JPH0362005A - Method for retrieving appropriate heating condition at connection of optical fiber - Google Patents
Method for retrieving appropriate heating condition at connection of optical fiberInfo
- Publication number
- JPH0362005A JPH0362005A JP1198753A JP19875389A JPH0362005A JP H0362005 A JPH0362005 A JP H0362005A JP 1198753 A JP1198753 A JP 1198753A JP 19875389 A JP19875389 A JP 19875389A JP H0362005 A JPH0362005 A JP H0362005A
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- discharge
- distance
- heating conditions
- face
- 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.)
- Granted
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
- G02B6/24—Coupling light guides
- G02B6/255—Splicing of light guides, e.g. by fusion or bonding
- G02B6/2551—Splicing of light guides, e.g. by fusion or bonding using thermal methods, e.g. fusion welding by arc discharge, laser beam, plasma torch
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Mechanical Coupling Of Light Guides (AREA)
- Measuring Temperature Or Quantity Of Heat (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、光ファイバ同士を相互に融着接続する場合に
おいて、光ファイバの適正加熱条件を検索する方法に関
する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method of searching for appropriate heating conditions for optical fibers when fusion splicing optical fibers to each other.
光ファイバの融着接続は、相互に接続される光ファイバ
の端部が放電加熱により溶融されて行なわれる。Fusion splicing of optical fibers is performed by melting the ends of the optical fibers to be interconnected by electrical discharge heating.
このとき、放電加熱温度が所定の適正温度範囲内にない
場合には、接続された光ファイバ相互間における接続損
失が大きくなってしまう。例えば、放電加熱温度が適正
温度範囲を超え、與常に高かった場合には、光ファイバ
の端面同士が接する前にこれに加えられる熱量により過
度の溶融を起こし、結果として、第6図に示したように
、光ファイバ1のコア2が接続部付近で変形してしまい
、接続損失が大きくなる。At this time, if the discharge heating temperature is not within a predetermined appropriate temperature range, connection loss between the connected optical fibers will increase. For example, if the discharge heating temperature exceeds the appropriate temperature range and is consistently high, the amount of heat added to the end faces of the optical fibers before they come into contact causes excessive melting, resulting in the melting of the fibers shown in Figure 6. As a result, the core 2 of the optical fiber 1 is deformed near the splicing portion, resulting in increased splicing loss.
従って、光ファイバの放電加熱温度を適正温度範囲内で
制御することが要求される。Therefore, it is required to control the discharge heating temperature of the optical fiber within an appropriate temperature range.
放電電極相互間に流れる放電電流値と放電加熱温度との
間に所定の関係があることに着目し、放電加熱温度を制
御するための目安として、この放電電流値を計測するこ
とが知られている(例えば、昭和63年電子情報通信学
会春季全国大会資料、井出貴史氏らによるB−613r
SM多心−括融着における融着条件の最適化」と題する
論文参照)。Focusing on the fact that there is a predetermined relationship between the discharge current value flowing between the discharge electrodes and the discharge heating temperature, it is known that this discharge current value is measured as a guideline for controlling the discharge heating temperature. (For example, 1986 Institute of Electronics, Information and Communication Engineers spring national conference materials, B-613r by Takashi Ide et al.
(See the paper entitled "Optimization of fusion conditions in SM multi-core-brace fusion").
しかし、放電加熱温度を制御するための目安として、放
電電極間の放電電流値を用いても、放電を繰り返すうち
に、放電電極は付着物や酸化によって劣化する。放電電
極が劣化すると、これに伴い、放電電流値が一定である
にも拘らず、放電加熱温度が上昇することが経験的に知
られている。However, even if the discharge current value between the discharge electrodes is used as a guideline for controlling the discharge heating temperature, the discharge electrodes deteriorate due to deposits and oxidation as discharge is repeated. It is empirically known that when a discharge electrode deteriorates, the discharge heating temperature increases even though the discharge current value remains constant.
このため、第7図に示したように、放電を繰り返すうち
に光ファイバの接続損失が徐々に増加することとなる。Therefore, as shown in FIG. 7, the connection loss of the optical fiber gradually increases as the discharge is repeated.
かかる事情から、放電電流を目安に放電加熱温度を制御
する場合には、放電回数の増加に伴い放電電流値を下げ
る等の調整が必要となる。ところが、このような放電電
流値の調整をするには、厳密には、電流計、パワーメー
タ等の測定機器を駆使して、放電電流値と接続損失との
関係を調べ、第8図の如きグラフを作製し、作製したグ
ラフから放電加熱温度が適正温度範囲内におさまるよう
な放電電流値を求めざるを得ない。実際に、光ファイバ
の融着接続を行なう工事現場において、このような作業
を行なうことは困難であり、また、作業時間が長くなる
という不具合があった。For this reason, when controlling the discharge heating temperature using the discharge current as a guide, it is necessary to make adjustments such as lowering the discharge current value as the number of discharges increases. However, in order to adjust the discharge current value in this way, strictly speaking, the relationship between the discharge current value and the connection loss must be investigated using measuring instruments such as an ammeter and a power meter, as shown in Figure 8. There is no choice but to create a graph and use the created graph to find a discharge current value that will keep the discharge heating temperature within the appropriate temperature range. In fact, it is difficult to perform such work at a construction site where optical fiber fusion splicing is performed, and there is also the problem that the work takes a long time.
そこで、上述の事情に鑑み、本発明は、放電加熱温度が
適正温度範囲内におさまり得る適正加熱条件を、容易に
求めることができる光ファイバ接続部の適正加熱条件検
索方法を堤供することを目的としている。Therefore, in view of the above-mentioned circumstances, an object of the present invention is to provide a method for searching for appropriate heating conditions for an optical fiber connection part, which can easily determine appropriate heating conditions under which the discharge heating temperature can be kept within an appropriate temperature range. It is said that
上述の目的を達成するため、本発明による光ファイバ接
続時の適正加熱条件検索方法においては、互いに離間し
て設けられた一対の放電電極の相互間に光ファイバの端
面を位置決めし、この光ファイバの端部を放電加熱によ
り溶融させ、溶融前後における光ファイバ端面の位置か
らその端面が溶融により後退した距離を求め、この後退
距離に基づいて、光ファイバ端部を放電加熱したときの
光ファイバの放電加熱条件が光ファイバ融着接続時の放
電加熱条件として適しているか否かが判別されるように
なっている。In order to achieve the above-mentioned object, in the method of searching for suitable heating conditions when connecting optical fibers according to the present invention, the end face of the optical fiber is positioned between a pair of discharge electrodes provided apart from each other, and the end face of the optical fiber is The end of the optical fiber is melted by electrical discharge heating, and the distance that the end face retreats due to melting is determined from the position of the optical fiber end face before and after melting. Based on this retreating distance, the distance of the optical fiber when the end of the optical fiber is heated by electrical discharge is determined. It is determined whether the discharge heating conditions are suitable as discharge heating conditions for optical fiber fusion splicing.
このようにすることによって、光ファイバ端部の溶けぐ
あいから、光ファイバの放電加熱温度が適正温度範囲に
納まり得る適正加熱条件が求められる。By doing this, appropriate heating conditions can be found that allow the discharge heating temperature of the optical fiber to fall within an appropriate temperature range from the melting of the optical fiber end.
また、放電電極間に、対をなす光ファイバ端面を相互に
対向させて位置決めし、これら光ファイバ端部の溶けぐ
あいを観察することにより、対をなす先ファイバ端部の
溶けぐあいを平均化して適正加熱条件を求めることがで
きる。In addition, by positioning the end faces of a pair of optical fibers facing each other between the discharge electrodes and observing the degree of melting at the ends of these optical fibers, the degree of melting at the ends of the pair of fibers can be averaged. Appropriate heating conditions can be determined.
以下、本発明の実施例について第1図〜第5図を参照し
つつ、説明する。Embodiments of the present invention will be described below with reference to FIGS. 1 to 5.
第1図は、本発明を実施する場合の工程を順に示してい
る。FIG. 1 sequentially shows the steps in implementing the present invention.
第1図(a)に示したように、まず、光ファイバの融着
接続装置に光ファイバ1を装着する。融着接続装置には
、互いに離間して一対の放電電極3が設けられており、
放電電極3の相互間に、先ファイバ1の端部が位置決め
される。この位置決めの後、位置決めされた光ファイバ
端面の位置(初期位置)が計7111される。この計測
は、例えば、融着接続装置に設けられた図示しない顕微
鏡、CCDカメラ、画像処理装置等からなる観察手段に
よって光ファイバ1の端部が撮像され、得られたファイ
バ像の輝度分布に基づいて画像処理が行なわれることに
よってなされる。As shown in FIG. 1(a), first, the optical fiber 1 is attached to an optical fiber fusion splicer. The fusion splicing device is provided with a pair of discharge electrodes 3 spaced apart from each other,
The end of the tip fiber 1 is positioned between the discharge electrodes 3. After this positioning, a total of 7111 positions (initial positions) of the positioned optical fiber end faces are determined. This measurement is based on the brightness distribution of the obtained fiber image, in which the end of the optical fiber 1 is imaged by an observation means (not shown) provided in the fusion splicer, such as a microscope, a CCD camera, an image processing device, etc. This is done by performing image processing.
光ファイバ1の端面の初期位置が計測された後、同図(
b)に示したように、一対の放電電極3相互間に所定時
間、放電電圧が印加され、光ファイバ1の端部が放電に
より加熱溶融される。光ファイバ1が加熱される時間は
、光ファイバ1の端部が溶融するに十分な時間が必要で
あり、かつ、光ファイバ1の端部以外に変形が生じない
ような時間であることが望ましく、例えば、0.5秒以
上5.0秒以下の範囲内から適当に選定される。After the initial position of the end face of optical fiber 1 is measured, the same figure (
As shown in b), a discharge voltage is applied between the pair of discharge electrodes 3 for a predetermined period of time, and the end of the optical fiber 1 is heated and melted by the discharge. The time during which the optical fiber 1 is heated is sufficient to melt the end of the optical fiber 1, and desirably is such a time that deformation does not occur in any part other than the end of the optical fiber 1. , for example, is appropriately selected within the range of 0.5 seconds or more and 5.0 seconds or less.
この放電加熱により、同図(c)に示したように、光フ
ァイバ1の端部は溶融し、その表面張力によって丸まり
、その端面ば後退する。そして、この後退後の光ファイ
バ1の端面位置(溶融後位置)が、溶融前の初期位置と
同様にして計測される。上述のようにして、計測された
光ファイバ1端面の初期位置と溶融後位置とに基づき、
光ファイバ1の端面が溶融して後退した距離ΔL1が求
められる。この後退距離ΔL1は、光ファイバ端部の溶
けぐあいに応じた値となり、放電加熱により光ファイバ
に与えられた熱量あるいは放電加熱温度に応じた値とな
る。それゆえ、後退距離ΔL1は、放電加熱時間が変わ
らなくても放電電流値が変化することにより変化するし
、放電電流値が変わらなくても放電電極の劣化の程度に
応じて変化する。Due to this discharge heating, the end of the optical fiber 1 is melted and curled by its surface tension, and its end face recedes, as shown in FIG. 2(c). The end face position (post-melting position) of the optical fiber 1 after this retreat is measured in the same manner as the initial position before melting. As described above, based on the measured initial position and post-melting position of the end face of the optical fiber 1,
The distance ΔL1 that the end face of the optical fiber 1 melted and retreated is determined. This retreat distance ΔL1 has a value depending on the degree of melting of the end of the optical fiber, and has a value depending on the amount of heat given to the optical fiber by discharge heating or the discharge heating temperature. Therefore, the retreat distance ΔL1 changes due to a change in the discharge current value even if the discharge heating time does not change, and changes depending on the degree of deterioration of the discharge electrode even if the discharge current value does not change.
従って、この後退距離ΔL1を計測すれば、これに払づ
いて、光ファイバの放電加熱状態を評価することができ
る。すなわち、光ファイバの融着接続を行なって、許容
し得る程度に十分に低い接続損失が得られたときと同一
の放電加熱条件で光ファイバ端部を加熱溶融し、そのと
きの後退距離ΔL1を予め求めておく。この作業を繰り
返して行ない、求められた後退距離ΔL1のうち最大の
ものをΔL 1最小のものをΔL とする。Therefore, by measuring this retreat distance ΔL1, it is possible to evaluate the electrical discharge heating state of the optical fiber based on this distance. That is, the end of the optical fiber is heated and melted under the same discharge heating conditions as when the optical fiber was fusion spliced to obtain an acceptably low splice loss, and the retreat distance ΔL1 at that time was calculated. Ask for it in advance. This operation is repeated, and among the obtained retreat distances ΔL1, the maximum one is set as ΔL1, and the minimum one is set as ΔL.
wax sin
そして、光ファイバの融着接続の前に、光ファイバ端部
を上述したようにして溶融し、光ファイバ端面の後退距
離ΔL1を求め、この後退距離ΔL1が予め求められて
いる適正範囲内(ΔL1□以上ΔL 以下)に納まる
ように、放電電流値ax
が相対的に調整される。例えば、ここで求められた後退
距離ΔL が、ΔL より小さい場合にl
ain
は、熱量不足の場合であるので、放電電流値を高くし、
逆に、後退距離ΔL が、ΔL より大l
wax
きい場合には、熱量過多の場合であるので、放電電流値
を低くする。このようにして、後退距離ΔL が適正範
囲内(ΔL 0以上ΔL 以下)1
1111+
1aXに納まるように放電電流値が相対的に調整される
。wax sin Then, before fusion splicing the optical fiber, the end of the optical fiber is melted as described above, the retraction distance ΔL1 of the optical fiber end face is determined, and this retraction distance ΔL1 is within a predetermined appropriate range. The discharge current value ax is relatively adjusted so as to fall within the range (∆L1□ to ∆L). For example, if the retreat distance ΔL found here is smaller than ΔL, then l
ain is a case of insufficient heat, so the discharge current value is increased,
Conversely, if the retreat distance ΔL is greater than ΔL
When wax is too high, the amount of heat is excessive, so the discharge current value is lowered. In this way, the retreat distance ΔL is within the appropriate range (ΔL 0 or more and ΔL or less)1
1111+
The discharge current value is relatively adjusted so as to fall within 1aX.
ΔL 、及びΔL は、次のようにして求め+111
n IuaXられる。まず、光
ファイバ端部を加熱溶融してΔL を求める。そして、
この後退距離ΔL1が得られたときの光ファイバの放電
加熱条件を固定し、これと同一の放電加熱条件下(加熱
0開は具なっていてもよい)で、先ファイバ同士のFi
A着接続を行ない、その接続部の接続損失を計alll
する。この後退距離ΔL1と接続損失の計測を、放電電
流値を変えて繰り返し行ない、後退距離ΔL1と接続損
失との関係を、第2図に示したグラフとして予め求めて
おく。そして、このグラフから接続損失が許容できる程
度に十分に低くなる範囲の後退距離ΔL を求め、求め
られた後退距離ΔL1のうち、最大の後退距離をΔL
とし、最少のものIuaX
をΔL 、 とする。なお、ΔL 及びΔL1n巾+
n
maxは、融着接続装置のCPU、ROM、RAM等
からなる中央制御部に記憶される。これにより、光ファ
イバの融着接続前に求められた後退距離ΔL が、ΔL
、より小さい場合には、「放電1 m+n
弱い」と融着接続装置の表示部に表示し、後退距離ΔL
がΔL より大きい場合には、「放電l
max
強い」と表示し、後退距離ΔL1が適正範囲内(ΔL
以上ΔL 以下)に納まっている場l1in
aax
合には、「放電OKJと表示することができるようにな
っている。ΔL and ΔL are calculated as follows +111
n IuaX. First, the end of the optical fiber is heated and melted to determine ΔL. and,
The discharge heating conditions of the optical fiber when this retraction distance ΔL1 is obtained are fixed, and under the same discharge heating conditions (heating 0 open may be present), the Fi
Make the A connection and calculate the connection loss at that connection.
do. The measurement of the retraction distance ΔL1 and the connection loss is repeated by changing the discharge current value, and the relationship between the retraction distance ΔL1 and the connection loss is determined in advance as a graph shown in FIG. 2. Then, from this graph, find the retraction distance ΔL in a range where the connection loss is sufficiently low to an allowable extent, and set the maximum retraction distance ΔL among the calculated retraction distances ΔL1.
Let the smallest IuaX be ΔL. In addition, ΔL and ΔL1n width +
n
max is stored in the central control unit of the fusion splicer, which includes the CPU, ROM, RAM, and the like. As a result, the retreat distance ΔL determined before fusion splicing of the optical fiber is changed to ΔL
, the display of the fusion splicing device will display "discharge 1 m+n weak" and the retreat distance ΔL will be displayed.
is larger than ΔL, “discharge l
max strong” is displayed, and the retreat distance ΔL1 is within the appropriate range (ΔL
(more than ∆L or less), l1in
In case of aax, "Discharge OKJ" can be displayed.
なお、上述の実施例においては、一対の放電電極3に対
して一方の側に、光ファイバ1の端部が位置決めされ、
この光ファイバ端面の後退距離から放電加熱状態の適否
を判断しているが、第3図に示したように、一対の族7
Ii電極3に対して両側に、対をなす光ファイバ1の端
部を互いに向かい合わせて放電電極3相互間に位置決め
し、放電加熱を行なって、これらの後退距離に基づいて
放電加熱状態の適否を判断することもできる。この場合
には、光ファイバの端部が放電電極3から離れ過ぎない
ように、対をなす先ファイバの端面相互間隔は100μ
In以下とされ、放電加熱前における一対の光ファイバ
端面の相互間隔(初期間隔)Loが計7IP+される(
第3図(a))と共に、放電加熱後の間隔(溶融後間隔
)Ltが計測され(第3図(b))、計31された初期
間隔と溶融後間隔とに址づき、対をなす光ファイバの端
面がそれぞれ後退した距離の和としてΔL(−L −
Lo)が求められる。In the above embodiment, the end of the optical fiber 1 is positioned on one side with respect to the pair of discharge electrodes 3,
The suitability of the discharge heating state is judged from the retreat distance of the optical fiber end face.As shown in Fig. 3, a pair of group 7
The ends of the paired optical fibers 1 are positioned between the discharge electrodes 3 on both sides with respect to the electrode 3, facing each other, and discharge heating is performed, and the suitability of the discharge heating state is determined based on the retreat distance. It is also possible to judge. In this case, in order to prevent the end of the optical fiber from being too far away from the discharge electrode 3, the distance between the end faces of the pair of fibers is 100 μm.
In, the mutual distance (initial distance) Lo between the end faces of the pair of optical fibers before discharge heating is increased by 7 IP + (
Along with Fig. 3(a)), the interval after discharge heating (interval after melting) Lt is measured (Fig. 3(b)), and the initial interval and the interval after melting are 31 in total, forming a pair. ΔL(-L −
Lo) is required.
そして、この後退距離の和ΔLと接続損失との関係につ
いて、第2図に示したグラフと同様のグラフを作製し、
接続損失が許容し得る範囲となる後辺距離の和ΔLの範
囲(ΔL 以上ΔLffiaxin
以下)を求め、この範囲内に、後退距離の和ΔLが納ま
るように放電電流値を相対的に調整することによって、
放電電流値を求めずとも、接続損失の低い適正な放電加
熱条件が求められる。Then, a graph similar to the graph shown in FIG. 2 was created for the relationship between the sum of the retreat distances ΔL and the connection loss,
Find the range of the sum ΔL of the trailing distances within which the connection loss is allowable (ΔL or more and ΔLffiaxin or less), and relatively adjust the discharge current value so that the sum ΔL of the retreat distances falls within this range. By,
Appropriate discharge heating conditions with low connection loss can be determined without determining the discharge current value.
ところで、放電電極3に対して一方の側に、光ファイバ
1の端部を位置決めする場合には、放電電流値等の放電
加熱条件が変らなくとも、一対の放電電極3の先端を相
互に結ぶ仮想線から光ファイバ1の端面位置までの距離
(位置決め位置)が変ると、光ファイバ端部の溶けぐあ
いが変化する。By the way, when positioning the end of the optical fiber 1 on one side with respect to the discharge electrode 3, even if the discharge heating conditions such as the discharge current value do not change, the tips of the pair of discharge electrodes 3 are connected to each other. When the distance (positioning position) from the virtual line to the end face position of the optical fiber 1 changes, the degree of welding of the end of the optical fiber changes.
従って、この距離が一定となるように正確に位置決めす
る必要がある。もし、正確な位置決めができない場合に
は、適正加熱条件の検索精度が低下する。また、放電電
極3の劣化によって放電火花が飛ぶ位置が変ることもあ
り、放電電極3の劣化に伴い、適正加熱条件の検索精度
が低下することがある。これに対し、対をなす先ファイ
バ端部を放電電極3の両側に位置決めした場合には、放
電電極3に対する先ファイバ1の相対的な位置決め精度
が、光ファイバ1を放電電極3の一方側に位置決めする
場合に比べ低くても、対をなす光ファイバの端面相互の
相対的位置決めが正確になされていれば、対をなす光フ
ァイバ端部の溶けぐあい双方が考慮されるので、対をな
す光ファイバ端部の溶けぐあいを平均化したと同様とな
り、検索精度の低下を抑制できる。なお、対をなす光フ
ァイバ端面相互間の相対的位置決めは、CCDカメラに
よりその双方を認識できるので、高い精度で位置決めが
可能である。Therefore, it is necessary to position accurately so that this distance is constant. If accurate positioning is not possible, the accuracy of searching for appropriate heating conditions will be reduced. Furthermore, the position of discharge sparks may change due to deterioration of the discharge electrode 3, and the accuracy of searching for appropriate heating conditions may decrease as the discharge electrode 3 deteriorates. On the other hand, when the ends of the tip fibers forming a pair are positioned on both sides of the discharge electrode 3, the relative positioning accuracy of the tip fiber 1 with respect to the discharge electrode 3 is such that the optical fiber 1 is positioned on one side of the discharge electrode 3. Even if it is lower than when positioning, as long as the relative positioning of the end faces of the paired optical fibers is done accurately, the melting of the paired optical fiber ends is taken into account, so the pair of light This is similar to averaging the welds at the fiber ends, and it is possible to suppress a decrease in search accuracy. Note that relative positioning between the pair of optical fiber end faces can be performed with high accuracy because both can be recognized by a CCD camera.
第4図に、対をなす光ファイバの端部を、その端面相互
間が10μmとなるように位置決めし、放電電流値を一
定とし、放電時間を3.0秒として、先ファイバ端部を
放電加熱した場合における放電回数と端面間隔の広がり
(後退距離の和ΔL)との関係をグラフとして示す。こ
のグラフから、放電電流値が一定となっていても、放電
回数が増加するにつれ、後退距離の和ΔLが増加し、放
電回数が所定回数n。を越えた場合に、ΔLが接続損失
の許容し得る適正範囲(ΔL 0以上11n
ΔL 以下)を越えることが判明した。放電量ax
数が所定回数n。を越えた場合の接続損失とその発生度
数との関係を第5図に示す。同図(a)は放電電流値i
を一定(i−io)としたまま融着接続を行なった場合
を示し、同図(b)はΔLが適正範囲(ΔL 以上Δ
L 以下)内に納まl1in a+
ax
るように放電電流値iを11に下げて融着接続を行なっ
た場合を示している。この結果からも明らかなように、
ΔLが適正範囲内に納まるように放電電流fUiを;X
J整することによって、良好な接続時性が得られた。In Figure 4, the ends of a pair of optical fibers are positioned so that the distance between their end faces is 10 μm, the discharge current value is constant, the discharge time is 3.0 seconds, and the end of the first fiber is discharged. The relationship between the number of discharges and the spread of the end face spacing (sum of retreat distances ΔL) in the case of heating is shown as a graph. From this graph, even if the discharge current value is constant, as the number of discharges increases, the sum of retreat distances ΔL increases, and the number of discharges reaches the predetermined number n. It has been found that ΔL exceeds the allowable appropriate range of connection loss (ΔL 0 or more and 11n ΔL or less) when the value exceeds ΔL. The discharge amount ax is a predetermined number of times n. FIG. 5 shows the relationship between the connection loss and the frequency of occurrence when the connection loss exceeds . Figure (a) shows the discharge current value i
This figure shows the case where fusion splicing is performed while keeping constant (i-io), and in the same figure (b), ΔL is within the appropriate range (ΔL or more Δ
(L or less) 1in a+
This shows the case where the discharge current value i was lowered to 11 so that fusion splicing was performed. As is clear from this result,
Adjust the discharge current fUi so that ΔL falls within the appropriate range;
By adjusting J, good connection performance was obtained.
以上説明したように、本発明による光ファイバ接続時の
適1E加熱条件検索方法によれは、光ファイバ端部の溶
けぐあいに基づいて、放電電流を…対向に調整すること
などにより、光ファイバの適正加熱条件を容易に求める
ことができる。従ってN放電電流値を求める必要もない
し放電電極の劣化を考慮する必要もないので、野外等で
の先ファイバの接続作業においても容易に適正加熱条件
が求められる。殊に、標高が高い地域における光ファイ
バの融着接続作業では、気圧の低下に1↑う放電電極相
互間の電気抵抗の低下により、放電加熱温度が低下する
が、この場合にも、容易に適正加熱条件を求めることが
できる。As explained above, according to the method of searching for suitable 1E heating conditions when connecting optical fibers according to the present invention, it is possible to find the appropriate heating conditions for optical fibers by adjusting the discharge current in the opposite direction based on the melting condition of the optical fiber end. Heating conditions can be easily determined. Therefore, since there is no need to determine the N discharge current value or to take into account the deterioration of the discharge electrode, appropriate heating conditions can be easily determined even when connecting fibers in the field. Particularly in optical fiber fusion splicing work in high altitude areas, the electrical resistance between the discharge electrodes decreases due to the decrease in atmospheric pressure, which causes the discharge heating temperature to decrease. Appropriate heating conditions can be found.
また、光ファイバの溶けぐあいから、適正加熱条件を求
めているので、作業対象たる先ファイバの種類が変って
、その溶融温度が変った場合にも、先ファイバの適正加
熱条件を容易に求めることができる。In addition, since the appropriate heating conditions are determined based on the melting state of the optical fiber, even if the type of target fiber to be worked on changes and its melting temperature changes, the appropriate heating conditions for the target fiber can be easily determined. I can do it.
更に、放電電極間に、!I4をなす光ファイバ端面を相
互に対向させて位置決めし、これら光ファイバ端部の溶
けぐあいを観察することにより、対をなす先ファイバ端
部の溶けぐあいを平均化したと同様となり、先ファイバ
の位置決め誤差による適正加熱条件の検索誤差が抑制さ
れる。Furthermore, between the discharge electrodes! By positioning the end faces of the optical fibers forming I4 so as to face each other and observing the degree of welding of these optical fiber ends, the result is the same as that of averaging the degree of welding of the ends of the pair of tip fibers. Errors in searching for appropriate heating conditions due to positioning errors are suppressed.
第1図は本発明の実施例を示した図、第2図は後退距離
と接続損失の関係を示したグラフ、第3図は第1図に示
した実施例と異なる本発明の実施例を示した図、第4図
は放電回数と後追距離の和との関係を示したグラフ、第
5図は接続損失の分布を示したグラフ、第6図は光ファ
イバの接続不良例を示した図、第7図は放電回数と接続
損失の関係を示したグラフ、第8図は放電電流と接続損
失の関係を示したグラフである。
1・・・光ファイバ、2・・・コア、3・・・放電電極
。Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 is a graph showing the relationship between retreat distance and connection loss, and Fig. 3 is a diagram showing an embodiment of the present invention different from the embodiment shown in Fig. 1. Figure 4 is a graph showing the relationship between the number of discharges and the sum of trailing distances, Figure 5 is a graph showing the distribution of connection loss, and Figure 6 is an example of an optical fiber connection failure. 7 is a graph showing the relationship between the number of discharges and connection loss, and FIG. 8 is a graph showing the relationship between discharge current and connection loss. 1... Optical fiber, 2... Core, 3... Discharge electrode.
Claims (1)
に光ファイバの端面が位置決めされ、位置決めされた光
ファイバ端面の初期位置が計測される工程と、 前記一対の放電電極相互間に放電電圧が印加され、前記
光ファイバの端部が加熱溶融される加熱工程と、 前記光ファイバ端面の溶融後位置が計測される工程と、 前記初期位置及び前記溶融後位置に基づき、前記光ファ
イバ端面が前記初期位置から後退した距離が求められ、
この後退距離に基づき、前記加熱工程における光ファイ
バの放電加熱条件が光ファイバ融着接続時の放電加熱条
件として適しているか否かが判別される工程とを備えて
いることを特徴とする光ファイバ接続時の適正加熱条件
検索方法。 2、互いに離間して設けられた一対の放電電極の相互間
に、対をなす光ファイバの端面が互いに対向して位置決
めされ、位置決めされた光ファイバ端面相互間の初期間
隔が計測される工程と、前記一対の放電電極相互間に放
電電圧が印加され、前記光ファイバの端部が加熱溶融さ
れる加熱工程と、 前記光ファイバ端面相互間の溶融後間隔が計測される工
程と、 前記初期間隔及び前記溶融後間隔に基づき、前記光ファ
イバ端面がそれぞれ溶融して後退した距離の和が求めら
れ、この後退距離の和に基づき、前記加熱工程における
光ファイバの放電加熱条件が光ファイバ融着接続時の放
電加熱条件として適しているか否かを判別する工程とを
備えていることを特徴とする光ファイバ接続時の適正加
熱条件検索方法。[Claims] 1. A step of positioning an end face of an optical fiber between a pair of discharge electrodes provided apart from each other, and measuring an initial position of the positioned end face of the optical fiber; a heating step in which a discharge voltage is applied between the discharge electrodes and the end of the optical fiber is heated and melted; a step in which the position of the end face of the optical fiber after melting is measured; Based on this, the distance that the optical fiber end face has retreated from the initial position is determined,
and a step of determining whether or not the discharge heating conditions for the optical fiber in the heating step are suitable as the discharge heating conditions for optical fiber fusion splicing based on the retreat distance. How to search for appropriate heating conditions when connecting. 2. The step of positioning the end faces of the pair of optical fibers facing each other between a pair of discharge electrodes provided apart from each other, and measuring the initial distance between the positioned end faces of the optical fibers. , a heating step in which a discharge voltage is applied between the pair of discharge electrodes and the end portions of the optical fiber are heated and melted; a step in which a distance between the end surfaces of the optical fibers after melting is measured; and the initial distance. Based on the post-melting interval, the sum of the distances that the optical fiber end faces have melted and retreated is calculated, and based on the sum of the retreat distances, the discharge heating conditions for the optical fiber in the heating step are determined to be suitable for optical fiber fusion splicing. 1. A method for searching for appropriate heating conditions for optical fiber connection, the method comprising the step of determining whether or not the conditions are suitable as discharge heating conditions for an optical fiber connection.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1198753A JP2786682B2 (en) | 1989-07-31 | 1989-07-31 | How to search for proper heating conditions when connecting optical fibers |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1198753A JP2786682B2 (en) | 1989-07-31 | 1989-07-31 | How to search for proper heating conditions when connecting optical fibers |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0362005A true JPH0362005A (en) | 1991-03-18 |
| JP2786682B2 JP2786682B2 (en) | 1998-08-13 |
Family
ID=16396390
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1198753A Expired - Lifetime JP2786682B2 (en) | 1989-07-31 | 1989-07-31 | How to search for proper heating conditions when connecting optical fibers |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2786682B2 (en) |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01169331A (en) * | 1987-12-16 | 1989-07-04 | Fujikura Ltd | Method for measuring optical fiber heating |
-
1989
- 1989-07-31 JP JP1198753A patent/JP2786682B2/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01169331A (en) * | 1987-12-16 | 1989-07-04 | Fujikura Ltd | Method for measuring optical fiber heating |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2786682B2 (en) | 1998-08-13 |
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