JPS6025561Y2 - temperature measuring device - Google Patents
temperature measuring deviceInfo
- Publication number
- JPS6025561Y2 JPS6025561Y2 JP533379U JP533379U JPS6025561Y2 JP S6025561 Y2 JPS6025561 Y2 JP S6025561Y2 JP 533379 U JP533379 U JP 533379U JP 533379 U JP533379 U JP 533379U JP S6025561 Y2 JPS6025561 Y2 JP S6025561Y2
- Authority
- JP
- Japan
- Prior art keywords
- optical
- fiber
- measuring device
- temperature
- temperature measuring
- 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
Links
Landscapes
- Radiation Pyrometers (AREA)
Description
【考案の詳細な説明】
本考案は光ファイバを用い、電磁誘導を受けやすい場所
での温度測定が容易な温度測定器に関する。[Detailed Description of the Invention] The present invention relates to a temperature measuring device that uses an optical fiber and can easily measure temperature in places susceptible to electromagnetic induction.
光ファイバを用いた従来の温度計を第1図に示す。A conventional thermometer using an optical fiber is shown in FIG.
光ファイバ1を伝搬する光をレンズ2で一度平行ビーム
とし、レンズ2′で″集光してファイバ1′に効率よく
入射させている。The light propagating through the optical fiber 1 is once converted into a parallel beam by the lens 2, and is condensed by the lens 2' to efficiently enter the fiber 1'.
このレンズの間にバイメタル4に支持された遮蔽板3が
挿入されており、光ビームの一部をさえぎっている。A shielding plate 3 supported by a bimetal 4 is inserted between these lenses, and blocks part of the light beam.
遮蔽される光量が温度変化に伴なう遮へい板3の移動に
よって変化する。The amount of light to be blocked changes as the shielding plate 3 moves as the temperature changes.
この方法は光の損失により温度測定を行なうので電磁誘
導による誤動作がなく有効ではあるが、部品数が多く、
大型になり、又温度変化によって、ファイバ1,1′と
レンズ2,2′の位置が変化し、高温での測定には用い
られない。This method measures temperature using optical loss, so there is no malfunction due to electromagnetic induction, so it is effective, but it requires a large number of parts.
It is large in size, and the positions of the fibers 1, 1' and lenses 2, 2' change due to temperature changes, so it cannot be used for measurements at high temperatures.
本考案は部品数を削減し、比較的高温での測定をも可能
にしたものである。The present invention reduces the number of parts and enables measurement at relatively high temperatures.
以下本考案を図面を用いて実施例とともに説明する。The present invention will be described below with reference to drawings and embodiments.
第2図に本考案による一実施例の構成国を示す。FIG. 2 shows the constituent countries of an embodiment of the present invention.
1,1′は光ファイ入゛で、□゛5は円筒スリーブで、
ファイバの外径とスリーブの内径がほぼ等しい。1 and 1' are optical fibers, □゛5 is a cylindrical sleeve,
The outer diameter of the fiber and the inner diameter of the sleeve are approximately equal.
スリーブの両端6は接着剤又は圧着によりファイバに固
定されている。Both ends 6 of the sleeve are fixed to the fiber by adhesive or crimping.
スリーブ5とファイバ1.1′材マ4は、をの熱膨張係
数が前者が後者よりも小さモ;)という相違があり、こ
の違いによって、温度が上がると、ファイバめ接合部7
の端面にすき間が出来、ファイバ1,1′を伝搬する光
はこの部分でファイバ外にもれる。There is a difference between the sleeve 5 and the fiber 1.1' material 4 in that the former has a smaller thermal expansion coefficient than the latter, and due to this difference, when the temperature rises, the fiber joint 7
A gap is created at the end face of the fibers 1 and 1', and the light propagating through the fibers 1 and 1' leaks out of the fiber at this portion.
したがって、この伝搬損失を測ることによって温度が測
定出来る。Therefore, temperature can be measured by measuring this propagation loss.
゛実験自ま゛呂デ径總云、’ NA−0,16の石英フ
ァイバと、ステンレス製約5cmのスリーブを用いて0
℃のとき損失が0になる様に構成した。``Experimentally conducted,'' using a quartz fiber with NA-0.16 and a sleeve made of stainless steel with a length of about 5 cm.
It was constructed so that the loss would be 0 at ℃.
このときの測定結果を第3図に示す。The measurement results at this time are shown in FIG.
損失は0.02dB程度の変化が測定出来るので、この
温度計の感度は約0.4℃である。Since a change in loss of about 0.02 dB can be measured, the sensitivity of this thermometer is about 0.4°C.
この感度と測定可能温度範囲はスリーブの膨張係数と長
さによってきまるので、使用する場所によって決定すれ
ばよい。The sensitivity and measurable temperature range are determined by the expansion coefficient and length of the sleeve, so they can be determined depending on the location of use.
又実験ではO’Cから測定出来る様にしたが、ファイバ
とスリーブの接続位置をかえることにより測定範囲を任
意に設定できることは明らかである。Furthermore, in the experiment, it was possible to measure from O'C, but it is clear that the measurement range can be arbitrarily set by changing the connecting position of the fiber and the sleeve.
第4図に他の実施例の構成国を示す。FIG. 4 shows the constituent countries of another embodiment.
ファイバ1の外側をスリーブ5でおおい、一方、スリー
ブ5の一端6を接着剤又は圧着で固定する。The outside of the fiber 1 is covered with a sleeve 5, while one end 6 of the sleeve 5 is fixed with adhesive or crimping.
スリーブ5の他端には反射鏡8が軸に垂直に取付けであ
る。A reflecting mirror 8 is attached to the other end of the sleeve 5 perpendicularly to the axis.
以上の様に構成するとファイバ1を伝搬する光がミラー
8で反射されてくる光の光量を測定することによって、
温度が測定出来るのは明らかである。With the above configuration, by measuring the amount of light propagating through the fiber 1 and reflected by the mirror 8,
Obviously, temperature can be measured.
この場合、スリーブ5とファイバ1との熱膨張係数のち
がいにより、両者間にすき間が生じ、反射鏡8での反射
光がファイバ1に入射する量が変化し、温度測定が行な
える。In this case, due to the difference in thermal expansion coefficient between the sleeve 5 and the fiber 1, a gap is created between them, and the amount of light reflected by the reflecting mirror 8 that enters the fiber 1 changes, allowing temperature measurement to be performed.
以上説明した様に本考案によれば、簡単な構造で、小型
、軽量の温度測定器を構成出来る。As explained above, according to the present invention, a small, lightweight temperature measuring device can be constructed with a simple structure.
又発光源及び受光源と、センサ部をはなすと高圧線等の
近くであっても誘導ノイズを受けることなく、測定出来
る。Furthermore, if the light emitting source and light receiving source are separated from the sensor section, measurements can be made without being affected by induced noise even in the vicinity of high voltage lines or the like.
第1図は従来の温度測定器の構成国、第2図は本考案の
一実施例を示す構成国、第3図は同実施例による温度−
損失特性図、第4図は本考案の他の実施例を示す構成国
である。
1.1′・・・・・・光ファイバ、5・・・・・・スリ
ーブ、8・・・・・・反射鏡。Figure 1 shows the constituent countries of a conventional temperature measuring instrument, Figure 2 shows the constituent countries of an embodiment of the present invention, and Figure 3 shows the temperature measurement according to the same embodiment.
The loss characteristic diagram, FIG. 4, shows the components of another embodiment of the present invention. 1.1'...Optical fiber, 5...Sleeve, 8...Reflector.
Claims (1)
または反射する光媒体と、前記光伝送体または前記光媒
体とは異なる膨張係数を有し、前記光伝送体と前記光媒
体を可動状態に保持する保持体とからなり、前記光伝送
体と前記光媒体との間での光の損失により温度を測定す
ることを特徴とする温度測定器。an optical transmission body that transmits light; an optical medium that transmits or reflects light from the optical transmission body; and an expansion coefficient that is different from the optical transmission body or the optical medium, and the optical transmission body and the optical medium. 1. A temperature measuring device comprising: a holder for holding the optical fiber in a movable state; the temperature measuring device is characterized in that the temperature is measured by the loss of light between the optical transmitter and the optical medium.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP533379U JPS6025561Y2 (en) | 1979-01-20 | 1979-01-20 | temperature measuring device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP533379U JPS6025561Y2 (en) | 1979-01-20 | 1979-01-20 | temperature measuring device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS55105138U JPS55105138U (en) | 1980-07-22 |
JPS6025561Y2 true JPS6025561Y2 (en) | 1985-07-31 |
Family
ID=28811100
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP533379U Expired JPS6025561Y2 (en) | 1979-01-20 | 1979-01-20 | temperature measuring device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6025561Y2 (en) |
-
1979
- 1979-01-20 JP JP533379U patent/JPS6025561Y2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS55105138U (en) | 1980-07-22 |
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