JPS6151287B2 - - Google Patents

Info

Publication number
JPS6151287B2
JPS6151287B2 JP4470282A JP4470282A JPS6151287B2 JP S6151287 B2 JPS6151287 B2 JP S6151287B2 JP 4470282 A JP4470282 A JP 4470282A JP 4470282 A JP4470282 A JP 4470282A JP S6151287 B2 JPS6151287 B2 JP S6151287B2
Authority
JP
Japan
Prior art keywords
optical fiber
power
light
connection point
distance
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
JP4470282A
Other languages
Japanese (ja)
Other versions
JPS58162919A (en
Inventor
Yasuyuki Kato
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP4470282A priority Critical patent/JPS58162919A/en
Publication of JPS58162919A publication Critical patent/JPS58162919A/en
Publication of JPS6151287B2 publication Critical patent/JPS6151287B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/36Mechanical coupling means
    • G02B6/38Mechanical coupling means having fibre to fibre mating means
    • G02B6/3801Permanent connections, i.e. wherein fibres are kept aligned by mechanical means
    • G02B6/3803Adjustment or alignment devices for alignment prior to splicing

Description

【発明の詳細な説明】 本発明は、光通信に用いる光フアイバの接続方
法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for connecting optical fibers used in optical communications.

一般に光通信用線路は、短尺なケーブルを複数
本接続して構成されるが、信頼性の高い高品質な
線路を構成するためには、ケーブル相互の接続損
失をできる限り低減しなければならない。そのた
め従来より、第1図に示すような4段階の手順で
接続点の損失を厳密に測定しつつ接続が行なわれ
ている。すなわち、まず光源1を光源側光フアイ
バ2に接続し、接続点において、光パワーメータ
3で光源側光フアイバ2からの出射光パワーP1
測定する(第1図a)。次いで、接続しようとす
る受光側光フアイバ5と光源側光フアイバ2を接
続装置8に固定するとともに仮接続点4で接続
し、この時の受光側光フアイバ5の出射光パワー
P2を受光側光パワーメータ6で測定する。なお、
7はパワーメータ6の指示値を接続点4において
読み取るためのモニタ装置であり、特に接続装置
8が接続しようとする光フアイバ2,5の軸を調
心できる機能を持つ場合に使用される(第1図
b)。仮接続が完了すると、仮接続点4の接続損
失を測定するために、仮接続点4から放射モード
の影響が無視できるフアイバ長を受光側光フアイ
バ5に取り、接続点のパワーメータ3で出射光パ
ワーP3を測定する(第1図c)。最後に、再び光
フアイバ2と5を本接続点9で接続し、光パワー
メータ6で受光側光フアイバ5からの出射光パワ
ーP4を測定し、下記の式(1)で本接続点9における
損失αが算出される(第1図d)。
Generally, an optical communication line is constructed by connecting a plurality of short cables, but in order to construct a highly reliable and high quality line, it is necessary to reduce the connection loss between the cables as much as possible. Therefore, conventionally, connections have been made while strictly measuring the loss at the connection point using a four-step procedure as shown in FIG. That is, first, the light source 1 is connected to the light source side optical fiber 2, and at the connection point, the output light power P1 from the light source side optical fiber 2 is measured with the optical power meter 3 (FIG. 1a). Next, the receiving side optical fiber 5 and the light source side optical fiber 2 to be connected are fixed to the connecting device 8 and connected at the temporary connection point 4, and the output light power of the receiving side optical fiber 5 at this time is
P 2 is measured with an optical power meter 6 on the receiving side. In addition,
7 is a monitor device for reading the indicated value of the power meter 6 at the connection point 4, and is used especially when the connection device 8 has a function of aligning the axes of the optical fibers 2 and 5 to be connected. Figure 1 b). When the temporary connection is completed, in order to measure the splice loss at the temporary connection point 4, a fiber length from the temporary connection point 4 where the influence of the radiation mode can be ignored is connected to the receiving side optical fiber 5, and the output is measured using the power meter 3 at the connection point. Measure the emitted light power P3 (Fig. 1c). Finally, connect the optical fibers 2 and 5 again at the main connection point 9, measure the output light power P 4 from the receiving side optical fiber 5 with the optical power meter 6, and use the following equation (1) to connect the main connection point 9. The loss α at is calculated (Fig. 1d).

α=−10logP/P(dB) ……(1) しかしながら、接続される光フアイバ2と5は
数百mから数Kmの長さがあるため、接続点4,9
と受光点は別々のマンホール内で作業を行う必要
があり、第1図に示すように、2台の光パワーメ
ータ3,6や特別モニタ装置7のほか受光側に余
分な作業者が必要となる等、作業時間や経費の面
で問題があつた。
α=-10logP 3 P 4 /P 1 P 2 (dB) ...(1) However, since the optical fibers 2 and 5 to be connected have a length of several hundred meters to several kilometers, the connection points 4 and 9
It is necessary to perform the work in separate manholes for the light receiving point and the light receiving point, and as shown in Figure 1, in addition to two optical power meters 3 and 6 and a special monitor device 7, an extra worker is required on the light receiving side. There were problems in terms of work time and costs.

また第2図は、従来行なわれている光フアイバ
の他の接続方法を示したものであるが(特願昭56
−48463)、この方法は接続作業の簡略化を図るた
めに接続点9の後の受光側フアイバ5に曲げを与
え、この曲げ部分10から放射され光パワーメー
タ3で測定される光パワーが最大となるように接
続装置8を調節し接続している。そのため、作業
は接続点のみでよいとともにパワーメータも1台
で済むという利点がある一方、接続点9の損失が
わからないという大きな欠点があつた。
Furthermore, Fig. 2 shows another conventional method of connecting optical fibers (Patent Application No. 1983).
-48463), this method bends the light-receiving fiber 5 after the connection point 9 in order to simplify the connection work, and the optical power emitted from this bent portion 10 and measured by the optical power meter 3 is maximized. The connecting device 8 is adjusted so that the connection is made. Therefore, while there is an advantage in that the work only needs to be done at the connection point and only one power meter is required, there is a major disadvantage in that the loss at the connection point 9 cannot be determined.

本発明は、かかる欠点を除去し、接続作業時間
の短縮化、作業の簡略化および経費の節減を図る
とともに、伝送損失の少ない光フアイバの接続方
法を提供せんとするものであつて、その要旨とす
るところは、光源を光源側光フアイバに接続して
受光側光フアイバとの接続点における前記光源側
光フアイバからの出射光パワーP1を測定し、次い
で前記接続点において生じた放射モードのパワー
がこの距離だけ伝搬したときに導波モードのパワ
ーに対して無視できる値となる距離lの2倍の距
離2lに曲げ部分を設定した前記受光側光フアイバ
を前記光源側光フアイバと仮接続するとともに前
記曲げ部分からの出射光パワーP2を測定し、さら
に前記仮接続点からlの距離で前記受光側光フア
イバを切断してこの切断点における出射光パワー
P3を測定し、最後に前記仮接続点からlの距離を
有する前記受光側光フアイバを除去するとともに
前記切断点からlの距離に前記曲げ部分がくるよ
うになつた前記受光側光フアイバを前記光源側光
フアイバと接続して前記曲げ部分からの出射光パ
ワーP4を測定し、各工程で求められた各出射光パ
ワーP1〜P4で与えられる損失−10logP/P
(dB) ができるだけ最小となるように前記両光フアイバ
を軸合せ本接続することを特徴とする。
The present invention aims to eliminate such drawbacks, shorten connection work time, simplify work and reduce costs, and provide an optical fiber connection method with low transmission loss. In this method, a light source is connected to a light source side optical fiber, and the output light power P1 from the light source side optical fiber is measured at the connection point with the light receiving side optical fiber, and then the radiation mode generated at the connection point is measured. Temporarily connect the light receiving side optical fiber with the light source side optical fiber, the bending portion of which is set at a distance 2l, which is twice the distance l, where the power of the waveguide mode becomes negligible when the power propagates this distance. At the same time, the output light power P 2 from the bent portion is measured, and the receiving side optical fiber is cut at a distance l from the temporary connection point, and the output light power at this cutting point is measured.
P 3 is measured, and finally, the light-receiving optical fiber that is at a distance of l from the temporary connection point is removed, and the light-receiving optical fiber whose bent portion is now located at a distance of l from the cutting point is removed. The output light power P 4 from the bent portion connected to the light source side optical fiber is measured, and the loss given by each output light power P 1 to P 4 obtained in each step is −10logP 3 P 4 /P 1 P
2
(dB) is as minimum as possible, the two optical fibers are aligned and connected.

以下、第3図に示した実施例にもとずき、本発
明に係る光フアイバの接続方法について説明す
る。
Hereinafter, an optical fiber connecting method according to the present invention will be explained based on the embodiment shown in FIG.

まず光源1を光源側光フアイバ1に接続し、受
光側光フアイバ5との接続点において光源側光フ
アイバ2からの出射光パワーP1を光パワーメータ
3で測定する(第3図a)。本発明に係る接続方
法では、仮接続から本接続までの出射光パワーの
測定をすべて接続点において行うために、受光側
光フアイバ5の曲げ部分10を仮接続点4より2
lの距離に設定することがポイントとなる。こ
こでlは、接続点において生じた放射モードのパ
ワーがこの距離だけ伝搬したときに導波モードの
パワーに対して無視できる値となる距離であり、
一般には0.5m〜1.5mの範囲となる。従つて、仮
接続を行なう際に光パワーメータ3は接続点のご
く近傍に置くことができ、接続装置8で光フアイ
バの軸調心を行うときには光パワーメータ3を見
ながら行うことが可能となる。仮接続点において
両光フアイバ2および5を仮接続後、曲げ部分1
0から放射される光パワーP2が光パワーメータ3
により測定される(第3図b)。次いで、仮接続
点4からlの距離で受光側光フアイバ5を切断
し、光パワーメータ3で仮接続点からlの距離の
出射光パワーP3が測定される(第3図d)。仮接
続点からlの距離の出射光パワーP3が測定される
と、光源側光フアイバ2に仮接続されたlの距離
を有して残された受光側光フアイバ5を除去し、
両光フアイバ2および5は本接続点10において
接続装置8により接続される。この時、受光側光
フアイバ5に設けられた曲げ部分10は本接続点
9よりlの距離にあることになる。したがつて、
曲げ部10からの出射パワーP4を光パワーメータ
3で測定すると、最終的な本接続における損失α
が式(2)で求めることができる(第3図d)。
First, the light source 1 is connected to the light source side optical fiber 1, and the output light power P1 from the light source side optical fiber 2 is measured with an optical power meter 3 at the connection point with the light receiving side optical fiber 5 (FIG. 3a). In the connection method according to the present invention, in order to measure the output light power from the temporary connection to the actual connection at the connection point, the bent portion 10 of the light-receiving side optical fiber 5 is moved from the temporary connection point 4 to the point 2.
The key is to set the distance to l. Here, l is the distance at which the power of the radiation mode generated at the connection point becomes negligible compared to the power of the guided mode when propagated over this distance,
Generally, it will be in the range of 0.5m to 1.5m. Therefore, when making a temporary connection, the optical power meter 3 can be placed very close to the connection point, and when the optical fiber is aligned with the connection device 8, it is possible to do so while looking at the optical power meter 3. Become. After temporarily connecting both optical fibers 2 and 5 at the temporary connection point, the bent portion 1
The optical power P 2 emitted from 0 is the optical power meter 3
(Figure 3b). Next, the receiving optical fiber 5 is cut at a distance l from the temporary connection point 4, and the output light power P3 at a distance l from the temporary connection point is measured by the optical power meter 3 (FIG. 3d). When the output light power P 3 at a distance of l from the temporary connection point is measured, the receiving side optical fiber 5 remaining temporarily connected to the light source side optical fiber 2 at a distance of l is removed;
Both optical fibers 2 and 5 are connected by a connection device 8 at a main connection point 10 . At this time, the bent portion 10 provided on the light-receiving side optical fiber 5 is located at a distance l from the main connection point 9. Therefore,
When the output power P 4 from the bent part 10 is measured with the optical power meter 3, the loss α in the final connection is
can be determined using equation (2) (Fig. 3d).

α=−10logP/P(dB) ……(2) 以上、図面に示した実施例にもとずいて説明し
たように、本発明に係る接続方法によれば、接続
損失を接続点において厳密に測定できるほか、接
続点の透過光パワーをモニターしながら接続装置
を操作でき、受光側光フアイバの端末において光
パワーのモニタが使用できない海底光ケーブルに
おいて有用であるばかりでなく、接続損失をモニ
ターするのに従来のように特別なデータ伝送装置
を必要としない等、きわめて作業性、経済性に優
れた接続が可能となる。
α= -10logP3P4 / P1P2 ( dB ) ...(2) As explained above based on the embodiment shown in the drawings, according to the connection method according to the present invention, the connection loss In addition to being able to precisely measure the power at the connection point, it also allows the connection device to be operated while monitoring the transmitted optical power at the connection point, which is not only useful for submarine optical cables where it is not possible to monitor the optical power at the receiving end of the optical fiber. Unlike conventional methods, a special data transmission device is not required to monitor connection loss, making it possible to perform connections with extremely high workability and economic efficiency.

最後に、曲げ部分10における出射パワーの検
出感度について、検出が最も難しいとされる単一
モード光フアイバを例にとつて説明すると、比屈
折率差0.3%、コア径10μm、動作規格化周波数
を2.4、曲げ半径を2cmとすれば、曲げ損失は
10-4dB/cmとなる。光フアイバに−5dBmの光パ
ワーを入射できるとすれば、曲がり部10におけ
る出射パワーは−51dBmである。光パワーメー
タの検出感度は−70dBmであり、十分なダイナ
ミツクレンジである。また、光源の光をチヨツパ
等で一定周波数で断続変調し、パワーメータもこ
の周波数に位相ロツクすれば、さらにダイナミツ
クレンジを拡大することができる。
Finally, to explain the detection sensitivity of the output power at the bent portion 10, using a single mode optical fiber, which is said to be the most difficult to detect, as an example, the relative refractive index difference is 0.3%, the core diameter is 10 μm, and the normalized operating frequency is 2.4.If the bending radius is 2cm, the bending loss is
10 -4 dB/cm. If an optical power of -5 dBm can be input into the optical fiber, the output power at the bent portion 10 is -51 dBm. The detection sensitivity of the optical power meter is -70 dBm, which is a sufficient dynamic range. Furthermore, if the light from the light source is modulated intermittently at a constant frequency using a chopper or the like, and the power meter is also phase-locked to this frequency, the dynamic range can be further expanded.

また、第3図a〜dで測定した光パワーP1〜P4
から式(2)を用いて接続損失を求めるためには、曲
げ部分10の形状をa〜dの工程で一定に保つ必
要がある。これについては、光フアイバを円筒に
押しつけて固定するジグを用いることによつて安
易に実現可能となる。さらに式(2)が接続損失を表
わすためには、切断長lでの光損失が零でなけれ
ばならない。一般に光フアイバの損失は0.001d
B/m以下であり、切断長lでの光損失は無視で
きる。また、曲げ部分10で曲率を大きくとるこ
とがフアイバの信頼性の点でできない場合には、
光源の波長をより長くし、動作規格化周波数を小
さくすることにより信頼性に影響を及ぼさない小
さな曲率で出射パワーを増大することができる。
In addition, the optical powers P 1 to P 4 measured in Fig. 3 a to d
In order to obtain the connection loss using equation (2), it is necessary to keep the shape of the bent portion 10 constant in steps a to d. This can be easily achieved by using a jig that presses and fixes the optical fiber against the cylinder. Furthermore, in order for Equation (2) to represent the splice loss, the optical loss at the cutting length l must be zero. Generally the loss of optical fiber is 0.001d
B/m or less, and the optical loss at the cutting length l can be ignored. In addition, if it is not possible to have a large curvature at the bent portion 10 due to the reliability of the fiber,
By making the wavelength of the light source longer and reducing the normalized operating frequency, it is possible to increase the output power with a small curvature that does not affect reliability.

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

第1図および第2図は従来における接続点の損
失を測定しつつ接続を行う接続方法の説明図、第
3図は本発明における接続点の損失を測定しつつ
接続を行なう接続方法の説明図である。 図面中、1は光源、2は光源側光フアイバ、3
は接続点測定用の光パワーメータ、4は仮接続
点、5は受光側光フアイバ、6は受光側光パワー
メータ、7はモニタ装置、8は接続装置、9は本
接続点、10は受光側光フアイバの曲げ部分であ
る。
Figures 1 and 2 are explanatory diagrams of a conventional connection method in which connections are made while measuring loss at connection points, and Figure 3 is an explanatory diagram of a connection method in the present invention in which connections are made while measuring loss at connection points. It is. In the drawing, 1 is a light source, 2 is an optical fiber on the light source side, 3
is an optical power meter for connection point measurement, 4 is a temporary connection point, 5 is an optical fiber on the light receiving side, 6 is an optical power meter on the light receiving side, 7 is a monitor device, 8 is a connection device, 9 is a main connection point, 10 is a light receiver This is the bent part of the side optical fiber.

Claims (1)

【特許請求の範囲】 1 光源を光源側光フアイバに接続して受光側光
フアイバとの接続点における前記光源側光フアイ
バからの出射光パワーP1を側定し、次いで前記接
続点において生じた放射モードのパワーがこの距
離だけ伝搬したときに導波モードのパワーに対し
て無視できる値となる距離lの2倍の距離2 l
に曲げ部分を設定した前記受光側光フアイバを前
記光源側光フアイバと仮接続するとともに前記曲
げ部分からの出射光パワーP2を測定し、さらに前
記仮接続点からlの距離で前記受光側光フアイバ
を切断してこの切断点における出射光パワーP3
測定し、最後に前記仮接続点からlの距離を有す
る前記受光側光フアイバを除去するとともに前記
切断点からlの距離に前記曲げ部分がくるように
なつた前記受光側光フアイバを前記光源側光フア
イバと接続して前記曲げ部分からの出射光パワー
P4を測定し、各工程で求められた各出射光パワー
P1〜P4で与えられる損失−10logP/P(d
B)がで きるだけ最小となるように前記両光フアイバを軸
合せ本接続することを特徴とする光フアイバの接
続方法。
[Claims] 1. Connect a light source to a light source side optical fiber, determine the output light power P 1 from the light source side optical fiber at the connection point with the light receiving side optical fiber, and then determine the output power P 1 of the light generated at the connection point. A distance 2 l that is twice the distance l at which the power of the radiation mode becomes negligible compared to the power of the guided mode when the power of the radiation mode propagates this distance.
The light-receiving side optical fiber, which has a bent portion set at , is temporarily connected to the light source-side optical fiber, the output light power P 2 from the bent portion is measured, and the light-receiving side optical fiber is connected at a distance l from the temporary connection point. Cut the fiber and measure the output light power P 3 at this cutting point.Finally, remove the light-receiving optical fiber at a distance l from the temporary connection point and insert the bent portion at a distance l from the cutting point. The optical fiber on the light receiving side, which has become curved, is connected to the optical fiber on the light source side, and the output light power from the bent portion is adjusted.
Measure P 4 and obtain each output light power in each process.
Loss given by P 1 to P 4 - 10log P 3 P 4 /P 1 P 2 (d
A method for connecting optical fibers, characterized in that the two optical fibers are aligned and connected so that B) is minimized as much as possible.
JP4470282A 1982-03-23 1982-03-23 Connecting method of optical fiber Granted JPS58162919A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4470282A JPS58162919A (en) 1982-03-23 1982-03-23 Connecting method of optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4470282A JPS58162919A (en) 1982-03-23 1982-03-23 Connecting method of optical fiber

Publications (2)

Publication Number Publication Date
JPS58162919A JPS58162919A (en) 1983-09-27
JPS6151287B2 true JPS6151287B2 (en) 1986-11-08

Family

ID=12698742

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4470282A Granted JPS58162919A (en) 1982-03-23 1982-03-23 Connecting method of optical fiber

Country Status (1)

Country Link
JP (1) JPS58162919A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04506784A (en) * 1988-10-26 1992-11-26 イノバティブ バイシクル プロダクツ インコーポレーテッド anti-theft device

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4637683A (en) * 1985-01-28 1987-01-20 Trw Inc. Method for aligning optical fiber connectors

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04506784A (en) * 1988-10-26 1992-11-26 イノバティブ バイシクル プロダクツ インコーポレーテッド anti-theft device

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JPS58162919A (en) 1983-09-27

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