JPH0625730B2 - Analyzer - Google Patents
AnalyzerInfo
- Publication number
- JPH0625730B2 JPH0625730B2 JP18994786A JP18994786A JPH0625730B2 JP H0625730 B2 JPH0625730 B2 JP H0625730B2 JP 18994786 A JP18994786 A JP 18994786A JP 18994786 A JP18994786 A JP 18994786A JP H0625730 B2 JPH0625730 B2 JP H0625730B2
- Authority
- JP
- Japan
- Prior art keywords
- gas
- hydrogen
- concentration
- measurement
- sensor
- 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
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- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] 水素ガスはヘリウムガスを除く他のガスに比べてはるか
に大きな拡散計数をもっている。本発明は、このような
拡散係数の違いを利用して水素ガスの濃度を求める分析
計に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial application] Hydrogen gas has a much larger diffusion coefficient than other gases except helium gas. The present invention relates to an analyzer that determines the concentration of hydrogen gas by utilizing such a difference in diffusion coefficient.
[従来の技術] 従来、水素ガスの濃度を測定できる分析計としては、例
えばガスクロマトグラフがある。[Prior Art] Conventionally, as an analyzer capable of measuring the concentration of hydrogen gas, there is, for example, a gas chromatograph.
[発明が解決しようとする問題点] しかし、ガスクロマトグラフでは、連続測定が不可能で
あり、また広い測定範囲にしようとすると構成が複雑に
なるという問題点がある。[Problems to be Solved by the Invention] However, in a gas chromatograph, there are problems that continuous measurement is impossible and the structure becomes complicated when a wide measurement range is attempted.
本考案は上述した問題点を除去するためになされたもの
であり、測定ガス中の水素の濃度を広範囲に連続測定で
きる分析計を簡単な構成で実現することを目的とする。The present invention has been made to eliminate the above-mentioned problems, and an object thereof is to realize an analyzer capable of continuously measuring the concentration of hydrogen in a measurement gas in a wide range with a simple configuration.
[問題点を解決するための手段] 本発明は、 一定方向に定流量の特定ガスが流れていて、下流側の一
端では、この特定ガスに水素を含む測定ガスを混ぜ合わ
せ、水素を特定ガスの流れと逆方向に拡散させる測定管
と、 この測定管の所定の位置での水素の濃度を検出するセン
サと、 このセンサの検出信号から、測定ガス中の水素と他の成
分の拡散速度の相違をもとにして測定ガス中の水素の濃
度を求める演算部、 を具備した分析計である。[Means for Solving Problems] According to the present invention, a constant flow rate of a specific gas flows in a fixed direction, and at one end on the downstream side, the specific gas is mixed with a measurement gas containing hydrogen, and hydrogen is supplied to the specific gas. Measurement tube that diffuses in the direction opposite to the flow of the gas, a sensor that detects the hydrogen concentration at a predetermined position of this measurement tube, and the detection signal of this sensor that determines the diffusion rate of hydrogen and other components in the measurement gas. The analyzer is provided with a calculation unit for obtaining the concentration of hydrogen in the measurement gas based on the difference.
[実施例] 以下、図面を用いて本発明を説明する。[Examples] The present invention will be described below with reference to the drawings.
第1図は本発明にかかる分析計の一実施例の構成図であ
る。FIG. 1 is a block diagram of an embodiment of the analyzer according to the present invention.
図で、1は測定管であり、内部をガス供給器2によって
供給された特定ガスが一定方向(A方向)に定速で流れ
る。特定ガスは既知の成分のもので、例えば空気、酸
素、窒素ガス等である。測定管1の一端11では特定ガ
スと測定ガスが混ぜられる。In the figure, reference numeral 1 is a measuring tube, through which a specific gas supplied by a gas supplier 2 flows in a constant direction (direction A) at a constant speed. The specific gas has a known component, and is, for example, air, oxygen, nitrogen gas or the like. At one end 11 of the measuring tube 1, the specific gas and the measuring gas are mixed.
3は測定管1の流路に設けられていて、設置位置での水
素の濃度を検出する検出機である。センサ3としては例
えばジルコニア素子が用いられる。A detector 3 is provided in the flow path of the measuring tube 1 and detects the concentration of hydrogen at the installation position. As the sensor 3, for example, a zirconia element is used.
4は演算部であり、センサ3の検出信号から、水素と他
の気体との拡散速度の相違を利用して、測定ガス中の水
素の濃度を算出する。A calculation unit 4 calculates the concentration of hydrogen in the measurement gas from the detection signal of the sensor 3 by utilizing the difference in diffusion rate between hydrogen and another gas.
次に、このような分析計の測定原理について説明する。Next, the measurement principle of such an analyzer will be described.
測定管1の一端11を0位置として、特定ガスの流れと
逆方向を正方向としたX軸をとる。x=0の位置での測
定ガスの各成分の濃度をそれぞれC10,C20,…C
N0、位置xの測定ガスの各成分の濃度をそれぞれC1
(x),C2(x),…CN(x)とする。The one end 11 of the measuring tube 1 is set to the 0 position, and the X axis is taken with the direction opposite to the flow of the specific gas as the positive direction. The concentrations of the components of the measurement gas at the position of x = 0 are C 10 , C 20 , ... C, respectively.
The concentration of each component of the measurement gas at N 0 and the position x is C 1
(X), C 2 (x), ... C N (x).
ここで、位置xでのガスN(測定ガス中の一成分)の濃
度CN(x)の分布を求める。Here, the distribution of the concentration C N (x) of the gas N (one component in the measurement gas) at the position x is obtained.
ガスNの特定ガス中での拡散係数をDNとすると、拡散
によってガスNがx方向に運ばれる量JNは、もしこの
位置での流れがなければ、次式のように、ガスNの濃度
勾配に拡散係数をかけたものになる。If the diffusion coefficient of the gas N in the specific gas is D N , the amount J N of the gas N carried in the x direction by diffusion is calculated by the following equation if the gas N is not flowed at this position. It is the concentration gradient times the diffusion coefficient.
今、特定ガスは定流量で流れているので、濃度C
N(x)の気体が流速vで拡散の方向とは逆向きに運ば
れ、ガスNの正味の流れ量Kは、 となる。濃度CN(x)が特定ガスの流れの上流へいく
ほど薄くなることによって、ガスNの拡散量と流される
量が各位置で平衡している。平衡状態になったときに
は、K=0となるから、 となり、これによって濃度CN(x)は次式で与えられ
る。 Since the specific gas is flowing at a constant flow rate now, the concentration C
The gas of N (x) is carried at a flow velocity v in the direction opposite to the direction of diffusion, and the net flow amount K of the gas N is Becomes The concentration C N (x) becomes thinner toward the upstream of the flow of the specific gas, so that the diffusion amount of the gas N and the flow amount thereof are in equilibrium at each position. When in equilibrium, K = 0, so Therefore, the concentration C N (x) is given by the following equation.
式の計算結果の一例を第2図に示す。第2図のグラフ
では、縦軸にln{CN(x)}、横軸に位置xをとり
(lnは自然対数)、拡散計数DNをパラメータとした
ものである。 An example of the calculation result of the formula is shown in FIG. In the graph of FIG. 2, the vertical axis is l n {C N (x)}, the horizontal axis is the position x (1 n is a natural logarithm), and the diffusion coefficient D N is used as a parameter.
この図で、a1,a2,a3はそれぞれH2(水素)、
CH4(メタン)、CO(一酸化炭素)のグラフであ
る。In this figure, a 1 , a 2 , and a 3 are H 2 (hydrogen),
It is a graph of CH 4 (methane) and CO (carbon monoxide).
このような結果から、H2ガス計としての分析計を考え
る。センサが可燃ガスに対して感度をもつものを使った
と仮定すると、CO、CH4等による干渉が問題にな
る。拡散計数は、H2が0.611に対し、CH4は
0.196なので、流速が5cm/secで、H2、C
H4の初期の濃度がそれぞれ10%だったとすると、各
位置でのH2、CH4の濃度とこれらの気体の濃度比は
第3図のようになる。From such a result, an analyzer as an H 2 gas meter will be considered. Assuming that the sensor used has sensitivity to combustible gas, interference due to CO, CH 4, etc. becomes a problem. Diffusion counts, to H 2 is 0.611, CH 4 is so 0.196, a flow rate is 5cm / sec, H 2, C
Assuming that the initial concentration of H 4 is 10%, the concentrations of H 2 and CH 4 at each position and the concentration ratio of these gases are as shown in FIG.
CH4ガスの拡散係数はH2ガスの拡散係数よりも小さ
いので、図に示すように、x=5,10mmの位置では
CH4の濃度はH2の濃度に比べて十分小さくなってい
る。このため、干渉誤差は問題ない。Since the diffusion coefficient of CH 4 gas is smaller than that of H 2 gas, the concentration of CH 4 is sufficiently smaller than the concentration of H 2 at the position of x = 5,10 mm as shown in the figure. Therefore, the interference error is not a problem.
また、COの拡散計数はCH4の拡散係数よりも小さい
ので、干渉誤差は更に小さくなる。Further, since the diffusion coefficient of CO is smaller than the diffusion coefficient of CH 4 , the interference error becomes smaller.
実際の測定では、式でv,x,DNが既知でC
N(x)が測定値として求められるため、これらから測
定ガス中の水素濃度CN0を求める。In the actual measurement, v, x, D N are known in the equation, and C
Since N (x) is obtained as a measurement value, the hydrogen concentration C N0 in the measurement gas is obtained from these.
センサ3としてジルコニア素子を用いれば、1ppb
(parts per billion)以下でも測定
可能であるため、きわめて微量のものから100%に至
るまでの広い濃度範囲で使用可能なH2ガス計が実現で
きる。If a zirconia element is used as the sensor 3, 1 ppb
Since it is possible to measure even below (parts per billion), it is possible to realize an H 2 gas meter that can be used in a wide concentration range from a very small amount to 100%.
なお、分析計はH2ガス以外の拡散係数の大きなガス例
えばHe(ヘリウム)ガス等を測定するものであっても
よい。The analyzer may be a gas that has a large diffusion coefficient other than H 2 gas, such as He (helium) gas.
[効果] このような分析計によれば、水素の拡散係数が他のガス
よりも大きいことを利用して濃度を測定しているため、
干渉誤差が小さくなり、簡単な構成で広範囲の測定が可
能になる。例えば、第2図の例ではx=5mmを選ぶと
き、センサが10ppbまで測定可能ならば、1ppm
から100%までの106のダイナミックレンジでの測
定が可能になる。[Effect] According to such an analyzer, the concentration is measured by utilizing the fact that the diffusion coefficient of hydrogen is larger than that of other gases.
The interference error is reduced, and a wide range of measurement is possible with a simple configuration. For example, in the example of FIG. 2, when x = 5 mm is selected, if the sensor can measure up to 10 ppb, 1 ppm
It is possible to measure in a dynamic range of 10 6 from 10 to 100%.
これに加えて、センサ3が常時濃度検出を行っているた
め、連続測定が可能になる。In addition to this, since the sensor 3 constantly detects the concentration, continuous measurement is possible.
第1図は本発明にかかる分析計の一実施例の構成図、第
2図及び第3図は第1図装置の測定結果の一例を示した
図である。 1……測定管、11……一端、2……ガス供給器、3…
…センサ、4……演算部。FIG. 1 is a block diagram of an embodiment of the analyzer according to the present invention, and FIGS. 2 and 3 are diagrams showing an example of measurement results of the apparatus of FIG. 1 ... Measuring tube, 11 ... One end, 2 ... Gas supply device, 3 ...
... Sensor, 4 ... Calculator.
Claims (1)
て、下流側の一端では、この特定ガスに水素を含む測定
ガスを混ぜ合わせ、水素を特定ガスの流れと逆方向に拡
散させる測定管と、 この測定管の所定の位置での水素の濃度を検出するセン
サと、 このセンサの検出信号から、測定ガス中の水素と他の成
分の拡散速度の相違をもとにして測定ガス中の水素の濃
度を求める演算部、 を具備した分析計。1. A measurement in which a constant flow rate of a specific gas flows in a fixed direction, and a measurement gas containing hydrogen is mixed with this specific gas at one end on the downstream side to diffuse hydrogen in the direction opposite to the flow of the specific gas. A tube, a sensor that detects the hydrogen concentration at a predetermined position of this measuring tube, and the detection signal of this sensor, which is used to measure the concentration of hydrogen in the measuring gas based on the difference in the diffusion rates of hydrogen and other components. An analyzer equipped with a calculation unit for determining the hydrogen concentration of.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18994786A JPH0625730B2 (en) | 1986-08-13 | 1986-08-13 | Analyzer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18994786A JPH0625730B2 (en) | 1986-08-13 | 1986-08-13 | Analyzer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6345532A JPS6345532A (en) | 1988-02-26 |
| JPH0625730B2 true JPH0625730B2 (en) | 1994-04-06 |
Family
ID=16249861
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18994786A Expired - Lifetime JPH0625730B2 (en) | 1986-08-13 | 1986-08-13 | Analyzer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0625730B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0676960B2 (en) * | 1984-12-12 | 1994-09-28 | 株式会社日立製作所 | Method and apparatus for evaluating remaining life of mechanical structure subjected to repeated load |
| CN107787311A (en) | 2015-04-24 | 2018-03-09 | 康宁股份有限公司 | With reference to zirconia refractory and the method that manufactures it |
| JP7103641B2 (en) * | 2018-10-29 | 2022-07-20 | 株式会社グッドマン | Leakage search device and leak search method |
-
1986
- 1986-08-13 JP JP18994786A patent/JPH0625730B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6345532A (en) | 1988-02-26 |
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