JPS60253837A - Optical fiber analyzer - Google Patents
Optical fiber analyzerInfo
- Publication number
- JPS60253837A JPS60253837A JP10990284A JP10990284A JPS60253837A JP S60253837 A JPS60253837 A JP S60253837A JP 10990284 A JP10990284 A JP 10990284A JP 10990284 A JP10990284 A JP 10990284A JP S60253837 A JPS60253837 A JP S60253837A
- Authority
- JP
- Japan
- Prior art keywords
- point
- points
- optical fiber
- indication
- displayed
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
- G01M11/3109—Reflectometers detecting the back-scattered light in the time-domain, e.g. OTDR
- G01M11/3145—Details of the optoelectronics or data analysis
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- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
(?L)発明の技術分野
この発明は、複数の接続点を含む光ファイバかフィバの
減衰特性を測定するようにした光フアイバアナライザに
おいて、各接続点の接続損失に起因する段差を明確に表
示することにより、光ファイバの単位長損失や全区間の
接続損失などを同時に算出できるようにするものである
。Detailed Description of the Invention (?L) Technical Field of the Invention The present invention provides an optical fiber analyzer for measuring the attenuation characteristics of an optical fiber or fibers including a plurality of connection points. By clearly displaying the resulting step difference, it is possible to simultaneously calculate the unit length loss of the optical fiber, the splice loss of the entire section, etc.
(b) 従来技術と問題点 最初に、従来装置の構成図を第1図に示す。(b) Conventional technology and problems First, a configuration diagram of a conventional device is shown in FIG.
第1図の1は光源、2は方向性結合器、3は測定される
光ファイバ、4は検出器、5はCRTである。In FIG. 1, 1 is a light source, 2 is a directional coupler, 3 is an optical fiber to be measured, 4 is a detector, and 5 is a CRT.
第1図の光源1は方向性結合器2を経由して測定光を光
ファイバ3に入射する。光フフイバ3による測定光の反
射波は方向性結合器2を経由して検出器4に入射する6
ei出器4で電気信号に変換された反射波は、CRT5
に表示される。A light source 1 shown in FIG. 1 inputs measurement light into an optical fiber 3 via a directional coupler 2. The reflected wave of the measurement light from the optical fiber 3 enters the detector 4 via the directional coupler 2 6
The reflected wave converted into an electric signal by the ei output device 4 is sent to the CRT 5.
will be displayed.
次に、第1図のCRT、5に表示される反射波形の一例
を第2図に示す。Next, FIG. 2 shows an example of the reflected waveform displayed on the CRT 5 of FIG. 1.
第2図の波形CIの左側が光ファイバ3の入射端31例
の状態を示し、右側に進むにつれて光フいる。The left side of the waveform CI in FIG. 2 shows the state of an example of the input end 31 of the optical fiber 3, and as it moves to the right side, the light beam decreases.
波形CIす右下りになっており、右側にいくにつれて反
射波形か減衰することを示している。The waveform CI slopes downward to the right, indicating that the reflected waveform attenuates as it goes to the right.
波形CIの点C目、点CI2では段差か生じているが、
これらの段差は光ファイバ3の接続損失のために生じた
ものである。第2図の波形から光ファイバ3は3個の光
ファイバを接続したものであることが分る。There is a step at point C and point CI2 of waveform CI, but
These steps are caused by connection loss of the optical fiber 3. It can be seen from the waveform in FIG. 2 that the optical fiber 3 is a combination of three optical fibers.
点C11%点CI2に生ずる段差は上下に垂直な波形で
はなく、右側にずれた波形になっている。The level difference occurring at point C11% and point CI2 is not a vertical waveform vertically, but a waveform shifted to the right.
これはアナライザかを限の帯域幅をもっているためで、
通常は段差の横方向の長さは光ファイバ3に入射する測
定光のパルス幅の2倍以下であり。This is because the analyzer has a limited bandwidth.
Usually, the lateral length of the step is less than twice the pulse width of the measurement light incident on the optical fiber 3.
理想状態では測定光の1パルス分の幅たけずれる。In an ideal state, the width is shifted by one pulse of the measurement light.
第2図のような波形では各段差による接続損失は不明確
であり、複数の接続点を含む光ファイバの各単位長損失
や全区間の接続損失などを測定するのは困難である。In the waveform shown in FIG. 2, the splice loss due to each level difference is unclear, and it is difficult to measure the loss of each unit length of an optical fiber including a plurality of splice points, the splice loss of the entire section, etc.
(c) 発明の目的
この発明は、波形上に現れる段差の始めを指定点とする
とともに、各指定点から一定の長さだけ光ファイバの端
末側に寄ったととろを定点とし、定点と次の指定点の間
を直線化することにより、複数の接続点をもつ光ファイ
バの各段差を明確にし、光ファイバの緒特性を測定する
ととができるようにするものである。(c) Purpose of the Invention This invention uses the beginning of a step that appears on a waveform as a designated point, and also defines a point that is a certain length from each designated point toward the end of the optical fiber as a fixed point, and By making straight lines between specified points, each level difference in an optical fiber having a plurality of connection points can be clarified and the optical fiber characteristics can be measured.
(d) 発明の実施例
まず、この発明による指定点と定点の決め方を第3図に
より説明する。(d) Embodiments of the Invention First, the method of determining designated points and fixed points according to the present invention will be explained with reference to FIG.
第3図の波形C2は第2図の波形C+ と同じように、
7S1図の光ファイバ3に対し入射端31側から測定光
を入射した場合の波形である。Waveform C2 in Figure 3 is similar to waveform C+ in Figure 2,
This is a waveform when measurement light is incident on the optical fiber 3 in FIG. 7S1 from the input end 31 side.
第3図は3つの光ファイバを接続した場合の波形を例示
したものであり、点C21と点C23は段差の始めの部
分である。この発明では、この段差の始+6 (’)
点C2+ 1点C23を指定点とする。FIG. 3 shows an example of a waveform when three optical fibers are connected, and points C21 and C23 are the beginning of a step. In this invention, the start of this step +6 (')
Point C2+ 1 Point C23 is designated as the designated point.
点C21%点C23に続く部分は横方向にずれた形にな
っている。これは第2図の場合にも説明したとおり、ア
ナラ・イザが佇限の帯域幅をもっているためである。Point C21% The portion following point C23 is shifted in the horizontal direction. This is because, as explained in the case of FIG. 2, the analyzer has a limited bandwidth.
理想状態ではn1定光のパルス幅の長さたけ、通常は測
定光のパルス幅の2倍以」二の長さたけ指定点021、
点C23から光ファイバ3の端末側に寄った点C2゜、
点C24のところでは段差の影響がない波形になってい
る。In an ideal state, the specified point 021 is as long as the pulse width of the n1 constant light, usually more than twice the pulse width of the measurement light.
A point C2° closer to the terminal side of the optical fiber 3 from point C23,
At point C24, the waveform is not affected by the level difference.
なお、測定光にはパルス幅が0.1〜2μs程度のパル
スを使用することが多い。Note that a pulse with a pulse width of about 0.1 to 2 μs is often used as the measurement light.
この発明では、点C22、点C24を定点とする。In this invention, point C22 and point C24 are fixed points.
例えば定点C22と次の指定点C2Gの間を直線で結ぶ
ようにし、この直線の延長線と指定点C21からの垂線
との交点を点C16とずれば、点C2+と点C25の長
さか点C2+の部分の段差番ごよる減衰量を示す。For example, if a straight line connects fixed point C22 and the next designated point C2G, and the intersection of the extension of this straight line and the perpendicular from designated point C21 is shifted from point C16, then the length of point C2+ and point C25 or point C2+ It shows the amount of attenuation depending on the step number of the part.
このように、この発明ではCRTδ上に表示されを波形
のうち、各段差の始めの部分を指定点とし、各指定点か
ら測定光のパルス幅以上の長さたけ先ファイバの端末側
に寄ったところをそれぞれ定点とし、各定点と次の指定
点の間を直線化することにより各段差の減衰量を明確に
する。In this way, in this invention, in the waveform displayed on the CRT δ, the beginning of each step is set as a designated point, and the distance from each designated point to the end of the destination fiber is determined by a distance equal to or longer than the pulse width of the measurement light. However, by setting each point as a fixed point and creating a straight line between each fixed point and the next designated point, the amount of attenuation at each level difference is clarified.
(o)仝叩の呑り里
この発明によれば、複数の接続点を含む光ファイバから
の反射光をCRTに表示させたとき、各接続点の接続損
失による減衰量が明確になるので、光ファイバの単位長
損失や全区間の接続損失などを同時に算出することがで
きる。(o) According to this invention, when reflected light from an optical fiber including multiple connection points is displayed on a CRT, the amount of attenuation due to connection loss at each connection point becomes clear. It is possible to simultaneously calculate the unit length loss of an optical fiber, the splice loss of the entire length, etc.
第1図は従来装置の構成図、
第2図は第1図のCRT5に表示される反射波 −形の
一例、
第3図はこの発明による指定点と定点の決め方の説明図
。
1・ 光源、2・・・・・・方向性結合器、3・・・・
・・光ファイバ、4・・・・・検出器、5・・・・・−
CRT、31・・・・・・入射端、32・・・・・・端
末。
特許出願人 東北電力株式会社
安藤電気株式会社
代理人 弁理士 小俣欽司FIG. 1 is a configuration diagram of a conventional device, FIG. 2 is an example of a reflected waveform displayed on the CRT 5 shown in FIG. 1, and FIG. 3 is an explanatory diagram of how to determine designated points and fixed points according to the present invention. 1. Light source, 2... Directional coupler, 3...
...Optical fiber, 4...Detector, 5...-
CRT, 31...Incidence end, 32...Terminal. Patent applicant: Tohoku Electric Power Co., Ltd. Ando Electric Co., Ltd. Agent: Kinji Omata, patent attorney
Claims (1)
、前記光ファイバによる前記測定光の反り(波を検出器
で検出し、前記検出器出力をCRTに表示する光フアイ
バアナライザにおいて、前記CRTに表示された波形の
うち、前記複数の接続点の接続損失に起因する段差の始
めを指定点とし、 前記各指定点から前記測定光のパルス幅以上の長さだけ
前記光ファイバの端末側に寄ったところをそれぞれ定点
とし、 前記定点と次の指定点の間をそれぞれ直線化して表示す
ることを特徴とする光フアイバアリライザ。[Claims] 1. Injecting measurement light into an optical fiber including a plurality of connection points, detecting the warpage (waves) of the measurement light by the optical fiber with a detector, and displaying the output of the detector on a CRT. In the optical fiber analyzer, among the waveforms displayed on the CRT, the beginning of the step caused by connection loss at the plurality of connection points is designated as a designated point, and from each designated point the length is equal to or longer than the pulse width of the measurement light. An optical fiber analyzer characterized in that the points near the terminal side of the optical fiber are set as fixed points, and the points between the fixed point and the next specified point are each displayed in a straight line.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10990284A JPS60253837A (en) | 1984-05-30 | 1984-05-30 | Optical fiber analyzer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10990284A JPS60253837A (en) | 1984-05-30 | 1984-05-30 | Optical fiber analyzer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60253837A true JPS60253837A (en) | 1985-12-14 |
Family
ID=14522051
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10990284A Pending JPS60253837A (en) | 1984-05-30 | 1984-05-30 | Optical fiber analyzer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60253837A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5654366A (en) * | 1979-09-18 | 1981-05-14 | Tektronix Inc | Waveform display for digital oscilloscope |
JPS58113831A (en) * | 1981-12-28 | 1983-07-06 | Fujitsu Ltd | Measuring device for loss distribution |
-
1984
- 1984-05-30 JP JP10990284A patent/JPS60253837A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5654366A (en) * | 1979-09-18 | 1981-05-14 | Tektronix Inc | Waveform display for digital oscilloscope |
JPS58113831A (en) * | 1981-12-28 | 1983-07-06 | Fujitsu Ltd | Measuring device for loss distribution |
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