JPS5836047Y2 - Temperature sensor for cryogenic temperatures - Google Patents
Temperature sensor for cryogenic temperaturesInfo
- Publication number
- JPS5836047Y2 JPS5836047Y2 JP218379U JP218379U JPS5836047Y2 JP S5836047 Y2 JPS5836047 Y2 JP S5836047Y2 JP 218379 U JP218379 U JP 218379U JP 218379 U JP218379 U JP 218379U JP S5836047 Y2 JPS5836047 Y2 JP S5836047Y2
- Authority
- JP
- Japan
- Prior art keywords
- temperature sensor
- resistance wire
- platinum
- cryogenic temperatures
- cobalt
- 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
- Measuring Temperature Or Quantity Of Heat (AREA)
Description
【考案の詳細な説明】
本考案は極低温領域の計測に適した温度センサの構造に
関する。[Detailed Description of the Invention] The present invention relates to the structure of a temperature sensor suitable for measurement in an extremely low temperature region.
従来白金抵抗線材料等を用いた温度センサの低温側の測
定限界は、第1図の感度特性曲線1で示すようにIOK
でありそれ以下は抵抗変化が無く測定不能であった。The measurement limit on the low temperature side of conventional temperature sensors using platinum resistance wire materials, etc. is IOK as shown in sensitivity characteristic curve 1 in Figure 1.
Below that, there was no change in resistance and measurement was impossible.
しかし近年、白金にコバルトを一定の割合で混合させた
合金抵抗線材料によって2に〜300に1で温度測定で
きる技術が開発されつつある。However, in recent years, a technology is being developed that can measure temperatures at a rate of 2 to 1 in 300 using an alloy resistance wire material made by mixing platinum and cobalt at a certain ratio.
第1図(2)の曲線は0.45mol俤のコバルト混合
率、(3) 、 (4)は夫々0.75mo1%、1.
06mol咎の場合の感度特性を示すもので、(3)
、 (4)の場合不連続点が存在し、結局0.5 mo
1φ付近がセンサとして好適であることがわかる。The curve in FIG. 1 (2) shows a cobalt mixing ratio of 0.45 mol, and the curves (3) and (4) show a cobalt mixing ratio of 0.75 mol % and 1.
This shows the sensitivity characteristics in the case of 0.6 mol.
, In the case of (4), there is a discontinuity point, and eventually 0.5 mo
It can be seen that around 1φ is suitable as a sensor.
このような抵抗線材料を用いて極低温を測定対象とする
センサを構成する場合に要求される特性としては、
(1) 抵抗温度特性の再現性が良いこと。When constructing a sensor that measures extremely low temperatures using such resistance wire materials, the required characteristics are: (1) good reproducibility of resistance-temperature characteristics;
(2)極低温での熱伝導が良く、測定対象の温度変動に
敏速に応答すること。(2) It has good heat conduction at extremely low temperatures and responds quickly to temperature fluctuations of the measurement target.
(3)構造が簡単で、振動、衝撃、熱衝撃に対して強い
こと。(3) The structure is simple and resistant to vibration, shock, and thermal shock.
が挙げられる。can be mentioned.
特にセンサは常温300により極低温2に程度の間で急
激な熱変化(熱衝撃)を受けるので、抵抗線材料と巻枠
および絶縁用コーテイング材の3者は、極低温領域から
常温に至る範囲で線膨張係数が等しいものを使用しない
と、抵抗線材料に歪が加わり測定誤差を生ずる原因とな
る。In particular, the sensor is subject to sudden thermal changes (thermal shock) between room temperature 300°C and cryogenic temperature 2°C, so the resistance wire material, winding frame, and insulating coating material are If wires with the same coefficient of linear expansion are not used, strain will be added to the resistance wire material, causing measurement errors.
又、巻枠とコーテイング材は急激な熱衝撃を受けても破
損しない強度を有するものが必要である。In addition, the winding frame and coating material must be strong enough not to be damaged even if subjected to sudden thermal shock.
0.3〜0.75 mo 1 %の白金・コバルト合金
抵抗線材料の線膨張係数は約9.lX10−6である。The linear expansion coefficient of 0.3 to 0.75 mo 1 % platinum/cobalt alloy resistance wire material is approximately 9. It is lX10-6.
この線膨張係数に略等しい線膨張係数を有し、熱伝導特
性も良くかつ同一材でコーティングも可能な巻枠用の絶
縁材を種々検討した結果、硼硅酸ガラス(線膨張係数約
9. I X 10−6)が極めて適していることを見
出した。After studying various insulating materials for the winding frame that have a linear expansion coefficient approximately equal to this linear expansion coefficient, have good thermal conductivity, and can be coated with the same material, we found borosilicate glass (with a linear expansion coefficient of about 9. IX 10-6) was found to be extremely suitable.
本考案は、第2図に示すように、白金に0.5mo1%
近傍のコバルトを混合した合金抵抗線材料1を、硼硅酸
ガラス材の蓋枠2に巻回し、硼硅酸ガラス材3による0
、 5 mm程度のコーティングを表面に施した構成を
特徴とする。The present invention, as shown in Figure 2, uses 0.5mol1% of platinum.
The alloy resistance wire material 1 mixed with nearby cobalt is wound around a lid frame 2 made of borosilicate glass material, and
, is characterized by a structure in which a coating of about 5 mm is applied to the surface.
4.4IrIま抵抗線材料1の両端部に接続甜る4線式
の引出線であり、白金線が用いられる。4.4 IrI is a four-wire lead wire connected to both ends of the resistance wire material 1, and a platinum wire is used.
向、リード線としては抵抗線材料をそのまま延長するよ
うに構成してもよい。Alternatively, the lead wire may be constructed by extending the resistance wire material as it is.
本考案によれば、2に程度までの極低温領域を高精度、
高感度で測定でき、衝撃にも強い優れた温度センサを実
現することができる。According to the present invention, the extremely low temperature region up to about 2 can be controlled with high precision.
It is possible to create an excellent temperature sensor that can measure with high sensitivity and is resistant to shock.
硼硅酸ガラスによる巻枠は加工が極めて容易であり、径
は使用場所に合せて自由に選択することができる。A winding frame made of borosilicate glass is extremely easy to process, and its diameter can be freely selected depending on the location of use.
抵抗線材料を細いもので形成すれば、極めて小型で、チ
ップ状の温度センサを製作することも容易である。If the resistance wire material is made of thin material, it is easy to manufacture an extremely small and chip-shaped temperature sensor.
第1図は白金及び白金・コバルト合金抵抗線材料の感度
特性図、第2図は本考案温度センサの一実施例を示す構
成図である。
1・・・白金・コバルト合金抵抗線材料、2・・・硼硅
酸ガラス巻線、3・・・硼硅酸ガラスコーティング、4
.4′・・・引出線。FIG. 1 is a sensitivity characteristic diagram of platinum and platinum-cobalt alloy resistance wire materials, and FIG. 2 is a configuration diagram showing an embodiment of the temperature sensor of the present invention. 1... Platinum-cobalt alloy resistance wire material, 2... Borosilicate glass winding wire, 3... Borosilicate glass coating, 4
.. 4'...Leader line.
Claims (1)
抗線材料を硼硅酸ガラス材の巻枠に巻回すると共に上記
ガラス材と同一ガラス材で表面をコーティングしてなる
極低温用温度センサ。A cryogenic temperature sensor made by winding an alloy resistance wire material made of platinum mixed with cobalt of around 0.5 molφ around a borosilicate glass material, and coating the surface with the same glass material as the above glass material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP218379U JPS5836047Y2 (en) | 1979-01-12 | 1979-01-12 | Temperature sensor for cryogenic temperatures |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP218379U JPS5836047Y2 (en) | 1979-01-12 | 1979-01-12 | Temperature sensor for cryogenic temperatures |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS55103534U JPS55103534U (en) | 1980-07-19 |
JPS5836047Y2 true JPS5836047Y2 (en) | 1983-08-13 |
Family
ID=28805020
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP218379U Expired JPS5836047Y2 (en) | 1979-01-12 | 1979-01-12 | Temperature sensor for cryogenic temperatures |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5836047Y2 (en) |
-
1979
- 1979-01-12 JP JP218379U patent/JPS5836047Y2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS55103534U (en) | 1980-07-19 |
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