JPH0421130B2 - - Google Patents
Info
- Publication number
- JPH0421130B2 JPH0421130B2 JP60194638A JP19463885A JPH0421130B2 JP H0421130 B2 JPH0421130 B2 JP H0421130B2 JP 60194638 A JP60194638 A JP 60194638A JP 19463885 A JP19463885 A JP 19463885A JP H0421130 B2 JPH0421130 B2 JP H0421130B2
- Authority
- JP
- Japan
- Prior art keywords
- fiber
- polarization
- maintaining
- change
- axis component
- 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 - Lifetime
Links
- 239000000835 fiber Substances 0.000 claims description 69
- 230000010287 polarization Effects 0.000 claims description 27
- 238000005253 cladding Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 238000009529 body temperature measurement Methods 0.000 description 3
- 230000008602 contraction Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000010363 phase shift Effects 0.000 description 2
- 208000025174 PANDAS Diseases 0.000 description 1
- 208000021155 Paediatric autoimmune neuropsychiatric disorders associated with streptococcal infection Diseases 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 230000004927 fusion Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 230000001550 time effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/24—Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
- G01L1/242—Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet the material being an optical fibre
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Temperature Or Quantity Of Heat (AREA)
- Light Guides In General And Applications Therefor (AREA)
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明はフアイバを用いた温度センサに関す
る。とくに、偏光面保持フアイバにレーザ光を通
して温度を測定する温度センサに関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a temperature sensor using fiber. In particular, the present invention relates to a temperature sensor that measures temperature by passing a laser beam through a polarization-maintaining fiber.
[従来の技術]
偏光面保持フアイバを用いた温度センサの一例
(たとえば、昭和59年度電気関係学会 東北支部
連合大会、文献番号2F17)を第2図に示し、説
明する。[Prior Art] An example of a temperature sensor using a polarization-maintaining fiber (for example, 1985 Tohoku Branch Federation Conference of Electrical Related Associations, Document No. 2F17) is shown in FIG. 2 and will be described.
第2図において、10は温度センサとして用い
られる偏光面保持フアイバ、21はガス・レーザ
や半導体レーザであるレーザ装置、22はレーザ
装置21の出力光を偏光面45゜(直交成分1:1)
で偏光するための偏光子、23は偏光子22を通
過した光をフアイバ10に入射せしめるためのレ
ンズ、24はフアイバの出射光に対して作用する
検光子、25は検光子24を通過した光を集める
ためのコリメータ、26はコリメータからの光の
強度を検出するための光電子増倍管、ホト・ダイ
オードがアバランシエ・ホト・ダイオードを含む
光検出器、27は光検出器26の出力を表示する
ためのブラウン管デイスプレイや、レコーダであ
る表示装置である。 In FIG. 2, 10 is a polarization plane-maintaining fiber used as a temperature sensor, 21 is a laser device such as a gas laser or a semiconductor laser, and 22 is an output light of the laser device 21 with a polarization plane of 45° (orthogonal components 1:1).
23 is a lens for making the light that has passed through the polarizer 22 enter the fiber 10; 24 is an analyzer that acts on the light emitted from the fiber; 25 is a light that has passed through the analyzer 24; 26 is a photomultiplier tube for detecting the intensity of light from the collimator, a photodetector whose photodiode includes an avalanche photodiode, and 27 is a photodetector for displaying the output of the photodetector 26. This is a display device such as a cathode ray tube display or a recorder.
偏光子22によつて偏光面保持フアイバ10に
入射される偏光のX軸成分とY軸成分は等しいも
のとなつているが、温度変化によつて偏光面保持
フアイバ10を通過する偏光のX軸成分とY軸成
分の通過時間(遅延時間)は変化し、その変化分
はX軸成分とY軸成分とでは異なつた値を示す。
すなわち、偏光面保持フアイバ10の出射端にお
いては、偏光のX軸成分とY軸成分の位相のずれ
が変化することになり、このX軸およびY軸成分
を合成した光の偏光面は、直線偏波から楕円偏
波、円偏波に変ることから、これを検光子24を
通して光検出器26により検出すると、光の強度
の変化として得られ、この強度変化が表示装置2
7に表示される。 The X-axis component and Y-axis component of the polarized light incident on the polarization-maintaining fiber 10 by the polarizer 22 are equal, but due to temperature changes, the X-axis component of the polarized light passing through the polarization-maintaining fiber 10 changes. The transit time (delay time) of the component and the Y-axis component changes, and the amount of change shows different values for the X-axis component and the Y-axis component.
That is, at the output end of the polarization-maintaining fiber 10, the phase shift between the X-axis component and the Y-axis component of the polarized light changes, and the polarization plane of the light that combines the X-axis and Y-axis components is a straight line. Since polarized waves change from polarized waves to elliptically polarized waves and circularly polarized waves, when this is detected by the photodetector 26 through the analyzer 24, it is obtained as a change in the intensity of the light, and this intensity change is displayed on the display device 2.
7 is displayed.
[発明が解決しようとする問題点]
ここで、偏光面保持フアイバ10の出射端にお
ける偏光面の角度の変化は、温度変化のみによつ
てもたらされるのではなく、偏光面保持フアイバ
10の軸方向に対する張力であるひずみによつ
も、もたらされる。[Problems to be Solved by the Invention] Here, the change in the angle of the polarization plane at the output end of the polarization-maintaining fiber 10 is not brought about only by temperature change, but also due to changes in the axial direction of the polarization-maintaining fiber 10. It is also caused by strain, which is the tension against.
一般に、温度変化は、偏光面保持フアイバ10
自身にも膨脹または収縮をもたらすものであり、
また、偏光面保持フアイバ10を保護するための
被覆があればそれの膨脹または収縮するひずみが
偏光面保持フアイバ10に加えられるから、偏光
面保持フアイバ10の出射光の偏光面の回転は温
度変化のみならず、ひずみをも同時に検出するも
のであり正確な温度を測定することはできなかつ
た。 In general, temperature changes will affect the polarization maintaining fiber 10.
It causes expansion or contraction of itself,
Furthermore, if there is a coating for protecting the polarization-maintaining fiber 10, the strain caused by its expansion or contraction is applied to the polarization-maintaining fiber 10, so the rotation of the polarization plane of the light emitted from the polarization-maintaining fiber 10 changes with temperature. Not only that, but it also detects strain at the same time, making it impossible to accurately measure temperature.
さらに、フアイバによる温度センサは、環境の
劣悪な場所に使用されることが多く、このような
場所では周辺から振動などのひずみがさらに加わ
り、温度測定の精度を一層劣化せしめていた。 Furthermore, fiber temperature sensors are often used in locations with poor environments, and in such locations, distortions such as vibrations are added from the surroundings, further deteriorating the accuracy of temperature measurement.
[問題点を解決するための手段]
本発明はこのような問題点を解決するためにな
されたもので、温度特性が異なりひずみ特性が同
じである2種の偏光面保持フアイバをそのフアイ
バの偏光軸を90゜ずらして接続し、これに偏光子
を通して光を入射すると、偏光のX軸成分および
Y軸成分の位相のずれに及ぼす入射端側の偏光面
保持フアイバの影響と、出射端側の偏光面保持フ
アイバの影響は反対の極性で作用する。すなわ
ち、入射端側の偏光面保持フアイバによつて偏光
面がたとえば右まわりに回転すると、出射端側の
偏光面保持フアイバによつて偏光面は左まわりに
回転せしめられることになり、ひずみによつて回
転する右まわりおよび左まわりの回転角が丁度打
消し合うように2種の偏光面保持フアイバを選択
した。[Means for Solving the Problems] The present invention has been made to solve the above problems, and it uses two types of polarization-maintaining fibers that have different temperature characteristics and the same strain characteristics to adjust the polarization of the fibers. If the axes are shifted by 90 degrees and light is incident on this through a polarizer, the effect of the polarization maintaining fiber on the input end side on the phase shift of the X-axis component and Y-axis component of polarized light, and the influence of the polarization plane-maintaining fiber on the output end side. The influence of polarization maintaining fibers operates with opposite polarity. In other words, when the plane of polarization is rotated clockwise by the polarization-maintaining fiber at the input end, the plane of polarization is rotated counterclockwise by the polarization-maintaining fiber at the output end, which causes distortion. Two types of polarization-maintaining fibers were selected so that the clockwise and counterclockwise rotation angles exactly cancel each other out.
[作用]
これによつて、2種の偏光面保持フアイバを通
つた光は、ひずみによる偏光面の回転は打消さ
れ、温度の変化による偏光面の回転のみが得られ
るから、精度の高い温度測定が可能となつた。[Effect] As a result, the rotation of the plane of polarization due to strain is canceled out for the light that passes through the two types of polarization-maintaining fibers, and only the rotation of the plane of polarization due to temperature changes is obtained, allowing for highly accurate temperature measurement. became possible.
[実施例]
本発明によるフアイバ温度センサを第1図に示
し説明する。[Example] A fiber temperature sensor according to the present invention is shown in FIG. 1 and will be described.
12は長さL1の偏光面保持フアイバ(第1フ
アイバ)、16は長さL2の偏光面保持フアイバ
(第2フアイバ)、であり、両フアイバは接続点1
9で融着により、あるいはコネクタにより接続さ
れている。この接続点19においては、たとえば
4μmのコア径を有するコア13とその周辺をと
りまく楕円クラツド14を含む直径125μmのフ
アイバ径を有する第1フアイバと、たとえば4μ
mのコアを有するコア17とその周辺をとりまく
楕円クラツド18とを含む直径125μmのフアイ
バ径を有する第2フアイバとがその偏光軸を90゜
ずらすために、楕円クラツド14および18の長
軸を直交せしめて接続されている。偏光保持フア
イバ中を偏光が通過するときに、温度変化やひず
みがX軸成分およびY軸成分に及ぼす遅延時間の
影響は異なつたものであるため、偏光が偏光面保
持フアイバ中を伝送するにしたがつてX軸成分と
Y軸成分との間に位相差を生じ、この両成分を合
成した偏光面は回転したものとなる。この位相差
の結果である偏光面の回転は、検光子(第2図の
24)を通過せしめることによつて光の強弱とし
て光検出器(第2図の26)によつて検出され
る。 12 is a polarization-maintaining fiber (first fiber) with length L 1 , 16 is a polarization-maintaining fiber (second fiber) with length L 2 , and both fibers are connected to connection point 1.
At 9, they are connected by fusion bonding or by connectors. At this connection point 19, for example,
For example, a first fiber having a fiber diameter of 125 μm includes a core 13 having a core diameter of 4 μm and an elliptical clad 14 surrounding the core 13;
A second fiber having a fiber diameter of 125 μm, which includes a core 17 having a core of 50 m and an elliptical cladding 18 surrounding it, has its long axes of the elliptical claddings 14 and 18 orthogonal in order to shift its polarization axis by 90°. At least it's connected. As polarized light passes through a polarization-maintaining fiber, temperature changes and strains have different delay time effects on the X-axis and Y-axis components; As a result, a phase difference occurs between the X-axis component and the Y-axis component, and the plane of polarization obtained by combining these two components becomes rotated. The rotation of the plane of polarization, which is a result of this phase difference, is detected by a photodetector (26 in FIG. 2) as the intensity of the light when the light passes through an analyzer (24 in FIG. 2).
ここで第1フアイバおよび第2フアイバの材質
は異なつたもので構成されており、温度変化やひ
ずみが位相差の変動に及ぼす影響力は両フアイバ
において異なつている。 Here, the first fiber and the second fiber are made of different materials, and the influence of temperature change and strain on the fluctuation of the phase difference is different between the two fibers.
そこで、第1フアイバの位相差の変化分を
ΔΦ1、位相差に及ぼす温度変化に対する温度係数
をA1、ひずみに対するひずみ係数をB1、ひずみ
による第1フアイバ12の長さの変化分をΔL1と
し、同様にして第2フアイバの位相差の変化分を
ΔΦ2、温度係数をA2、ひずみ係数をB2、ひずみ
による長さの変化分をΔL2とし、温度変化をΔT
とするならば
ΔΦ1=A1L1ΔT+B1ΔL1 (1)
ΔΦ2=A2L2ΔT+B2ΔL2 (2)
なる関係が得られる。ここで
B1ΔL1=B2ΔL2 (3)
となるように第1フアイバおよび第2フアイバを
選ぶ。 Therefore, ΔΦ 1 is the change in the phase difference of the first fiber, A 1 is the temperature coefficient for temperature change on the phase difference, B 1 is the strain coefficient for strain, and ΔL is the change in the length of the first fiber 12 due to strain. 1 , and similarly, the change in phase difference of the second fiber is ΔΦ 2 , the temperature coefficient is A 2 , the strain coefficient is B 2 , the change in length due to strain is ΔL 2 , and the temperature change is ΔT
Then, the following relationships are obtained: ΔΦ 1 =A 1 L 1 ΔT+B 1 ΔL 1 (1) ΔΦ 2 =A 2 L 2 ΔT+B 2 ΔL 2 (2). Here, the first fiber and the second fiber are selected so that B 1 ΔL 1 =B 2 ΔL 2 (3).
すなわち第1フアイバ12および第2フアイバ
16のひずみに対して生ずる位相差の変化分が等
しくなるようにする。 That is, the amount of change in phase difference caused by strain in the first fiber 12 and the second fiber 16 is made equal.
すると、第1フアイバ12と第2フアイバ16
とを直列に通過した光のX軸およびY軸の両成分
の位相差の変化分ΔΦは、第1フアイバ12と第
2フアイバ16との偏光軸が90゜ずれているため
に、
ΔΦ=ΔΦ1−ΔΦ2 (4)
となる。したがつて(1)式〜(4)式から
ΔΦ=(A1L1−A2L2)ΔT (5)
が得られる。 Then, the first fiber 12 and the second fiber 16
Since the polarization axes of the first fiber 12 and the second fiber 16 are shifted by 90 degrees, the change ΔΦ in the phase difference between the X-axis and Y-axis components of the light that has passed in series is ΔΦ=ΔΦ 1 −ΔΦ 2 (4). Therefore, from equations (1) to (4), ΔΦ=(A 1 L 1 −A 2 L 2 )ΔT (5) can be obtained.
この(5)式から明らかなように、位相差の変化分
ΔΦにはひずみの影響は全く無く、温度変化ΔT
による位相差の変化のみが得られることになる。 As is clear from equation (5), the change in phase difference ΔΦ is not affected by strain at all, and the temperature change ΔT
Only the change in phase difference due to is obtained.
以上の説明から明らかなように従来の温度セン
サとして用いられていた第2図に示す偏光保持フ
アイバ10に代えて、第1図に示し、(1)式〜(5)式
を用いて説明した特性を有する2種の偏光面保持
フアイバを直列に接続したフアイバを用いるなら
ばひずみの影響なく温度変化のみを精度よく測定
できる。 As is clear from the above explanation, instead of the polarization maintaining fiber 10 shown in FIG. 2 used as a conventional temperature sensor, the polarization maintaining fiber 10 shown in FIG. 1 and explained using equations (1) to (5) If a fiber is used in which two types of polarization-maintaining fibers having different characteristics are connected in series, only temperature changes can be accurately measured without the influence of distortion.
第1図における偏光面保持フアイバ12,16
には楕円クラツドのものを例示して説明したが、
パンダ型偏光面保持フアイバなど、他の偏光面保
持フアイバでも同様の結果が得られることは以上
の説明から明らかであろう。 Polarization maintaining fibers 12, 16 in FIG.
The explanation was given using an example of an elliptic cladding.
It will be apparent from the above description that similar results can be obtained with other polarization maintaining fibers, such as panda-type polarization maintaining fibers.
[発明の効果]
以上の説明から明らかなように、本発明によれ
ば、ひずみの影響を受けることなく温度変化を正
確に測定することが可能となり、とくに環境の悪
い振動の多い場所などでの温度計測に適したフア
イバ温度センサを提供するものであるから、その
効果は極めて大きい。[Effects of the Invention] As is clear from the above explanation, according to the present invention, it is possible to accurately measure temperature changes without being affected by distortion, and it is particularly useful in places with a lot of vibrations and poor environments. Since it provides a fiber temperature sensor suitable for temperature measurement, its effects are extremely large.
第1図は、本発明のフアイバ温度センサを示す
図、第2図は従来例を示す図である。
10,12,16……偏光面保持フアイバ、1
3,17……コア、14,18……楕円クラツ
ド、19……接続点、21……レーザ装置、22
……偏光子、23……レンズ、24……検光子、
25……コリメータ、26……光検出器、27…
…表示装置。
FIG. 1 is a diagram showing a fiber temperature sensor of the present invention, and FIG. 2 is a diagram showing a conventional example. 10, 12, 16... polarization maintaining fiber, 1
3, 17... Core, 14, 18... Elliptical cladding, 19... Connection point, 21... Laser device, 22
...Polarizer, 23...Lens, 24...Analyzer,
25...collimator, 26...photodetector, 27...
...Display device.
Claims (1)
光のX軸成分およびY軸成分の位相差の変化分が
等しく、前記第1フアイバとは温度変化に対して
生ずる偏光のX軸成分およびY軸成分の位相差の
変化分が異なる偏光面保持フアイバである第2フ
アイバとからなり、 前記第1フアイバと前記第2フアイバの偏光軸
が90゜ずれて接続されたものであることを特徴と
するフアイバ温度センサ。[Scope of Claims] 1. A first fiber that is a polarization plane-maintaining fiber, and the first fiber have the same amount of change in the phase difference between the X-axis component and the Y-axis component of polarized light caused by strain, and The fiber consists of a second fiber, which is a polarization plane-maintaining fiber, in which the change in the phase difference between the X-axis component and the Y-axis component of polarized light that occurs due to temperature changes is different, and the polarization of the first fiber and the second fiber is different from each other. A fiber temperature sensor characterized in that the axes are connected at an angle of 90°.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60194638A JPS6254133A (en) | 1985-09-03 | 1985-09-03 | Fiber temperature sensor |
| US06/900,506 US4773753A (en) | 1985-09-03 | 1986-08-26 | Fiber sensor |
| DE8686401918T DE3679126D1 (en) | 1985-09-03 | 1986-09-01 | FIBER OPTICAL SENSOR. |
| EP86401918A EP0214907B1 (en) | 1985-09-03 | 1986-09-01 | Fiber sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60194638A JPS6254133A (en) | 1985-09-03 | 1985-09-03 | Fiber temperature sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6254133A JPS6254133A (en) | 1987-03-09 |
| JPH0421130B2 true JPH0421130B2 (en) | 1992-04-08 |
Family
ID=16327840
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60194638A Granted JPS6254133A (en) | 1985-09-03 | 1985-09-03 | Fiber temperature sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6254133A (en) |
-
1985
- 1985-09-03 JP JP60194638A patent/JPS6254133A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6254133A (en) | 1987-03-09 |
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