JPS6140334B2 - - Google Patents
Info
- Publication number
- JPS6140334B2 JPS6140334B2 JP55143025A JP14302580A JPS6140334B2 JP S6140334 B2 JPS6140334 B2 JP S6140334B2 JP 55143025 A JP55143025 A JP 55143025A JP 14302580 A JP14302580 A JP 14302580A JP S6140334 B2 JPS6140334 B2 JP S6140334B2
- Authority
- JP
- Japan
- Prior art keywords
- gas
- measured
- temperature
- diffusion membrane
- hydrogen
- 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
- 239000007789 gas Substances 0.000 claims description 61
- 229910052739 hydrogen Inorganic materials 0.000 claims description 37
- 239000001257 hydrogen Substances 0.000 claims description 37
- 239000012528 membrane Substances 0.000 claims description 36
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 34
- 238000010438 heat treatment Methods 0.000 claims description 24
- 238000009792 diffusion process Methods 0.000 claims description 21
- 238000001514 detection method Methods 0.000 claims description 18
- 239000012466 permeate Substances 0.000 claims description 8
- 238000005259 measurement Methods 0.000 claims description 6
- 150000002431 hydrogen Chemical class 0.000 claims description 3
- YZCKVEUIGOORGS-NJFSPNSNSA-N Tritium Chemical compound [3H] YZCKVEUIGOORGS-NJFSPNSNSA-N 0.000 description 19
- 229910052722 tritium Inorganic materials 0.000 description 19
- 230000000694 effects Effects 0.000 description 5
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 4
- 230000002411 adverse Effects 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- WHXSMMKQMYFTQS-UHFFFAOYSA-N Lithium Chemical compound [Li] WHXSMMKQMYFTQS-UHFFFAOYSA-N 0.000 description 2
- KDLHZDBZIXYQEI-UHFFFAOYSA-N Palladium Chemical compound [Pd] KDLHZDBZIXYQEI-UHFFFAOYSA-N 0.000 description 2
- 230000004992 fission Effects 0.000 description 2
- 239000000446 fuel Substances 0.000 description 2
- 238000002955 isolation Methods 0.000 description 2
- 229910052744 lithium Inorganic materials 0.000 description 2
- 229910052759 nickel Inorganic materials 0.000 description 2
- 229910001220 stainless steel Inorganic materials 0.000 description 2
- 239000010935 stainless steel Substances 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 230000000712 assembly Effects 0.000 description 1
- 238000000429 assembly Methods 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 238000007599 discharging Methods 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 231100000989 no adverse effect Toxicity 0.000 description 1
- 229910052763 palladium Inorganic materials 0.000 description 1
- 239000000047 product Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 239000012857 radioactive material Substances 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T7/00—Details of radiation-measuring instruments
- G01T7/02—Collecting means for receiving or storing samples to be investigated and possibly directly transporting the samples to the measuring arrangement; particularly for investigating radioactive fluids
Landscapes
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Monitoring And Testing Of Nuclear Reactors (AREA)
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
本発明はたとえば原子炉内の燃料集合体や制御
棒などの破損を検出する際に好適した水素同位体
を連続的に測定できる水素同位体測定装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hydrogen isotope measuring device capable of continuously measuring hydrogen isotopes, which is suitable for detecting damage to fuel assemblies, control rods, etc. in a nuclear reactor, for example.
破損燃料検出系では核分裂生成物中にトリチウ
ムが少なからず含有されており、また制御棒のボ
ロン中に不純物としてリチウムが含有され、その
リチウムが核分裂してトリチウムを生成するため
に、これらからトリチウムを検出することは原子
炉の運転制御上から重要なことである。 In the damaged fuel detection system, the nuclear fission products contain a considerable amount of tritium, and the boron in the control rods contains lithium as an impurity, and the lithium fissions to produce tritium, so tritium is extracted from these. Detection is important from the standpoint of nuclear reactor operation control.
このトリチウムの含有量を測定するには従来か
らガスフローカウンターや比例計数管などの測定
器に直接流して測定する気体法などによつて行わ
れている。 The content of tritium has conventionally been measured using a gas method in which the tritium is directly passed through a measuring device such as a gas flow counter or proportional counter.
また、トリチウムが他の気体と混合している場
合には半導体放射線検出器によつてトリチウムの
検出とその含有量の測定を行つている。 Furthermore, when tritium is mixed with other gases, a semiconductor radiation detector is used to detect tritium and measure its content.
しかしながら、トリチウムの含有量が少量の場
合にはバツクグラウンドおよび検出器の性能によ
りトリチウムの量の測定が正確にできない欠点が
あつた。 However, when the tritium content is small, there is a drawback that the amount of tritium cannot be accurately measured due to the background and the performance of the detector.
そこで、放射性物質中に混合しているトリチウ
ムを何らかの手段で取り出すか、またはバツクグ
ラウドの低下や検出器の性能を向上させる必要性
が生じてきた。 Therefore, it has become necessary to take out the tritium mixed in radioactive materials by some means, or to reduce the background noise and improve the performance of the detector.
しかしながら、種々の機器を必要とし、機器そ
のものが複雑化ししかも高価になるなどの欠点が
あるため、トリチウムおよび水素を選択的に透過
させる金属膜を利用してトリチウムおよび水素の
濃度を測定する装置が提案されている。この装置
を第1図を参照して説明する。 However, there are drawbacks such as the need for various types of equipment, which makes the equipment itself complex and expensive. Proposed. This device will be explained with reference to FIG.
すなわち、被測定ガスを収納した上部のみ部分
的に示す被測定ガス室1の開口部2は、フランジ
3で着脱自在に閉塞されるが、このフランジ3に
は水素同位体検出部4に連通した管状体5が気密
に貫通して取り着けられている。管状体5の下端
には水素を選択的に透過させるたとえばニツケ
ル、ステンレス鋼などの金属製有底管状拡散膜部
6が接続されており、またこの拡散膜部6の外面
にヒータ7が直接巻回されている。ヒータ7は温
度検出素子8からの信号で温度制御装置9により
所定の温度に制御される。 That is, the opening 2 of the gas chamber 1 to be measured, whose upper part containing the gas to be measured is only partially shown, is removably closed by a flange 3, which is connected to the hydrogen isotope detection section 4. A tubular body 5 is attached therethrough in an airtight manner. A bottomed tubular diffusion membrane section 6 made of metal such as nickel or stainless steel that selectively permeates hydrogen is connected to the lower end of the tubular body 5, and a heater 7 is directly wound around the outer surface of this diffusion membrane section 6. It's being passed around. The heater 7 is controlled to a predetermined temperature by a temperature control device 9 based on a signal from a temperature detection element 8.
さらに拡散膜部6内には被測定室1外から管状
体5を貫通した輸送ガス供給管10が垂下されて
いる。輸送ガス供給管10はバルブ11を介して
輸送ガス源12に接続され、また検出部4には弁
13が設けられ測定後のガスを排出する弁13が
接続されている。ここで、拡散膜部6の温度制御
は検出部4の性能に直接影響を与えるため正確に
行う必要がある。輸送ガスとしてはヘリウムやア
ルゴンなどの希ガス中に少量の水素が含有された
ものが使用されて被測定ガス中の水素、トリチウ
ムなどが拡散膜部へ選択透過し易くなるようにし
ている。 Furthermore, a transport gas supply pipe 10 that penetrates the tubular body 5 from outside the measurement chamber 1 is suspended within the diffusion membrane section 6 . The transport gas supply pipe 10 is connected to a transport gas source 12 via a valve 11, and the detection unit 4 is provided with a valve 13, which is connected to the valve 13 for discharging the gas after measurement. Here, temperature control of the diffusion film section 6 must be performed accurately because it directly affects the performance of the detection section 4. As the transport gas, a rare gas such as helium or argon containing a small amount of hydrogen is used so that hydrogen, tritium, etc. in the gas to be measured can easily permeate selectively to the diffusion membrane section.
第1図に示した水素同位体測定装置においては
拡散膜部6の表面にヒータ7を直接巻回してある
ため、その膜部6が直接巻線7aの表面温度の影
響を受けるとともに膜部6の下端から上方向に温
度勾配が生じ、更に膜部6の内側を流れる輸送ガ
スの影響を受けるため正確な温度コントロールを
することが困難な欠点があつた。 In the hydrogen isotope measurement apparatus shown in FIG. 1, the heater 7 is directly wound around the surface of the diffusion membrane section 6, so that the membrane section 6 is directly affected by the surface temperature of the winding 7a, and the membrane section 6 There is a temperature gradient upward from the lower end of the membrane part 6, and it is further affected by the transport gas flowing inside the membrane part 6, so that it is difficult to accurately control the temperature.
また膜部6の表面を流れる被測定ガスの流れを
ヒータ7により妨げられるため被測定ガス中の水
素、トリチウムが膜部6を透過する際に悪影響を
与えるため正確な水素同位体濃度を測定すること
が困難な欠点であつた。 In addition, since the flow of the gas to be measured flowing on the surface of the membrane part 6 is obstructed by the heater 7, hydrogen and tritium in the gas to be measured have an adverse effect when permeating through the membrane part 6, so accurate hydrogen isotope concentration can be measured. This was a difficult drawback.
本発明は上記欠点を除去するためになされたも
ので、水素、トリチウムを選択的に透過させる拡
散膜部がヒーターの表面温度の影響を受けずに拡
散膜部の表面の温度勾配をなくし、かつ輸送ガス
の影響をなくすことにより拡散膜部の温度コント
ロールを精度良く行うことができ、またヒーター
による被測定ガスに対する流れの影響をなくすこ
とにより信頼性が大きく正確に水素同位体の濃度
を測定し得る水素同位体測定測量を提供すること
にある。 The present invention has been made to eliminate the above-mentioned drawbacks, and has a diffusion membrane that selectively transmits hydrogen and tritium, which eliminates the temperature gradient on the surface of the diffusion membrane without being affected by the surface temperature of the heater. By eliminating the influence of the transport gas, it is possible to accurately control the temperature of the diffusion membrane part, and by eliminating the influence of the flow of the gas to be measured due to the heater, it is possible to measure the concentration of hydrogen isotopes with high reliability and accuracy. The purpose of this research is to provide hydrogen isotope measurement surveys.
以下、本発明に係る水素同位体測定装置の一実
施例を第2図によつて説明する。 Hereinafter, one embodiment of the hydrogen isotope measuring device according to the present invention will be described with reference to FIG.
なお、第2図において第1図と同一部分は同一
符号で示し、重複した部分の説明は省略してあ
る。すなわち、この発明は被測定ガス室1の開口
部2にフランジ3が水平に直接装着されており、
このフランジ3に被測定ガスが流通する筒状体2
0が固定されている。この筒状体20は被測定ガ
スを下方から上方へ向けて流すガス流入孔21お
よび流出孔22が設けられている。この筒状体2
0内にはたとえばステンレス製管状体5が取付け
られている。この管状体5には中央部から下方へ
向けてスリーブ状拡散膜部6が接続されている。
拡散膜部6としては水素を選択的に透過させるパ
ラジウム、鉄、ニツケル等が使用される。この拡
散膜部6の下方に第1の加熱源23が設けられ、
また筒状体20のガス流出孔22付近の管状体5
には第2の加熱源24が設けられている。加熱源
23,24には温度検知素子25,26と温度制
御装置27,28により、所定温度に調整され
る。フランジの上方には前記膜部6を透過した水
素、トリチウムを検出部4へ輸送する輸送ガス用
の輸送ガス源12と隔離弁11、輸送された水
素、トリチウムを検出する水素同位体検出部4お
よび大気隔離用弁13を設置して水素同位体測定
装置が構成される。 Note that in FIG. 2, the same parts as in FIG. 1 are indicated by the same reference numerals, and explanations of overlapping parts are omitted. That is, in this invention, the flange 3 is directly attached horizontally to the opening 2 of the gas chamber 1 to be measured,
A cylindrical body 2 through which gas to be measured flows through this flange 3
0 is fixed. This cylindrical body 20 is provided with a gas inflow hole 21 and an outflow hole 22 through which the gas to be measured flows from below to above. This cylindrical body 2
A tubular body 5 made of stainless steel, for example, is attached inside the housing 0. A sleeve-shaped diffusion membrane portion 6 is connected to the tubular body 5 from the center downward.
As the diffusion membrane portion 6, palladium, iron, nickel, or the like, which selectively permeates hydrogen, is used. A first heat source 23 is provided below this diffusion film section 6,
Also, the tubular body 5 near the gas outlet hole 22 of the tubular body 20
A second heating source 24 is provided. The heating sources 23 and 24 are adjusted to a predetermined temperature by temperature detection elements 25 and 26 and temperature control devices 27 and 28. Above the flange are a transport gas source 12 and isolation valve 11 for transporting hydrogen and tritium that have passed through the membrane section 6 to the detection section 4, and a hydrogen isotope detection section 4 that detects the transported hydrogen and tritium. A hydrogen isotope measuring device is constructed by installing an atmospheric isolation valve 13.
なお、前記輸送ガスは輸送ガス用ノズル10に
取付けられている第3加熱源29により加熱され
る。この加熱源29は温度検知素子30と温度制
御装置31により所定温度に調整される。かかる
上記測定装置において筒状体20のガス流入孔2
1から流入する被測定ガスは第1の加熱源23に
より加熱され浮力を受け上昇し、流路32を通り
ガス流出孔22から放出される。 Note that the transport gas is heated by a third heating source 29 attached to the transport gas nozzle 10. This heating source 29 is adjusted to a predetermined temperature by a temperature sensing element 30 and a temperature control device 31. In such a measuring device, the gas inflow hole 2 of the cylindrical body 20
The gas to be measured flowing in from the first heating source 23 is heated by the first heating source 23, rises due to buoyancy, passes through the flow path 32, and is discharged from the gas outlet hole 22.
つまり筒状体20と第1の加熱源23および第
2の加熱源24により生じる自然対流を利用しガ
スを循環させ、第1加熱源23により被測定ガス
を加熱し、その被測定ガスにより膜部6を加熱す
る。 In other words, gas is circulated using natural convection generated by the cylindrical body 20, the first heating source 23, and the second heating source 24, the first heating source 23 heats the gas to be measured, and the gas to be measured forms a film. Heat section 6.
さらに管状体5から熱伝導による逃げを防ぐた
めに第2の加熱源24を設けることにより、膜部
6が直接加熱源23による表面温度の影響をなく
し、下方から上方への温度勾配をなくすことが可
能となる。ここで、さらに輸送ガスを第3の加熱
源29、温度検知素子30、温度制御装置31に
より所定温度に調整することにより正確な膜部6
の温度コントロールの働きを保持させることがで
きる。 Furthermore, by providing the second heating source 24 to prevent heat from escaping from the tubular body 5 due to heat conduction, the membrane portion 6 can eliminate the influence of the surface temperature caused by the direct heating source 23, and eliminate the temperature gradient from the bottom to the top. It becomes possible. Here, the transport gas is further adjusted to a predetermined temperature using a third heating source 29, a temperature detection element 30, and a temperature control device 31, so that the membrane part 6 can be accurately adjusted.
temperature control function can be maintained.
なお、第2図中温度検知素子25,26,30
はたとえば熱電対が使用され、また筒状体20に
は熱しやへい体が使用される。ここで、本発明に
おいて筒状体20のガス流入孔21から流入し第
1の加熱源23で加熱され所定の温度に維持さ
れ、、膜部6を透過し、輸送ガスにより水素同位
体検出部4まで運ばれ検出される。 In addition, temperature sensing elements 25, 26, 30 in FIG.
For example, a thermocouple is used, and the cylindrical body 20 is a heating or shielding body. Here, in the present invention, the gas flows in from the gas inflow hole 21 of the cylindrical body 20, is heated by the first heating source 23, is maintained at a predetermined temperature, passes through the membrane part 6, and is transported by the hydrogen isotope detection part. 4 and is detected.
つまり第1の加熱源23を膜部6の表面に取付
けることなく、自然対流による強制循環が可能と
なるため、被測定ガス中の水素、トリチウムが膜
部6を透過する際の悪影響をなくし正確な水素同
位体の濃度を測定し得る水素同位体測定装置を提
供するそとが可能となる。 In other words, forced circulation by natural convection is possible without attaching the first heating source 23 to the surface of the membrane part 6, which eliminates the negative effects of hydrogen and tritium in the gas to be measured when they permeate through the membrane part 6, thereby ensuring accuracy. It becomes possible to provide a hydrogen isotope measurement device that can measure the concentration of hydrogen isotopes.
たとえば前記第1図に示した装置においては膜
部6の表面のヒーター7のみで設定値500℃まで
昇温した際、温度勾配は膜部6の長さ100mmの時
下端から上端では50℃温度となり、またヒーター
7の表面温度の直接の影響と輸送ガスによる影響
を受けるため、設定値を保持することが非常にむ
ずかしく常に±10℃の幅で振れている。 For example, in the apparatus shown in FIG. 1, when the temperature is raised to a set value of 500°C using only the heater 7 on the surface of the membrane part 6, the temperature gradient is 50°C from the lower end to the upper end when the length of the membrane part 6 is 100 mm. Since it is directly affected by the surface temperature of the heater 7 and by the transport gas, it is very difficult to maintain the set value and it always fluctuates within a range of ±10°C.
次に標準ガスを用いて較正を行つた測定値の不
規則な分布値は±20%程度もあり非常に再現性の
悪い結果であつた。 Next, calibration was performed using a standard gas, and the irregular distribution of measured values was about ±20%, resulting in extremely poor reproducibility.
これに対して第2図に示す本発明に係る装置は
膜部6の設定値を同じく500℃とした場合全く温
度勾配は見られず±2℃以内で設定値を保持する
ことが可能であつた。 On the other hand, in the device according to the present invention shown in FIG. 2, when the set value of the membrane section 6 is also set at 500°C, no temperature gradient is observed and the set value can be maintained within ±2°C. Ta.
つぎに標準ガスを用いて較正を行つた結果、ば
らつきもなく非常に再現性の良い結果を得た。 Next, we performed calibration using a standard gas, and as a result, we obtained results with very good reproducibility and no variation.
つまり本発明によれば温度コントロールを精度
良く行うことを可能とし、更に膜部6を水素、ト
リチウムが透過する際の悪影響をなくし、信頼で
きる水素同位体濃度を得ることが可能となつた。 In other words, according to the present invention, it is possible to perform temperature control with high precision, and furthermore, it has become possible to eliminate the adverse effects when hydrogen and tritium permeate through the membrane portion 6, and to obtain a reliable hydrogen isotope concentration.
以上述べたように本発明によれば水素、トリチ
ウムを選択透過させる拡散膜部に直接温度検知素
子を取り付けることができるので筒状体20と第
1の加熱源23および第2の加熱源24によつて
起る自然対流によつて被測定ガスを循環させ、か
つ第3の加熱源29で輸送ガスによる悪影響をな
くすことができ、拡拡散膜部の温度コントロール
を精度良く行うことが可能となり、したがつて膜
部6を水素、トリチウムが透過する際の悪影響も
なくなり、信頼性の高い水素同位体測定装置を提
供することができる。 As described above, according to the present invention, since the temperature sensing element can be directly attached to the diffusion membrane part that selectively permeates hydrogen and tritium, The gas to be measured can be circulated by the natural convection that occurs, and the third heating source 29 can eliminate the adverse effects of the transport gas, making it possible to accurately control the temperature of the diffusion membrane section. Therefore, there is no adverse effect when hydrogen and tritium permeate through the membrane portion 6, and a highly reliable hydrogen isotope measuring device can be provided.
また自然対流を利用して拡散膜部を加熱するこ
とによつて、水素同位体検出部の水素同位体を直
接測定することができる。 Furthermore, by heating the diffusion membrane section using natural convection, it is possible to directly measure the hydrogen isotope in the hydrogen isotope detection section.
さらに被測定ガスのサンプリングラインが不要
となるため装置が大幅に小型化でき、スペース的
に余裕のない場所にも設定でき、しかもコストダ
ウンできる効果がある。 Furthermore, since there is no need for a sampling line for the gas to be measured, the device can be significantly downsized, can be installed in locations with limited space, and has the effect of reducing costs.
第1図は従来の水素同位体測定装置を一部ブロ
ツク的に示す断面図、第2図は本発明に係る水素
同位体測定装置の一実施例を一部ブロツク的に示
す断面図である。
1……被測定ガス、2……開口部、3……フラ
ンジ、4……水素同位体検出部、5……管状体、
6……拡散膜部、7……ヒータ、8……温度検出
素子、9……温度制御装置、10……輸送ガス供
給管、11……バルブ、12……輸送ガス源、1
3……弁、20……筒状体、21……ガス流入
孔、22……ガス流出孔、23……第1の加熱
部、24……第2の加熱源、25,26,30…
…温度検出素子、27,28,31……温度制御
装置、29……第3の加熱源、32……ガス流
路。
FIG. 1 is a partially block sectional view of a conventional hydrogen isotope measuring device, and FIG. 2 is a partially block sectional view of an embodiment of the hydrogen isotope measuring device according to the present invention. DESCRIPTION OF SYMBOLS 1... Gas to be measured, 2... Opening, 3... Flange, 4... Hydrogen isotope detection section, 5... Tubular body,
6... Diffusion membrane section, 7... Heater, 8... Temperature detection element, 9... Temperature control device, 10... Transport gas supply pipe, 11... Valve, 12... Transport gas source, 1
3... Valve, 20... Cylindrical body, 21... Gas inflow hole, 22... Gas outflow hole, 23... First heating section, 24... Second heating source, 25, 26, 30...
... Temperature detection element, 27, 28, 31 ... Temperature control device, 29 ... Third heating source, 32 ... Gas flow path.
Claims (1)
された水素の同位体を検出する検出部と、この検
出部に連通しかつ前記被測定ガス室内に気密に挿
入され水素を選択的に透過させる拡散膜部を接続
した管状体と、前記被測定ガス室外に配置された
輸送ガス源からバルブを介して前記管状体内に挿
入されかつ前記被散膜部内の下部近傍まで垂下し
た輸送ガス供給パイプと、被測定ガス室内に設け
られ前記管状体を空間を存して包囲しかつ被測定
ガスを下方から上方へ向けて流すガス流入孔およ
び流出孔を有する筒状体と、この筒状体内の下部
に配置され前記拡散膜部外面のほぼ底部を間接加
熱する第1の加熱源と、前記筒状体と拡散膜部と
のほぼ接続部分近傍を直接加熱する第2の加熱源
と、前記被測定ガス室外の輸送ガス供給パイプを
加熱する第3の加熱源とを具備したことを特徴と
する水素同位体測定装置。 2 輸送ガスは加熱源により所定の温度に加熱さ
れ温度制御されて拡散膜部に流入されることを特
徴とする特許請求の範囲第1項記載の水素同位体
測定装置。 3 第1から第3の加熱源にはそれぞれ温度検出
素子の信号によつて任意の温度に温度制御される
温度制御装置が設けられ被測定ガスを所定の温度
に保持することを特徴とする特許請求の範囲第1
項記載の水素同位体測定装置。[Scope of Claims] 1. A gas chamber to be measured, a detection section arranged outside the gas chamber for detecting a hydrogen isotope, and a gas chamber connected to the detection section and inserted airtight into the gas chamber to be measured. A tubular body connected to a diffusion membrane portion that selectively permeates hydrogen, and a transport gas source placed outside the measured gas chamber inserted into the tubular body via a valve and extending to the vicinity of the lower portion within the diffusion membrane portion. A cylindrical body having a hanging transport gas supply pipe, a gas inflow hole and an outflow hole that are provided in a gas to be measured chamber and surround the tubular body with a space therein, and allow the gas to be measured to flow from below to above. , a first heat source disposed at the lower part of the cylindrical body that indirectly heats substantially the bottom of the outer surface of the diffusion membrane portion; and a second heat source that directly heats substantially the vicinity of the connection portion between the cylindrical body and the diffusion membrane portion. A hydrogen isotope measuring device comprising: a heating source; and a third heating source that heats a transport gas supply pipe outside the measured gas chamber. 2. The hydrogen isotope measurement device according to claim 1, wherein the transport gas is heated to a predetermined temperature by a heating source, temperature-controlled, and then flows into the diffusion membrane section. 3. A patent characterized in that each of the first to third heating sources is provided with a temperature control device that controls the temperature to an arbitrary temperature based on a signal from a temperature detection element, and maintains the gas to be measured at a predetermined temperature. Claim 1
Hydrogen isotope measuring device described in Section 2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55143025A JPS5767871A (en) | 1980-10-15 | 1980-10-15 | Measuring device for hydrogen isotope |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55143025A JPS5767871A (en) | 1980-10-15 | 1980-10-15 | Measuring device for hydrogen isotope |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5767871A JPS5767871A (en) | 1982-04-24 |
| JPS6140334B2 true JPS6140334B2 (en) | 1986-09-09 |
Family
ID=15329154
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55143025A Granted JPS5767871A (en) | 1980-10-15 | 1980-10-15 | Measuring device for hydrogen isotope |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5767871A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0641982B2 (en) * | 1984-09-29 | 1994-06-01 | アロカ株式会社 | Device for measuring tritium radioactivity in gas |
-
1980
- 1980-10-15 JP JP55143025A patent/JPS5767871A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5767871A (en) | 1982-04-24 |
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