JPH056864B2 - - Google Patents

Info

Publication number
JPH056864B2
JPH056864B2 JP3509685A JP3509685A JPH056864B2 JP H056864 B2 JPH056864 B2 JP H056864B2 JP 3509685 A JP3509685 A JP 3509685A JP 3509685 A JP3509685 A JP 3509685A JP H056864 B2 JPH056864 B2 JP H056864B2
Authority
JP
Japan
Prior art keywords
infrared
gas
cell
measurement
measurement gas
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
Application number
JP3509685A
Other languages
Japanese (ja)
Other versions
JPS61194333A (en
Inventor
Ryuzo Kano
Kenji Hirai
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP60035096A priority Critical patent/JPS61194333A/en
Publication of JPS61194333A publication Critical patent/JPS61194333A/en
Publication of JPH056864B2 publication Critical patent/JPH056864B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/35Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
    • G01N21/3504Investigating 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

Landscapes

  • 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】 (イ) 産業上の利用分野 この発明は赤外線ガス分析計に関し、詳しくは
赤外線領域におけるガス分子の赤外線吸収の強さ
によりガス濃度を測定する非分散型赤外線ガス分
析計に関する。
[Detailed Description of the Invention] (a) Industrial Application Field This invention relates to an infrared gas analyzer, and more specifically, a non-dispersive infrared gas analyzer that measures gas concentration based on the strength of infrared absorption of gas molecules in the infrared region. Regarding.

(ロ) 従来の技術 一般に赤外線ガス分析計は、測定用の赤外線透
過セル(以下測定セルと称す。)と比較用の赤外
線透過セル(以下比較セルと称す。)を備え、こ
の両セルの赤外線透過光量の差を、コンデンサー
マイクロホン又はマイクロフローセンサーを用い
たガス封入形の検出器(ニユーマテイク検出器)
で圧力の差として検出するものである。
(B) Prior art In general, an infrared gas analyzer is equipped with an infrared transmission cell for measurement (hereinafter referred to as the measurement cell) and an infrared transmission cell for comparison (hereinafter referred to as the comparison cell), and the infrared rays of both cells are A gas-filled detector (Numatake detector) uses a condenser microphone or micro flow sensor to detect the difference in the amount of transmitted light.
It is detected as a pressure difference.

従来上記検出器を用いた測定方法には、ネガテ
イブフイルタ法とポジテイブフイルタ法とがあ
る。
Conventional measurement methods using the above detector include a negative filter method and a positive filter method.

このネガテイブフイルタ法の光学系は、第7図
に示すように、一対の光源エレメント1,1から
の赤外線が、それぞれ窒素ガスなどの不活性ガス
を封入した赤外線透過セル2と測定対象ガスを封
入した赤外線透過セル(3、以下ガスセルと称
す。)を透過し、さらに測定ガスが流通する測定
セル4と比較セル5とをそれぞれ透過し検出器6
のコンデンサ膜7によつて仕切られた2つの赤外
線吸収室8,9に入射されるよう構成されてい
る。なお、10はチヨツパー、11はチヨツパ駆
動モータである。
In the optical system of this negative filter method, as shown in FIG. 7, infrared rays from a pair of light source elements 1, 1 are transmitted through an infrared transmitting cell 2 filled with an inert gas such as nitrogen gas and a gas to be measured, respectively. The infrared transmitting cell (3, hereinafter referred to as gas cell) is transmitted through the infrared transmission cell (3, hereinafter referred to as gas cell), and further transmitted through the measurement cell 4 and comparison cell 5 through which the measurement gas flows.
The infrared light is incident on two infrared absorption chambers 8 and 9 separated by a capacitor film 7. Note that 10 is a chopper and 11 is a chopper drive motor.

この方式において、両赤外線吸収室8,9に赤
外線が入射されると、両赤外線吸収室8,9内の
圧力が変化してコンデンサ膜7を測定セル4透過
後の赤外線が入射する赤外線吸収室8側にわん曲
させる。これによつて検出器6のコンデンサ容量
が変化して測定ガス中の測定対象成分の濃度が測
定される。
In this method, when infrared rays are incident on both infrared absorption chambers 8 and 9, the pressure inside both infrared absorption chambers 8 and 9 changes, and the infrared rays enter the capacitor film 7 after passing through the measurement cell 4. Curve it to the 8th side. As a result, the capacitor capacity of the detector 6 changes, and the concentration of the component to be measured in the measurement gas is measured.

第8図及び第9図はチヨツパ10の回転による
コンデンサ膜7のわん曲状態を示す図及び検出器
6のコンデンサ容量の変化を示すグラフである。
8 and 9 are diagrams showing the curved state of the capacitor film 7 due to the rotation of the chopper 10, and graphs showing changes in the capacitor capacitance of the detector 6. FIG.

上記方式で測定ガスの濃度を測定した場合、測
定セル4透過後の赤外線が入射する赤外線吸収室
8では測定ガス中の測定対象成分と干渉成分の赤
外線の吸収が起る。一方もう1つの赤外線吸収室
9ではガスセル3で測定ガス中の測定対象成分の
殆どが吸収されるので、わずかな測定対象成分の
吸収と干渉成分の吸収が起る。このとき干渉成分
の吸収量を他の赤外線吸収室8の吸収量とほぼ同
じ大きさになるようにすると干渉のない測定を行
うことができる。
When the concentration of the measurement gas is measured by the above method, absorption of the infrared rays of the components to be measured and interference components in the measurement gas occurs in the infrared absorption chamber 8 into which the infrared rays after passing through the measurement cell 4 are incident. On the other hand, in the other infrared absorption chamber 9, most of the component to be measured in the measurement gas is absorbed by the gas cell 3, so that a small amount of the component to be measured and the interference component are absorbed. At this time, if the absorption amount of the interference component is made to be approximately the same as the absorption amount of the other infrared absorption chambers 8, measurement without interference can be performed.

しかし、この場合、比較セル5透過後の赤外線
が入射する赤外線吸収室9においても測定ガス中
の測定対象成分の吸収がわずかに起つているた
め、別の赤外線吸収室8での測定ガス中の測定対
象成分の吸収がキヤンセルされる。これによつて
ネガテイブフイルタ法ではポジテイブフイルタ法
に比べ3〜4割検出器6の出力が小さくなる。し
たがつてネガテイブフイルタ法では測定ガス中の
測定対象成分の濃度が限界値より低くなると、そ
の濃度を測定できなくなる不都合があつた。ま
た、干渉を補償する場合、測定セル4と比較セル
5との長さを同一にすると、干渉の補償が大きく
なり干渉が負になることがある。したがつて、こ
の点を考慮してネガテイブフイルタ法の光学系を
設計する必要があつた。
However, in this case, slight absorption of the component to be measured in the measurement gas occurs even in the infrared absorption chamber 9 into which the infrared rays after passing through the comparative cell 5 enter, so that the absorption of the measurement target component in the measurement gas in another infrared absorption chamber 8 occurs. Absorption of the component to be measured is canceled. As a result, in the negative filter method, the output of the detector 6 becomes 30 to 40% smaller than in the positive filter method. Therefore, the negative filter method has the disadvantage that when the concentration of the component to be measured in the measurement gas becomes lower than a limit value, the concentration cannot be measured. Furthermore, when compensating for interference, if the lengths of the measurement cell 4 and the comparison cell 5 are made the same, the compensation for interference becomes large and the interference may become negative. Therefore, it was necessary to design an optical system for the negative filter method in consideration of this point.

この発明は以上の事情に鑑みなされたもので、
その主要な目的の1つは、ネガテイブフイルタ法
のコンデンサマイクロホンの出力が従来の2倍の
出力になるように構成し、測定ガス中の測定対象
成分の濃度が低くても高感度にその濃度を測定き
るようにすることにあり、もう1つの主要な目的
は、比較セルの長さを測定セルの長さに関係なく
干渉補償が最適になる長さにすることができきる
よう構成し、干渉の小さい光学系を作ることがで
きるようにすることにある。
This invention was made in view of the above circumstances,
One of the main objectives is to configure a negative filter condenser microphone to have twice the output of a conventional condenser microphone, and to detect the concentration of the target component in the measurement gas with high sensitivity even when the concentration is low. Another main purpose is to configure the length of the comparison cell to be the length that optimizes interference compensation regardless of the length of the measurement cell. The objective is to make it possible to create a small optical system.

(ハ) 構成 この発明は、赤外線ガス分析計であつて、赤外
線を対向して放射する一対の光源と、この両光源
間の光路上に設けられた赤外線透過セルと、この
赤外線透過セルに接続された赤外線検出器とを備
え、赤外線透過セルに測定ガス導入部及び測定ガ
ス排出部を設けるとともに、赤外線検出器を、光
路を介して対向して設置されかつ測定ガス又はこ
のガスと同等のガスが充填された一対の赤外線吸
収室と、光路を遮断しないよう両赤外線吸収室を
連結する連結部と、両赤外線吸収室間の光路上に
回動可能に設置された両面反射鏡と、両赤外線吸
収室に両光源からの赤外線が交互に入射しうるよ
う両面反射鏡を回動させる反射鏡駆動手段と、前
記連結部内に設けられ両赤外線吸収室内の圧力差
を検出し測定ガス中の測定対象成分の濃度測定信
号を出力する検出手段とから構成したものであ
る。
(c) Structure This invention is an infrared gas analyzer, which includes a pair of light sources that emit infrared rays in opposition, an infrared transmitting cell provided on the optical path between the two light sources, and a connection to the infrared transmitting cell. The infrared transmitting cell is equipped with an infrared detector and an infrared detector, and the infrared transmitting cell is provided with a measurement gas introduction part and a measurement gas discharge part. A pair of infrared absorption chambers filled with a reflector driving means for rotating a double-sided reflector so that the infrared rays from both light sources can be alternately incident on the absorption chamber; and a reflector drive means provided in the connecting part for detecting the pressure difference between the two infrared absorption chambers to be measured in the measurement gas. and a detection means for outputting a component concentration measurement signal.

すなわち、この発明は、測定ガス中の測定対象
成分の濃度測定に際し、反射鏡駆動手段で反射鏡
を回動させると、赤外線が両赤外線吸収室に交互
に入射し、これによつて生ずる両赤外線吸収室の
圧力差を検出手段で検出するように構成したもの
である。
In other words, in the present invention, when the reflector is rotated by the reflector drive means when measuring the concentration of the component to be measured in the measurement gas, infrared rays are alternately incident on both infrared absorption chambers, and both infrared rays are thereby generated. It is configured so that the pressure difference in the absorption chamber is detected by a detection means.

(ホ) 実施例 以下第1図から第5図に示す実施例に基づいて
この発明を詳述する。なお、これによつてこの発
明が限定されるものではない。
(E) Embodiments The present invention will be described in detail below based on embodiments shown in FIGS. 1 to 5. Note that this invention is not limited to this.

第1図におい赤外線ガス分析計12は、赤外線
を対向して放射する一対の光源13,13と、両
光源13,13間の光路14上にその一方の光源
13側から他方の光源13側に向かつて順に連設
された測定セル15、赤外線検出器16、比較セ
ル17及び測定ガスが封入されたガスセル18と
から主として構成される。
In FIG. 1, the infrared gas analyzer 12 includes a pair of light sources 13, 13 that emit infrared rays in opposite directions, and an optical path 14 between the two light sources 13, 13 from one light source 13 side to the other light source 13 side. It mainly consists of a measurement cell 15, an infrared detector 16, a comparison cell 17, and a gas cell 18 filled with a measurement gas, which are arranged in series in this order.

測定セル15及び比較セル17は、筒状の赤外
線透過セルからなり、その筒壁には測定ガス導入
部19,20と測定ガス排出部21,22とがそ
れぞれ設けられている。
The measurement cell 15 and the comparison cell 17 are made of cylindrical infrared transmitting cells, and the cylindrical walls thereof are provided with measurement gas introduction sections 19 and 20 and measurement gas discharge sections 21 and 22, respectively.

赤外線検出器16は、第2図及び第3図に示す
ように、測定ガスが充填された一対の赤外線吸収
室23,23と、両面反射鏡(ミラー)24と、
ミラー駆動モータ25と、両赤外線吸収室23の
圧力差を検出し検出信号を出力する検出手段26
とを備え、両赤外線吸収室23は、前記光路14
を介して光路14に直交する方向に対向して設置
され、光路14を遮断しないように赤外線検出器
16に設けられた連結部27によつて連結されて
いる。一方、ミラー24は、その面が光路14に
直交し両赤外線吸収室23側に回動可能に光路1
4上に設置されている。また、上記検出手段26
は、金属薄膜(コンデンサ膜)28と対極29と
からなるコンデンサマイクロホンで構成されてい
る。なお、検出手段26としてはこの他、マイク
ロフローセンサを用いてもよい。
As shown in FIGS. 2 and 3, the infrared detector 16 includes a pair of infrared absorption chambers 23, 23 filled with a measurement gas, a double-sided reflector (mirror) 24,
Mirror drive motor 25 and detection means 26 that detects the pressure difference between both infrared absorption chambers 23 and outputs a detection signal.
Both infrared absorption chambers 23 are provided with the optical path 14.
are installed facing each other in a direction perpendicular to the optical path 14, and are connected by a connecting portion 27 provided on the infrared detector 16 so as not to interrupt the optical path 14. On the other hand, the mirror 24 has its surface perpendicular to the optical path 14 and is rotatable toward both the infrared absorption chambers 23.
It is installed on 4. Further, the detection means 26
is composed of a capacitor microphone consisting of a metal thin film (capacitor film) 28 and a counter electrode 29. In addition, as the detection means 26, a micro flow sensor may be used.

次に上記分析計12の作動を説明する。なお、
測定ガスとしては、一酸化炭素、二酸化イオン、
一酸化窒素などの排ガスが用いられる。
Next, the operation of the analyzer 12 will be explained. In addition,
Measurement gases include carbon monoxide, dioxide ions,
Exhaust gas such as nitrogen monoxide is used.

まず、測定ガスを測定セル15及び比較セル1
7に導入する。次いで測定ガス中の測定対象成分
の濃度測定に際し、ミラー駆動モータ25を作動
させてミラー24を回動させると、赤外線が両赤
外線吸収室23に交互に入射される。そこで、両
赤外線吸収室23内に圧力差が生じ、これによつ
て金属薄膜28は第4図に示すように両赤外線吸
収室23側に交互にわん曲し、検出手段26から
第5図に示すような信号が出力される。そしてこ
の出力信号に基づいて上記濃度が測定される。
First, the measurement gas is applied to the measurement cell 15 and comparison cell 1.
7 will be introduced. Next, when measuring the concentration of the component to be measured in the measurement gas, when the mirror drive motor 25 is operated to rotate the mirror 24, infrared rays are alternately incident on both the infrared absorption chambers 23. Therefore, a pressure difference is generated in both infrared absorption chambers 23, and as a result, the metal thin film 28 is bent alternately toward both infrared absorption chambers 23 as shown in FIG. A signal like the one shown is output. The concentration is then measured based on this output signal.

このように検出手段26のコンデンサ容量の変
化は従来の2倍となり高感度の濃度測定を行うこ
とができる。また、測定セル15と光源13との
間に不活性ガスを封入したセルを設ける必要がな
いので、従来より高感度の濃度測定ができる。さ
らに、測定セルの長さに関係なく比較セルの長さ
を設定できるため、干渉影響を極めて小さくする
ことができ、その上比較セルのみの長さを変えて
も余分な空間が分析計に生ずることがなくなるた
め、測定値が分析計周囲のガスの影響を受けるこ
とがなくなる。以上によつてS/N値の優れた赤
外線分析計を得ることができる。
In this manner, the change in capacitance of the capacitor of the detection means 26 is twice that of the conventional method, allowing concentration measurement to be performed with high sensitivity. Further, since there is no need to provide a cell filled with inert gas between the measurement cell 15 and the light source 13, concentration measurement can be performed with higher sensitivity than in the past. Furthermore, since the length of the comparison cell can be set regardless of the length of the measurement cell, the influence of interference can be minimized, and even if only the length of the comparison cell is changed, extra space will be created in the analyzer. Therefore, the measured values are no longer affected by the gas surrounding the analyzer. As a result of the above, an infrared analyzer with an excellent S/N value can be obtained.

第6図は他の実施例の示す図で、13a,13
aは光源、15aは測定セル、23a,23aは
赤外線吸収室、24aはミラーである。この実施
例は、第1実施例の比較セル17及びガスセルを
除いて構成したものである。
FIG. 6 is a diagram showing another embodiment, 13a, 13
a is a light source, 15a is a measurement cell, 23a, 23a are infrared absorption chambers, and 24a is a mirror. This example is constructed by omitting the comparative cell 17 and gas cell of the first example.

(ヘ) 効果 この発明は、両光源からの赤外線が交互に両赤
外線吸収室に入射しうるよう構成したものである
から、検出手段の出力信号を従来の2倍にするこ
とができる。したがつて、高感度に測定ガス中の
測定対象成分の濃度を測定することができる効果
を奏する。
(F) Effects This invention is configured so that infrared rays from both light sources can be incident on both infrared absorbing chambers alternately, so that the output signal of the detection means can be doubled compared to the conventional one. Therefore, it is possible to measure the concentration of the component to be measured in the measurement gas with high sensitivity.

【図面の簡単な説明】[Brief explanation of drawings]

第1図はこの発明に係る赤外線ガス分析装置の
一実施例を示す構成説明図、第2図はこの検出器
の縦断面図、第3図は第2図のA−A断面図、第
4図はこの金属薄膜のわん曲状態説明図、第5図
はコンデンサマイクロホンの出力信号を示すグラ
フ、第6図はこの他の実施例の第1図相当図、第
7図、第8図及び第9図はそれぞれ従来例の第1
図、第4図及び第5図相当図である。 12……赤外線ガス分析計、13……光源、1
4……光路、15……測定セル(赤外線透過セ
ル)、16……赤外線検出器、19……測定ガス
導入部、21……測定ガス排出部、23……赤外
線吸収室、24……ミラー(反射鏡)、25……
ミラー駆動モータ(反射鏡駆動手段)、26……
検出手段、27……連結部。
Fig. 1 is a configuration explanatory diagram showing one embodiment of an infrared gas analyzer according to the present invention, Fig. 2 is a longitudinal sectional view of this detector, Fig. 3 is a sectional view taken along line A-A in Fig. The figure is an explanatory diagram of the curved state of this metal thin film, Figure 5 is a graph showing the output signal of the condenser microphone, Figure 6 is a diagram corresponding to Figure 1 of other embodiments, Figures 7, 8 and 8. Figure 9 shows the first conventional example.
FIG. 4 is a diagram corresponding to FIG. 4 and FIG. 5. 12...Infrared gas analyzer, 13...Light source, 1
4... Optical path, 15... Measurement cell (infrared transmission cell), 16... Infrared detector, 19... Measurement gas introduction section, 21... Measurement gas discharge section, 23... Infrared absorption chamber, 24... Mirror (Reflector), 25...
Mirror drive motor (reflector drive means), 26...
Detection means, 27...connection section.

Claims (1)

【特許請求の範囲】 1 赤外線を対向して放射する一対の光源と、こ
の両光源間の光路上に設けられた赤外線透過セル
と、この赤外線透過セルに接続された赤外線検出
器とを備え、赤外線透過セルに測定ガス導入部及
び測定ガス排出部を設けるとともに、赤外線検出
器を、光路を介して対向して設置されかつ測定ガ
ス又はこのガスと同等のガスを充填された一対の
赤外線吸収室と、光路を遮断しないよう両赤外線
吸収室を連結する連結部と、両赤外線吸収室間の
光路上に回動可能に設置された両面反射鏡と、両
赤外線吸収室に両光源からの赤外線が交互に入射
しうるよう両面反射鏡を回動させる反射鏡駆動手
段と、前記連結部内に設けられ両赤外線吸収室内
の圧力差を検出し測定ガス中の測定対象成分の濃
度測定信号を出力する検出手段とから構成してな
る赤外線分析計。 2 検出手段が、コンデンサマイクロホンもしく
はマイクロフローセンサからなる請求の範囲第1
項記載の赤外線分析計。 3 赤外線検出器側の光源と赤外線検出器との間
の光路上に、赤外線検出器に接続され測定ガス導
入部及び測定ガス排出部を備えた比較用の赤外線
透過セルと、この赤外線透過セルの赤外線検出器
とは反対側に接続され測定ガス又はこのガスと同
等のガスが封入された赤外線透過セルとを設けて
なる請求の範囲第1項記載の赤外線ガス分析計。
[Claims] 1. A device comprising: a pair of light sources that emit infrared rays in opposition; an infrared transmitting cell provided on an optical path between the two light sources; and an infrared detector connected to the infrared transmitting cell; An infrared transmission cell is provided with a measurement gas introduction part and a measurement gas discharge part, and an infrared detector is installed facing each other via an optical path, and a pair of infrared absorption chambers are filled with a measurement gas or a gas equivalent to this gas. , a connecting part that connects both infrared absorption chambers so as not to interrupt the optical path, a double-sided reflector that is rotatably installed on the optical path between both infrared absorption chambers, and an infrared ray from both light sources that enters both infrared absorption chambers. a reflector drive means for rotating the double-sided reflector so that the infrared rays can be incident alternately; and a detection device provided in the connecting portion for detecting the pressure difference between the two infrared absorption chambers and outputting a concentration measurement signal of the component to be measured in the measurement gas. An infrared analyzer consisting of means. 2. Claim 1 in which the detection means is a condenser microphone or a microflow sensor.
Infrared analyzer described in section. 3. On the optical path between the light source and the infrared detector on the infrared detector side, there is an infrared transmitting cell for comparison that is connected to the infrared detector and equipped with a measurement gas introduction part and a measurement gas discharge part, and an infrared transmission cell of this infrared transmission cell. 2. The infrared gas analyzer according to claim 1, further comprising an infrared transmission cell connected to the opposite side of the infrared detector and filled with a measurement gas or a gas equivalent to this gas.
JP60035096A 1985-02-22 1985-02-22 infrared gas analyzer Granted JPS61194333A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60035096A JPS61194333A (en) 1985-02-22 1985-02-22 infrared gas analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60035096A JPS61194333A (en) 1985-02-22 1985-02-22 infrared gas analyzer

Publications (2)

Publication Number Publication Date
JPS61194333A JPS61194333A (en) 1986-08-28
JPH056864B2 true JPH056864B2 (en) 1993-01-27

Family

ID=12432410

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60035096A Granted JPS61194333A (en) 1985-02-22 1985-02-22 infrared gas analyzer

Country Status (1)

Country Link
JP (1) JPS61194333A (en)

Also Published As

Publication number Publication date
JPS61194333A (en) 1986-08-28

Similar Documents

Publication Publication Date Title
US3872315A (en) Radiation sensitive fluid analyzer
US4236827A (en) Opto-acoustic gas analyzer
US5559333A (en) Apparatus of non-dispersive infrared analyzer
CN114813574A (en) Differential photoacoustic spectrum gas concentration detection device based on dual-channel T-shaped photoacoustic cell
US4281248A (en) Nondispersive infrared gas analyzer
US4598201A (en) Infrared fluid analyzer employing a pneumatic detector
JP2009257808A (en) Infrared gas analyzer
US3970387A (en) Nondispersion, two beam, infrared gas analyzer
JPH07128231A (en) Infrared gas sensor
JP3070177B2 (en) Two-component gas analyzer
US3968369A (en) Non-dispersive infrared gas analysis device with triple layer receiver
JPH056864B2 (en)
JPH0217429A (en) Concentration measuring method by using laser type gas sensor
JP2001188037A (en) Gas analyzer
JPH0529061B2 (en)
JP2811563B2 (en) CO analyzer
US20220236175A1 (en) Nondispersive infrared-type carbon dioxide gas sensor
JP3177379B2 (en) Oil concentration meter
JPH0412822B2 (en)
JP2004061207A (en) Infrared gas analyzer
JPH06281578A (en) Gas analyzer
JPH048350Y2 (en)
JP3046673B2 (en) Gas analyzer
JPS61243343A (en) Ultraviolet ray absorption gas analyzer
JPH018993Y2 (en)