JPH0135292B2 - - Google Patents
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- Publication number
- JPH0135292B2 JPH0135292B2 JP616084A JP616084A JPH0135292B2 JP H0135292 B2 JPH0135292 B2 JP H0135292B2 JP 616084 A JP616084 A JP 616084A JP 616084 A JP616084 A JP 616084A JP H0135292 B2 JPH0135292 B2 JP H0135292B2
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- Prior art keywords
- gas
- cell
- interference
- filled
- cells
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3504—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing gases, e.g. multi-gas analysis
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- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は干渉除去セルを実質的に除去すること
により小型化を可能にした多成分赤外線ガス分析
計に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a multi-component infrared gas analyzer that can be miniaturized by substantially eliminating an interference cancellation cell.
ガス中に含まれる各成分がそれぞれ一定の波長
域の赤外線を吸収することを利用して被測定ガス
中の含有成分、濃度を測定する赤外線ガス分析計
は、測定濃度範囲が広いこと、多成分中の一成分
を検出でき選択性に富むこと、各成分の連続で迅
速な分析ができること、ほとんど全ての気体は赤
外線を吸収するので、いろいろな工程管理に使用
でき応用分野が広いことなど多くの優れた特徴を
有している。そして、この種の赤外線ガス分析計
は、一般にCO、CO2、CH4等の混合ガスとして
の被測定ガス入れた試料セル(サンプルセル)に
赤外線を照射し、このセルを透過した透過光を一
定の回転数で回転するロータに設けた特別なフイ
ルターを通し、さらにこれを例えば半導体素子
(フオトセル)のような光電変換素子で電気的に
検出することにより、各ガス成分の検出値を比較
測定するように構成されている。
Infrared gas analyzers, which measure the content and concentration of gases by utilizing the fact that each component contained in the gas absorbs infrared rays in a certain wavelength range, have a wide measurement concentration range and are capable of measuring multiple components. It has many advantages, such as being able to detect one component in the gas and being highly selective, being able to continuously and quickly analyze each component, and almost all gases absorb infrared rays, so it can be used for various process control and has a wide range of applications. It has excellent characteristics. This type of infrared gas analyzer generally irradiates a sample cell (sample cell) containing a gas to be measured in the form of a mixed gas such as CO, CO 2 , CH 4 , etc. with infrared rays, and then detects the transmitted light that has passed through the cell. The detected values of each gas component are compared and measured by passing it through a special filter installed on a rotor that rotates at a constant rotational speed, and then electrically detecting it with a photoelectric conversion element such as a semiconductor element (photocell). is configured to do so.
ところで、かゝる赤外線ガス分析計において
は、2成分以上の混合気体の定量分析を行う場
合、測定対象ガス以外のガス成分による干渉を除
去するため、通常特定波長域の赤外線だけを通す
光学フイルターを使用している。しかし、このフ
イルターの通過領域に吸収波長を有するガス成分
が光路上に存在すると、このガス成分によつて干
渉を受ける。そこで、この干渉を除去する手段と
して干渉成分ガスを封入した干渉除去セルを光路
上に配設することが一般的に行われている。 By the way, in such an infrared gas analyzer, when performing quantitative analysis of a gas mixture of two or more components, an optical filter is usually installed that passes only infrared rays in a specific wavelength range in order to eliminate interference from gas components other than the gas to be measured. are using. However, if a gas component having an absorption wavelength in the passage region of this filter exists on the optical path, interference will occur due to this gas component. Therefore, as a means for removing this interference, it is common practice to dispose an interference removal cell filled with an interference component gas on the optical path.
ここで、干渉除去セルを用いた従来の赤外線分
析計を第1図に基づいて概略説明すると、1は光
源、2は測定対象ガス10としての例えば4.3μm
に吸収スペクトルを有するCO2を含んだ混合ガス
が連続的に供給されるサンプルセル、3は高速回
転されるロータ、4は測定ガス(CO2)と同じガ
スが高濃度で封入されたリフアレンスセル、5は
赤外線に対して不活性(赤外線を吸収しない)な
ガス(通常N2 ガス)が封入された不活性ガス
封入セル、6は前記リフアレンスセル4を透過す
る赤外線過波長領域に吸収波長を持つガスを干渉
成分ガスとして高濃度で封入した干渉除去セル、
7は集光器、8は検出器で、前記リフアレンスセ
ル4と不活性ガス封入セル5とは前記ロータ3に
配設されている。また、これら両セル4,5には
測定対象となる吸収波長帯(4.3μm)の近辺だけ
通過し、それ以外の波長域の通過を遮断する狭帯
域透過型干渉フイルタ9をそれぞれ備えている。
したがつて、CO2ガスが封入された前記サンプル
セル4に光源1からの赤外線を照射すると、その
透過特性は、第2図に示されるように中心波長
4.3μm、半値幅0.2μm以下の波長領域の赤外線が
透過する。 Here, a conventional infrared analyzer using an interference removal cell will be briefly explained based on FIG.
3 is a rotor that rotates at high speed, and 4 is a reference chamber that is filled with the same gas as the measurement gas (CO 2 ) at a high concentration. A cell 5 is an inert gas-filled cell filled with a gas (usually N2 gas) that is inert to infrared rays (does not absorb infrared rays); 6 is an inert gas-filled cell that absorbs in the infrared overwavelength region that passes through the reference cell 4; Interference removal cell filled with a high concentration of gas with a wavelength as an interference component gas,
7 is a condenser, 8 is a detector, and the reference cell 4 and the inert gas-filled cell 5 are arranged on the rotor 3. Further, both cells 4 and 5 are each equipped with a narrowband transmission type interference filter 9 that allows only the vicinity of the absorption wavelength band (4.3 μm) to be measured to pass through and blocks the passage of other wavelength bands.
Therefore, when the sample cell 4 filled with CO 2 gas is irradiated with infrared rays from the light source 1, its transmission characteristics change to the center wavelength as shown in FIG.
Infrared rays in the wavelength range of 4.3 μm and a half width of 0.2 μm or less are transmitted.
CO2ガスの測定に際して、先ずサンプルセル2
中の測定対象ガス10を無視した場合、光源1か
ら放射された赤外線はロータ3の回転に伴い光路
11を交互に横切るリフアレンスセル4と不活性
ガス封入セル5を通過し、更に干渉徐去セル6を
通過した後集光器7によつて集光され、検出器8
で検出される。この時の光量の変動を第3図に示
すと、aは不活性ガス封入セル5に通過した赤外
線の光量、bはリフアレンスセル4を通過した赤
外線の光量である。同図bの黒く塗りつぶした縦
線部分はCO2によつて吸収された光量で、これは
CO2の吸収が4.3μm付近のすべての波長に対して
生じるのではなく、4.3μm付近のある特定(複
数)の波長のみが吸収をうけるためである。そし
て、同図aの光量(斜線部)が前記検出器8によ
つて電気信号に変換され、増幅器によつて増幅さ
れた後測定信号(電圧)となり、bの光量(斜線
部)が同じく検出器8によつて電気信号に変換さ
れ基準電圧となる。 When measuring CO 2 gas, first
When the gas to be measured 10 inside is ignored, the infrared rays emitted from the light source 1 pass through the reference cell 4 and the inert gas-filled cell 5, which alternately cross the optical path 11 as the rotor 3 rotates, and further eliminate interference. After passing through the cell 6, the light is collected by a condenser 7 and sent to a detector 8.
Detected in The variation in the amount of light at this time is shown in FIG. 3, where a is the amount of infrared light that has passed through the inert gas filled cell 5, and b is the amount of infrared light that has passed through the reference cell 4. The black vertical line in Figure b is the amount of light absorbed by CO 2 , which is
This is because absorption of CO 2 does not occur at all wavelengths around 4.3 μm, but only at certain specific (plural) wavelengths around 4.3 μm. The amount of light (shaded area) in figure a is converted into an electrical signal by the detector 8, which is amplified by the amplifier and becomes a measurement signal (voltage), and the amount of light shown in b (shaded area) is also detected. The signal is converted into an electrical signal by the converter 8 and becomes a reference voltage.
次に、サンプルセル2中にCO2が存在すると、
CO2によつて波長4.3μm付近の赤外線が吸収(こ
の場合も第3図bのような吸収となる)されるた
め、不活性ガス封入セル5を透過する測定光の光
量は減少する。同様にリフアレンスセル4を透過
する基準光の光量もサンプルセル2中のCO2によ
る吸収により減少するが、その減少の割合は既に
サンプルセル2中のCO2で吸収されているため、
前記不活性ガス封入セル5における光量の減少よ
り少ない。演算回路では通常〔測定光の減少割合
>基準光の減少割合〕のとき出力が正になるよう
に回路が作られている。 Next, if CO 2 is present in sample cell 2,
Since infrared rays having a wavelength of around 4.3 μm are absorbed by CO 2 (absorption as shown in FIG. 3b also occurs in this case), the amount of measurement light transmitted through the inert gas-filled cell 5 decreases. Similarly, the amount of reference light transmitted through the reference cell 4 also decreases due to absorption by CO 2 in the sample cell 2, but the proportion of this decrease has already been absorbed by the CO 2 in the sample cell 2.
This is smaller than the decrease in the amount of light in the inert gas filled cell 5. The arithmetic circuit is usually constructed so that the output becomes positive when [reduction rate of measurement light>reduction rate of reference light].
そして、あらかじめCO2ガスの濃度と出力との
関係を測定しておけば、実ガスの濃度を測定する
ことができる。 If the relationship between the concentration of CO 2 gas and the output is measured in advance, the concentration of the actual gas can be measured.
ところで、前記狭帯域透過型干渉フイルタ9の
透過波長領域に吸収波長を持つガス(CO2に対し
て例えばCO)がサンプルセル2中に存在すると
干渉を生じる。この場合出力が正、負のとちらに
シフトするかは干渉成分ガスと測定対象ガス
(CO2)の吸収波長の違いによつて異なり、(イ)干
渉成分ガスの吸収波長がCO2の吸収波長と重なる
場合、(ロ)干渉成分ガスの吸収波長がCO2の吸収波
長と重ならない場合および(ハ)干渉成分ガスの吸収
波長がCO2の吸収波長と一部重なり他が重らない
場合とがある。 By the way, if a gas having an absorption wavelength in the transmission wavelength region of the narrowband transmission type interference filter 9 (for example, CO as opposed to CO 2 ) exists in the sample cell 2, interference will occur. In this case , whether the output shifts to positive or negative depends on the difference in absorption wavelength between the interference component gas and the gas to be measured (CO 2 ). (b) When the absorption wavelength of the interfering component gas does not overlap with the absorption wavelength of CO 2 ; and (c) When the absorption wavelength of the interfering component gas partially overlaps with the absorption wavelength of CO 2 but not others. There is.
(イ)の場合、第4図a,bに示すようにCO2の吸
収波長λaに干渉ガスが吸収波長を持つと、〔測定
光の減少割合>基準光の減少割合〕となり、干渉
ガスにより出力は正にシフトする。一方、(ロ)の場
合は同図c,dに示すようにCO3の吸収波長以外
の波長λbに干渉ガスが吸収波長を持つと、〔測定
光の減少割合<基準光の減少割合〕となり、出力
は負にシフトする。例えば、測定光10に対して
1の減少、基準光5に対して同じく1の減少の場
合、これらはそれぞれ10%および20%に当り、前
述の不当式<を成立させる。そして、(ハ)の場合
は、同図e,fに示すようにCO2と重る部分λaと
重らない部分λbとに干渉ガスが吸収波長を持つ
と、λaとλbとでの吸収割合の違いで
測定光の減少割合>基準光の減少割合
〃 〃 < 〃 〃
〃 〃 = 〃 〃
の3つの場合が生じ、干渉ガスによるシフトは
正、負、0(無)になる。 In the case of (a), if the interference gas has an absorption wavelength at the absorption wavelength λa of CO 2 as shown in Figure 4 a and b, then [reduction rate of measurement light > reduction rate of reference light], and the interference gas The output shifts positively. On the other hand, in case (b), as shown in c and d of the same figure, if the interference gas has an absorption wavelength at a wavelength λb other than the absorption wavelength of CO 3 , [reduction rate of measurement light < reduction rate of reference light]. , the output shifts negatively. For example, if the measurement light 10 is decreased by 1 and the reference light 5 is also decreased by 1, these correspond to 10% and 20%, respectively, and the above-mentioned unreasonable expression < holds true. In the case of (c), if the interfering gas has an absorption wavelength in the part λa that overlaps with CO 2 and the part λb that does not overlap with CO 2, as shown in e and f in the same figure, the absorption ratio between λa and λb will be Due to the difference in the rate of decrease of the measurement light > the rate of decrease of the reference light, three cases occur: 〃 〃 < 〃 〃 〃 〃 = 〃 〃, and the shift due to the interference gas is positive, negative, or 0 (nothing).
このように狭帯域透過型干渉フイルタ9の通過
領域に吸収波長を有するガス成分が光路11上に
存在すると、それにより干渉を受けるため、これ
を防ぐべく従来は干渉成分ガスを封入した干渉除
去セル6を光路11上に配設しているが、このよ
うな構成においては光軸方向の長さが長くなり、
分析部、換言すれば分析計自体の長大化まねき、
しかも部品としてセルが1個増加するという不都
合があつた。 If a gas component having an absorption wavelength in the passage area of the narrowband transmission interference filter 9 exists on the optical path 11, it will cause interference.To prevent this, conventional interference removal cells filled with interference component gas have been used. 6 is disposed on the optical path 11, but in such a configuration, the length in the optical axis direction becomes long,
The analysis department, in other words, the analyzer itself, will become longer.
Moreover, there was the problem that one cell was added as a component.
そこで、このような不都合を解消するものとし
て、例えば、各測定ガス成分を個々に封入してな
るリフアレンスセルに付加的フイルタ点を設け、
その中に干渉ガス成分を封入することにより実質
的に干渉除去セルを除去してなる多成分赤外線分
析計(特公昭56−34814号公報)がある。しかし、
このような装置においても、各リフアレンスセル
に同じ濃度で飽和状態の干渉ガス成分を封入する
必要があるため、その手間が面倒であつた。 Therefore, as a solution to this inconvenience, for example, an additional filter point may be provided in a reference cell in which each measurement gas component is individually sealed.
There is a multi-component infrared spectrometer (Japanese Patent Publication No. 34814/1983) in which an interference removal cell is substantially eliminated by enclosing an interfering gas component therein. but,
Even in such a device, it is necessary to fill each reference cell with an interfering gas component in a saturated state at the same concentration, which is troublesome.
本発明は上述したような点に鑑みてなされたも
ので、各測定ガス成分を個別に封入した複数個の
リフアレンスセルと、これらリフアレンスセルと
同数個の不活性ガス封入セルと、測定対象ガスが
供給されるサンプルセルとを備え、前記各リフア
レンスセルもしくはこれと対応する前記不活性ガ
ス封入セルのいずれか一方に、干渉ガスによる減
光比がこれら両セルほぼ同等となるよう干渉ガス
を封入して構成することにより、干渉ガスを封入
するための手間を簡素化し得るようにした多成分
赤外線ガス分析計を供給するものである。
The present invention has been made in view of the above-mentioned points, and includes a plurality of reference cells individually filled with each measurement gas component, the same number of inert gas filled cells as these reference cells, and a measurement target. A sample cell to which a gas is supplied, and an interference gas is supplied to either the reference cell or the corresponding inert gas filled cell so that the attenuation ratio due to the interference gas is approximately the same for both cells. The purpose of the present invention is to provide a multicomponent infrared gas analyzer which can simplify the effort required to enclose interference gas by encapsulating the interfering gas.
以下、本発明を図面に示す実施例に基づいて詳
細に説明する。 Hereinafter, the present invention will be described in detail based on embodiments shown in the drawings.
第5図は本発明の一実施例を示す断面図、第6
図はロータの正面図である。これらの図におい
て、20はロータ3を一定速度で高速回転させる
モータ、21は増幅器、22は前記ロータ3にリ
フアレンスセル4および不活性ガス封入セル5を
狭帯域透過型干渉フイルタ9と共に形成する赤外
線透過窓(例えばフツ化カルシウム(CaF2))で
ある。
FIG. 5 is a sectional view showing one embodiment of the present invention, and FIG.
The figure is a front view of the rotor. In these figures, 20 is a motor that rotates the rotor 3 at a constant speed, 21 is an amplifier, and 22 is a reference cell 4 and an inert gas-filled cell 5 formed on the rotor 3 together with a narrowband transmission type interference filter 9. An infrared transparent window (eg calcium fluoride (CaF 2 )).
前記リフアレンスセル4としては前記ロータ3
にその回転中心を中心とする同一周面上に周方向
に適宜間隔をおいて2個形成され、その一方の4
aに例えば測定ガス成分としてのCO2が高濃度で
封入され、他方4bに他の測定ガス成分としての
COが高濃度で封入されている。同様に、前記不
活性ガス封入セル5も前記ロータ3に前記リフア
レンスセル4と同一円周上に各リフアレンスセル
4a,4bに対応して2個5a,5b設けられ、
その夫々に赤外線に対して不活性なN2、O2ガス
(通常N2 ガス)が封入されている。 As the reference cell 4, the rotor 3
Two pieces are formed on the same circumferential surface centered on the rotation center at appropriate intervals in the circumferential direction, and one of the four
For example, CO 2 as a measurement gas component is sealed in 4b at a high concentration, and 4b is filled with other measurement gas components.
Contains a high concentration of CO. Similarly, two inert gas filled cells 5 are provided on the rotor 3 on the same circumference as the reference cell 4, corresponding to each reference cell 4a, 4b,
Each of them is filled with N 2 and O 2 gases (usually N 2 gas) that are inert to infrared rays.
ここで、サンプルセル2に測定対象ガス10と
して、4.3μmと4.7μmにそれぞれ吸収スペクトル
を持つCO2とCOを含んだ混合ガスを連続的に供
給して測定する場合には、一方の測定対象ガス
(例えばCO2)に対して他方の測定対象ガス
(CO)が同じ狭帯域透過干渉フイルタ9の透過波
長領域に吸収波長を持つため、干渉ガスとして作
用する。同様にCOの測定に際してはCO2が干渉
ガスとして作用する。そこで、測定対象ガスCO2
を封入してなる前記一方のリフアレンスセル4a
(もしくは該リフアレンスセル4aに対応する不
活性ガス封入セル5a)には更にCOが干渉ガス
として封入される。このCOの濃度は前記サンプ
ルセル2および不活性ガス封入セル5aを透過し
て検出器8により検出される測定光と、前記サン
プルセル2およびリフアレンスセル4aを透過し
て検出される基準光の減少割合がほぼ同等になる
ように設定される。同様に測定対象ガスCOを封
入してなる他方のリフアレンスセル4b(もしく
はリフアレンスセル4bに対応する不活性ガス封
入セル5b)にも干渉ガスとしてCO2が封入され
ており、その濃度は、前記サンプルセル2および
不活性ガス封入セル5bを透過して検出される測
定光と、前記サンプルセル2およびリフアレンス
セル4bを透過して検出される基準光の減少割合
がほぼ同等になるよう設定されている。 Here, when measuring by continuously supplying a mixed gas containing CO 2 and CO, which have absorption spectra at 4.3 μm and 4.7 μm, respectively, as the measurement target gas 10 to the sample cell 2, one of the measurement targets Since the gas (CO) to be measured, which is the other gas (for example, CO 2 ), has an absorption wavelength in the transmission wavelength region of the same narrow band transmission interference filter 9, it acts as an interference gas. Similarly, CO 2 acts as an interfering gas when measuring CO. Therefore, the gas to be measured, CO 2
The one reference cell 4a is enclosed with
(or the inert gas filled cell 5a corresponding to the reference cell 4a) is further filled with CO as an interference gas. The concentration of CO is determined by the measurement light transmitted through the sample cell 2 and inert gas-filled cell 5a and detected by the detector 8, and the reference light transmitted through the sample cell 2 and reference cell 4a and detected. The reduction rate is set to be approximately the same. Similarly, the other reference cell 4b (or the inert gas filled cell 5b corresponding to the reference cell 4b) filled with the measurement target gas CO is also filled with CO 2 as an interference gas, and its concentration is as follows. Set so that the reduction rate of the measurement light transmitted through the sample cell 2 and the inert gas filled cell 5b and the reference light transmitted through the sample cell 2 and the reference cell 4b is approximately the same. has been done.
干渉ガス(CO、CO2)の封入に際しては前述
した通り干渉ガスと測定対象ガスの吸収波長の違
いにより、(イ)干渉成分ガスの吸収波長がCO2の吸
収波長と重る場合、(ロ)重らない場合および(ハ)一部
が重る場合の3態様があるため、(イ)の重る場合に
は不活性ガス封入セル5a,5bにそれぞれ干渉
ガスを封入して測定先の減少割合を小さくし、干
渉をなくす(干渉ガスのある濃度で干渉は0とな
る。)。一方、(ロ)の重らない場合にはリフアレンス
セル4a,4bに測定対象ガス(CO2、CO)と
共に干渉ガス(CO、CO2)をそれぞれ封入して
基準光の減少割合を小さくし、干渉を減らす(干
渉ガスのある濃度で干渉は0となる)。そして(ハ)
の一部が重り他が重らない場合には、測定光と基
準光の減少割合により出力のシフト方向が正また
は負を知ることで、正のときには上記(イ)を、負の
ときは上記(ロ)を採用し、干渉を減らす(干渉ガス
のある濃度で干渉は0となる)。 When enclosing an interfering gas (CO, CO 2 ), as mentioned above, due to the difference in absorption wavelength between the interfering gas and the gas to be measured, (a) if the absorption wavelength of the interfering component gas overlaps with the absorption wavelength of CO 2 , (b) There are three cases: (a) no overlap and (c) a partial overlap.In the case of (b), interference gas is filled in the inert gas filled cells 5a and 5b, respectively, and the measurement target is Reduce the rate of decrease and eliminate interference (at a certain concentration of interfering gas, interference becomes 0). On the other hand, in the case of (b) when there is no overlap, interference gases (CO, CO 2 ) are filled in the reference cells 4a and 4b together with the gas to be measured (CO 2 , CO ) to reduce the rate of decrease in the reference light. , reduce the interference (at a certain concentration of the interfering gas the interference becomes 0). And (c)
If some of them are heavy and others do not overlap, then by knowing whether the output shift direction is positive or negative depending on the reduction ratio of the measurement light and reference light, if it is positive, use the above (a), and if it is negative, use the above (b) is adopted to reduce interference (interference becomes 0 at a certain concentration of interfering gas).
なお、前記各干渉ガス(CO、CO2)を不活性
ガス封入セル5a,5bに封入した場合には、実
質的にこれらのセル5a,5bが干渉除去セルを
構成するため、不活性ガスN2の封入を必要とし
ない。 Note that when each of the interference gases (CO, CO 2 ) is sealed in the inert gas filled cells 5a, 5b, these cells 5a, 5b substantially constitute an interference removal cell, so the inert gas N 2 does not require inclusion.
また、第5図において第1図と同一構成要素の
ものに対しては同一符号を以つて示し、その説明
を省略する。 Further, in FIG. 5, the same components as those in FIG. 1 are designated by the same reference numerals, and their explanations will be omitted.
かくしてこのような構成からなる赤外線ガス分
析装置によれば、干渉ガス(CO、CO2)をリフ
アレンスセル4a,4bもしくは不活性ガス封入
セル5a,5bのいずれか一方にそれぞれ封入し
ているので、第1図に示した干渉除去セル6を除
去することができ、したがつて光路11を干渉除
去セル6の長さだけ短かくすることが可能とな
る。 According to the infrared gas analyzer having such a configuration, the interference gas (CO, CO 2 ) is sealed in either the reference cells 4a, 4b or the inert gas filled cells 5a, 5b. , the interference cancellation cell 6 shown in FIG. 1 can be removed, and therefore the optical path 11 can be shortened by the length of the interference cancellation cell 6.
また、干渉ガス(CO、CO2)は測定光の減少
割合と基準光の減少割合とがほぼ同等になるよう
にその濃度を変えてリフアレンスセル4a,4b
もしくは不活性ガス封入セル5a,5bのいずれ
か一方にそれぞれ封入すればよいので、干渉ガス
の封入作業が双方に封入する場合に比べて簡単で
あり、しかも不活性ガス封入セル5a,5bに封
入する場合には不活性ガス自身の封入を不要と
し、経済的である。 In addition, the concentration of the interference gas (CO, CO 2 ) is changed so that the rate of decrease in the measurement light and the rate of decrease in the reference light are approximately the same, and the interference gases (CO, CO 2 ) are used in the reference cells 4a and 4b.
Alternatively, it is sufficient to fill either one of the inert gas filled cells 5a, 5b, respectively, so the work of filling the interfering gas is easier than filling both of them, and moreover, the interfering gas is filled in the inert gas filled cells 5a, 5b. In this case, it is not necessary to fill in the inert gas itself, which is economical.
また、従来は干渉ガスを高濃度で封じなければ
ならず、特にリフアレンスセル4a,4bにはそ
の性質から測定対象ガスも高濃度で封入する必要
がある。このため、リフアレンスセル4a,4b
の内圧が高くなり、赤外線透過窓22の接着強度
を高める必要がある。そこで内圧を低くするため
セル長を長くする方法もあるが、その場合には構
造が大きくなる欠点がある。 Furthermore, conventionally, interference gas must be sealed at a high concentration, and in particular, the reference cells 4a and 4b must also be filled with a gas to be measured at a high concentration due to their properties. For this reason, the reference cells 4a, 4b
As the internal pressure of the infrared ray transmitting window 22 increases, it is necessary to increase the adhesive strength of the infrared transmitting window 22. Therefore, there is a method of increasing the cell length in order to lower the internal pressure, but this method has the disadvantage of increasing the size of the structure.
これに対して本発明は測定光と基準光の減少割
合がほぼ等しくなる濃度でよいため上記のような
問題を解決することができる。 On the other hand, the present invention can solve the above-mentioned problem because it is sufficient that the concentration is such that the reduction rate of the measurement light and the reference light are almost equal.
連続測定の過程においてサンプルセル2中の干
渉ガスの濃度が変化すれば、多成誤差を生じる
が、プロセス計測においては実用上の支障はな
い。 If the concentration of the interfering gas in the sample cell 2 changes during the process of continuous measurement, a multicomponent error will occur, but this will not cause any practical problems in process measurement.
なお、上記実施例は2成分のガス(CO2、CO)
を測定する場合について説明したが、本発明はこ
れに限らず、3成分、例えばCO2、CH4、COの
測定も可能でその場合には3個のリフアレンスセ
ルと3個の不活性ガス封入セルが使用される。 Note that the above example uses two component gases (CO 2 and CO).
Although the present invention is not limited to this, it is also possible to measure three components such as CO 2 , CH 4 , and CO, and in that case, three reference cells and three inert gases are required. Encapsulated cells are used.
以上説明したように本発明に係る多成分赤外線
ガス分析計は、それぞれ測定対象ガスを個別に封
入してなる各リフアレンスセルもしくはこれに対
応する不活性ガス封入セルのいずれか一方に、干
渉ガスによる測定光と基準光の減少割合が両セル
ほぼ同等になるよう前記干渉ガスを封入して構成
したので、干渉ガスの封入の手間が少なく、不活
性ガス封入セルに封入する場合には不活性ガスの
封入を必要とせず、またリフアレンスセルもしく
は不活性ガス封入セルが干渉除去セルを兼用する
ため、従来必要とされていた干渉除去セルを除去
でき、光路の短縮化、換言すれば分析計の小型化
を可能にする。また、干渉除去セルの除去により
セルが1つ減り、安価な分析計を提供することが
できる。
As explained above, the multi-component infrared gas analyzer according to the present invention has an interference gas in either the reference cells individually filled with the gases to be measured or the corresponding inert gas filled cells. Since the interference gas is filled in so that the reduction rate of the measurement light and the reference light is almost the same in both cells, there is less effort to fill in the interference gas, and when it is filled in an inert gas filled cell, it is possible to fill in an inert gas. Since there is no need to fill in gas, and the reference cell or inert gas filled cell also serves as an interference removal cell, the interference removal cell that was previously required can be removed, shortening the optical path, or in other words, making it easier for the analyzer to Enables downsizing. Further, by removing the interference cancellation cell, the number of cells is reduced by one, and an inexpensive analyzer can be provided.
第1図は従来の赤外線ガス分析計の一例を示す
断面図、第2図はCO2の透過特性を示す吸収スペ
クトル、第3図a,bはそれぞれ不活性ガス封入
セルとリフアレンスセルを透過した赤外線の光量
と波長との関係を示す図、第4図a〜fは干渉ガ
スによる出力のシフトを説明するための図、第5
図は本発明に係る多成分赤外線ガス分析計の一実
施例を示す断面図、第6図はロータの正面図であ
る。
1……光源、2……サンプルセル、3……ロー
タ、4,4a,4b………リフアレンスセル、
5,5a,5b……不活性ガス封入セル、8……
検出器、9……狭帯域透過型干渉フイルタ、10
……測定対象ガス、11……光路。
Figure 1 is a cross-sectional view showing an example of a conventional infrared gas analyzer, Figure 2 is an absorption spectrum showing the transmission characteristics of CO 2 , and Figures 3 a and b are transmission through an inert gas-filled cell and a reference cell, respectively. Figures 4a to 4f are diagrams showing the relationship between the amount of infrared rays and the wavelength;
The figure is a sectional view showing an embodiment of the multi-component infrared gas analyzer according to the present invention, and FIG. 6 is a front view of the rotor. 1...Light source, 2...Sample cell, 3...Rotor, 4, 4a, 4b...Reference cell,
5, 5a, 5b...Inert gas filled cell, 8...
Detector, 9...Narrowband transmission type interference filter, 10
...Gas to be measured, 11...Optical path.
Claims (1)
個のリフアレンスセルと、これらのリフアレンス
セルにそれぞれ対応する複数個の不活性ガス封入
セルとを高速回転するロータに該ロータの回転中
心から半径方向に等距離離れて周方向に設け、前
記各リフアレンスセルの透過光をこれに対応する
前記不活性ガス封入セルを透過した光とそれぞれ
比較して常時光軸上にあるサンプルセル内ガスの
複数のガス成分の各濃度を検出する多成分赤外線
ガス分析計において、前記各リフアレンスセルも
しくはこれと対応する前記不活性ガス封入セルの
いずれか一方に、干渉ガスによる減光比がこれら
両セルほぼ同等となるよう干渉ガスを封入したこ
とを特徴とする多成分赤外線ガス分析計。1. A plurality of reference cells individually filled with two or more measurement gas components and a plurality of inert gas filled cells corresponding to these reference cells are mounted on a rotor rotating at high speed from the rotation center of the rotor. The sample cells are arranged circumferentially at equal distances apart in the radial direction, and the light transmitted through each reference cell is compared with the light transmitted through the corresponding inert gas-filled cell, and the gas inside the sample cell is always on the optical axis. In a multi-component infrared gas analyzer that detects the respective concentrations of a plurality of gas components, either the reference cell or the corresponding inert gas-filled cell has an attenuation ratio due to an interference gas in both of them. A multi-component infrared gas analyzer characterized by filling an interference gas so that the cells are almost the same.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59006160A JPS60149949A (en) | 1984-01-17 | 1984-01-17 | Multi-component infrafed gas analyser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59006160A JPS60149949A (en) | 1984-01-17 | 1984-01-17 | Multi-component infrafed gas analyser |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60149949A JPS60149949A (en) | 1985-08-07 |
| JPH0135292B2 true JPH0135292B2 (en) | 1989-07-25 |
Family
ID=11630771
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59006160A Granted JPS60149949A (en) | 1984-01-17 | 1984-01-17 | Multi-component infrafed gas analyser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60149949A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2024181535A1 (en) * | 2023-03-02 | 2024-09-06 | 富士電機株式会社 | Gas analysis device |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2618554B1 (en) * | 1987-07-22 | 1990-02-23 | Moulene Daniel | METHOD FOR THE OPTICAL ANALYSIS OF A GAS IN A GAS MIXTURE |
| USRE36489E (en) * | 1994-04-06 | 2000-01-11 | Janos Technology Inc. | Spectral analyzer with new high efficiency collection optics and method of using same |
| US5428222A (en) * | 1994-04-06 | 1995-06-27 | Janos Technology Inc. | Spectral analyzer with new high efficiency collection optics and method of using same |
| US5585635A (en) * | 1994-09-26 | 1996-12-17 | Marquette Electronics, Inc. | Infrared gas analyzer and method |
| WO2006085646A1 (en) * | 2005-02-14 | 2006-08-17 | Japan Science And Technology Agency | Apparatus for gas concentration measuring according to gas correlation method |
| EP3561487B1 (en) | 2018-04-25 | 2023-01-18 | ABB Schweiz AG | Measuring device for analysis of a composition of a combustible gas with a filter chamber arranged in front of a detector |
-
1984
- 1984-01-17 JP JP59006160A patent/JPS60149949A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2024181535A1 (en) * | 2023-03-02 | 2024-09-06 | 富士電機株式会社 | Gas analysis device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60149949A (en) | 1985-08-07 |
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