JPH0560687A - Infrared analyzer - Google Patents

Infrared analyzer

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Publication number
JPH0560687A
JPH0560687A JP3225804A JP22580491A JPH0560687A JP H0560687 A JPH0560687 A JP H0560687A JP 3225804 A JP3225804 A JP 3225804A JP 22580491 A JP22580491 A JP 22580491A JP H0560687 A JPH0560687 A JP H0560687A
Authority
JP
Japan
Prior art keywords
gas
infrared
cell
light
wavelength
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.)
Pending
Application number
JP3225804A
Other languages
Japanese (ja)
Inventor
Takeo Ishigaki
武夫 石垣
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP3225804A priority Critical patent/JPH0560687A/en
Publication of JPH0560687A publication Critical patent/JPH0560687A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

(57)【要約】 【目的】 本発明は、産業用計測分野に用いられる赤外
分析装置に関するものであり、従来必ず必要であった参
照用標準セルを必要とせず、多種類ガス濃度を、一つの
焦電型リニアアレイセンサで同時測定することを目的と
する。 【構成】 赤外光源11の光を測定用ガスセル14に導
き、セルから出力した光を集光分光し、焦電形リニアア
レイ検出素子18で検知する。ガス吸収が少なく、大気
透過率の良い3.7μmの光により基準レベルを測定し
て、ガスセル中に導入されたCO2 ,CO,NO2 のガ
ス濃度により対応して得られた信号出力との差分をとる
ことにより参照用標準セルを用いることなく多種類のガ
ス濃度を同時に測定することができる。
(57) [Summary] [Object] The present invention relates to an infrared analyzer used in the field of industrial measurement, and does not require a standard cell for reference, which has always been necessary, and is capable of measuring various gas concentrations. The purpose is to perform simultaneous measurement with one pyroelectric linear array sensor. [Structure] The light from an infrared light source 11 is guided to a measurement gas cell 14, the light output from the cell is condensed and separated, and detected by a pyroelectric linear array detection element 18. The reference level was measured by 3.7 μm light with low gas absorption and good atmospheric transmittance, and the signal output was obtained corresponding to the gas concentration of CO 2 , CO, and NO 2 introduced into the gas cell. By taking the difference, it is possible to measure many kinds of gas concentrations at the same time without using a reference standard cell.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は環境計測、公害ガス計測
等の産業用計測分野、地球規模でのリモートセンシング
に用いられる赤外分析装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an industrial measuring field such as environmental measurement and pollution gas measurement, and an infrared analyzer used for remote sensing on a global scale.

【0002】[0002]

【従来の技術】近年、赤外分析装置は、公害ガス、自動
車排ガス測定に良く用いられている。また、人工衛星に
搭載した地球環境リモートセンシングにも用いられよう
としている。
2. Description of the Related Art In recent years, infrared analyzers have been widely used for measuring pollution gas and automobile exhaust gas. In addition, it is about to be used for remote sensing of the global environment mounted on artificial satellites.

【0003】以下、従来の赤外分析装置について説明す
る。図4は従来の赤外分析装置の構成を示すものであ
る。図4において、1は赤外光源である。2はチョッパ
ーの羽根である。3はモーターで、2のチョッパー羽根
を一定の速度で回転するものである。4は測定用ガスセ
ルである。5は4のガスセルの透過窓材である。6は参
照用標準セルであり一般的に乾燥窒素ガスが封入されて
いる。7はその透過窓材で6と同じものである。8は測
定対象ガスの吸収波長に合わせた赤外干渉フィルターで
あり、9はその波長の赤外光を検知する赤外センサであ
る。
A conventional infrared analyzer will be described below. FIG. 4 shows the configuration of a conventional infrared analyzer. In FIG. 4, 1 is an infrared light source. 2 is a chopper blade. 3 is a motor which rotates the chopper blades of 2 at a constant speed. 4 is a gas cell for measurement. 5 is a transparent window material for the gas cell of 4. Reference numeral 6 is a reference standard cell, which is generally filled with dry nitrogen gas. 7 is the same transparent window material as 6. Reference numeral 8 is an infrared interference filter that matches the absorption wavelength of the gas to be measured, and 9 is an infrared sensor that detects infrared light of that wavelength.

【0004】以上のように構成された赤外分析装置につ
いて、以下その動作について説明する。まず、赤外光源
1からの赤外線を測定用ガスセル4に導入されたある濃
度を持つガス層を通過させると、層透過後の特定波長の
赤外線の強さIは Lambert-Beerの法則に従う。
The operation of the infrared analyzer having the above structure will be described below. First, when the infrared ray from the infrared light source 1 is passed through the gas layer having a certain concentration introduced into the measuring gas cell 4, the intensity I of the infrared ray having the specific wavelength after passing through the layer follows Lambert-Beer's law.

【0005】[0005]

【数1】 [Equation 1]

【0006】ここで、 I0 ;入射光の強さ k(λ);波長(λ)の光の吸収係数 c ;ガス濃度 x ;ガス層の厚さ である。濃度が低い時には、k(λ)cx《1となるの
で、
Here, I 0 is the intensity of incident light k (λ); the absorption coefficient of light of wavelength (λ) c is the gas concentration x is the thickness of the gas layer. When the concentration is low, k (λ) cx << 1, so

【0007】[0007]

【数2】 [Equation 2]

【0008】と現され、赤外線の変化量△Iは、The change amount ΔI of infrared rays is expressed as

【0009】[0009]

【数3】 [Equation 3]

【0010】となり、△Iとガス濃度xとは比例する。
ふつうプリズムやグレーティングの様な光の分散装置を
有するものは少なく、一般に光源よりでた全ての波長域
の赤外線が測定に使用される。それ故、非分散型赤外線
ガス分析計(NDIR;Non Dispersive Infra-Red gasanal
yzer:のんデイスパーシブ インフラーレッド ガス
アナライザー)と呼ばれる。NDIRも使用する検出器の種
類によって正フィルター形と負フィルター形に分けられ
る。正フィルター形は検出器が波長依存性がある場合で
あり、負フィルター形は検出器に波長依存性がない場合
である。後者の場合、特定の波長に選択性をもたすには
赤外干渉フィルターを用いる。図4に示した赤外干渉フ
ィルター8は、特定ガス吸収線に合わせたものであり、
例えばCO2 であれば4.3μmを中心とした狭帯域フ
ィルターを用いる。この場合、ゼロ濃度レベルの赤外線
入射光の強さI0が必要になる。このI0 を得るため
に、一般的には吸収の無い乾燥窒素を封入した参照用標
準セルを設ける。このセルを測定用セルとならべて設置
し、チョッパーにより両セルを通る赤外光を交互に断続
し、両セルを通った光を合成することにより測定用セル
のガス濃度がゼロの時出力がゼロとなる様にした差分出
力法である。
Therefore, ΔI is proportional to the gas concentration x.
Usually, there are few devices having a light dispersion device such as a prism or a grating, and generally infrared rays in all wavelength regions emitted from a light source are used for measurement. Therefore, non-dispersive infrared gas analyzer (NDIR; Non Dispersive Infra-Red gasanal)
yzer: Non Dispersive Infra Red Gas
Analyzer) is called. NDIR is also divided into positive filter type and negative filter type depending on the type of detector used. The positive filter type is the case where the detector is wavelength dependent, and the negative filter type is the case where the detector is not wavelength dependent. In the latter case, an infrared interference filter is used to give selectivity to a specific wavelength. The infrared interference filter 8 shown in FIG. 4 is adapted to a specific gas absorption line,
For CO 2 , for example, a narrow band filter centering on 4.3 μm is used. In this case, the intensity I 0 of the infrared incident light at the zero density level is required. To obtain this I 0 , a reference standard cell filled with dry nitrogen, which generally does not absorb, is provided. This cell is installed side by side with the measuring cell, the infrared light that passes through both cells is alternately turned on and off by the chopper, and the light that passes through both cells is combined to produce an output when the gas concentration in the measuring cell is zero. This is a difference output method that is set to zero.

【0011】また、低エネルギーの赤外線の広い領域の
スペクトルを同時に計測できる方法は、特開昭59ー1
93341号公報に記載の内容にある。この場合にも、
基準レベルをとる必要があり、基本的には参照用標準セ
ルと同等のものが必要となる。
Further, a method capable of simultaneously measuring the spectrum of a wide range of low-energy infrared rays is disclosed in JP-A-59-1.
The contents are described in Japanese Patent No. 93341. Also in this case,
It is necessary to take the standard level, and basically the same as the standard cell for reference is required.

【0012】[0012]

【発明が解決しようとする課題】しかしながら上記の従
来の構成では、必ず基準をとるための参照用標準セルま
たは、それに相当する基準が必要であり、両セルの条件
差が誤差の原因となるという課題を有していた。
However, in the above-mentioned conventional structure, a reference standard cell for taking a reference or a reference corresponding thereto is necessary, and the difference in conditions between the two cells causes an error. Had challenges.

【0013】本発明は上記従来技術の課題を解決するも
ので、参照用標準セルを必要とせず、多種類ガス濃度を
一つの一次元赤外センサで同時測定できる赤外分析装置
を提供することを目的とする。
The present invention solves the above-mentioned problems of the prior art, and provides an infrared analyzer which does not require a reference standard cell and can simultaneously measure the concentrations of various kinds of gases with one one-dimensional infrared sensor. With the goal.

【0014】[0014]

【課題を解決するための手段】この目的を達成するため
に本発明は、赤外の波長の中でガス吸収の無い波長を選
択し、その波長の出力を基準とする。従って、参照用標
準セルを具備せず測定セルのみにて基準を得る構成を有
している。
In order to achieve this object, the present invention selects a wavelength that does not absorb gas among infrared wavelengths and uses the output of that wavelength as a reference. Therefore, the standard cell for reference is not provided and the standard is obtained only by the measurement cell.

【0015】[0015]

【作用】本発明は上記構成によって、ガス吸収のない波
長をつかって基準信号を得、その基準信号と測定信号の
差を取り出すことにより、2つのセルを使った時の誤差
原因を取り除きいつも安定にガス濃度を知る事ができ
る.
According to the present invention, with the above configuration, a reference signal is obtained by using a wavelength without gas absorption, and the difference between the reference signal and the measurement signal is taken out to eliminate the cause of error when two cells are used and always stabilize. You can know the gas concentration.

【0016】[0016]

【実施例】以下、本発明の一実施例について、図面を参
照しながら説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

【0017】図1は本発明の一実施例における赤外分析
装置の構成図である。図1において、11は赤外光源、
12はチョッパー羽根、13はモーターで12のチョッ
パー羽根を回転する。14はガスセル、15はガスセル
の赤外透過窓材である。16はガスセルを透過してきた
光を集める集光系、17は集光した光を分光する分光
器、18は分光した赤外光を波長別に検知できる焦電型
リニアアレイ検出素子である。
FIG. 1 is a block diagram of an infrared analyzer according to an embodiment of the present invention. In FIG. 1, 11 is an infrared light source,
12 is a chopper blade, and 13 is a motor for rotating the 12 chopper blades. Reference numeral 14 is a gas cell, and 15 is an infrared transmission window material of the gas cell. Reference numeral 16 is a condensing system that collects the light that has passed through the gas cell, 17 is a spectroscope that disperses the condensed light, and 18 is a pyroelectric linear array detection element that can detect the separated infrared light for each wavelength.

【0018】以上のように構成された赤外分析装置につ
いて、図2に示す赤外スペクトルを用いてその原理を説
明する。まず、CO2,CO,NO,SO2等の環境に影
響を与えるガスは4〜8μmの赤外波長域に吸収を持
つ。各ガスの吸収波長位置及び吸収係数を(表1)に示
す。
The principle of the infrared analyzer constructed as described above will be described with reference to the infrared spectrum shown in FIG. First, gases such as CO 2 , CO, NO, and SO 2 that affect the environment have absorption in the infrared wavelength range of 4 to 8 μm. The absorption wavelength position and absorption coefficient of each gas are shown in (Table 1).

【0019】[0019]

【表1】 [Table 1]

【0020】この(表1)から明らかなように、C
2,CO,NO,SO2は各々4.3μm、4.7μ
m、5.3μm、7.4μmに中心吸収帯を持ってい
る。また、図3に示すように大気の赤外透過特性は水分
の影響が大きいが、3〜5μm帯、8〜12μm帯はよ
く知られているように大気の窓といわれ、よく赤外線を
透過する。例えば、3.5〜3.8μmにおいてはガス
吸収の影響が少なく、大気の透過率もよい。本実施例に
おいては、分光器17を3.5μm〜7μm帯域分光と
し上記3種類のガス(CO2,CO,NO)の検知がで
きるようにした。焦電型リニアアレイ検出素子は16素
子構成(ピッチ0.4mm)とした。この場合、一番端
の素子が3.5〜3.8μm帯に対応するので、この素
子の信号出力を基準として他素子の信号出力との差分を
とることによりガス濃度と対応する出力を得ることがで
きた。
As is clear from this (Table 1), C
O 2 , CO, NO and SO 2 are 4.3 μm and 4.7 μm, respectively
It has central absorption bands at m, 5.3 μm, and 7.4 μm. Further, as shown in FIG. 3, the infrared transmission characteristics of the atmosphere are largely influenced by water, but the 3 to 5 μm band and the 8 to 12 μm band are known to be the windows of the atmosphere and transmit infrared rays well. . For example, in the range of 3.5 to 3.8 μm, the effect of gas absorption is small, and the atmospheric transmittance is good. In the present embodiment, the spectroscope 17 is a 3.5 μm to 7 μm band spectroscope so that the above three kinds of gases (CO 2 , CO, NO) can be detected. The pyroelectric linear array detection element had a 16-element configuration (pitch 0.4 mm). In this case, since the element at the extreme end corresponds to the 3.5 to 3.8 μm band, the signal output of this element is used as a reference to obtain the output corresponding to the gas concentration by taking the difference from the signal output of other elements. I was able to.

【0021】以上のように本実施例によれば、測定用ガ
スセルのみを用い、赤外分光器と焦電型リニアアレイ検
出素子の組み合わせを設けることにより、ガス吸収が少
なく大気透過率の良い3.7μm帯の信号出力を基準と
してとることができ、参照用標準セルを用いること無く
多種類のガス濃度を同時に計測することができる。
As described above, according to this embodiment, by using only the measuring gas cell and providing the combination of the infrared spectroscope and the pyroelectric linear array detecting element, the gas absorption is small and the atmospheric transmittance is good. The signal output in the band of 0.7 μm can be used as a reference, and various kinds of gas concentrations can be simultaneously measured without using a reference standard cell.

【0022】[0022]

【発明の効果】以上のように本発明は赤外分光器と焦電
型リニアアレイ検出素子を組み合わせを設けることによ
り、参照用標準セルを用いること無く多種類のガス濃度
を同時に計測することができる優れた赤外分析装置を実
現できるものである。
As described above, according to the present invention, by providing a combination of an infrared spectroscope and a pyroelectric linear array detection element, it is possible to simultaneously measure various kinds of gas concentrations without using a reference standard cell. It is possible to realize an excellent infrared analyzer that can be used.

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

【図1】本発明の一実施例における赤外分析装置のブロ
ック結線図
FIG. 1 is a block diagram of an infrared analyzer according to an embodiment of the present invention.

【図2】同実施例における赤外分析装置の対象ガスの吸
収特性を示すガス吸収パターン図
FIG. 2 is a gas absorption pattern diagram showing absorption characteristics of a target gas of the infrared analyzer in the same Example.

【図3】同実施例における赤外分析装置の大気吸収特性
FIG. 3 is an atmospheric absorption characteristic diagram of the infrared analyzer in the same example.

【図4】従来の赤外分析装置のブロック結線図FIG. 4 is a block connection diagram of a conventional infrared analyzer.

【符号の説明】[Explanation of symbols]

1 赤外光源 2 チョッパー羽根 3 モーター 4 測定用ガスセル 5 透過窓材 6 参照用標準セル 7 透過窓材 8 赤外干渉フィルター 9 赤外センサ 11 赤外光源 12 チョッパー羽根 13 モーター 14 ガスセル 15 赤外透過窓材 16 集光系 17 分光器 18 焦電形リニアアレイ検出素子 1 infrared light source 2 chopper blade 3 motor 4 measurement gas cell 5 transmission window material 6 reference standard cell 7 transmission window material 8 infrared interference filter 9 infrared sensor 11 infrared light source 12 chopper blade 13 motor 14 gas cell 15 infrared transmission Window material 16 Condensing system 17 Spectroscope 18 Pyroelectric linear array detector

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】赤外光源と、赤外光を断続するチョッパー
と、測定対象ガスを流すガスセルと、対象ガスの吸収を
うけた赤外光を集光する集光系と、集光された赤外光を
波長別に分光する分光器と、分光された赤外光を検知す
るリニアアレイ素子で構成され、参照用標準セルを用い
ずガス吸収の無い波長の信号出力を基準とする機構を具
備する赤外分析装置。
1. An infrared light source, a chopper for connecting and disconnecting infrared light, a gas cell for flowing a gas to be measured, and a light condensing system for condensing infrared light absorbed by the gas to be measured. Consists of a spectroscope that separates infrared light by wavelength and a linear array element that detects the separated infrared light, and has a mechanism that uses a signal output of a wavelength without gas absorption as a reference without using a reference standard cell. Infrared analyzer.
【請求項2】基準信号をとる波長として、3.5〜3.
8μmを用いた請求項1記載の赤外分析装置。
2. A wavelength range of 3.5-3.
The infrared analyzer according to claim 1, wherein the infrared analyzer has a thickness of 8 μm.
【請求項3】基準信号とする波長に対応する素子の出力
と他の素子の差を出力する回路を組み込んだ請求項1記
載の赤外分析装置。
3. An infrared analyzer according to claim 1, wherein a circuit for outputting the difference between the output of the element corresponding to the wavelength used as the reference signal and the other element is incorporated.
【請求項4】リニアアレイ素子に焦電型センサを用いた
請求項1記載の赤外分析装置。
4. The infrared analyzer according to claim 1, wherein a pyroelectric sensor is used for the linear array element.
JP3225804A 1991-09-05 1991-09-05 Infrared analyzer Pending JPH0560687A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3225804A JPH0560687A (en) 1991-09-05 1991-09-05 Infrared analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3225804A JPH0560687A (en) 1991-09-05 1991-09-05 Infrared analyzer

Publications (1)

Publication Number Publication Date
JPH0560687A true JPH0560687A (en) 1993-03-12

Family

ID=16835051

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3225804A Pending JPH0560687A (en) 1991-09-05 1991-09-05 Infrared analyzer

Country Status (1)

Country Link
JP (1) JPH0560687A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9663991B2 (en) 2011-08-29 2017-05-30 Basf Se Ladder
CN108507966A (en) * 2018-07-02 2018-09-07 青岛海纳光电环保有限公司 A kind of infrared spectrum gas sensor and data processing method
CN110618102A (en) * 2019-09-25 2019-12-27 成都太阳神鸟智能控制有限公司 Gas detection method and device based on dispersion spectrum analysis and artificial intelligence
CN111141695A (en) * 2019-12-24 2020-05-12 中国船舶重工集团公司第七一八研究所 Non-dispersive infrared multi-component Freon gas detection system

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60501916A (en) * 1983-07-28 1985-11-07 シ−エムアイ,インコ−ポレ−テツド breath analyzer
JPS6337242A (en) * 1986-07-31 1988-02-17 Shimadzu Corp Infrared type gas analyser
JPH01301149A (en) * 1987-12-03 1989-12-05 Mutek Laser & Optoelectronisch Geraete Gmbh Method and apparatus for gas analysis

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60501916A (en) * 1983-07-28 1985-11-07 シ−エムアイ,インコ−ポレ−テツド breath analyzer
JPS6337242A (en) * 1986-07-31 1988-02-17 Shimadzu Corp Infrared type gas analyser
JPH01301149A (en) * 1987-12-03 1989-12-05 Mutek Laser & Optoelectronisch Geraete Gmbh Method and apparatus for gas analysis

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9663991B2 (en) 2011-08-29 2017-05-30 Basf Se Ladder
CN108507966A (en) * 2018-07-02 2018-09-07 青岛海纳光电环保有限公司 A kind of infrared spectrum gas sensor and data processing method
CN110618102A (en) * 2019-09-25 2019-12-27 成都太阳神鸟智能控制有限公司 Gas detection method and device based on dispersion spectrum analysis and artificial intelligence
CN111141695A (en) * 2019-12-24 2020-05-12 中国船舶重工集团公司第七一八研究所 Non-dispersive infrared multi-component Freon gas detection system

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