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JPS6350658B2 - - Google Patents
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JPS6350658B2 - - Google Patents

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Publication number
JPS6350658B2
JPS6350658B2 JP50063690A JP6369075A JPS6350658B2 JP S6350658 B2 JPS6350658 B2 JP S6350658B2 JP 50063690 A JP50063690 A JP 50063690A JP 6369075 A JP6369075 A JP 6369075A JP S6350658 B2 JPS6350658 B2 JP S6350658B2
Authority
JP
Japan
Prior art keywords
atmosphere
measured
gas
room
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
Application number
JP50063690A
Other languages
Japanese (ja)
Other versions
JPS51139396A (en
Inventor
Ikuhiko Kimura
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.)
Figaro Engineering Inc
Original Assignee
Figaro Engineering Inc
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 Figaro Engineering Inc filed Critical Figaro Engineering Inc
Priority to JP6369075A priority Critical patent/JPS51139396A/en
Publication of JPS51139396A publication Critical patent/JPS51139396A/en
Publication of JPS6350658B2 publication Critical patent/JPS6350658B2/ja
Granted legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)

Description

【発明の詳細な説明】 本発明は喫煙室等の雰囲気の汚染度、すなわち
極く低い濃度のガスによる汚染を正確に検出しう
るようにした方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for accurately detecting the degree of contamination of the atmosphere of a smoking room or the like, that is, contamination due to extremely low concentration of gas.

最近、一酸酸化炭素やアルコール等の還元性ガ
ス検出用の検知素子として、SnO2N型半導体等
の金属酸化物半導体素子が広く用いられるように
なつてきた。しかしながらこの素子を喫煙室内の
汚染、自動車の車外に対する車内の汚染、エンジ
ン排ガス中のCOによる車庫内の汚染等を検知す
る素子として用いる場合、極めて低濃度のガスを
検知する必要がありかつ素子自体が室内の湿度の
変化等によつて影響をうけ、このため素子によつ
て直接に室内雰囲気を計測する方法では充分な精
度での検出はできない。
Recently, metal oxide semiconductor elements such as SnO 2 N-type semiconductors have come to be widely used as sensing elements for detecting reducing gases such as carbon monoxide and alcohol. However, when this element is used as an element to detect pollution in a smoking room, pollution inside a car compared to the outside, pollution inside a garage due to CO in engine exhaust gas, etc., it is necessary to detect extremely low concentration gases, and the element itself has to be detected. is affected by changes in indoor humidity, etc., and for this reason, it is not possible to detect with sufficient accuracy using a method that directly measures the indoor atmosphere using an element.

本発明はこのような点に鑑みてなされたもので
あり、金属酸化物半導体ガスセンサーを、被計測
室雰囲気と室外の大気とに交互に触れさせて、該
センサーの被計測室雰囲気と大気とにおける出力
の相違を求め、これにより被計測室雰囲気と大気
とに共通した環境変動の影響を除去して、被計測
雰囲気中のガス濃度を検出することを特徴とする
室内雰囲気中の低濃度ガス検出方法である。
The present invention has been made in view of these points, and includes a metal oxide semiconductor gas sensor that is brought into contact with the atmosphere of the room to be measured and the outside atmosphere alternately, so that the sensor can interact with the atmosphere of the room to be measured and the atmosphere. Low-concentration gas in a room atmosphere is characterized in that the gas concentration in the atmosphere to be measured is detected by determining the difference in the output of This is a detection method.

一般に上記素子の抵抗値(Rs)は雰囲気中の
ガス濃度(C)若しくはその累乗根にほぼ反比例して
変化し、第1図に示すように両者の対数logRs、
logCの関係は直線的反比例の関係になる。従つ
て素子の抵抗値の変化により雰囲気中のガス濃度
を知ることができるが、上記抵抗値とガス濃度と
の関係の特性は経時的に変化する。すなわち、素
子に通電すると時間の経過と共に上記特性を示す
線Aは一定の勾配を保つたままで下降し(線A1
A2)、また無通電の状態で放置すると上記特性を
示す線は次第に上昇する。従つて実際の使用状態
では通電―無通電の繰返しの間隔、周期によつて
ガス濃度に対応する素子の抵抗値は変化すること
になつて測定の正確さを欠き、とくに喫煙室等の
低濃度のガスでしかも湿度の変化もある雰囲気の
汚染度の検出には適用できなかつた。
In general, the resistance value (Rs) of the above element changes in almost inverse proportion to the gas concentration (C) in the atmosphere or its power root, and as shown in Figure 1, the logarithm of both, logRs,
The relationship of logC is a linear inversely proportional relationship. Therefore, the gas concentration in the atmosphere can be determined by the change in the resistance value of the element, but the characteristics of the relationship between the resistance value and the gas concentration change over time. In other words, when the device is energized, as time passes, the line A showing the above characteristics decreases while maintaining a constant slope (line A 1 ,
A 2 ), and when left in a non-energized state, the line showing the above characteristics gradually rises. Therefore, in actual usage conditions, the resistance value of the element corresponding to the gas concentration changes depending on the interval and cycle of repeated energization and de-energization, resulting in a lack of measurement accuracy, especially in low concentrations such as smoking rooms. This method could not be applied to detecting the degree of contamination in an atmosphere containing many gases and humidity changes.

上記特性を示す線(A,A1,A2)は素子に与
えられた熱履歴によつても変動するが、これらの
変動によつても線(A,A1,A2)の勾配はほと
んど変化しないという事実が実験的に確認されて
いる。従つてこの事実、すなわち上記線(A,
A1,A2)の勾配が素子の経時変化や熱履歴によ
つては変化しないという特性を利用すればガス濃
度の測定を正確に行なうことが可能である。
The line (A, A 1 , A 2 ) indicating the above characteristics varies depending on the thermal history given to the element, but the slope of the line (A, A 1 , A 2 ) also changes due to these variations. It has been experimentally confirmed that there is almost no change. Therefore, this fact, that is, the above line (A,
Gas concentration can be measured accurately by utilizing the characteristic that the slope of A 1 , A 2 ) does not change due to aging or thermal history of the element.

一般に検出素子の抵抗はつぎの式で表わされ
る。
Generally, the resistance of a detection element is expressed by the following formula.

Rs=K/C〓 Kおよびαはガスおよび素子の種類によつて決
まる定数であり、αは通常の素子では0.5〜0.8) 従つて大気中の素子の抵抗(Rss)および被計
測雰囲気中の素子の抵抗(Rsx)は Rss=K/Cs〓 (Csは大気のガス濃度) Rsx=K/Cx〓 (Cxは被計測雰囲気のガス濃度) Cx=Cs(Rss/Rsx)1/〓 上式よりCsは既知であるから、Rss/Rsxの値
等を求めれば被計測雰囲気のガス濃度(Cx)が
求められる。
Rs=K/C〓 K and α are constants determined by the gas and the type of element, and α is 0.5 to 0.8 for normal elements. Therefore, the resistance of the element in the atmosphere (Rss) and the resistance in the atmosphere to be measured are The resistance of the element (Rsx) is Rss=K/Cs〓 (Cs is the gas concentration in the atmosphere) Rsx=K/Cx〓 (Cx is the gas concentration in the atmosphere to be measured) Cx=Cs (Rss/Rsx) 1/ 〓 Above formula Therefore, since Cs is known, the gas concentration (Cx) of the atmosphere to be measured can be found by finding the value of Rss/Rsx.

以下本発明の実施例を図面によつて説明する。
1は定電圧電源、2は金属酸化物半導体からなる
ガスセンサーであり、該センサー2にはスイツチ
3を介してインピーダンス変換器4またはインピ
ーダンス変換器5およびインバータ6を切替え可
能に接続し、さらにスイツチ8、抵抗9を介して
スイツチ10とコンデンサー11と積分器12と
からなる並列回路を接続し、これを零検出器13
を通してコントローラ14に接続している。この
コントローラ14はスイツチ3,8およびスイツ
チ10を制御すると共に上記センサー2を配置し
たガス検出部30を制御する。スイツチ3,8は
リレーまたはFET等からなるアナログスイツチ
で構成する。
Embodiments of the present invention will be described below with reference to the drawings.
1 is a constant voltage power supply; 2 is a gas sensor made of a metal oxide semiconductor; an impedance converter 4 or an impedance converter 5 and an inverter 6 are switchably connected to the sensor 2 via a switch 3; 8. Connect a parallel circuit consisting of a switch 10, a capacitor 11, and an integrator 12 via a resistor 9, and connect this to a zero detector 13.
It is connected to the controller 14 through. This controller 14 controls the switches 3, 8 and 10, and also controls the gas detection section 30 in which the sensor 2 is arranged. Switches 3 and 8 are constructed from analog switches such as relays or FETs.

ガス検出部30は計測すべき喫煙室等の室内雰
囲気60と室外雰囲気(大気)50とを隔てる壁
40の貫通孔に配置し、センサー2を断面L字形
の保持板31によつて保持させている。この保持
板31は図示しない制御手段によつて回転して図
示の実線の位置および二点鎖線の位置に交互に変
位するように、これによつてセンサー2を被計測
雰囲気60および室外雰囲気50に触れさせる。
The gas detection unit 30 is disposed in a through hole in a wall 40 that separates an indoor atmosphere 60 of a smoking room or the like to be measured from an outdoor atmosphere (atmosphere) 50, and the sensor 2 is held by a holding plate 31 having an L-shaped cross section. There is. This holding plate 31 is rotated by a control means (not shown) and is alternately displaced to the position shown by the solid line and the position shown by the two-dot chain line, thereby placing the sensor 2 in the measurement atmosphere 60 and the outdoor atmosphere 50. Let me touch you.

つぎにこの装置によつてガス検出をする方法を
説明する。まずスイツチ10をオンにしてコンデ
ンサ11の残留電圧をシヨートし、積分器12の
出力電圧を零にした状態で該スイツチ10をオフ
にする。
Next, a method of gas detection using this device will be explained. First, switch 10 is turned on to shoot out the residual voltage in capacitor 11, and with the output voltage of integrator 12 set to zero, switch 10 is turned off.

センサー2が標準雰囲気となる室外雰囲気50
に接しているときにはスイツチ3はターミナル2
6側に、スイツチ8はターミナル28側に接続さ
れている。この状態で一定時間(Ts)保持する
と、コンデンサ11の充電作用によつて積分器1
2の出力電圧は漸次増加していき、積分器出力に
はセンサー2の標準ガス中における電圧(Vss)
xTsに比例した電圧があらわれる。次に保持板3
1を回転させてセンサー2が被計測雰囲気60に
触れるようにする(第3図実線位置)と共にスイ
ツチ3をターミナル27に、スイツチ8をターミ
ナル29に接続させる。この場合にはターミナル
29にはインバータ6によつて負の電圧が表われ
る。従つて積分器12はこの信号によつて放電
し、一定時間(Tx)後に積分器出力は零になる。
すなわち Vss×Ts−Vsx×Tx=0 (Vsx:被計測室雰囲気中における電圧) Tx=Ts・Vss/Vsx=Ts・Rss/Rsx となり、この放電時間(Tx)を測定すれば
Rss/Rsxに比例した出力が得られ、Rss/Rsxが
求められる。また積分器出力が零になると、これ
を検出した零検出器13からの信号によつてコン
トローラ14がスイツチ3,8を作動させてそれ
ぞれターミナル26,28に接続させるように切
換えると共にガス検出部30に信号を送つて保持
板31を回転させ、センサー2を二点鎖線の位置
に移し、室外雰囲気に接触させる。以下同様の操
作を一定周期で繰返すことによつて上記充電時間
(Ts)に対する放電時間を求め、これによつて
Rss/Rsxを求める。この値が求まると第1図の
log C−log Rsの関係から被計測雰囲気中の一
酸化炭素等のガス濃度を知ることができる。この
場合、素子の特性(log Cとlog Rsとの関係)
は経時変化等によつて例えば線A→A1→A2のよ
うに変動するが、その勾配は一定であるために被
計測ガスの濃度は経時変化等に影響されることな
く常に正確な測定がなされる。
Outdoor atmosphere 50 where sensor 2 becomes the standard atmosphere
switch 3 is terminal 2 when it is in contact with
6 side, switch 8 is connected to the terminal 28 side. When this state is maintained for a certain period of time (Ts), the integrator 1
The output voltage of sensor 2 gradually increases, and the integrator output shows the voltage (Vss) of sensor 2 in the standard gas.
A voltage proportional to xTs appears. Next, holding plate 3
1 is rotated so that the sensor 2 comes into contact with the atmosphere to be measured 60 (solid line position in FIG. 3), and the switch 3 is connected to the terminal 27 and the switch 8 is connected to the terminal 29. In this case, a negative voltage appears at terminal 29 by inverter 6. Therefore, the integrator 12 is discharged by this signal, and the integrator output becomes zero after a certain time (Tx).
In other words, Vss×Ts−Vsx×Tx=0 (Vsx: voltage in the atmosphere of the room being measured) Tx=Ts・Vss/Vsx=Ts・Rss/Rsx, and by measuring this discharge time (Tx),
An output proportional to Rss/Rsx is obtained, and Rss/Rsx is calculated. When the integrator output becomes zero, the controller 14 operates the switches 3 and 8 to connect them to the terminals 26 and 28, respectively, in response to a signal from the zero detector 13 that detects this, and the gas detection section 30 A signal is sent to rotate the holding plate 31, and the sensor 2 is moved to the position indicated by the two-dot chain line, and brought into contact with the outdoor atmosphere. By repeating the same operation at regular intervals, the discharging time for the above charging time (Ts) is determined.
Find Rss/Rsx. Once this value is determined, the figure 1
The concentration of gases such as carbon monoxide in the atmosphere to be measured can be determined from the relationship log C-log Rs. In this case, the characteristics of the element (relationship between log C and log Rs)
changes over time, for example, as shown in the line A → A 1 → A 2 , but since the slope is constant, the concentration of the gas to be measured is not affected by changes over time, etc., and can always be accurately measured. will be done.

つまり、同一素子の短時間ごとの抵抗値比等が
検出されるので、その検出時における素子の特性
が例えば第1図中の線Aであれば、この線A上の
2点が被計測室雰囲気と大気とにおけるセンサー
出力に相当するものとなり、この2点の検出に要
する程度の短い時間では殆ど経時変化が生じな
い。また、その後に比較的長時間が経過して素子
の特性が例えば線A1に変化したときに改めて検
出が行われると、今度は線A1上の2点が被計測
室雰囲気と大気とにおけるセンサー出力に相当す
るものとなるが、線Aと線A1とで勾配に変わり
がないことから、上記抵抗値比等は線A上で求め
た場合と同等に得られる。こうして経時的な特性
変動が相殺されると共に、被計測室雰囲気と大気
とにおける出力の相違が求められることによつて
被計測室雰囲気と大気とに共通した環境変動、例
えば温度、湿度、大気汚染等も相殺される。従つ
て、これらの一般的変動要因の影響が除去され、
大気中と比較した被計測室雰囲気の汚染度が正確
に検出されることとなる。
In other words, since the resistance value ratio etc. of the same element are detected every short time, if the characteristic of the element at the time of detection is, for example, line A in Fig. 1, two points on this line A are in the room to be measured. This corresponds to the sensor output for the atmosphere and atmosphere, and there is almost no change over time in the short time required to detect these two points. Furthermore, if detection is performed again after a relatively long period of time has passed and the characteristics of the element change to, for example, line A 1 , the two points on line A 1 will be different from the atmosphere in the room to be measured and the atmosphere. This corresponds to the sensor output, but since there is no difference in slope between line A and line A1 , the above resistance value ratio etc. can be obtained in the same way as when calculated on line A. In this way, changes in characteristics over time are canceled out, and by determining the difference in output between the atmosphere in the room to be measured and the atmosphere, common environmental fluctuations in the atmosphere in the room to be measured and the atmosphere, such as temperature, humidity, air pollution, etc. etc. are also canceled out. Therefore, the influence of these common variables is removed and
The degree of contamination of the atmosphere in the measurement room compared to the atmosphere can be accurately detected.

被計測室内の雰囲気が所定の汚染度に達したと
きにはその計測信号によつて警報器を作動させる
ようにすればよく、あるいは換気扇を作動させて
室内の換気を行なうようにしてもよい。
When the atmosphere in the room to be measured reaches a predetermined degree of contamination, the measurement signal may be used to activate an alarm, or a ventilation fan may be activated to ventilate the room.

なお、上記実施例においては1個の素子を用い
てこれを室内外の雰囲気に交互に触れさせる例に
ついて示したが、素子を室内と室外とに交互に移
動させたりあるいは配管によつて室内雰囲気と室
外雰囲気とを交互に素子に接触させるようにして
もよい。また素子の抵抗値の比等を求める方法に
ついても上記以外の種々の方法が採用可能であ
る。
In addition, in the above embodiment, an example was shown in which one element is used and exposed to the indoor and outdoor atmosphere alternately, but the element may be alternately moved indoors and outdoors, or the indoor atmosphere may be exposed to the indoor atmosphere using piping. The element may be brought into contact with the outdoor atmosphere and the outdoor atmosphere alternately. Furthermore, various methods other than those described above can be used for determining the ratio of the resistance values of the elements.

以上説明したように、本発明は金属酸化物半導
体ガスセンサーの被計測室雰囲気と大気とにおけ
る出力の比較により、環境変動の影響等を除去し
て被計測雰囲気中のガス濃度を求めるようにした
ものであり、従来不可能と考えられていた低濃度
ガス雰囲気の喫煙室等室内の汚染度の計測を可能
にしたものである。
As explained above, the present invention eliminates the influence of environmental changes and determines the gas concentration in the atmosphere to be measured by comparing the output of the metal oxide semiconductor gas sensor between the atmosphere in the chamber to be measured and the atmosphere. This makes it possible to measure the degree of contamination in rooms such as smoking rooms with low-concentration gas atmospheres, which was previously thought to be impossible.

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

第1図は金属酸化物半導体素子におけるガス濃
度と抵抗値との関係図、第2図は本発明の方法を
実施する装置の一例を示す回路図、第3図はその
ガス検出部の断面説明図である。 2…センサー、3,8…スイツチ、4,5…イ
ンピーダンス変換器、6…インバータ、12…積
分器、14…コントローラ、30…ガス検出部、
50…室外雰囲気、60…室内雰囲気。
Fig. 1 is a diagram showing the relationship between gas concentration and resistance value in a metal oxide semiconductor element, Fig. 2 is a circuit diagram showing an example of an apparatus for carrying out the method of the present invention, and Fig. 3 is a cross-sectional explanation of the gas detection section. It is a diagram. 2... Sensor, 3, 8... Switch, 4, 5... Impedance converter, 6... Inverter, 12... Integrator, 14... Controller, 30... Gas detection section,
50...Outdoor atmosphere, 60...Indoor atmosphere.

Claims (1)

【特許請求の範囲】[Claims] 1 金属酸化物半導体ガスセンサーを、被計測室
雰囲気と室外の大気とに交互に触れさせて、該セ
ンサーの被計測室雰囲気と大気とにおける出力の
相違を求め、これにより被計測室雰囲気と大気と
に共通した環境変動の影響を除去して、被計測雰
囲気中のガス濃度を検出することを特徴とする室
内雰囲気中の低濃度ガス検出方法。
1. A metal oxide semiconductor gas sensor is brought into contact with the atmosphere of the room to be measured and the atmosphere outside the room, and the difference in the output of the sensor between the atmosphere of the room to be measured and the atmosphere is determined. A method for detecting a low concentration gas in an indoor atmosphere, characterized by detecting a gas concentration in an atmosphere to be measured while removing the influence of environmental changes common to both.
JP6369075A 1975-05-27 1975-05-27 Method of detecting pollution degree in air in a room Granted JPS51139396A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6369075A JPS51139396A (en) 1975-05-27 1975-05-27 Method of detecting pollution degree in air in a room

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6369075A JPS51139396A (en) 1975-05-27 1975-05-27 Method of detecting pollution degree in air in a room

Publications (2)

Publication Number Publication Date
JPS51139396A JPS51139396A (en) 1976-12-01
JPS6350658B2 true JPS6350658B2 (en) 1988-10-11

Family

ID=13236612

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6369075A Granted JPS51139396A (en) 1975-05-27 1975-05-27 Method of detecting pollution degree in air in a room

Country Status (1)

Country Link
JP (1) JPS51139396A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5832A (en) * 1981-06-23 1983-01-05 Sharp Corp Air conditioner with automatic ventilating function

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS494395U (en) * 1972-04-13 1974-01-16

Also Published As

Publication number Publication date
JPS51139396A (en) 1976-12-01

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