JPH0416749A - Method and apparatus for measuring ozone concentration - Google Patents
Method and apparatus for measuring ozone concentrationInfo
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- JPH0416749A JPH0416749A JP11991890A JP11991890A JPH0416749A JP H0416749 A JPH0416749 A JP H0416749A JP 11991890 A JP11991890 A JP 11991890A JP 11991890 A JP11991890 A JP 11991890A JP H0416749 A JPH0416749 A JP H0416749A
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- wavelength
- ozone
- ozone concentration
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Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、オゾン濃度測定方法及び装置に関し、特に、
試料セル内にオゾン水又はオゾンガス等の試料を導入す
るオゾン測定方法において、高精度の測定を行うための
新規な改良に間する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a method and apparatus for measuring ozone concentration, and in particular,
New improvements will be made to perform highly accurate measurements in an ozone measurement method that introduces a sample such as ozone water or ozone gas into a sample cell.
従来、用いられていたこの種のオゾン濃度測定方法とし
ては種々あるが、その中で代表的なものについて述べる
と、第3図にて示す特開昭63−218842号公報の
方法を挙げることができる。There are various methods of measuring ozone concentration of this type that have been used in the past, but the most representative one is the method disclosed in Japanese Patent Application Laid-Open No. 63-218842, shown in FIG. can.
すなわち、図において符号1で示されるものはオゾン濃
度計であり、このオゾン濃度計1内には、基準水を収容
した基準水用セル2及びオゾン水を収容したオゾン水用
セル3が設けられている。That is, what is indicated by the reference numeral 1 in the figure is an ozone concentration meter, and inside this ozone concentration meter 1, a reference water cell 2 containing reference water and an ozone water cell 3 containing ozone water are provided. ing.
前記基準水用セル2には、基準水容器4からの基準水が
第1配管5を介して導入されており、前記オゾン水用セ
ル3には、オゾン水容器6からのオゾン水が第2配管7
を介して導入されている。Reference water from a reference water container 4 is introduced into the reference water cell 2 via a first pipe 5, and ozone water from an ozone water container 6 is introduced into the ozone water cell 3 through a second pipe. Piping 7
has been introduced through.
従って、各セル2.3に光を照射し、透過光量を測定し
で、オゾンのスペクトル吸収特性によって、セル中のオ
ゾン濃度を計測し、この計測した値をランバート・ベー
ルの法則を適用してオゾン濃度を求めていた。Therefore, by irradiating each cell 2.3 with light and measuring the amount of transmitted light, the ozone concentration in the cell is measured based on the spectral absorption characteristics of ozone, and this measured value is applied to the Lambert-Beer law. I was looking for ozone concentration.
本発明によるオゾン濃度測定方法は、試料にオゾンの吸
収スペクトルに適合するスペクトルを照射し、透過した
透過光量を測定すると共に、オゾンのスペクトル吸収特
性によってオゾン濃度を測定するようにしたオゾン濃度
測定方法において、前記オゾンの最大吸収帯の第1波長
及び前記第1波長とは異なる波長の第2波長と検出し、
前記第1波長及び第2波長の検出量の割合を基に、オゾ
ン濃度を測定するようにした方法である。The ozone concentration measuring method according to the present invention irradiates a sample with a spectrum matching the absorption spectrum of ozone, measures the amount of transmitted light, and measures the ozone concentration based on the spectral absorption characteristics of ozone. , detecting a first wavelength of the maximum absorption band of the ozone and a second wavelength different from the first wavelength,
In this method, the ozone concentration is measured based on the ratio of the detected amounts of the first wavelength and the second wavelength.
また、他の発明であるオゾン濃度測定装置は、試料にオ
ゾンの吸収スペクトルに適合するスペクトルを光源から
照射し、透過した透過光量を測定すると共に、オゾンの
スペクトル吸収特性によってオゾン濃度を測定するよう
にしたオゾン濃度測定装置において、前記光源からの光
を受ける試料セルと、前記試料セルからの透過光を受け
る第1波長検出部及び第2波長検出部と、前記各波長検
出部に設けられた干渉フィルタ及び信号変換部と、前記
各波長検出部からの出力信号を処理するための信号処理
部とを備えた構成である。Another invention, an ozone concentration measuring device, irradiates a sample with a spectrum matching the absorption spectrum of ozone from a light source, measures the amount of transmitted light, and measures the ozone concentration based on the spectral absorption characteristics of ozone. In the ozone concentration measuring device according to the present invention, a sample cell that receives light from the light source, a first wavelength detection section and a second wavelength detection section that receive transmitted light from the sample cell, and a first wavelength detection section and a second wavelength detection section that are provided in each of the wavelength detection sections. This configuration includes an interference filter, a signal conversion section, and a signal processing section for processing output signals from each of the wavelength detection sections.
本発明によるオゾン濃度測定方法及び装置においては、
オゾンの最大吸収帯の第1波長及び前記第1波長とは異
なる波長の第2波長を、第1波長検出部及び第2波長検
出部を介して検出し、各波長の検出量の割合を基にして
信号処理部でオゾン濃度を測定することができる。In the ozone concentration measuring method and device according to the present invention,
A first wavelength of the maximum absorption band of ozone and a second wavelength different from the first wavelength are detected via a first wavelength detector and a second wavelength detector, and the ratio of the detected amount of each wavelength is determined. ozone concentration can be measured using the signal processing section.
従って、前記各波長の受光量の比を見ることによって試
料セルの汚れをキャンセルできると共に、光源の劣化に
よる第1波長のスペクトル強度の変動をキャンセルでき
、常に安定した高精度のオゾン濃度の測定を行うことが
できる。Therefore, by looking at the ratio of the amount of light received at each wavelength, it is possible to cancel contamination of the sample cell, and also to cancel fluctuations in the spectral intensity of the first wavelength due to deterioration of the light source, making it possible to always measure stable and highly accurate ozone concentration. It can be carried out.
以下、図面と共に本発明によるオゾン濃度測定方法及び
装置の好適な実施例について詳細に説明する。Hereinafter, preferred embodiments of the ozone concentration measuring method and apparatus according to the present invention will be described in detail with reference to the drawings.
尚、従来例と同−又は同等部分には、同一符号を付して
説明する。It should be noted that the same or equivalent parts as in the conventional example will be described with the same reference numerals.
第1図及び第2図は、本発明によるオゾン濃度測定方法
及び装置を示すためのもので、第1図は全体構成を示す
ブロック図、第2区は測定状態を示す構成図である。1 and 2 are for illustrating the ozone concentration measuring method and apparatus according to the present invention. FIG. 1 is a block diagram showing the overall configuration, and the second section is a configuration diagram showing the measurement state.
図において符号1で示されるものは、オゾン濃度測定装
置であり、このオゾン濃度測定装置1の光源10からの
オゾンの吸収スペクトルに適合するスペクトルを有する
光は、1個の試料セル11に照射され、この試料セル1
1内には、オゾン水又はオゾンガスからなる試料が収容
されている。What is indicated by the reference numeral 1 in the figure is an ozone concentration measuring device, and light having a spectrum matching the absorption spectrum of ozone from a light source 10 of this ozone concentration measuring device 1 is irradiated onto one sample cell 11. , this sample cell 1
1 contains a sample made of ozone water or ozone gas.
前記試料セル11を透過した透過光は、第1波長検出部
12及び第2波長検出部13に供給され、前記各波長検
出部12.13は、干渉フィルタ14.14a、信号変
換部15.15a及び電気信号増幅器16,16aとか
ら各々構成されている。The transmitted light that has passed through the sample cell 11 is supplied to a first wavelength detection section 12 and a second wavelength detection section 13, and each of the wavelength detection sections 12.13 includes an interference filter 14.14a and a signal conversion section 15.15a. and electric signal amplifiers 16 and 16a, respectively.
前記第1波長検出部12は、オゾンの最大吸収帯の第1
波長を検出するもので、この第1波長は、253.7
nmである。従って、オゾン水に吸収されなかった光の
うちで253.7 nm付近の光は干渉フィルタ14に
より選択的に透過され、光信号を電気信号に変換する信
号変換部15に供給される。ここで、前記干渉フィルタ
14は、オゾンの最大吸収帯波長の253.7 nm付
近だけを透過させるバンドパスフィルタが望ましいが、
ロングパスフィルタ、ショートバスフィルタなどを組み
合わせて構成しても良い、また、前記信号変換部15は
、オゾンの最大吸収帯波長の253.7 n面に感度を
もつフォトセンサなどで構成されている。また、前述の
253.7 na+alにしか感度をもたない信号変換
部15を用いた場合には、干渉フィルタ14を用いる必
要はない。The first wavelength detection unit 12 detects the first wavelength of the maximum absorption band of ozone.
It detects the wavelength, and this first wavelength is 253.7
It is nm. Therefore, out of the light that is not absorbed by the ozonated water, light around 253.7 nm is selectively transmitted by the interference filter 14 and supplied to the signal converter 15 that converts the optical signal into an electrical signal. Here, it is preferable that the interference filter 14 is a bandpass filter that transmits only the wavelength around 253.7 nm, which is the maximum absorption band wavelength of ozone.
The signal converter 15 may be configured by combining a long pass filter, a short bus filter, etc. The signal converter 15 is configured by a photosensor or the like sensitive to the 253.7 n-plane, which is the wavelength of the maximum absorption band of ozone. Furthermore, when the signal converter 15 described above is used, which is sensitive only to 253.7 na+al, it is not necessary to use the interference filter 14.
また、信号変換部15の出力は極めて微小な信号の為、
後段の電気信号増幅器16において、所定のレベルまで
増幅し、信号処理部17が必要とする電圧信号又は電流
信号のレベルに変換する。In addition, since the output of the signal converter 15 is an extremely small signal,
The subsequent electric signal amplifier 16 amplifies the signal to a predetermined level, and converts it to a voltage signal or current signal level required by the signal processing section 17.
次に、前記第2波長検出部13は前記第1波長以外の第
2波長を検出するものであり、オゾンの吸収帯以外の波
長を検出する。従って、第1波長検出部12がオゾンの
吸収を検出するのに対して、第2波長検出部13は、オ
ゾンの濃度を正確に求めるために設けられ、光源の劣化
、オゾン以外の物質による吸収を検出するためのもので
ある。Next, the second wavelength detection section 13 detects a second wavelength other than the first wavelength, and detects a wavelength other than the absorption band of ozone. Therefore, while the first wavelength detection section 12 detects ozone absorption, the second wavelength detection section 13 is provided to accurately determine the ozone concentration, and detects deterioration of the light source and absorption by substances other than ozone. The purpose is to detect
さらに、前記干渉フィルタ14aは、第2波長のみを通
過させるバンドパスフィルタが望ましいが、ロングパス
フィルタ、ショートバスフィルタなどを組み合わせて構
成しても良い。前記信号変換部15aは第1波長で使用
した波長以外の波長の光量を電気信号に変換する機能を
有し、フォトセンサなどを使用する。また、この信号変
換部15aが選択した第2波長のみに感度をもつもので
あれば、干渉フィルタ14aを省略することができる。Further, the interference filter 14a is preferably a bandpass filter that passes only the second wavelength, but may be configured by combining a longpass filter, a shortpass filter, or the like. The signal converter 15a has a function of converting the amount of light of a wavelength other than the wavelength used in the first wavelength into an electrical signal, and uses a photo sensor or the like. Furthermore, if the signal converter 15a is sensitive only to the selected second wavelength, the interference filter 14a can be omitted.
また、前記信号変換部15aの出力は、微小信号の為、
後段の電気信号増幅部16aにおいて。Furthermore, since the output of the signal converter 15a is a minute signal,
In the subsequent electrical signal amplification section 16a.
所定のレベルまで増幅し、信号処理部17が必要とする
電圧信号又は電流信号に変換する。The signal is amplified to a predetermined level and converted into a voltage signal or current signal required by the signal processing section 17.
前記第1波長検出部12の出力信号A及び、第2波長検
出部13の出力信号Bを基に、ランバートベールの法則
に従い、信号処理部17で演算し、その結果を表示器1
8で表示あるいは記録することができるように構成され
ている。Based on the output signal A of the first wavelength detection section 12 and the output signal B of the second wavelength detection section 13, a signal processing section 17 performs calculations according to Lambert Beer's law, and the results are displayed on the display 1.
It is configured so that it can be displayed or recorded with 8.
本発明によるオゾン濃度測定装置は、前述したように構
成されており、以下に、その測定方法について説明する
。The ozone concentration measuring device according to the present invention is configured as described above, and the measuring method thereof will be explained below.
まず、光源10より放射される第1波長の光強度をPl
、第2波長の光強度を22とする。光源10より放射さ
れる光は、光源10の電源電圧Vに依存しているので、
式(1)、式(2)で表わされる。First, the light intensity of the first wavelength emitted from the light source 10 is Pl
, the light intensity of the second wavelength is 22. Since the light emitted from the light source 10 depends on the power supply voltage V of the light source 10,
It is expressed by equations (1) and (2).
p、 = t、、・ ■ ・ ・
・ (1)P、=に、・ ■ ・ ・
・ ・ (2)次に、試料セル11の汚れによる吸収
係数をρとすると共に、この汚れを通過した後の第1波
長の光の強度をP3、第2波長の光の強度をP、とすれ
ばP、及びP、は式(3)、式(4)となる。p, = t, ・ ■ ・ ・
・ (1) P, = to, ・ ■ ・ ・
・ ・ (2) Next, let the absorption coefficient due to dirt on the sample cell 11 be ρ, and let the intensity of the light of the first wavelength after passing through this dirt be P3, and the intensity of the light of the second wavelength be P. Then, P and P become equations (3) and (4).
P、=ρ・P、=ρ・kl・■ ・・・(3)P4=ρ
・P、=ρ・k2・■ ・・・(4)そこで、前記第1
波長の光の強度P、はオゾンによる吸収を受けP、とな
り、前記第2波長の光の強度P、は水、その他の物質に
吸収を受けP6となる。尚、前述のP、及びP6は、干
渉フィルタ14,14aにより選択的に各信号変換部1
515aにより検出されるものとする。また、各信号変
換部15.15aに、それぞれ、第1波長及び第2波長
にのみ感度をもつものを設けた場合には、前述したよう
に、干渉フィルタ14.14aを省略することができる
。P, = ρ・P, = ρ・kl・■ ...(3) P4=ρ
・P,=ρ・k2・■...(4) Therefore, the first
The intensity P of the light of the second wavelength becomes P6 when absorbed by ozone, and the intensity P of the light of the second wavelength becomes P6 when absorbed by water or other substances. Incidentally, the above-mentioned P and P6 are selectively connected to each signal converter 1 by the interference filters 14 and 14a.
515a. Furthermore, if each signal converter 15.15a is provided with one sensitive only to the first wavelength and the second wavelength, the interference filter 14.14a can be omitted, as described above.
前述の条件により、P、とP、及びP、とP6の間には
、ランバートベールの法則による式(5)の関係が成立
する。According to the above-mentioned conditions, the relationship of equation (5) according to Lambert Beer's law holds between P and P and between P and P6.
I = I ae−”c・・・(5) 工 :溶液の透過光の強度 ■。:純溶媒の透過光の強度 α :モル吸光係数 L :吸収物質層の厚さ C:吸収物質の濃度 故に、下記の式(6)、式(7)が成立する。I = I ae-”c...(5) Technique: Intensity of light transmitted through solution ■. :Intensity of transmitted light of pure solvent α: Molar extinction coefficient L: Thickness of absorbing material layer C: concentration of absorbing substance Therefore, the following equations (6) and (7) hold true.
P5=P3・e −al“L、CI 、 e−mloL
、cm、、、に、、y −(6)P、=P、−e−“
°1°’2 −2− L −c 2 、 ρ、に2.v
、 、 、 (7゜e
式(6)と式(7)の比をとると、
式(8)をC1について解くと、式(9)となる。P5=P3・e-al“L, CI, e-mloL
,cm,,,,y −(6)P,=P,−e−“
°1°'2 −2− L −c 2 , ρ, 2. v
, , , (7°e Taking the ratio of equation (6) and equation (7), Solving equation (8) for C1 yields equation (9).
式(9)において、k k2.C1,α、、C2,Lは事 前に測定する事により知ることができる量である。In equation (9), k k2. C1, α, , C2, L are things This is a quantity that can be known by measuring it in advance.
従って、オゾン濃度C1は、P、及びP6を測定するこ
とにより得る事ができる。Therefore, the ozone concentration C1 can be obtained by measuring P and P6.
また、式(9)にはρ、■が含まれておらず、オゾン濃
度CIはセルの汚れ及び光源の電源電圧の変動による影
響を受けることがない。Furthermore, Equation (9) does not include ρ and ■, and the ozone concentration CI is not affected by cell contamination or fluctuations in the power supply voltage of the light source.
本発明によるオゾン濃度測定方法及び装置は、以上のよ
うに構成されているため、次のような効果を得ることが
できる。Since the ozone concentration measuring method and apparatus according to the present invention are configured as described above, the following effects can be obtained.
すなわち、オゾンの吸収スペクトル帯である第1波長と
第1波長以外の第2波長の受光量の比をみることにより
、試料セルの汚れのキャンセル、光源の劣化による第1
波長のスペクトル強度の変動のキャンセル等を達成する
ことができ5オゾン濃度の高精度な測定を行うことがで
きる。In other words, by looking at the ratio of the amount of light received at the first wavelength, which is the absorption spectrum band of ozone, and the amount of light received at a second wavelength other than the first wavelength, it is possible to cancel the contamination of the sample cell and to cancel the first wavelength due to deterioration of the light source.
It is possible to cancel fluctuations in wavelength spectrum intensity, etc., and to perform highly accurate measurement of ozone concentration.
また、従来方法では、基準水を必要としていたが、本発
明の方法では、基準水は全く必要でなくなり、試料であ
るオゾン水又はオゾンガスの導入だけでも良くなるため
、装置の全体形状を大巾に小形化することができると共
に、同時に、コストダウンを達成することができる。In addition, the conventional method required reference water, but the method of the present invention eliminates the need for reference water at all and only requires the introduction of ozone water or ozone gas as a sample, so the overall shape of the device can be changed considerably. It is possible to downsize the device and at the same time achieve cost reduction.
第1図及び第2図は、本発明によるオゾン濃度測定方法
及び装置を示すためのもので、第1図は全体構成を示す
ブロック図、第2図は測定状態を示す構成図、第3図は
従来のオゾン−濃度測定方法を示す構成図である。
10は光源、11は試料セル、12は第1波長検出部、
13は第2波長検出部、15.15aは信号変換部、A
、Bは出力信号、17は信号処理部である。
第1図
第2図
第3図
手続補正書
平成2年8月3日1 and 2 are for illustrating the ozone concentration measuring method and apparatus according to the present invention. FIG. 1 is a block diagram showing the overall configuration, FIG. 2 is a configuration diagram showing the measurement state, and FIG. 3 is a block diagram showing the overall configuration. 1 is a configuration diagram showing a conventional ozone concentration measuring method. 10 is a light source, 11 is a sample cell, 12 is a first wavelength detection section,
13 is a second wavelength detection section, 15.15a is a signal conversion section, A
, B are output signals, and 17 is a signal processing section. Figure 1 Figure 2 Figure 3 Procedural Amendment Statement August 3, 1990
Claims (2)
るスペクトルを照射し、透過した透過光量を測定すると
共に、オゾンのスペクトル吸収特性によつてオゾン濃度
を測定するようにしたオゾン濃度測定方法において、 前記オゾンの最大吸収帯の第1波長及び前記第1波長と
は異なる波長の第2波長を検出し、前記第1波長及び第
2波長の検出量の割合を基に、オゾン濃度を測定するこ
とを特徴とするオゾン濃度測定方法。(1) An ozone concentration measuring method in which the sample (11) is irradiated with a spectrum matching the absorption spectrum of ozone, the amount of transmitted light is measured, and the ozone concentration is measured based on the spectral absorption characteristics of ozone. , detecting a first wavelength of the maximum absorption band of the ozone and a second wavelength different from the first wavelength, and measuring the ozone concentration based on the ratio of the detected amounts of the first wavelength and the second wavelength. A method for measuring ozone concentration characterized by the following.
るスペクトルを光源(10)から照射し、透過した透過
光量を測定すると共に、オゾンのスペクトル吸収特性に
よってオゾン濃度を測定するようにしたオゾン濃度測定
方法において、 前記光源(10)からの光を受ける試料セル(11)と
、前記試料セル(11)からの透過光を受ける第1波長
検出部(12)及び第2波長検出部(13)と、前記各
波長検出部(12、13)に設けられた信号変換部(1
5、15a)と、前記各波長検出部(12、13)から
の出力信号(A、B)を処理するための信号処理部(1
7)とを備え、 前記各波長検出部(12、13)からの互いに異なる第
1波長及び第2波長の検出量の割合を基に、オゾン濃度
を測定するようにしたことを特徴とするオゾン濃度測定
装置。(2) Ozone concentration in which the sample (11) is irradiated with a spectrum matching the absorption spectrum of ozone from the light source (10), the amount of transmitted light is measured, and the ozone concentration is measured based on the spectral absorption characteristics of ozone. In the measurement method, a sample cell (11) receives light from the light source (10), and a first wavelength detection section (12) and a second wavelength detection section (13) that receive transmitted light from the sample cell (11). and a signal converter (1) provided in each of the wavelength detectors (12, 13).
5, 15a), and a signal processing unit (1) for processing the output signals (A, B) from each wavelength detection unit (12, 13).
7), wherein the ozone concentration is measured based on the ratio of the detected amounts of the first wavelength and the second wavelength, which are different from each other from each of the wavelength detection units (12, 13). Concentration measuring device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11991890A JPH0416749A (en) | 1990-05-11 | 1990-05-11 | Method and apparatus for measuring ozone concentration |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11991890A JPH0416749A (en) | 1990-05-11 | 1990-05-11 | Method and apparatus for measuring ozone concentration |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0416749A true JPH0416749A (en) | 1992-01-21 |
Family
ID=14773404
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11991890A Pending JPH0416749A (en) | 1990-05-11 | 1990-05-11 | Method and apparatus for measuring ozone concentration |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0416749A (en) |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2000171394A (en) * | 1998-12-01 | 2000-06-23 | Tetra Laval Holdings & Finance Sa | Method and apparatus for determining the concentration of a substance in a sample in which interfering materials are present |
| JP2002062257A (en) * | 2000-08-23 | 2002-02-28 | Fuji Xerox Co Ltd | Measuring instrument for measuring ozone concentration |
| JP2002139429A (en) * | 2000-11-06 | 2002-05-17 | Kurabo Ind Ltd | Dissolved ozone concentration measurement device |
| KR100724877B1 (en) * | 2003-06-27 | 2007-06-04 | 세이코 엡슨 가부시키가이샤 | Paper feeder |
| JP2009517641A (en) * | 2005-11-29 | 2009-04-30 | ジーイー・ヘルスケア・バイオサイエンス・アクチボラグ | Method and apparatus for measuring the concentration of a substance in a solution |
| US7936460B2 (en) | 2006-05-31 | 2011-05-03 | Toyota Jidosha Kabushiki Kaisha | Sensor unit in exhaust gas analyzer |
| JP2011169875A (en) * | 2010-02-22 | 2011-09-01 | Hemmi Slide Rule Co Ltd | Ozone detection sensor |
| US8085404B2 (en) | 2006-08-23 | 2011-12-27 | Toyota Jidosha Kabushiki Kaisha | Gas analyzer and gas analyzing method |
| JP2019203889A (en) * | 2018-05-21 | 2019-11-28 | 修 三浦 | Method for observing ozone layer |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01244341A (en) * | 1988-03-25 | 1989-09-28 | Seki Electron Kk | Light absorbing type ozone concentration measuring device |
-
1990
- 1990-05-11 JP JP11991890A patent/JPH0416749A/en active Pending
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01244341A (en) * | 1988-03-25 | 1989-09-28 | Seki Electron Kk | Light absorbing type ozone concentration measuring device |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2000171394A (en) * | 1998-12-01 | 2000-06-23 | Tetra Laval Holdings & Finance Sa | Method and apparatus for determining the concentration of a substance in a sample in which interfering materials are present |
| JP2002062257A (en) * | 2000-08-23 | 2002-02-28 | Fuji Xerox Co Ltd | Measuring instrument for measuring ozone concentration |
| JP2002139429A (en) * | 2000-11-06 | 2002-05-17 | Kurabo Ind Ltd | Dissolved ozone concentration measurement device |
| KR100724877B1 (en) * | 2003-06-27 | 2007-06-04 | 세이코 엡슨 가부시키가이샤 | Paper feeder |
| JP2009517641A (en) * | 2005-11-29 | 2009-04-30 | ジーイー・ヘルスケア・バイオサイエンス・アクチボラグ | Method and apparatus for measuring the concentration of a substance in a solution |
| US7936460B2 (en) | 2006-05-31 | 2011-05-03 | Toyota Jidosha Kabushiki Kaisha | Sensor unit in exhaust gas analyzer |
| US8085404B2 (en) | 2006-08-23 | 2011-12-27 | Toyota Jidosha Kabushiki Kaisha | Gas analyzer and gas analyzing method |
| JP2011169875A (en) * | 2010-02-22 | 2011-09-01 | Hemmi Slide Rule Co Ltd | Ozone detection sensor |
| JP2019203889A (en) * | 2018-05-21 | 2019-11-28 | 修 三浦 | Method for observing ozone layer |
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