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JPS62217139A - Measuring instrument for gas concentration - Google Patents

Measuring instrument for gas concentration

Info

Publication number
JPS62217139A
JPS62217139A JP6122286A JP6122286A JPS62217139A JP S62217139 A JPS62217139 A JP S62217139A JP 6122286 A JP6122286 A JP 6122286A JP 6122286 A JP6122286 A JP 6122286A JP S62217139 A JPS62217139 A JP S62217139A
Authority
JP
Japan
Prior art keywords
temperature
gas
humidity
chamber
gas concentration
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
JP6122286A
Other languages
Japanese (ja)
Inventor
Shoji Doi
土肥 正二
Akira Sawada
亮 澤田
Iwao Sugiyama
巌 杉山
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP6122286A priority Critical patent/JPS62217139A/en
Publication of JPS62217139A publication Critical patent/JPS62217139A/en
Pending legal-status Critical Current

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  • Optical Measuring Cells (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To stabilize a measured value by condensing dew in a chamber which contains an optical path of measurement by cooling fins and making the humidity constant in the chamber. CONSTITUTION:The outside air 15 is cooled successively by cooling fins 16 provided in the middle of a pipe 20 to reach saturated steam pressure. Excessive steam is condensed into dew on the fins, the temperature measured by a temperature sensor 22 is monitored on a temperature measuring instrument 23, and the dew point is controlled by a temperature controller 14 through an electronic cooler 21. Objective gas in the chamber 17 wherein the admitted gas is controlled by the cooling fins 16 to constant temperature and 100% humidity is absorbed and reference gas 6 is also absorbed to find the gas concentration. The temperature and humidity of the air in the chamber 17 are controlled, so the influence of steam is superposed upon the measured gas concentration by a constant quantity, so the quantity of the superposition is inputted to a computer 1, so that the influence of steam is removed stably even if the admitted outside air 15 varies in humidity.

Description

【発明の詳細な説明】 〔概 要〕 本発明は、特定ガスの固有吸収線での赤外吸収量からガ
ス11:4度を求めるガスfll[測定装置(以下ガス
センサと呼ぶ)に2いて、対象としている吸収線の近傍
に存在する水蒸気による吸□収が変動して測定値変動の
影9を除くため、測定光路を納めたチェンバー内の湿[
−冷却フィンで結露させて一定にすることにより、湿度
一定にし、測定値を安定化させたものである。
[Detailed Description of the Invention] [Summary] The present invention provides a method for determining gas 11:4 degrees from the amount of infrared absorption at the characteristic absorption line of a specific gas. In order to eliminate the shadow 9 of measured value fluctuations due to fluctuations in absorption due to water vapor existing near the absorption line of interest, the moisture in the chamber containing the measurement optical path [
- By condensing with cooling fins and making it constant, the humidity is kept constant and the measured values are stabilized.

〔産業上の利用分野〕[Industrial application field]

本発明はガスセンサの測定精度向上、特に水蒸気による
測定誤差を除くための装置構成に関する。
The present invention relates to improving the measurement accuracy of a gas sensor, and particularly to an apparatus configuration for eliminating measurement errors caused by water vapor.

ガスセンサは赤外領域にある強い吸収線r利用するので
、高感匣が期待されるが、各ガスには数百本から数千本
の吸収線があるため、対象ガスの対象吸収線を利用しよ
うとしても水蒸気の吸収線が対象吸収線近傍に存在する
ことがらシ、測定ガス濃度の誤差要因となる。このため
湿度を一定にして水蒸気の量’kfill1goする方
法が必要とされる。
Gas sensors use strong absorption lines r in the infrared region, so high sensitivity is expected, but each gas has hundreds to thousands of absorption lines, so it is best to use the target absorption line of the target gas. Even if an attempt is made to do so, the water vapor absorption line exists near the target absorption line, which causes an error in the measured gas concentration. Therefore, a method is required to keep the humidity constant and reduce the amount of water vapor.

〔従来の技術〕[Conventional technology]

従来のガスセンサの構a′lc第3図に示す。 The structure of a conventional gas sensor a'lc is shown in FIG.

図中1はコンピュータ、2はレーザ電源、8はレーザ、
4はレンズ95はビームスプリッタ。
In the figure, 1 is a computer, 2 is a laser power supply, 8 is a laser,
4, lens 95 is a beam splitter.

6は参照ガスセル、7は集光レンズ、8は検知器、9は
長光路光学系、IOは集光レンズ。
6 is a reference gas cell, 7 is a condenser lens, 8 is a detector, 9 is a long optical path optical system, and IO is a condenser lens.

11は検知器、12.12’は信号検出回路。11 is a detector, 12.12' is a signal detection circuit.

18は比較器、19はIUe表示回路である。18 is a comparator, and 19 is an IUe display circuit.

図示のように、対象ガスを既知濃度封入した参照ガスセ
ル4通して得た吸収量とオープン大気中の対象ガスによ
って長光路光学系で吸収された鼠とから比較1(既知ガ
ス1虹×測定側の信号/参照側の信号)してガス連用を
求める装置である。
As shown in the figure, a comparison 1 (known gas 1 rainbow x measurement side signal/reference side signal) to determine the continuous use of gas.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来のガスセンナでは長光路セル部が大気中に解放され
たtl造であったため、大気の湿度変化に伴なって対象
吸収線での水蒸気による吸収量が変化し、測定濃度値が
変化するといった問題?生じていた。
Conventional gas sensors have a TL structure in which the long optical path cell section is open to the atmosphere, so there is a problem that the amount of water vapor absorbed at the target absorption line changes as the atmospheric humidity changes, causing the measured concentration value to change. ? It was happening.

〔問題点を解決するための手段〕[Means for solving problems]

第1図は本発明の大気の湿度?一定にするためのtlり
造図である。20は大気15を導入するためのバイブで
ある。15は大気で、20の途中に設けた冷却フィン1
6で順次冷却され、飽和水蒸気圧に達する。余分の水蒸
気はフィン上で結露↓露点は温度センサー22で測った
温度r測温計28で監視し、温調2;14で例えば電子
冷却器21で制御する。
Figure 1 shows the atmospheric humidity of the present invention? This is a tl diagram to keep it constant. 20 is a vibrator for introducing the atmosphere 15. 15 is the atmosphere, and cooling fin 1 installed in the middle of 20
6, it is sequentially cooled and reaches the saturated water vapor pressure. Excess water vapor condenses on the fins ↓ The dew point is monitored by a thermometer 28, which measures the temperature r measured by a temperature sensor 22, and is controlled by, for example, an electronic cooler 21 in temperature control 2;14.

〔作 用〕[For production]

本発明のセンサでは、導入大気4が例えば温度0℃、湿
度100慢に制御され、測定光路内には4′の大気しか
ないので、水蒸気の影響はあるものの常に一定である。
In the sensor of the present invention, the temperature of the introduced atmosphere 4 is controlled to be 0.degree. C. and the humidity is 100, for example, and since only the atmosphere 4' is in the measurement optical path, the influence of water vapor is always constant.

この結果、導入大気4の湿度が変化しても測定値には影
響せず測定値が安定する。更に、0C9100*の条件
で水蒸気の影1’に6らかしめ測定して2けば、測定結
果に加減して補正すれば絶対8度も得られ、測定誤差を
除くことができる。
As a result, even if the humidity of the introduced atmosphere 4 changes, the measured value is not affected and the measured value is stabilized. Furthermore, if you measure the shadow 1' of water vapor by 6 degrees under the condition of 0C9100*, and correct it by adding or subtracting the measurement result, you can get an absolute value of 8 degrees, which eliminates measurement errors.

〔実施例〕〔Example〕

第2図は本発明め一実施例によるガスセンサの構成図で
ある。
FIG. 2 is a configuration diagram of a gas sensor according to a first embodiment of the present invention.

図中1はセンサの信号系を制御するコンビニーダ、2は
ンーザ電源、3はレーザ光源、4はレンズ、5はビーム
スプリフタ、6は参照ガスセル、7は集光レンズ、8は
検知器、9は測定用長光路光学系、10は集光レンズ、
11は検知器、12.12’は信号検出回路、13は比
較器、14は温調器、15は導入大気、16は冷却フィ
ン、17は9【覆うチェンバー、18は排出大気、19
は濃度表示器でちる。
In the figure, 1 is a combination kneader that controls the signal system of the sensor, 2 is a sensor power supply, 3 is a laser light source, 4 is a lens, 5 is a beam splitter, 6 is a reference gas cell, 7 is a condenser lens, 8 is a detector, 9 10 is a long optical path optical system for measurement, 10 is a condensing lens,
11 is a detector, 12.12' is a signal detection circuit, 13 is a comparator, 14 is a temperature controller, 15 is an introduced atmosphere, 16 is a cooling fin, 17 is a chamber to cover 9, 18 is an exhaust atmosphere, 19
is determined by the concentration display.

導入大気15は16冷却フインで一定温度、湿度100
チに制御された17チエンバー内の対象ガスによる吸収
と、6参照ガスによる吸収からガス濃[r求める。この
実施例によれば、チェンバー内大気の温湿度が制御され
ているため(測定ガス濃度に水蒸気の影響が一定量ゴな
畳してイア:r カ% @ijもってこの重畳ff1v
lコンピユータに入力し6ておけば、導入大気15の湿
度変動があっても安定に水蒸気の影響を除去することが
できる。
The introduced atmosphere 15 has a constant temperature and humidity of 100 using cooling fins 16.
The gas concentration [r is calculated from the absorption by the target gas in the chamber 17 and the absorption by the reference gas 6. According to this embodiment, since the temperature and humidity of the atmosphere inside the chamber are controlled (the effect of water vapor on the measured gas concentration is a certain amount), this superposition ff1v
By inputting the information into a computer 6, it is possible to stably remove the influence of water vapor even if there are fluctuations in the humidity of the introduced atmosphere 15.

〔発明の効果〕〔Effect of the invention〕

本発明によれば大気の湿度変化によって対象ガス−翼が
影響?受けていたもの?湿度茶件一定にしているので、
測定値の変動要因を除去できる。更に湿屁争件が一定で
あれば測定値の補正を容易に行なえて、絶対測定′M度
が向上する効果がある。
According to the present invention, is the target gas-blade affected by changes in atmospheric humidity? What did you receive? Since the humidity is kept constant,
It is possible to remove factors that cause fluctuations in measured values. Furthermore, if the wet fart content is constant, the measured value can be easily corrected, which has the effect of improving the absolute measurement degree.

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

第1図は本発明の詳細な説明する図、第2図は本発明の
一実施例を示すガスセンサ構成図。 第8図は従来例に示す構成図である。 図1c ?イて、1はコンビ二一夕、2はレーザ電源、
8拡レーザ光源、4はレンズ、5はビームスプリフタ、
6は参照ガスセル、7は集光レンズ、8は検知器、9は
長光路光学系、10は集光レンズ、11は検知器、z2
.j;:八21は信号検出回路、1Bは比!2器、14
は温HA5゜15は導入大気、15′は除湿大気、L6
は冷却フィン、17はチェンバー、18は放出大気。 19は濃度表示器、20は導入バイブ、21は電子冷却
器、22は温關センサ、23はa++温器である。 ′$1m −づ(:J1巴イ蒼す 第2図
FIG. 1 is a diagram explaining the present invention in detail, and FIG. 2 is a configuration diagram of a gas sensor showing an embodiment of the present invention. FIG. 8 is a configuration diagram showing a conventional example. Figure 1c? 1 is a combination unit, 2 is a laser power supply,
8 expanded laser light source, 4 lens, 5 beam splitter,
6 is a reference gas cell, 7 is a condensing lens, 8 is a detector, 9 is a long optical path optical system, 10 is a condensing lens, 11 is a detector, z2
.. j;:821 is the signal detection circuit, 1B is the ratio! 2 vessels, 14
is the temperature HA5゜15 is the introduced atmosphere, 15' is the dehumidified atmosphere, L6
17 is a cooling fin, 17 is a chamber, and 18 is a discharged atmosphere. 19 is a concentration display, 20 is an introduction vibrator, 21 is an electronic cooler, 22 is a temperature sensor, and 23 is an a++ warmer. '$1m -zu(:J1 Tomoe Aosu Figure 2

Claims (1)

【特許請求の範囲】[Claims] 波長可変光源と該光源からの光を伝搬させる光学系を有
し、特定ガスの固有吸収線で吸収された赤外線吸収量か
らガス濃度を求める測定装置において、測定光路を覆う
チェンバー17と該チェンバー17への導入口に一定温
度に冷却するフィン16と該フィン16を冷却する冷却
器21と一定温度に制御する温調器14とを有すること
を特徴とするガス濃度測定装置。
In a measuring device that has a variable wavelength light source and an optical system that propagates light from the light source and determines gas concentration from the amount of infrared absorption absorbed by a specific absorption line of a specific gas, there is provided a chamber 17 that covers a measurement optical path; A gas concentration measuring device characterized in that it has a fin 16 that cools the fin 16 to a constant temperature, a cooler 21 that cools the fin 16, and a temperature regulator 14 that controls the temperature to a constant temperature at an inlet.
JP6122286A 1986-03-19 1986-03-19 Measuring instrument for gas concentration Pending JPS62217139A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6122286A JPS62217139A (en) 1986-03-19 1986-03-19 Measuring instrument for gas concentration

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6122286A JPS62217139A (en) 1986-03-19 1986-03-19 Measuring instrument for gas concentration

Publications (1)

Publication Number Publication Date
JPS62217139A true JPS62217139A (en) 1987-09-24

Family

ID=13164960

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6122286A Pending JPS62217139A (en) 1986-03-19 1986-03-19 Measuring instrument for gas concentration

Country Status (1)

Country Link
JP (1) JPS62217139A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5340987A (en) * 1991-03-15 1994-08-23 Li-Cor, Inc. Apparatus and method for analyzing gas
US6369387B1 (en) 1999-10-15 2002-04-09 Li-Cor, Inc. Gas analyzer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5340987A (en) * 1991-03-15 1994-08-23 Li-Cor, Inc. Apparatus and method for analyzing gas
US6369387B1 (en) 1999-10-15 2002-04-09 Li-Cor, Inc. Gas analyzer

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