JPS6245531B2 - - Google Patents
Info
- Publication number
- JPS6245531B2 JPS6245531B2 JP55038168A JP3816880A JPS6245531B2 JP S6245531 B2 JPS6245531 B2 JP S6245531B2 JP 55038168 A JP55038168 A JP 55038168A JP 3816880 A JP3816880 A JP 3816880A JP S6245531 B2 JPS6245531 B2 JP S6245531B2
- Authority
- JP
- Japan
- Prior art keywords
- fiber core
- optical fiber
- tension member
- fiber cable
- fiber
- 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
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/44—Mechanical structures for providing tensile strength and external protection for fibres, e.g. optical transmission cables
- G02B6/4479—Manufacturing methods of optical cables
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Insulated Conductors (AREA)
Description
【発明の詳細な説明】
本発明は、テンシヨンメンバの周囲にフアイバ
心線を撚り合わせてなる光フアイバケーブルの高
温度域における伝送損失の増加を阻止した光フア
イバケーブルの製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing an optical fiber cable that prevents an increase in transmission loss in a high temperature range of an optical fiber cable made by twisting fiber cores around a tension member.
伝送損失を他のフアイバと比較して極めて低く
抑えることが可能な石英系フアイバは、特に通信
用としての将来性が大いに期待されており、これ
をケーブル化する試みが各所で盛んに行なわれつ
つある。一般に、石英系フアイバのコアとして使
用される石英ガラスの伝送損失は、セ氏数百度と
いう高温にならない限り変化することがない。と
ころで、この石英系フアイバを用いて光フアイバ
ケーブルを製造する場合、フアイバ心線となる石
英系フアイバは合成樹脂の被覆が施され、テンシ
ヨンメンバや介在線等の他のケーブル構成材料と
一体的に纒められてケーブルとなる。この場合、
前記合成樹脂の被覆材料や他のケーブル構成材料
と石英系フアイバとの温度特性、特に線膨張率の
違いに基づく低温度域での伝送損失の増大という
重大な欠点のあることが知られている。例えば、
フアイバ心線の断面を表わす第1図に示すよう
に、石英系フアイバ1を被覆する被覆材2がナイ
ロンの場合、その線膨張率は1×10-4cm/degで
あるが、石英ガラスの線膨張率は6×10-7cm/
degであり、被覆材2の線膨張率の方が石英系フ
アイバ1の線膨張率よりも二桁以上大きいことに
なる。従つて、このフアイバ心線3を冷却するに
伴い被覆材も大きな収縮を起こすが、この収縮が
ある程度以上になると、フアイバ心線3の中心に
占位する石英系フアイバ1が座屈してマイクロベ
ンデイングなる蛇行現象を生じ、これが石英系フ
アイバ1内を伝搬していた光を外部に漏出させ、
伝送損失増加の主因をなすものである。 Silica fiber, which can keep transmission loss extremely low compared to other fibers, holds great promise especially for communication applications, and many attempts are being made to create cables using it. be. Generally, the transmission loss of silica glass used as the core of a silica-based fiber does not change unless the temperature is raised to several hundred degrees Celsius. By the way, when manufacturing an optical fiber cable using this quartz fiber, the quartz fiber that becomes the fiber core is coated with synthetic resin and is integrated with other cable constituent materials such as tension members and intervening wires. It is bundled into a cable. in this case,
It is known that there is a serious drawback of increased transmission loss in the low temperature range due to the difference in temperature characteristics, especially linear expansion coefficient, between the synthetic resin coating material or other cable constituent materials and the quartz fiber. . for example,
As shown in Figure 1, which shows the cross section of the fiber core, when the coating material 2 covering the silica fiber 1 is made of nylon, its coefficient of linear expansion is 1 x 10 -4 cm/deg. The coefficient of linear expansion is 6×10 -7 cm/
deg, and the coefficient of linear expansion of the covering material 2 is greater than that of the quartz fiber 1 by two orders of magnitude or more. Therefore, as the fiber core 3 is cooled, the coating material also undergoes a large contraction, but when this contraction exceeds a certain level, the quartz fiber 1 occupying the center of the fiber core 3 buckles and causes microbending. A meandering phenomenon called deing occurs, which causes the light propagating within the silica fiber 1 to leak to the outside.
This is the main cause of increased transmission loss.
そこで、低温度域におけるこのフアイバ心線3
のマイクロベンデイングの発生を防止するため、
フアイバ心線3をケーブル化した断面構造を表わ
す第2図に示すように、外被4とテンシヨンメン
バ5との間に形成された介在線からなる緩衝層6
中のテンシヨンメンバ5の周囲に複数本のフアイ
バ心線3を螺旋状に撚り合わせ、金属製のテンシ
ヨンメンバ5の線膨張率が複合材としての光フア
イバ心線3の線膨張率よりも小さいことを利用し
て、低温度域でフアイバ心線3を緊張した状態に
維持するようにした光フアイバケーブル7が開発
された。このような光フアイバケーブル7の温度
に対する線膨張歪の割合を我が国における工場内
室温である20℃の時の歪の状態を零として第3図
に示すが、図中の実線がフアイバ心線3に相当
し、破線がテンシヨンメンバ5に相当する。この
グラフから、20℃より低温度域ではテンシヨンメ
ンバ5の収縮量がフアイバ心線3の収縮量よりも
小さく、このフアイバ心線3はテンシヨンメンバ
5によつて緊張された状態となることが容易に判
断され、これによつて低温度域へでのフアイバ心
線3のマイクロベンデイングの発生を防止するこ
とが可能となる。 Therefore, this fiber core wire 3 in the low temperature range
In order to prevent the occurrence of microbending,
As shown in FIG. 2, which shows the cross-sectional structure of the fiber core wire 3 made into a cable, a buffer layer 6 consisting of an intervening wire is formed between the jacket 4 and the tension member 5.
A plurality of fiber core wires 3 are twisted spirally around the inner tension member 5, and the linear expansion coefficient of the metal tension member 5 is higher than the linear expansion coefficient of the optical fiber core wire 3 as a composite material. An optical fiber cable 7 has been developed that takes advantage of its small size to maintain the fiber core 3 in a taut state in a low temperature range. The ratio of linear expansion strain to temperature of such an optical fiber cable 7 is shown in Figure 3, with the strain state at 20°C, which is the factory room temperature in Japan, being zero. The broken line corresponds to the tension member 5. From this graph, it can be seen that in the temperature range lower than 20°C, the amount of contraction of the tension member 5 is smaller than the amount of contraction of the fiber core 3, and this fiber core 3 is in a state under tension by the tension member 5. can be easily determined, thereby making it possible to prevent microbending of the fiber core 3 in the low temperature range.
ところが、20℃よりも高温度域ではフアイバ心
線3の膨張量がテンシヨンメンバ5の膨張量より
も大きくなるため、フアイバ心線3にマイクロベ
ンデイングが発生し、伝送損失の増加を来たすこ
とが判明した。 However, in a temperature range higher than 20°C, the amount of expansion of the fiber core 3 is greater than the expansion amount of the tension member 5, so microbending occurs in the fiber core 3, resulting in an increase in transmission loss. There was found.
本発明はこのような知見に基づき、高温度域に
おいてもフアイバ心線にマイクロベンデイングが
発生しないと光フアイバケーブルを提供すること
を目的とし、この目的を達成する本発明の光フア
イバケーブルの製造方法にかかる構成は、中心心
にテンシヨンメンバを有し且つその周囲に当該テ
ンシヨンメンバの線膨張率よりも大きな線膨張率
を有する複数本のフアイバ心線が撚り合わされた
光フアイバケーブルにおいて、前記フアイバ心線
を前記光フアイバケーブルとして使用する際の温
度以上に加熱しながら撚り合わせるようにしたこ
とを特徴とする。 Based on such knowledge, the present invention aims to provide an optical fiber cable in which microbending does not occur in the fiber core even in a high temperature range, and the present invention aims to manufacture the optical fiber cable of the present invention to achieve this purpose. The configuration according to the method includes an optical fiber cable in which a plurality of fiber core wires having a tension member at the center and a plurality of fiber core wires having a coefficient of linear expansion larger than the coefficient of linear expansion of the tension member are twisted around the tension member, The present invention is characterized in that the fiber core wires are twisted together while being heated to a temperature higher than that at which they are used as the optical fiber cable.
つまり、本発明はフアイバ心線をテンシヨンメ
ンバに巻き付ける際にフアイバ心線を高温度に加
熱しておき、テンシヨンメンバに対してフアイバ
心線が常に緊張した状態を維持するように配慮し
たものである。例えば、フアイバ心線の加熱温度
をTとしてこの温度を基準とする光フアイバケー
ブルの温度に対する線膨張歪の割合を第4図に示
すが、このTより低温度域で光フアイバケーブル
を使用するようにした場合、破線で示すテンシヨ
ンメンバの収縮量が実線で示すフアイバ心線の収
縮量よりも常に小さくなり、フアイバ心線はテン
シヨンメンバによつて常時緊張された状態となる
ため、フアイバ心線にマイクロベンデイングが発
生せず、従つて伝送損失の増加もない。Tの温度
は光フアイバケーブルの最高使用温度に設定すれ
ば実用上問題がなく、一般的には60℃程度が妥当
と考えられる。 In other words, the present invention is designed to heat the fiber to a high temperature when winding it around the tension member so that the fiber is always kept under tension with respect to the tension member. It is. For example, assuming that the heating temperature of the fiber core is T, the ratio of linear expansion strain to the temperature of the optical fiber cable is shown in Figure 4, which is based on this temperature. , the amount of contraction of the tension member shown by the broken line is always smaller than the amount of contraction of the fiber core shown by the solid line, and the fiber core is always under tension by the tension member. No microbending occurs in the wire and therefore no increase in transmission loss. There is no practical problem if the temperature of T is set to the maximum operating temperature of the optical fiber cable, and generally around 60°C is considered appropriate.
一方、加熱に関しては装置全体を高温に保つ必
要性はなく、フアイバ心線のみをそれらが撚り合
わされる直前までに加熱しておけば充分であり、
例えば撚り合わせダイスを加熱しておいたり、撚
り合わせ直前のフアイバ心線に熱風を吹き付けた
り、或いは撚り合わせ直前のフアイバ心線の周囲
を加熱炉で取り囲み、前述したようにフアイバ心
線を60℃程度に加熱するとよい。 On the other hand, regarding heating, there is no need to keep the entire device at a high temperature; it is sufficient to heat only the fiber cores just before they are twisted together.
For example, by heating the twisting die, by blowing hot air onto the fiber core just before twisting, or by surrounding the fiber core just before twisting in a heating furnace, the fiber core can be heated to 60°C as described above. It is best to heat it to a certain degree.
このように本発明の光フアイバケーブルの製造
方法によると、フアイバ心線を撚り合わせる際の
温度を光フアイバケーブルとして使用する際の温
度よりも高くすることによつて、テンシヨンメン
バの収縮歪よりもフアイバ心線の収縮歪の方が常
に大きくなるようにしたので、フアイバ心線はテ
ンシヨンメンバに対して緊張した状態となつて、
フアイバ心線にマイクロベンデイングが発生せ
ず、従つて高温度域における光フアイバケーブル
の伝送損失が増加する虞が全くなくなつた。 As described above, according to the method of manufacturing an optical fiber cable of the present invention, the shrinkage strain of the tension member is reduced by making the temperature when the fiber core wires are twisted higher than the temperature when used as an optical fiber cable. Since the shrinkage strain of the fiber core was always larger than that of the fiber core, the fiber core was in a state of tension against the tension member.
Microbending does not occur in the fiber core, and therefore, there is no possibility that the transmission loss of the optical fiber cable will increase in a high temperature range.
第1図は光フアイバケーブルの一構成要素であ
るフアイバ心線の断面図、第2図は六心光フアイ
バケーブルの断面図の一例、第3図は従来の光フ
アイバケーブルの線膨張歪と温度との関係を表わ
すグラフであり、それぞれ実線がフアイバ心線、
破線がテンシヨンメンバを表わす。又、第4図は
本発明による光フアイバケーブルの線膨張歪と温
度との関係を原理的に表わすグラフであり、それ
ぞれ実線がフアイバ心線、破線がテンシヨンメン
バを表わす。
図面中、3はフアイバ心線、5はテンシヨンメ
ンバ、7は光フアイバケーブルである。
Figure 1 is a cross-sectional view of a fiber core that is a component of an optical fiber cable, Figure 2 is an example of a cross-sectional view of a six-core optical fiber cable, and Figure 3 is a linear expansion strain and temperature of a conventional optical fiber cable. This is a graph showing the relationship between
Dashed lines represent tension members. FIG. 4 is a graph showing the relationship between linear expansion strain and temperature of the optical fiber cable according to the present invention, in which the solid line represents the fiber core and the broken line represents the tension member. In the drawing, 3 is a fiber core, 5 is a tension member, and 7 is an optical fiber cable.
Claims (1)
に当該テンシヨンメンバの線膨張率よりも大きな
線膨張率を有する複数本のフアイバ心線が撚り合
わせれた光フアイバケーブルにおいて、前記フア
イバ心線を前記光フアイバケーブルとして使用す
る際の温度以上に加熱しながら撚り合わせるよう
にしたことを特徴とする光フアイバケーブルの製
造方法。 2 フアイバ心線をテンシヨンメンバの周囲に撚
り合わせる撚り合わせダイスを加熱することによ
り、前記フアイバ心線の加熱を行なうようにした
ことを特徴とする特許請求の範囲第1項記載の光
フアイバケーブルの製造方法。 3 撚り合わせダイスの直前部に位置する撚り合
わせ前のフアイバ心線を熱風で加熱するようにし
たことを特徴とする特許請求の範囲第1項記載の
光フアイバケーブルの製造方法。 4 撚り合わせダイスの直前部に位置する撚り合
わせ前のフアイバ心線の周囲に加熱炉を設置し、
この加熱炉で前記フアイバ心線を加熱するように
したことを特徴とする特許請求の範囲第1項記載
の光フアイバケーブルの製造方法。[Claims] 1. An optical fiber cable having a tension member at the center and a plurality of fiber cores twisted around the tension member having a linear expansion coefficient larger than that of the tension member, A method for manufacturing an optical fiber cable, characterized in that the fiber core wires are twisted together while being heated to a temperature higher than that at which they are used as the optical fiber cable. 2. The optical fiber cable according to claim 1, wherein the fiber core is heated by heating a twisting die that twists the fiber core around a tension member. manufacturing method. 3. The method for manufacturing an optical fiber cable according to claim 1, wherein the fiber core wires before twisting located immediately before the twisting die are heated with hot air. 4. Install a heating furnace around the untwisted fiber core located just before the twisting die,
2. The method for manufacturing an optical fiber cable according to claim 1, wherein the fiber core is heated in this heating furnace.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3816880A JPS56135804A (en) | 1980-03-27 | 1980-03-27 | Production of optical fiber cable |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3816880A JPS56135804A (en) | 1980-03-27 | 1980-03-27 | Production of optical fiber cable |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56135804A JPS56135804A (en) | 1981-10-23 |
| JPS6245531B2 true JPS6245531B2 (en) | 1987-09-28 |
Family
ID=12517861
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3816880A Granted JPS56135804A (en) | 1980-03-27 | 1980-03-27 | Production of optical fiber cable |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56135804A (en) |
-
1980
- 1980-03-27 JP JP3816880A patent/JPS56135804A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56135804A (en) | 1981-10-23 |
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