Japan
Prior art keywords
layer
strands
pitch
nth
equation
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
JP60019035A
Other languages
Japanese (ja)
Other versions
JPS61180632A (en
Inventor
Ryoichi Imanishi
Toshinori Shimada
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.)
Tatsuta Electric Wire and Cable Co Ltd
Original Assignee
Tatsuta Electric Wire and Cable Co 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 Tatsuta Electric Wire and Cable Co Ltd filed Critical Tatsuta Electric Wire and Cable Co Ltd
Priority to JP1903585A priority Critical patent/JPS61180632A/en
Publication of JPS61180632A publication Critical patent/JPS61180632A/en
Publication of JPH0520180B2 publication Critical patent/JPH0520180B2/ja
Granted legal-status Critical Current

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Description

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

<産業上の利用分野> 本発明は、各層同方向に順次撚り合せた後、各
層ごとに圧縮成形してなる円形圧縮撚線に関す
る。 <従来技術とその問題点> 従来の円形圧縮撚線には次の構成のものがあ
る。 (a) 各層を右撚り、左撚りというように交互に反
対方向に撚り合せたもの。 この構成のものでは、内外層の素線が交叉接
触しているので、圧縮成形したときに、接触部
の変形が他の部分に比べて大きく、機械的特性
や可とう性が悪いという難点がある。 (b) 各層を総て右撚り、あるいは左撚りに同方向
に撚り合せ、その際、内層の素線よりも外層の
素線の径を細くするか、第1層以降の任意の第
n層における素線数を非圧縮円形層撚線のごと
く6n(nは整数)といつた規則性を持たせず
に、たとえば5n+1にするなどして、圧縮成
形をしやすくしたもの。 この構成のものでは、撚線製造時の素線径や素
線数の管理が複雑であり、しかも、外層素線が内
層素線の間隙に落ち込んで外観が悪くなることが
ある。 本発明は、上述の問題点に鑑みてなされたもの
であつて、表面が平滑で、しかも機械的性質や可
とう性に優れた円形圧縮撚線が得られるようにす
ることを目的とする。 <問題点を解決するための手段> 本発明は上記の目的を達成するため鋭意研究し
た結果、各層の外径および撚りピツチを選定すれ
ば、直径のほぼ等しい素線を各層正構成、すなわ
ち、中心層、第1層、第2層、…、第n−1層、
第n層(最外層)の素線数が1,6,12,…,6
(n−1),6nで、かつ、同方向に撚り合わせた
場合でも、隣接する内外層の撚りピツチ倍数が異
なるので、外層素線が内層素線間隙に落ち込まな
いことが分かつた。 すなわち、第1図に示すように、 Dn,Dn-1;第n層、第n−1層の外径 dn,dn-1;第n層、第n−1層の素線径 Pn,Pn-1;第n層、第n−1層のピツチ としたとき、 第n層の層心径はDn−dn、 第n−1層の層心径はDn-1−dn-1、 第n層の層心径に対するピツチ倍数Φnは、 Φn=Pn/(Dn−dn) (1) 第n−1層の層心径に対するピツチ倍数Φn-1
は、 Φn-1=Pn-1/Dn-1−dn-1) (2) となる。そして、このときのΦnとΦo-1とが互い
に近似した値になるほど外層素線が内層素線間に
落ち込みやすい。これを防止するには、隣接する
内外層のピツチ倍数を互いに異なるように設定す
ればよいが、このとき、内層のピツチ倍数を外層
のピツチ倍数よりも小さく設定すると、長尺の素
線が必要になるため不経済である。したがつて、
内層のピツチ倍数を外層のピツチ倍数よりも大き
く設定する方が好ましい。そこで、ピツチ倍数を
どの程度大きく設定すれば良いかを検討したとこ
ろ、 Φn-1/Φn≧1.03 (3) の条件を満たせば良いことが、後述する別表1,
2の結果などから明らかとなつた。 なお、外層素線の内層素線間への落ち込み防止
の観点からは、隣接する内外層のピツチ倍数の比
Φn-1/Φnに上限を設ける必要はないけれども、
可とう性を良好に保つ上では、後述するように、
内外層のピツチは、Pn-1≦Pn,Pn-2≦Pn-1、…
となることが好ましい。 そこで、(3)式に(1),(2)式を代入すれば、
Pn-1/Pn≧1.03(Dn-1−dn-1)/(Dn−dn) (4) となる。 また、 Dn-1/Dn=Kn とおくと、 dn=(Dn−Dn-1)/2 =Dn(1−Kn)/2dn-1=(Dn-1−Dn-2)/
2 =(Dn-1−Dn-1Kn-1)/2 =Dn-1(1−Kn-1)/2 であるから、これらの式を(4)式に代入すると、 Pn-1/Pn≧1.03(DnKn−DnKn(1−Kn-1)/
2)/(Dn−Dn(1−Kn)/2)≧1.03DnKn(1
−1/2+Ko-1/2) Dn(1−1/2+Kn/2) ≧1.03Kn(1+Kn-1/(1+Kn) ∴Pn-1≧1.03PnKn(1+Kn-1)/(1+Kn) (5) そこで、外層のピツチPnをまず選定し、その後
(5)式を満足するようにPn-1を選定し、以下順次
Pn-2,Pn-3、…を選定すれば良い。 なお、各層を形成する元の素線(以下、投入素
線という)の径をほぼ同一とし、各層の圧縮率を
ほぼ同一とする場合は、 Kn=Dn-1/Dn=√-1 (6) Kn-1=Dn-2/Dn-1=√-2 -1 (7) (ここに、Nn,Nn-1、……;第n層、第n−
1層……の各素線数)となる。 この場合のKn,Kn-1、…の各値は第1表に示
すとおりである。
<Industrial Application Field> The present invention relates to a circular compression stranded wire which is formed by sequentially twisting each layer in the same direction and then compression molding each layer. <Prior art and its problems> Conventional circular compression stranded wires have the following configurations. (a) Each layer is twisted in opposite directions alternately, such as right-handed and left-handed. With this configuration, the strands of the inner and outer layers are in cross-contact, so when compression molding is performed, the deformation of the contact area is larger than that of other areas, resulting in poor mechanical properties and flexibility. be. (b) All layers are twisted in the same direction, either right-handed or left-handed, and in this case, the diameter of the outer layer wires is smaller than that of the inner layer wires, or any n layer after the first layer is twisted. The number of strands in the wire is not as regular as 6n (n is an integer) like uncompressed circular layer stranded wire, but is made easier to compression mold by, for example, 5n+1. With this configuration, it is complicated to manage the wire diameter and the number of wires during the production of stranded wires, and furthermore, the outer layer wires may fall into the gaps between the inner layer wires, resulting in poor appearance. The present invention was made in view of the above-mentioned problems, and it is an object of the present invention to provide a circular compressed stranded wire having a smooth surface and excellent mechanical properties and flexibility. <Means for Solving the Problems> As a result of intensive research to achieve the above object, the present invention has found that by selecting the outer diameter and twisting pitch of each layer, wires with approximately equal diameters can be arranged in a normal configuration in each layer. central layer, first layer, second layer, ..., n-1th layer,
The number of strands in the nth layer (outermost layer) is 1, 6, 12, ..., 6
(n-1), 6n, and even when twisted in the same direction, it was found that the outer layer strands do not fall into the gap between the inner layer strands because the twist pitch multiples of the adjacent inner and outer layers are different. That is, as shown in Fig. 1, Dn, Dn -1 ; Outer diameter of the nth layer and n-1st layer dn, dn -1 ; Wire diameter of the nth layer and n-1st layer Pn, Pn -1 ; When the pitch of the nth layer and the n-1th layer is set, the core diameter of the nth layer is Dn-dn, the core diameter of the n-1st layer is Dn -1 -dn -1 , the nth The pitch multiple Φn for the core diameter of the layer is Φn=Pn/(Dn-dn) (1) The pitch multiple Φn -1 for the core diameter of the n-1th layer
is Φn -1 = Pn -1 /Dn -1 −dn -1 ) (2). Then, the closer Φn and Φ o-1 become to each other, the more likely the outer layer strands fall between the inner layer strands. To prevent this, the pitch multiples of the adjacent inner and outer layers can be set to be different from each other, but in this case, if the pitch multiple of the inner layer is set smaller than the pitch multiple of the outer layer, long strands of wire will be required. Therefore, it is uneconomical. Therefore,
It is preferable to set the pitch multiple of the inner layer to be larger than the pitch multiple of the outer layer. Therefore, we considered how large the pitch multiple should be set, and found that it is sufficient to satisfy the condition Φn -1 /Φn≧1.03 (3), as shown in Appendix 1 below.
This became clear from the results of 2. Note that from the viewpoint of preventing the outer layer strands from falling between the inner layer strands, it is not necessary to set an upper limit on the pitch multiple ratio Φn -1 /Φn of the adjacent inner and outer layers.
In order to maintain good flexibility, as described later,
The pitch of the inner and outer layers is Pn -1 ≦Pn, Pn -2 ≦Pn -1 ,...
It is preferable that Therefore, by substituting equations (1) and (2) into equation (3), we get
Pn -1 /Pn≧1.03 ( Dn -1 −dn -1 ) / (Dn − dn) (4). Also, if we set Dn -1 /Dn = Kn, then dn = (Dn - Dn -1 ) / 2 = Dn (1 - Kn) / 2dn -1 = (Dn -1 - Dn -2 ) /
2 = (Dn -1 −Dn -1 Kn -1 )/2 = Dn -1 (1−Kn -1 )/2, so by substituting these equations into equation (4), Pn -1 /Pn ≧1.03(DnKn−DnKn(1−Kn -1 )/
2)/(Dn-Dn(1-Kn)/2)≧1.03DnKn(1
-1/2+K o-1 /2) Dn (1-1/2+Kn/2) ≧1.03Kn (1+Kn -1 / (1+Kn) ∴Pn -1 ≧1.03PnKn (1+Kn -1 ) / (1+Kn) (5) Therefore, we first select the pitch Pn of the outer layer, and then
Select Pn -1 so as to satisfy equation (5), and then
It is sufficient to select Pn -2 , Pn -3 ,... In addition, when the diameter of the original wire (hereinafter referred to as input wire) forming each layer is almost the same and the compression ratio of each layer is approximately the same, Kn=Dn -1 /Dn=√ -1 (6 ) Kn -1 = Dn -2 / Dn -1 = √ -2 -1 (7) (Here, Nn, Nn -1 , ...; nth layer, nth -
(number of each strand in one layer). The values of Kn, Kn -1 , ... in this case are as shown in Table 1.

【表】 一般に、 Kn>Kn-1 (8) であるから、(5)式において、 (1+Kn-1)/(1+Kn)<1 となる。 したがつて、(5)式から 1.03PnKn(1+Kn-1)/(1+Kn) <1.03PnKn したがつて、 Pn-1>1.03PnKn (9) とし、(9)式にしたがつて各層のピツチを選定すれ
ば、 より安全であり、設計も容易である。 いま、 X=(1−Pn-1/Pn)/Kn とおくと、 Pn-1/Pn=1−KnX (10) (10)式を(9)式に代入すると、 1−KnX>1.03Kn ∴X<1/Kn−1.03 (11) すなわち、(11)式を満足すれば(9)式を満足するこ
とになる。 また、(10)式において、X=0とおくと、 Pn-1=Pn となる。 Pn-1>Pnとなることは好ましくない、すなわ
ち、可とう性を良好に保つには、Pn-1≦Pnであ
ることが好ましいので、 0<X<1/Kn−1.03 (12) とすれば、多層撚線の各層とも同じ値のXで計算
できる。 <実施例> 以下、本発明を実施例に基づいて説明すれば、
別表1に示した各円形圧縮撚線は、ほぼ同一径の
素線を用い、各層の圧縮率をほぼ等しくしたもの
について、X値を定めて各層のピツチを選定した
ものである。(3)式を満足するためには、(11)式を満
足すれば十分であり、別表1から明らかなよう
に、(11)式を満足するためには、最外層とその下の
層との関係において、Xは次の範囲にあることが
好ましい。 500mm2(61本撚り)の場合は0≦X≦0.254 120mm2(37本撚り)の場合は0≦X≦0.364 50mm2(19本撚り)の場合は0≦X≦0.617 また、別表2は(5)式、したがつて、(3)式に基づ
いてピツチを選定したもので、PaはΦn-1/Φnを
1.03に、Pbは1.02に、Pcは1.01にそれぞれ設定し
た場合であり、Φn-1/Φnが1.03以上にあればよ
いことが分かる。
[Table] Generally, since Kn>Kn -1 (8), in equation (5), (1+Kn -1 )/(1+Kn)<1. Therefore, from equation (5), 1.03PnKn (1+Kn -1 )/(1+Kn) <1.03PnKn Therefore, Pn -1 >1.03PnKn (9), and the pitch of each layer is determined according to equation (9). If selected, it will be safer and easier to design. Now, if we set X=(1-Pn -1 /Pn)/Kn, Pn -1 /Pn=1-KnX (10) Substituting equation (10) into equation (9), 1-KnX>1.03Kn ∴X<1/Kn−1.03 (11) That is, if formula (11) is satisfied, formula (9) is satisfied. Furthermore, in equation (10), if X=0, then Pn -1 =Pn. It is not preferable that Pn -1 > Pn. In other words, in order to maintain good flexibility, it is preferable that Pn -1 ≦Pn, so 0<X<1/Kn−1.03 (12) For example, calculations can be made using the same value of X for each layer of a multilayer twisted wire. <Examples> Hereinafter, the present invention will be explained based on examples.
Each of the circular compressed strands shown in Attached Table 1 uses strands of approximately the same diameter, and the compression ratio of each layer is approximately equal, and the pitch of each layer is selected by determining the X value. In order to satisfy equation (3), it is sufficient to satisfy equation (11), and as is clear from Appendix 1, in order to satisfy equation (11), the outermost layer and the layer below it must be In this relationship, it is preferable that X be in the following range. For 500mm 2 (61 strands), 0≦X≦0.254 For 120mm 2 (37 strands), 0≦X≦0.364 For 50mm 2 (19 strands), 0≦X≦0.617 The pitch is selected based on equation (5), therefore, equation (3), and Pa is Φn -1 /Φn.
This is the case where Pb is set to 1.03, Pb is set to 1.02, and Pc is set to 1.01, and it can be seen that it is sufficient if Φn -1 /Φn is 1.03 or more.

【表】【table】

【表】 表中の記号 ○;良い、△;やや悪い、
×;悪い
[Table] Symbols in the table ○: Good, △: Fairly poor.
×;Bad

【表】 表中の記号 ○;良い、△;やや悪
い、×;悪い
<発明の効果> 以上の例からも明らかなように、本発明によれ
ば、外観が平滑で、しかも、可とう性、機械的性
質に優れた同方向撚りの円形圧縮撚線が得られ
る。また、複雑な素線管理をする必要もない。し
たがつて、架橋ポリエチレン絶縁電力ケーブルに
本発明を適用すれば、絶縁体の導体間隙への食い
込みを防ぐためのセパレータテープが不要である
などの極めて大きな効果が得られる。
[Table] Symbols in the table ○: Good, △: Fairly bad
Bad; Bad <Effects of the Invention> As is clear from the above examples, according to the present invention, a circular compression twisted twisted in the same direction which has a smooth appearance and excellent flexibility and mechanical properties can be obtained. A line is obtained. Further, there is no need for complicated wire management. Therefore, if the present invention is applied to a cross-linked polyethylene insulated power cable, extremely large effects such as no need for a separator tape to prevent the insulator from digging into the conductor gap can be obtained.

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

図面は本発明の一実施例を示す円形圧縮撚線の
横断面図である。 Dn,Dn-1、…は第n層、第n−1層、…の外
径、dn,dn-1、…は各層の撚線半径方向の厚さ
である。
The drawing is a cross-sectional view of a circular compression strand showing an embodiment of the present invention. Dn, Dn -1 , . . . are the outer diameters of the n-th layer, n-1 layer, . . . , and dn, dn -1 , .

Claims (1)

【特許請求の範囲】 1 直径のほぼ等しい素線を各層同方向に順次撚
り合わせた後、各層ごとに圧縮成形してなり、中
心層、第1層、第2層、…、第n−1層、第n層
(最外層)の素線数が、1,6,12,…、6(n−
1)、6nである円形圧縮撚線において、 Dn,Dn-1、…;第n層、第n−1層、…の外
径 Pn,Pn-1、…;第n層、第n−1層、…の撚
りピツチ Kn,Kn-1、…;Dn-1/Dn,Dn-2/Dn-1、…
(nは整数)としたとき、 Pn-1/Pn≧1.03Kn(1+Kn-1)/(1+Kn),
Pn-2/Pn-1≧1.03Kn-1(1+Kn-2)/(1+
Kn-1)、… となり、かつ Pn-1≦Pn,Pn-2≦Pn-1、…となるように各層
の外径および撚りピツチを選定してなることを特
徴とする円形圧縮撚線。 2 前記中心層、第1層、第2層、…、第n−1
層、第n層(最外層)の素線数、1,6,12,
…、6(n−1),6nを、N0,N1,N2,…Nn-1
Nnとし、圧縮後の各層の半径方向の厚さdn,
dn-1、…がほぼ等しいものとし、かつ、隣接層の
外径の比がKn=√-1,Kn-1=√-2
Nn-1、…となるように選定してなることを特徴
とする特許請求の範囲第1項に記載の円形圧縮撚
線。 3 Pn-1/Pn≧1.03Kn,Pn-2/Pn-1
1.03Kn-1、…となるように、各層の外径および
撚ピツチを選定してなることを特徴とする特許請
求の範囲第1項または第2項に記載の円形圧縮撚
線。
[Claims] 1. Each layer is made by sequentially twisting strands of substantially equal diameter in the same direction, and then compression molding each layer to form a central layer, first layer, second layer, ..., n-1th layer. layer, the number of strands in the n-th layer (outermost layer) is 1, 6, 12, ..., 6 (n-
1), 6n circular compressed stranded wire, Dn, Dn -1 , ...; nth layer, n-1th layer, ... outer diameter Pn, Pn -1 , ...; nth layer, n-1th layer Twisting pitch of layer, Kn, Kn -1 ,...; Dn -1 /Dn, Dn -2 /Dn -1 ,...
(n is an integer), Pn -1 /Pn≧1.03Kn (1+Kn -1 )/(1+Kn),
Pn -2 /Pn -1 ≧1.03Kn -1 (1+Kn -2 )/(1+
Kn -1 ),..., and the outer diameter and twist pitch of each layer are selected so that Pn -1 ≦Pn, Pn -2 ≦Pn -1 , .... 2 The central layer, the first layer, the second layer, ..., the n-1th layer
layer, number of strands in nth layer (outermost layer), 1, 6, 12,
..., 6(n-1), 6n, N 0 , N 1 , N 2 ,...Nn -1 ,
Let Nn be the radial thickness dn of each layer after compression,
dn -1 , ... are almost equal, and the ratio of the outer diameters of adjacent layers is Kn = √ -1 , Kn -1 = √ -2
The circular compressed stranded wire according to claim 1, characterized in that Nn -1 , . . . 3 Pn -1 /Pn≧1.03Kn, Pn -2 /Pn -1
The circular compressed stranded wire according to claim 1 or 2, characterized in that the outer diameter and twisting pitch of each layer are selected so that 1.03Kn -1 , . . .
JP1903585A 1985-02-01 1985-02-01 circular compression strands Granted JPS61180632A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1903585A JPS61180632A (en) 1985-02-01 1985-02-01 circular compression strands

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1903585A JPS61180632A (en) 1985-02-01 1985-02-01 circular compression strands

Publications (2)

Publication Number Publication Date
JPS61180632A JPS61180632A (en) 1986-08-13
JPH0520180B2 true JPH0520180B2 (en) 1993-03-18

Family

ID=11988177

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1903585A Granted JPS61180632A (en) 1985-02-01 1985-02-01 circular compression strands

Country Status (1)

Country Link
JP (1) JPS61180632A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0318624U (en) * 1989-06-30 1991-02-25

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5584240A (en) * 1978-12-15 1980-06-25 Vnii Mechizunoi Puromishiyuren Preparation of stranded wireelike wire product and product manufactured by said preparation

Also Published As

Publication number Publication date
JPS61180632A (en) 1986-08-13

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