JPH0129245B2 - - Google Patents
Info
- Publication number
- JPH0129245B2 JPH0129245B2 JP57049911A JP4991182A JPH0129245B2 JP H0129245 B2 JPH0129245 B2 JP H0129245B2 JP 57049911 A JP57049911 A JP 57049911A JP 4991182 A JP4991182 A JP 4991182A JP H0129245 B2 JPH0129245 B2 JP H0129245B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- atomic
- liquid
- liquid helium
- electrical resistance
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
Landscapes
- Physics & Mathematics (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
本発明は金属容器内の液体ヘリウムの液面を測
定する液面計に関するものである。
従来の液体ヘリウムの液面計は液面検出の素子
としてNb―Ti(ニオブチタン)合金よりなる超
電導線が使用されているが、
(1) Nb―Ti超電導線の超電導転移温度(Tc)は
液体ヘリウム温度より高い為、液面直上も超電
導となるので、常電導にする為に電流を流し
(70mA程度)ジユール熱で昇温する必要があ
り、液体ヘリウムの消費量が多い(0.02/hou
r程度)。
(2) Nb―Ti超電導線は常電導状態でも電気抵抗
が小さく測定の感度を上げる為に、線径を細く
する必要があり(約0.2φmm)機械的強度、特に
耐衝撃性に弱いという欠点がある。
本発明は前記欠点を解消するために、液面の検
出素子として、Nb―Ti超電導材にかえて溶融状
態より超急冷凝固により作製した非晶質超電導材
を使用し、両端の電気抵抗値を測定することによ
り、液面の位置を検出するもので、非晶質超電導
材としてZaMb(Q+Al)c系超電導材のうち、
超電導転移温度が液体ヘリウム温度4.2〓にほぼ
等しい4.2〜5.0〓のものを使用するものである。
但し、前式の示すものは、ZがZr、Hf、Tiのい
ずれか1種、MがV、Nb、Taのいずれか1種ま
たは2種以上、QがSi、Geのいずれか1種また
は両種からなり、aは10〜90原子%、bは80原子
%以下、cは10〜25原子%の範囲にあり、Qは2
原子%以上、Alは0.1〜15原子%からなる非晶質
相をその体積率で20%以上含む合金及びQ+Al
の一部をC、B、Snのいずれか1種または2種
以上で12原子%以下置換した組成からなる、やは
り非晶質相をその体積率で20%以上含む合金であ
る。
前記超電導材は超電導転移温度が液体ヘリウム
温度にほぼ一致する為、ヒーター等の加熱機構を
特別に付加することによつて、ジユール熱を与え
る必要がなく正確な液面を検出できるので液体ヘ
リウムの消費量を減少することができ、又超電導
材は電気抵抗が大きい為に細線にして感度を上げ
る必要がなく、従来の4端子法による測定に対
し、2端子法で充分であり機構簡単にして、信頼
性の高い液面計を作ることができる。
前記組成の合金を溶融状態から超急冷凝固させ
ることにより得られた超電導材は、例えば、下記
の表1に示されるがこれらはいずれも液体ヘリウ
ム温度4.21〓にほぼ等しい4.2〜5.0〓の超電導転
移温度をもち、高い常電導抵抗及び良好な強度、
テープ形成能をもつた非晶質単相又は非晶質相を
体積率で20%以上含む結晶質相との混合相であ
る。該非晶質超電導材のうちいずれかを液体ヘリ
ウム容器の大きさに合せて長さ約100〜1000mm、
幅0.1〜5mm、板厚5〜50μにしたものを検出素子
として使用するものである。
The present invention relates to a liquid level gauge for measuring the level of liquid helium in a metal container. Conventional liquid helium level gauges use a superconducting wire made of Nb-Ti (niobium titanium) alloy as the liquid level detection element, but (1) the superconducting transition temperature (Tc) of the Nb-Ti superconducting wire is Because it is higher than the helium temperature, it becomes superconducting even just above the liquid surface, so in order to make it normal conductive, it is necessary to run a current (about 70 mA) and raise the temperature with Joule heat, which consumes a large amount of liquid helium (0.02/hou).
r degree). (2) Nb-Ti superconducting wire has low electrical resistance even in the normal conduction state, and in order to increase measurement sensitivity, the wire diameter must be made thinner (approximately 0.2φmm), and its mechanical strength, especially impact resistance, is weak. There is. In order to eliminate the above-mentioned drawbacks, the present invention uses an amorphous superconducting material produced by ultra-rapid solidification from a molten state as a liquid level detection element instead of the Nb-Ti superconducting material, and calculates the electrical resistance value at both ends. It detects the position of the liquid level by measuring, and among ZaMb(Q+Al)c-based superconducting materials as amorphous superconducting materials,
A material with a superconducting transition temperature of 4.2 to 5.0〓, which is approximately equal to the liquid helium temperature of 4.2〓, is used.
However, in the above formula, Z is one of Zr, Hf, or Ti, M is one or more of V, Nb, or Ta, and Q is one or more of Si, Ge, or Consisting of both types, a is in the range of 10 to 90 atom%, b is in the range of 80 atom% or less, c is in the range of 10 to 25 atom%, and Q is 2
Alloys containing an amorphous phase with a volume percentage of 20% or more and Q+Al
It is an alloy having a composition in which 12 atomic % or less of C, B, or Sn is substituted for a part of the alloy by one or more of C, B, and Sn, and also contains an amorphous phase with a volume fraction of 20% or more. Since the superconducting transition temperature of the superconducting material is almost the same as the liquid helium temperature, by adding a special heating mechanism such as a heater, it is not necessary to apply Joule heat and the liquid level can be detected accurately. Consumption can be reduced, and since superconducting materials have high electrical resistance, there is no need to increase sensitivity by using thin wires.In contrast to the conventional four-terminal method, a two-terminal method is sufficient and the mechanism is simpler. , it is possible to make a highly reliable liquid level gauge. Superconducting materials obtained by ultra-rapidly solidifying an alloy having the above composition from a molten state are shown in Table 1 below, and all of them have a superconducting transition of 4.2 to 5.0〓, which is approximately equal to the liquid helium temperature of 4.21〓. temperature, high normal conductivity resistance and good strength,
It is an amorphous single phase or a mixed phase with a crystalline phase containing at least 20% by volume of the amorphous phase, which has the ability to form a tape. One of the amorphous superconducting materials has a length of about 100 to 1000 mm, depending on the size of the liquid helium container.
A plate having a width of 0.1 to 5 mm and a plate thickness of 5 to 50 μm is used as a detection element.
【表】【table】
【表】
以下実施例について説明する。
第1図は本発明にもとづく液面計で、第2図は
超電導材のうちZr80Nb5Al8Si7の組成のものの液
体ヘリウムの液面上の長さとその電気抵抗との関
係を表わしたものである。
1は容器、1aは容器の基準面、2は液体ヘリ
ウムで、2aは液面である。3は計測器、4はメ
ーター、5は絶縁材、6は絶縁材と一体のボル
ト、7はロツド、7aは上部支え、7bは下端部
である。8は超電導材で、上端部8a、下端部8
bで液体ヘリウムの液面2aとの交点が8cであ
る。9は支えバネ、10及び11はリード線で、
11a,11bは電源及びメーターへ連結されて
いる。12は超電導材8とリード線11とを導通
している連結線で、13は低温ハンダ又は銀ペー
ストで、14は接着剤である。8dはリード線1
0と超電導材8の上端部8aとの接点で、前記下
端部8bのごとく低温ハンダ及び接着剤で固定さ
れ容器1の基準面1aと一致している。Hは液体
ヘリウムの液面と前記8dとの距離で、容器内の
液体ヘリウムの量を表わす基準値である。
以上の構成においてリード線10及び11に通
電すれば液体ヘリウム内に於ける超電導材の電気
抵抗は0となるためにメーターに表示される数値
は液面2aと超電導材8dとの距離Hの抵抗値を
表わすことになり、容器の基準面から液面の距離
が測定でき液体ヘリウムが増加または減少すれば
Hの増、減となりメーターに表示することにな
る。線材はヘリウム容器の全高さの一部にほぼ鉛
直に支持され、その長さは0.1〜3.0mである。
尚、該超電導材のうち、その超電導転移温度が
4.5〜5.0〓程度の場合には前記リード線を使用し
て超電導材にジユール熱を発生させて4.2〓に一
致する超電導材と同一として使用することもで
き、この場合においてもジユール熱は極めて少量
である。
以上述べた様に本発明は液体ヘリウムの液化温
度4.2〓と超電導転移温度が一致する超電導材を
液面検出素子として使用することにより液体ヘリ
ウム液面上の電気抵抗を測定することにより容易
に液体ヘリウムの液面を測定することが出来、構
造簡単にして極めて信頼性のある液面計である。[Table] Examples will be described below. Figure 1 shows a liquid level gauge based on the present invention, and Figure 2 shows the relationship between the length of a superconducting material with a composition of Zr 80 Nb 5 Al 8 Si 7 above the liquid helium surface and its electrical resistance. It is something that 1 is a container, 1a is a reference surface of the container, 2 is liquid helium, and 2a is a liquid level. 3 is a measuring device, 4 is a meter, 5 is an insulating material, 6 is a bolt integral with the insulating material, 7 is a rod, 7a is an upper support, and 7b is a lower end portion. 8 is a superconducting material, which has an upper end 8a and a lower end 8.
The intersection point 8c with the liquid surface 2a of liquid helium at point b is 8c. 9 is a support spring, 10 and 11 are lead wires,
11a, 11b are connected to a power source and a meter. Reference numeral 12 is a connecting wire that connects the superconducting material 8 and the lead wire 11, 13 is a low-temperature solder or silver paste, and 14 is an adhesive. 8d is lead wire 1
0 and the upper end 8a of the superconducting material 8, which is fixed with low temperature solder and adhesive like the lower end 8b and coincides with the reference surface 1a of the container 1. H is the distance between the liquid helium level and the above-mentioned 8d, and is a reference value representing the amount of liquid helium in the container. In the above configuration, if the lead wires 10 and 11 are energized, the electrical resistance of the superconducting material in liquid helium becomes 0, so the value displayed on the meter is the resistance of the distance H between the liquid level 2a and the superconducting material 8d. The distance of the liquid level from the reference surface of the container can be measured, and if the liquid helium increases or decreases, H increases or decreases and is displayed on the meter. The wire rod is supported substantially vertically over a portion of the total height of the helium container, and its length is 0.1 to 3.0 m. Furthermore, among the superconducting materials, the superconducting transition temperature is
In the case of 4.5 to 5.0〓, it is possible to generate Joule heat in the superconducting material using the lead wire and use it as the same as the superconducting material corresponding to 4.2〓. Even in this case, Joule heat is extremely small. It is. As described above, the present invention uses a superconducting material whose superconducting transition temperature matches the liquefaction temperature of liquid helium (4.2〓) as a liquid level detection element to measure the electrical resistance on the surface of liquid helium. It is a liquid level meter that can measure the helium liquid level and has a simple structure and is extremely reliable.
第1図は本発明による液面計の概略断面図で、
イはA〜A断面図、ロはB〜B断面図、ハはC部
の一部破断した拡大図である。そして、第2図は
超電導材のZr80Nb5Al8Si7の組成のものの液体ヘ
リウム液面上の長さと電気抵抗との関係を表わす
グラフである。
FIG. 1 is a schematic cross-sectional view of a liquid level gauge according to the present invention.
A is a cross-sectional view from A to A, B is a cross-sectional view from B to B, and C is a partially broken enlarged view of part C. FIG. 2 is a graph showing the relationship between the length above the liquid helium surface and the electrical resistance of a superconducting material with a composition of Zr 80 Nb 5 Al 8 Si 7 .
Claims (1)
合金はZaMb(Q+Al)cで示されるが、但しこ
の式はZがZr、Hf、Tiのいずれか1種、MがV、
Nbのいずれか1種または2種以上、QがSi、Ge
のいずれか1種または両種から成り、aは10〜90
原子%、bは80原子%以下、cは10〜25原子%の
範囲にあり、Qは2原子%以上、Alは0.1〜15原
子%からなる非結質相をその体積率で20%以上含
む合金及びQ+Alの一部をC、B、Snのいずれ
か1種または2種以上で12原子%以下置換した組
成からなる、やはり非結質相をその体積率で20%
以上含む合金をさし、該超電導合金のうち、超電
導転移温度が液体ヘリウム温度である4.21〓にほ
ぼ等しい4.2〜5.0Kである合金を電気抵抗線材と
して用い、液体ヘリウム容器内の全高さはその一
部に長さ0.1〜3.0mにわたつて鉛直に支持し、該
電気抵抗線の超電導領域を電気抵抗値として連続
に測定することにより容器内の液体ヘリウムの量
を測定する液面計。1 A superconducting alloy produced by ultra-rapid solidification from a liquid is represented by ZaMb(Q+Al)c, but in this formula, Z is one of Zr, Hf, or Ti, M is V,
One or more types of Nb, Q is Si, Ge
Consisting of one or both of the following, a is 10 to 90
atomic%, b is 80 atomic% or less, c is in the range of 10 to 25 atomic%, Q is 2 atomic% or more, and Al is 0.1 to 15 atomic%. Alloy containing Q+A composition in which a part of Al is replaced with 12 atomic % or less of any one or more of C, B, and Sn, and the volume percentage of the non-solid phase is 20%.
Among these superconducting alloys, alloys with a superconducting transition temperature of 4.2 to 5.0 K, which is approximately equal to the liquid helium temperature of 4.21〓, are used as electrical resistance wires, and the total height inside the liquid helium container is A liquid level gauge that measures the amount of liquid helium in a container by continuously measuring the superconducting region of the electrical resistance wire as an electrical resistance value, by vertically supporting a part over a length of 0.1 to 3.0 m.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4991182A JPS58166220A (en) | 1982-03-26 | 1982-03-26 | Liquid level indicator of liquid helium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4991182A JPS58166220A (en) | 1982-03-26 | 1982-03-26 | Liquid level indicator of liquid helium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58166220A JPS58166220A (en) | 1983-10-01 |
| JPH0129245B2 true JPH0129245B2 (en) | 1989-06-08 |
Family
ID=12844191
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4991182A Granted JPS58166220A (en) | 1982-03-26 | 1982-03-26 | Liquid level indicator of liquid helium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58166220A (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60111926A (en) * | 1983-11-22 | 1985-06-18 | Aisin Seiki Co Ltd | Liquid helium liquid-level meter |
| JPS60216224A (en) * | 1984-04-12 | 1985-10-29 | Aisin Seiki Co Ltd | Liquid helium level gauge |
| JPS60216225A (en) * | 1984-04-12 | 1985-10-29 | Aisin Seiki Co Ltd | Detector section for level gauge comprising thin film |
| JPS60165817U (en) * | 1984-04-12 | 1985-11-02 | アイシン精機株式会社 | Detection part of liquid helium level gauge |
| JPS61173027U (en) * | 1985-04-17 | 1986-10-28 | ||
| US5114907A (en) * | 1991-03-15 | 1992-05-19 | Illinois Superconductor Corporation | Cryogenic fluid level sensor |
| US5593949A (en) * | 1993-07-06 | 1997-01-14 | Lockheed Martin Corporation | High temperature conductor probes for determining liquid level of cryogens |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5854514B2 (en) * | 1975-10-17 | 1983-12-05 | 三菱電機株式会社 | Ekimenkei |
-
1982
- 1982-03-26 JP JP4991182A patent/JPS58166220A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58166220A (en) | 1983-10-01 |
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