JPH02248835A - Measurement of eccentricity of core for optical fiber base material - Google Patents
Measurement of eccentricity of core for optical fiber base materialInfo
- Publication number
- JPH02248835A JPH02248835A JP7105989A JP7105989A JPH02248835A JP H02248835 A JPH02248835 A JP H02248835A JP 7105989 A JP7105989 A JP 7105989A JP 7105989 A JP7105989 A JP 7105989A JP H02248835 A JPH02248835 A JP H02248835A
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- eccentricity
- core
- base material
- directions
- 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.)
- Pending
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 46
- 239000000463 material Substances 0.000 title claims abstract description 13
- 238000005259 measurement Methods 0.000 title abstract description 9
- 238000009826 distribution Methods 0.000 claims abstract description 14
- 238000005253 cladding Methods 0.000 claims description 13
- 238000000691 measurement method Methods 0.000 claims description 2
- 238000004519 manufacturing process Methods 0.000 abstract description 8
- 238000000034 method Methods 0.000 description 4
- 230000003287 optical effect Effects 0.000 description 2
- 230000002950 deficient Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000009987 spinning Methods 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B37/00—Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
- C03B37/01—Manufacture of glass fibres or filaments
- C03B37/012—Manufacture of preforms for drawing fibres or filaments
- C03B37/01205—Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
- C03B37/01225—Means for changing or stabilising the shape, e.g. diameter, of tubes or rods in general, e.g. collapsing
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B37/00—Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
- C03B37/01—Manufacture of glass fibres or filaments
- C03B37/012—Manufacture of preforms for drawing fibres or filaments
- C03B37/01205—Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Geochemistry & Mineralogy (AREA)
- Manufacturing & Machinery (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Manufacture, Treatment Of Glass Fibers (AREA)
Abstract
Description
この発明は、光ファイバのコアの偏心量を、焼結され透
明ガラス化された光ファイバ母材の段階で測定する方法
に関する。The present invention relates to a method for measuring the eccentricity of an optical fiber core at the stage of an optical fiber preform that has been sintered and made into transparent glass.
従来では、光ファイバのコアの偏心量は、光ファイバ母
材を線引して紡糸することによって光ファイバ素線とし
て出来上がったものの端面を観察して測定するのが通常
である。すなわち、光ファイバの端面においてコアの中
心とクラッドの中心とのずれ量を測定し、このずれ量を
コア偏心量としている。Conventionally, the amount of eccentricity of the core of an optical fiber is usually measured by observing the end face of an optical fiber produced by drawing and spinning an optical fiber preform. That is, the amount of deviation between the center of the core and the center of the cladding at the end face of the optical fiber is measured, and this amount of deviation is taken as the amount of core eccentricity.
しかしながら、従来のコア偏心量測定法では、光ファイ
バ素線の状態で測定するため測定精度に欠け、また光フ
ァイバ母材製造工程へのフィードバックも遅いという問
題がある。すなわち、直径的125μmの光ファイバ素
線端面を観察するため、高精度の測定器が必要である等
のさまざまな制約が課せられ、しかも高い測定精度を得
ることが難しい。さらに、光ファイバのコアの偏心の原
因の多くは光ファイバ母材製造工程によるものであるが
、光ファイバ素線の段階で測定するのでは、光ファイバ
母材を線引し光ファイバ素線とした後測定することにな
るため、光ファイバ母材製造工程へのフィードバックが
遅れることになる。
この発明は、コア偏心量を高い精度で容易に測定するこ
とができるとともに、光ファイバ母材製造工程へのフィ
ードバックも早めることができる、光ファイバ母材のコ
ア偏心量測定法を提供することを目的とする。However, the conventional core eccentricity measurement method lacks measurement accuracy because it measures the optical fiber in its strand state, and the feedback to the optical fiber preform manufacturing process is also slow. That is, in order to observe the end face of an optical fiber having a diameter of 125 μm, various restrictions are imposed, such as the need for a high-precision measuring instrument, and it is difficult to obtain high measurement accuracy. Furthermore, most of the causes of eccentricity in the core of optical fibers are due to the manufacturing process of the optical fiber base material, but measuring it at the optical fiber stage requires drawing the optical fiber base material and forming it into a raw optical fiber. Since the measurement must be carried out after the measurement, feedback to the optical fiber preform manufacturing process will be delayed. The present invention aims to provide a method for measuring the amount of core eccentricity of an optical fiber preform, which can easily measure the amount of core eccentricity with high accuracy, and can also speed up feedback to the optical fiber preform manufacturing process. purpose.
上記目的を達成するため、この発明による光ファイバ母
材のコア偏心量測定法においては、まず、光ファイバ母
材の中心軸にほぼ直角な平面上の互いに異なる3方向よ
り該母材の屈折角分布を測定し、つぎに、これら3方向
の屈折角分布よりそれぞれコア部の中心点とクラッド部
の中心点との間の距離を求め、さらに、これら3方向の
角度と距離とからサインカーブを近似し、該サインカー
ブの振幅を算出することを特徴とする。In order to achieve the above object, in the method for measuring the core eccentricity of an optical fiber preform according to the present invention, first, the refraction angle of the preform is measured from three different directions on a plane substantially perpendicular to the central axis of the optical fiber preform. The distribution is measured, and then the distance between the center point of the core and the center of the cladding is determined from the refraction angle distribution in these three directions.Furthermore, a sine curve is calculated from the angle and distance in these three directions. It is characterized by approximating and calculating the amplitude of the sine curve.
光ファイバ母材を、その中心軸を回転中心軸として回転
させ、その側方の一定方向から観察すると、コア部が偏
心している場合は、このコア部の中心点は回転角度に対
してサインカーブを描く。
そして、このサインカーブの振幅がコア部の偏心量に対
応することになる。
そして、光ファイバ母材を線引することによって光ファ
イバが得られるため、光ファイバ母材の断面形状は光フ
ァイバの断面形状と相似であると見なせる。そのため、
光ファイバ母材の段階で求めたコア部の偏心量は光ファ
イバのコアの偏心量ということができる。
そこで、光ファイバ母材の側方から、つまり光ファイバ
母材の中心軸にほぼ直角な平面上の適当な1つの方向か
ら屈折角の分布を測定する。この屈折角の分布より、コ
ア部の中心点とクラッド部の中心点とをそれぞれ求める
ことができ、それらの間の距離を求めることができる。
この距離を、上記の平面上の、上記の方向とは異なる2
方向より求める。
すると、これら3方向の角度と距離により表わされる点
は、サインカーブの上にのることになるので、これら3
方向の角度と距離とからサインカーブを近似することが
できる。このようにしてサインカーブが求められれば、
上記のようにその振幅からコア部の偏心量を求めること
ができる。When an optical fiber base material is rotated around its central axis and observed from a certain direction on the side, if the core is eccentric, the center point of this core will be a sine curve with respect to the rotation angle. draw The amplitude of this sine curve corresponds to the amount of eccentricity of the core portion. Since the optical fiber is obtained by drawing the optical fiber preform, the cross-sectional shape of the optical fiber preform can be considered to be similar to the cross-sectional shape of the optical fiber. Therefore,
The amount of eccentricity of the core portion determined at the optical fiber preform stage can be said to be the amount of eccentricity of the core of the optical fiber. Therefore, the distribution of the refraction angle is measured from the side of the optical fiber preform, that is, from one suitable direction on a plane substantially perpendicular to the central axis of the optical fiber preform. From this distribution of refraction angles, the center point of the core portion and the center point of the cladding portion can be determined, and the distance therebetween can be determined. Set this distance to two points on the above plane that are different from the above direction.
Determine from the direction. Then, the points represented by the angles and distances in these three directions will be on the sine curve, so these three
A sine curve can be approximated from the direction angle and distance. If the sine curve is found in this way,
As described above, the amount of eccentricity of the core portion can be determined from the amplitude.
つぎにこの発明の一実施例について図面を参照しながら
説明する。まず、プリフォームアナライザなどの光ファ
イバ母材の光学的性質を調べる測定器を用いて、光ファ
イバ母材の側方、つまり光ファイバ母材の中心軸にほぼ
直角な平面上の適当な1つの方向から屈折角分布を測定
する。すると、この屈折角分布は第3図Bのようになり
、第3図Aに示す光ファイバ母材1の断面形状に対応す
ることになる。すなわち、屈折角分布上のP、8点はク
ラッド部3のエツジ付近に、Q、R点はコア部2とクラ
ッド部との境界にそれぞれ対応する。
そして、このP、8点の中点はクラッド部3の中心点、
Q、R点の中点はコア部2の中心点となるため、これら
の中点よりコア部2とクラッド部3のそれぞれの中心点
を求めることができる。このようにしてそれぞれの中心
点が求められれば、それらの間の距離りも求められる。
このような屈折角分布を、光コアイノく母材1をクラッ
ド部3の中心軸を回転中心軸として回転させて、クラッ
ド部3の中心軸にほぼ直角な平面上の3方向、この実施
例ではO’ 、90°、180°の各方向から測定する
。これにより、第1図A。
B、Cに示すように3方向でのコア部2の中心点とクラ
ッド部3の中心点との距離La、Lb、LCを求める。
つぎにこの距離La、Lb、Lcとそれを取得した角度
とで表わされる3点のデータを用いて、第2図のように
サインカーブを近似する。このようにサインカーブが近
似できたら、そのサインカーブの振幅Lmを算出する。
すると、この振幅Lmはクラッド部3の中心軸に対する
コア部2の中心軸の偏心量に対応することになる。
なお、3つの異なる角度でのコア部2の中心点とクラッ
ド部3の中心点との距離りが求められれば、第2図に示
すように1つのサインカーブを近・似することができる
ため、屈折角分布を求める方向は上記のように0°、9
0° 180°に限定されず、任意に選ぶことができ
る。Next, an embodiment of the present invention will be described with reference to the drawings. First, using a measuring instrument such as a preform analyzer to examine the optical properties of the optical fiber preform, measure one suitable point on the side of the optical fiber preform, that is, on a plane approximately perpendicular to the central axis of the optical fiber preform. Measure the refraction angle distribution from the direction. Then, this refraction angle distribution becomes as shown in FIG. 3B, which corresponds to the cross-sectional shape of the optical fiber preform 1 shown in FIG. 3A. That is, points P and 8 on the refraction angle distribution correspond to the vicinity of the edge of the cladding portion 3, and points Q and R correspond to the boundary between the core portion 2 and the cladding portion, respectively. Then, the middle point of this P, 8 points is the center point of the cladding part 3,
Since the midpoint between points Q and R becomes the center point of the core portion 2, the respective center points of the core portion 2 and the cladding portion 3 can be determined from these midpoints. If each center point is found in this way, the distance between them can also be found. Such a refraction angle distribution can be obtained by rotating the optical core base material 1 about the central axis of the cladding part 3, in three directions on a plane substantially perpendicular to the central axis of the cladding part 3, in this embodiment. Measurements are taken from the O', 90°, and 180° directions. As a result, FIG. 1A. As shown in B and C, the distances La, Lb, and LC between the center point of the core portion 2 and the center point of the cladding portion 3 in three directions are determined. Next, a sine curve is approximated as shown in FIG. 2 using data at three points represented by the distances La, Lb, and Lc and the angles at which they were obtained. Once the sine curve has been approximated in this way, the amplitude Lm of the sine curve is calculated. Then, this amplitude Lm corresponds to the amount of eccentricity of the central axis of the core section 2 with respect to the central axis of the cladding section 3. Furthermore, if the distances between the center point of the core portion 2 and the center point of the cladding portion 3 at three different angles are determined, one sine curve can be approximated as shown in Figure 2. , the directions for calculating the refraction angle distribution are 0° and 9 as described above.
It is not limited to 0° to 180° and can be arbitrarily selected.
この発明の光ファイバ母材のコア偏心量測定法によれば
、大きな光ファイバ母材の段階でコア偏心量の測定が可
能になったため、測定精度を向上させることが容易であ
る。また、光ファイバ母材の段階で測定できるため、光
ファイバ母材製造工程へのフィードバックも早くするこ
とができ、母材段階で良品選別等が可能となる。According to the method for measuring the amount of core eccentricity of an optical fiber preform of the present invention, it is possible to measure the amount of core eccentricity at the stage of a large optical fiber preform, so it is easy to improve the measurement accuracy. Furthermore, since measurement can be performed at the optical fiber preform stage, feedback to the optical fiber preform manufacturing process can be made faster, and non-defective products can be selected at the preform stage.
第1図A、B、C1第2図、第3図A、Bはすべてこの
発明の一実施例にかかるもので、第1図A、B、Cは光
ファイバ母材の側方の3方向がら見たコア部中心とクラ
ッド部中心との距離を示す図、第2図は近似されるサイ
ンカーブを示す図、第3図A、Bは光ファイバ母材断面
とそれに対応する屈折角分布とをそれぞれ示す図である
。
1・・・光ファイバ母材、2・・・コア部、3・・・ク
ラッド部。Figure 1 A, B, C1 Figure 2, Figure 3 A, B all relate to one embodiment of the present invention, Figure 1 A, B, C shows the three lateral directions of the optical fiber preform. Figure 2 is a diagram showing the approximated sine curve, and Figures 3A and B are the cross-sections of the optical fiber base material and the corresponding refraction angle distribution. FIG. DESCRIPTION OF SYMBOLS 1... Optical fiber base material, 2... Core part, 3... Clad part.
Claims (1)
いに異なる3方向より該母材の屈折角分布を測定し、つ
ぎに、これら3方向の屈折角分布よりそれぞれコア部の
中心点とクラッド部の中心点との間の距離を求め、さら
に、これら3方向の角度と距離とからサインカーブを近
似し、該サインカーブの振幅を算出することを特徴とす
る光ファイバ母材のコア偏心量測定法。(1) Measure the refraction angle distribution of the optical fiber base material from three different directions on a plane substantially perpendicular to the central axis of the optical fiber base material, and then measure the refraction angle distribution of the optical fiber base material from each of the three directions at the center of the core. and the center point of the cladding part, and further approximates a sine curve from the angles and distances in these three directions, and calculates the amplitude of the sine curve. Eccentricity measurement method.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7105989A JPH02248835A (en) | 1989-03-23 | 1989-03-23 | Measurement of eccentricity of core for optical fiber base material |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7105989A JPH02248835A (en) | 1989-03-23 | 1989-03-23 | Measurement of eccentricity of core for optical fiber base material |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02248835A true JPH02248835A (en) | 1990-10-04 |
Family
ID=13449572
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7105989A Pending JPH02248835A (en) | 1989-03-23 | 1989-03-23 | Measurement of eccentricity of core for optical fiber base material |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02248835A (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6366435A (en) * | 1986-09-09 | 1988-03-25 | Sumitomo Electric Ind Ltd | Structure measuring apparatus |
-
1989
- 1989-03-23 JP JP7105989A patent/JPH02248835A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6366435A (en) * | 1986-09-09 | 1988-03-25 | Sumitomo Electric Ind Ltd | Structure measuring apparatus |
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