JP2017015678A - Gas concentration measurement device - Google Patents
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Abstract
Description
本発明は、ガス濃度測定装置に関し、より詳細には、2濃度検査にて高精度なガス濃度測定が可能な算出式を用いたガス濃度測定装置に関する。 The present invention relates to a gas concentration measuring apparatus, and more particularly to a gas concentration measuring apparatus using a calculation formula capable of highly accurate gas concentration measurement in a two-concentration test.
従来から大気中の測定対象ガスの濃度測定を行うガス濃度測定装置として、ガスの種類によって吸収される赤外線の波長が異なることを利用し、この吸収量を検出することによりそのガス濃度を測定する非分散赤外吸収型(Non−Dispersive Infrared)ガス濃度測定装置が知られている。この原理を用いたガス濃度測定装置としては、例えば、測定対象ガスが吸収特性を持つ波長に限定した赤外線を透過するフィルタ(透過部材)と赤外線センサを組み合わせ、赤外線の吸収量を測定することによってガスの濃度を測定するようにしたものが挙げられる。 Conventionally, as a gas concentration measurement device that measures the concentration of the gas to be measured in the atmosphere, the gas concentration is measured by detecting the amount of absorption using the fact that the wavelength of infrared rays that are absorbed depends on the type of gas Non-dispersive Infrared gas concentration measuring devices are known. As a gas concentration measurement device using this principle, for example, by combining a filter (transmission member) that transmits infrared light limited to a wavelength with which the measurement target gas has absorption characteristics and an infrared sensor, the amount of infrared absorption is measured. The gas concentration can be measured.
また、この原理の応用を用いたガス濃度測定装置として、例えば、特許文献1に記載のものは、測定対象ガスによる赤外線の吸収が生じない波長域の赤外線を選択的に透過する参照用フィルタと、測定対象ガスによる赤外線の吸収が生じる波長域の赤外線を選択的に透過する測定用フィルタをそれぞれ配置した赤外線検出素子を複数配置し、それぞれの赤外線検出素子からの出力信号に基づいて測定対象ガスの検出や濃度測定をしており、検出精度や出力の安定性を向上させた炭酸ガス濃度測定装置及び炭酸ガス検出方法である。
以下、これらも含めて、ガス濃度測定装置及びガス濃度測定方法ともいう。その動作原理は、波長による吸収度合いの差異を、炭酸ガス検出に応用したものである。光源であるセラミックヒータから放射された赤外線において、波長4.3μm付近の赤外線は、気体容器内の炭酸ガスにより吸収されて、その放射強度が低下する。一方、波長3.9μmの赤外線は、炭酸ガスによる吸収はなく、その放射強度が低下することはない。
In addition, as a gas concentration measuring device using the application of this principle, for example, the one described in Patent Document 1 is a reference filter that selectively transmits infrared light in a wavelength range in which infrared absorption by the measurement target gas does not occur. , A plurality of infrared detection elements each having a measurement filter that selectively transmits infrared light in a wavelength range in which infrared absorption by the measurement target gas occurs, and the measurement target gas based on an output signal from each infrared detection element Are a carbon dioxide concentration measuring device and a carbon dioxide detection method that improve detection accuracy and output stability.
In the following, these are also referred to as a gas concentration measuring device and a gas concentration measuring method. The principle of operation is that the difference in the degree of absorption depending on the wavelength is applied to carbon dioxide gas detection. In the infrared rays emitted from the ceramic heater as the light source, the infrared rays having a wavelength of about 4.3 μm are absorbed by the carbon dioxide gas in the gas container, and the radiation intensity is reduced. On the other hand, infrared rays having a wavelength of 3.9 μm are not absorbed by carbon dioxide gas, and their radiation intensity does not decrease.
そして、ガス測定装置の気体容器内を通過した異なる波長を含む赤外線から、波長4.3μmと波長3.9μmとの2波を、2波それぞれに対応した通過帯域を有する2種類の光学フィルタで濾波選別する。これら波長の異なる赤外線それぞれの放射強度に基づいて、気体容器内の炭酸ガスの濃度が算出される。セラミックヒータの放射強度分布は、炭酸ガスの赤外線吸収スペクトルを含む、2μm〜50μmの波長領域でブロードであり、炭酸ガスの赤外線吸収スペクトル付近の波長領域で十分な放射強度を有する。したがって、光源にセラミックヒータを用いたガス測定装置の検出精度及び出力の安定性は向上する。 Then, from the infrared rays including different wavelengths that have passed through the gas container of the gas measuring device, two waves with a wavelength of 4.3 μm and a wavelength of 3.9 μm are two types of optical filters having passbands corresponding to the two waves respectively. Filter selection. Based on the radiation intensity of each of the infrared rays having different wavelengths, the concentration of carbon dioxide in the gas container is calculated. The radiation intensity distribution of the ceramic heater is broad in the wavelength region of 2 μm to 50 μm including the infrared absorption spectrum of carbon dioxide, and has a sufficient radiation intensity in the wavelength region near the infrared absorption spectrum of carbon dioxide. Therefore, the detection accuracy and output stability of the gas measuring device using a ceramic heater as the light source are improved.
非分散赤外吸収型ガス濃度測定装置では、理想的にはランバートベールの法則(Lambert−Beer_law)に基づいて得られる下記式(1)に則った測定用赤外線検出部の出力が得られる。 In the non-dispersive infrared absorption type gas concentration measuring device, the output of the infrared detecting unit for measurement is ideally obtained according to the following equation (1) obtained based on Lambert-Beer's law (Lambert-Beer_law).
(式中、cはガスの濃度、εは吸光度係数、l(エル)は実態的な光路長、Vout(0)は測定対象ガスによる吸収が無い場合の測定用赤外線検出部の仮想出力、Voutは測定対象ガスによる吸収が有る場合の測定用赤外線検出部の出力である。)
しかし、測定用赤外線検出部の出力に含まれる回路的、光学的オフセットなど影響によって、実際の出力特性は式(1)のようなLogの関数から乖離する。ここでいう回路的オフセットとは、例えば測定用赤外線検出部に含まれる増幅回路によって生じる。また、光学的オフセットとは、例えば測定対象ガスによって吸収されない波長の光の測定用赤外線検出部への入射等によって生じる。
(Where c is the gas concentration, ε is the absorbance coefficient, l (el) is the actual optical path length, V out (0) is the virtual output of the infrared detector for measurement when there is no absorption by the gas to be measured, V out is the output of the measurement infrared detector when there is absorption by the gas to be measured.)
However, the actual output characteristics deviate from the Log function as shown in Equation (1) due to the influence of circuit and optical offset included in the output of the measurement infrared detection unit. The circuit-like offset here is caused by, for example, an amplifier circuit included in the measurement infrared detector. The optical offset is caused by, for example, incidence of light having a wavelength that is not absorbed by the measurement target gas into the measurement infrared detection unit.
さらに、光源から測定用赤外線検出部までの光路長や、測定対象ガスによる吸収が無い場合の測定用赤外線検出部の仮想出力は個体ごとにばらつきが生じる。
そのため、2濃度検査を前提に測定対象ガスの濃度値を演算する場合、従来は、例えば、測定用赤外線検出部の出力を変数とし測定対象ガスの濃度を出力する2次関数を定義し、2次関数に含まれる3つの係数のうち1つの係数を固定値とし、2濃度の検査から残りの2つの係数を求めることで、濃度演算用の関数を決定していた。しかしこの演算方法では、回路的、光学的オフセットの影響や多数の光路の影響、光路長や測定対象ガスによる吸収が無い場合の測定用赤外線検出部の仮想出力ばらつきの影響を完全に補償できないため、演算精度は低いものであった。
Further, the optical path length from the light source to the measurement infrared detection unit and the virtual output of the measurement infrared detection unit when there is no absorption by the measurement target gas vary from individual to individual.
Therefore, when calculating the concentration value of the measurement target gas on the premise of the two-concentration test, conventionally, for example, a quadratic function that outputs the concentration of the measurement target gas with the output of the measurement infrared detector as a variable is defined. A function for density calculation is determined by determining one of the three coefficients included in the next function as a fixed value and obtaining the remaining two coefficients from the two-density test. However, this calculation method cannot completely compensate for the effects of circuit and optical offsets, the effects of many optical paths, the optical output length of the measurement infrared detector when there is no absorption by the optical path length and the gas to be measured, and so on. The calculation accuracy was low.
本発明はこのような問題に鑑みてなされたもので、その目的とするところは、2濃度検査にて、高精度なガス濃度測定が可能なガス濃度測定装置を提供することにある。 The present invention has been made in view of such problems, and an object of the present invention is to provide a gas concentration measuring apparatus capable of measuring a gas concentration with high accuracy by a two-concentration test.
本発明者らは上記課題を解決するために鋭意検討した結果、以下の発明により上記課題を解決できることを見出し、本発明を完成させた。
本発明の様態は、光源と、光源からの光を受光し、光に応じた信号である測定出力を出力する測定用赤外線検出部と、測定出力が入力される演算部と、を備えたガス濃度測定装置であって、演算部は、第1の濃度の測定対象ガス中で光源を点灯させた時に測定用赤外線検出部が出力する第1の測定出力と、第1の濃度と異なる第2の濃度の測定対象ガス中で光源を点灯させた時に測定用赤外線検出部が出力する第2の測定出力と、基準濃度算出式から求まる濃度が第1の濃度であるときの変数の値である第1の解と、基準濃度算出式から求まる濃度が第2の濃度であるときの変数の値である第2の解と、から得られる係数と、基準濃度算出式を第1の解と第1の濃度で補正した式と、第1の濃度と、を含む濃度算出式に、測定時の測定出力を第1の測定出力で規格化して代入することで測定対象ガスの濃度を演算するガス濃度測定装置である。
As a result of intensive studies to solve the above problems, the present inventors have found that the above problems can be solved by the following invention, and have completed the present invention.
According to an aspect of the present invention, a gas including a light source, a measurement infrared detection unit that receives light from the light source and outputs a measurement output that is a signal corresponding to the light, and a calculation unit to which the measurement output is input. In the concentration measurement device, the calculation unit outputs a first measurement output that is output from the measurement infrared detection unit when the light source is turned on in the measurement target gas having the first concentration, and a second that is different from the first concentration. Is the second measurement output output from the measurement infrared detection unit when the light source is turned on in the measurement target gas having the concentration, and the value of the variable when the concentration obtained from the reference concentration calculation formula is the first concentration. The coefficient obtained from the first solution and the second solution which is the value of the variable when the concentration obtained from the reference concentration calculation formula is the second concentration, and the reference concentration calculation formula are expressed as the first solution and the first solution. The measurement output at the time of measurement is added to the density calculation formula including the formula corrected with the density of 1 and the first density. A gas concentration measuring apparatus which calculates a concentration of the measurement target gas by substituting normalized by the first measurement output.
本発明によれば、高精度なガス濃度測定が可能な演算を用いたガス濃度測定装置を実現することが可能になる。 ADVANTAGE OF THE INVENTION According to this invention, it becomes possible to implement | achieve the gas concentration measuring apparatus using the calculation which can measure a gas concentration with high precision.
以下の詳細な説明では、本発明の実施形態の完全な理解を提供するように多くの特定の具体的な構成について記載されている。しかしながら、このような特定の具体的な構成に限定されることなく他の実施態様が実施できることは明らかであろう。また、以下の実施形態は、特許請求の範囲に係る発明を限定するものではなく、実施形態で説明されている特徴的な構成の組み合わせの全てを含むものである。
以下、図面を参照して本発明の実施形態について説明する。
In the following detailed description, numerous specific specific configurations are described to provide a thorough understanding of embodiments of the invention. However, it will be apparent that other embodiments may be practiced without limitation to such specific specific configurations. Further, the following embodiments do not limit the invention according to the claims, but include all combinations of characteristic configurations described in the embodiments.
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
[実施形態]
図1は、本発明に係るガス濃度測定装置の実施形態を説明するための図である。図中符号1はガス濃度測定装置、10はガスセル、11はガス導入口、12はガス導出口、20は光源、31は測定用赤外線検出部、40は演算部、Lは最短距離の光路長を示している。なおここでは参考のため、ガスセル10を明示しているが、本発明においてガスセルは必須の構成ではなく、ガスセルの無い形態でも試験容器内等にガス濃度測定装置を配置することで下記と同様の2濃度検査を行うことが可能である。
[Embodiment]
FIG. 1 is a diagram for explaining an embodiment of a gas concentration measuring apparatus according to the present invention. In the figure, reference numeral 1 is a gas concentration measuring device, 10 is a gas cell, 11 is a gas inlet, 12 is a gas outlet, 20 is a light source, 31 is an infrared detector for measurement, 40 is a calculator, and L is the optical path length of the shortest distance. Is shown. In addition, although the
本実施形態のガス濃度測定装置1は、光源20と、光源20からの光を受光し、光に応じた信号である測定出力を出力する測定用赤外線検出部31と、測定出力が入力される演算部40と、を備えたガス濃度測定装置である。
演算部40は、第1の濃度の測定対象ガス中で光源20を点灯させた時に測定用赤外線検出部31が出力する第1の測定出力と、第1の濃度と異なる第2の濃度の測定対象ガス中で光源20を点灯させた時に測定用赤外線検出部31が出力する第2の測定出力と、基準濃度算出式から求まる濃度が第1の濃度であるときの変数の値である第1の解と、基準濃度算出式から求まる濃度が第2の濃度であるときの変数の値である第2の解と、から得られる係数と、基準濃度算出式を第1の解と第1の濃度で補正した式と、第1の濃度と、を含む濃度算出式に、測定時の測定出力を第1の測定出力で規格化して代入することで測定対象ガスの濃度を演算する。これにより、2濃度検査にて、高精度なガス濃度測定が可能なガス濃度測定装置を提供することが可能となる。
The gas concentration measuring apparatus 1 of the present embodiment receives a
The
また、本実施形態のガス濃度測定装置1において、係数が、第2の測定出力と第1の測定出力の比と、第2の解と第1の解の比と、から得られるものであってもよい。これによりさらに高精度な濃度演算が可能になるという効果を奏する。
また、本実施形態のガス濃度測定装置1において、基準濃度算出式がn次多項式であり、濃度算出式は、基準濃度算出式の1次〜n次の係数を、第1の解で補正し、0次の係数を第1の濃度で補正した式に、係数をかけ、さらに第1の濃度を足し合わせた式でああってもよい。これによりさらに高精度な濃度演算が可能になるという効果を奏する。
また、本実施形態のガス濃度測定装置1における基準濃度算出式がn次多項式(式(2))である場合、具体的なガス濃度の演算方法の一例としては、下記式(3)が挙げられる。
In the gas concentration measuring apparatus 1 of the present embodiment, the coefficient is obtained from the ratio between the second measurement output and the first measurement output, and the ratio between the second solution and the first solution. May be. As a result, there is an effect that density calculation with higher accuracy becomes possible.
In the gas concentration measuring apparatus 1 of the present embodiment, the reference concentration calculation formula is an nth order polynomial, and the concentration calculation formula corrects the first to nth order coefficients of the reference concentration calculation formula with the first solution. Alternatively, the equation obtained by correcting the zeroth-order coefficient with the first density may be multiplied by the coefficient, and then the first density may be added. As a result, there is an effect that density calculation with higher accuracy becomes possible.
Further, when the reference concentration calculation formula in the gas concentration measuring apparatus 1 of the present embodiment is an nth order polynomial (formula (2)), the following formula (3) is given as an example of a specific gas concentration calculation method. It is done.
(式中、anはn次の係数、Vstdは基準濃度算出式の変数である。) (Wherein, a n is the n-th order coefficient, V std is a variable reference density calculation formula.)
(式中、cはガスの濃度、c1は第1の濃度、c2は第2の濃度、Vout(c1)は第1の濃度における測定出力、Vout(c2)は第2の濃度における測定出力、Vstd(c1)は基準濃度算出式の出力が第1の濃度であるときの変数、Vstd(c2)は基準濃度算出式の出力が第2の濃度であるときの変数、Voutは測定時の測定出力である。)
式(3)は、第1の濃度および第2の濃度の、それぞれの濃度における測定出力Vout(c1)、Vout(c2)と、それぞれの濃度における基準濃度算出式の変数Vstd(c1)、Vstd(c2)と、基準濃度算出式のn次の係数anを定数としており、測定時の測定出力Voutを代入することのみで、濃度演算が可能であることが理解される。
(Where c is the gas concentration, c 1 is the first concentration, c 2 is the second concentration, V out (c 1 ) is the measurement output at the first concentration, and V out (c 2 ) is the second concentration. , V std (c 1 ) is a variable when the output of the reference concentration calculation formula is the first concentration, and V std (c 2 ) is the output of the reference concentration calculation formula is the second concentration. ( Vout is a measurement output at the time of measurement.)
Equation (3) is obtained by calculating the measured outputs V out (c 1 ) and V out (c 2 ) at the respective concentrations of the first concentration and the second concentration, and the variable V std of the reference concentration calculation formula at each concentration. (c 1), and V std (c 2), and the n-th coefficient a n constants reference density calculating equation, only substituting the measured output V out at the time of measurement, it is possible density arithmetic Is understood.
ここで式(3)をみると、基準濃度算出式の式(2)を本実施形態のガス濃度測定装置の濃度特性に即した演算式のように補正した形式となっており、これにより光源から測定用赤外線検出部までの光路長や、測定対象ガスによる吸収が無い場合の測定用赤外線検出部の仮想出力の個体ばらつきの影響が低減され、より高精度にガス濃度を演算することが可能となることがわかる。
また、本実施形態のガス濃度測定装置1における基準濃度算出式が対数関数(式(4))である場合、ガス濃度の具体的な演算方法の一例としては、式(5)が挙げられる。
Here, looking at the equation (3), the equation (2) of the reference concentration calculation equation is corrected to an arithmetic equation in accordance with the concentration characteristic of the gas concentration measuring device of the present embodiment, whereby the light source The gas path can be calculated with higher accuracy by reducing the influence of individual variations in the optical path length from the measurement infrared detector to the measurement infrared detector and the virtual output of the measurement infrared detector when there is no absorption by the measurement target gas. It turns out that it becomes.
Further, when the reference concentration calculation formula in the gas concentration measuring apparatus 1 of the present embodiment is a logarithmic function (Formula (4)), Formula (5) is given as an example of a specific calculation method of the gas concentration.
(式中、d1〜4は基準濃度算出式の係数である。) (In the formula, d 1 to 4 are coefficients of the reference concentration calculation formula.)
上記式(5)は、第1の濃度および第2の濃度の、それぞれの濃度における測定出力Vout(c1)、Vout(c2)と、それぞれの濃度における基準濃度算出式の変数Vstd(c1)、Vstd(c2)と、基準濃度算出式の係数d1〜4を定数としており、測定時の測定出力Voutを代入することのみで、濃度演算が可能であることが理解される。
ここで式(5)をみると、基準濃度算出式の式(4)を本実施形態のガス濃度測定装置の濃度特性に即した演算式のように補正した形式となっており、これにより光源から測定用赤外線検出部までの光路長や、測定対象ガスによる吸収が無い場合の測定用赤外線検出部の仮想出力の個体ばらつきの影響が低減され、より高精度にガス濃度を演算することが可能となることがわかる。
The above equation (5) is obtained by measuring the output V out (c 1 ) and V out (c 2 ) at the respective concentrations of the first concentration and the second concentration, and the variable V of the reference concentration calculation formula at each concentration. Std (c 1 ), V std (c 2 ) and coefficients d 1 to 4 of the reference concentration calculation formula are constants, and concentration calculation is possible only by substituting measurement output V out at the time of measurement. Is understood.
Here, looking at the equation (5), the equation (4) of the reference concentration calculation equation is corrected as an arithmetic equation in accordance with the concentration characteristic of the gas concentration measuring apparatus of the present embodiment, whereby the light source The gas path can be calculated with higher accuracy by reducing the influence of individual variations in the optical path length from the measurement infrared detector to the measurement infrared detector and the virtual output of the measurement infrared detector when there is no absorption by the measurement target gas. It turns out that it becomes.
また、式(5)と式(3)より、実施形態のガス濃度測定装置において、第1の濃度の測定対象ガス中で光源を点灯させた時に測定用赤外線検出部が出力する第1の測定出力と、第1の濃度と異なる第2の濃度の測定対象ガス中で光源を点灯させた時に測定用赤外線検出部が出力する第2の測定出力と、濃度算出式から求まる濃度が第1の濃度であるときの変数の値である第1の解と、基準濃度算出式から求まる濃度が第2の濃度であるときの変数の値である第2の解と、から得られる係数と、基準濃度算出式を第1の解と前記第1の濃度で補正した式と、第1の濃度と、を含む濃度算出式に、測定時の測定出力を第1の測定出力で規格化して代入することで、高精度な濃度演算が可能になることが理解される。
また、式(5)と式(3)より、本実施形態のガス濃度測定装置において、係数が、第2の測定出力と第1の測定出力の比と、第2の解と第1の解の比と、から得ることで、高精度な濃度演算が可能になることが理解される。
Further, from the equations (5) and (3), in the gas concentration measurement apparatus of the embodiment, the first measurement output from the measurement infrared detection unit when the light source is turned on in the measurement target gas having the first concentration. The output, the second measurement output output from the measurement infrared detection unit when the light source is turned on in the measurement target gas having the second concentration different from the first concentration, and the concentration obtained from the concentration calculation formula are the first A coefficient obtained from a first solution that is a value of a variable when it is a concentration, a second solution that is a value of a variable when the concentration obtained from the reference concentration calculation formula is a second concentration, and a reference The measurement output at the time of measurement is normalized with the first measurement output and substituted into the concentration calculation expression including the first solution, the expression obtained by correcting the concentration calculation expression with the first solution, the first concentration, and the first concentration. Thus, it is understood that highly accurate concentration calculation is possible.
Further, from the equations (5) and (3), in the gas concentration measurement apparatus of the present embodiment, the coefficient is the ratio between the second measurement output and the first measurement output, the second solution, and the first solution. It is understood that the density calculation can be performed with high accuracy by obtaining from the above ratio.
<式(3)の導出>
以下、式(3)の導出過程について説明する。
ランバートベールの法則(Lambert−Beer_law)より、本実施形態のガス濃度測定装置では、式(6)に基づいて測定対象ガスの濃度を演算できるはずである。
<Derivation of Formula (3)>
Hereinafter, the derivation process of Formula (3) will be described.
From the Lambert-Beer law (Lambert-Beer_law), the gas concentration measurement device of this embodiment should be able to calculate the concentration of the measurement target gas based on the equation (6).
(式中、cはガスの濃度、εは吸光度係数、l(エル)は実態的な光路長、Vout(0)は測定対象ガスによる吸収が無い場合の仮想の測定出力、Voutは測定時の測定出力である。)
しかし、式(6)は個体ごとにばらつく実態的な光路長lや測定対象ガスによる吸収が無い場合の仮想の測定出力Vout(0)を含んでいる。そこで、任意の既知の第1の濃度および第2の濃度における測定出力から、これらのばらつき要因を含まない数式を導出する。
任意の既知の第1の濃度の測定対象ガス中で前記光源を点灯させた時に測定用赤外線検出部が出力する第1の測定出力Vout(c1)とすると、第1の濃度c1は式(7)で表される。
(Where c is the gas concentration, ε is the absorbance coefficient, l is the actual optical path length, V out (0) is the virtual measurement output when there is no absorption by the gas to be measured, and V out is the measurement. (Measurement output at the time.)
However, equation (6) includes the actual optical path length l that varies from individual to individual and the virtual measurement output V out (0) when there is no absorption by the measurement target gas. Therefore, a mathematical expression that does not include these variation factors is derived from the measurement output at any known first density and second density.
Assuming that the first measurement output V out (c 1 ) output from the measurement infrared detection unit when the light source is turned on in the measurement target gas having any known first concentration, the first concentration c 1 is It is represented by Formula (7).
上記式(6)、(7)から、下記式(8)が得られる。 From the above formulas (6) and (7), the following formula (8) is obtained.
任意の既知の第2の濃度c2の測定対象ガス中で、光源を点灯させた時に得られる測定用出力をVout(c2)とし、上記式(8)に代入して変形すると、式(9)が得られる。 When the measurement output obtained when the light source is turned on in any measurement gas having a known second concentration c 2 is V out (c2) and is substituted into the above equation (8) and transformed, the equation ( 9) is obtained.
式(8)に式(9)を代入すると式(10)を得ることが出来る。 By substituting equation (9) into equation (8), equation (10) can be obtained.
しかしながら、測定用赤外線検出部の出力に含まれる回路的、光学的オフセットの影響などによって、実際の特性は上記式(10)のようなLogの関数からは乖離がある。回路的オフセットは、例えば測定用赤外線検出部に含まれる増幅回路で生じる。また、光学的オフセットは、例えば測定対象ガスによって吸収されない波長の光の測定用赤外線検出部への入射等によって生じる。
そこで、式(2)のような基準濃度算出式を定義し、そこから濃度算出式を導出する。ここでの基準濃度算出式とは、本実施形態のガス濃度測定装置と近いガス濃度特性を示す、別個体のガス濃度測定装置におけるガス濃度特性の近似式、つまりは濃度算出式である。
However, due to the influence of circuit and optical offset included in the output of the measurement infrared detection unit, the actual characteristics deviate from the Log function such as the above equation (10). The circuit-like offset is generated in, for example, an amplifier circuit included in the measurement infrared detection unit. The optical offset is caused by, for example, incidence of light having a wavelength that is not absorbed by the measurement target gas into the measurement infrared detection unit.
Therefore, a reference concentration calculation formula such as equation (2) is defined, and the concentration calculation formula is derived therefrom. The reference concentration calculation formula here is an approximate expression of a gas concentration characteristic in a separate gas concentration measurement apparatus showing a gas concentration characteristic close to that of the gas concentration measurement apparatus of the present embodiment, that is, a concentration calculation expression.
(式中、anはn次の係数、Vstdは基準濃度算出式の変数である。)
式(10)を式(11)のように変形する。
(Wherein, a n is the n-th order coefficient, V std is a variable reference density calculation formula.)
Expression (10) is transformed into Expression (11).
(式中、Vstd(c1)は基準濃度算出式から求まる値が第1の濃度であるときの基準濃度算出式の変数である。)
また、式(10)のLogの関数を多項式に置き換えると、式(12)が得られる。
(In the formula, V std (c 1 ) is a variable of the reference concentration calculation formula when the value obtained from the reference concentration calculation formula is the first concentration.)
Further, when the Log function of Expression (10) is replaced with a polynomial, Expression (12) is obtained.
(式中、bnはn次の係数である。)
式(12)のVoutをVstdに、Vout(c1)をVstd(c1)に、Vout(c2)をVstd(c2)に置き換えると式(13)が得られる。
(Where b n is an n-th order coefficient.)
Replacing V out in equation (12) with V std , V out (c 1 ) with V std (c 1 ), and V out (c 2 ) with V std (c 2 ) yields equation (13). .
(式中、Vstd(c2)は基準濃度算出式から求まる値が第2の濃度であるときの基準濃度算出式の変数である。)
式(11)と式(13)が等しいと仮定して、bnなどの係数を求めると、式(14−0)〜式(14−n)が得られる。
(In the formula, V std (c 2 ) is a variable of the reference concentration calculation formula when the value obtained from the reference concentration calculation formula is the second concentration.)
Assuming that Expression (11) is equal to Expression (13) and obtaining coefficients such as b n , Expression (14-0) to Expression (14-n) are obtained.
式(14−0)〜式(14−n)を式(12)に代入すると、式(3)を得ることができる。 When Expression (14-0) to Expression (14-n) are substituted into Expression (12), Expression (3) can be obtained.
<式(5)の導出>
以下、式(3)の導出過程について説明する。
先述の通り、式(10)は実際の特性からは乖離があるため、式(4)のような基準濃度算出式を定義し、そこから濃度算出式を導出する。ここでの基準濃度算出式とは、本実施形態のガス濃度測定装置と近いガス濃度特性を示す、別個体のガス濃度測定装置におけるガス濃度特性の近似式、つまりは濃度算出式である。
<Derivation of Formula (5)>
Hereinafter, the derivation process of Formula (3) will be described.
As described above, since the formula (10) has a deviation from the actual characteristics, a reference density calculation formula like the formula (4) is defined, and the density calculation formula is derived therefrom. The reference concentration calculation formula here is an approximate expression of a gas concentration characteristic in a separate gas concentration measurement apparatus showing a gas concentration characteristic close to that of the gas concentration measurement apparatus of the present embodiment, that is, a concentration calculation expression.
(式中、d1〜4は定数、Vstdは基準濃度算出式の変数である。)
式(4)を式(5)のように変形する。
( Where d 1 to 4 are constants, and V std is a variable of the reference concentration calculation formula.)
Equation (4) is transformed into Equation (5).
(式中、Vstd(c1)は基準濃度算出式から求まる値が第1の濃度であるときの基準濃度算出式の変数である。)
また、式(10)のLogの関数にオフセットなどを加味すると、式(16)が得られる。
(In the formula, V std (c 1 ) is a variable of the reference concentration calculation formula when the value obtained from the reference concentration calculation formula is the first concentration.)
Further, when an offset or the like is added to the Log function of Expression (10), Expression (16) is obtained.
(式中、e1〜4は定数である。)
式(16)のVoutをVstdに、Vout(c1)をVstd(c1)に、Vout(c2)をVstd(c2)に置き換えると式(17)が得られる。
( Wherein e 1 to 4 are constants)
When V out in equation (16) is replaced with V std , V out (c 1 ) is replaced with V std (c 1 ), and V out (c 2 ) is replaced with V std (c 2 ), equation (17) is obtained. .
(式中、Vstd(c2)は基準濃度算出式から求まる値が第2の濃度であるときの基準濃度算出式の変数である。)
式(15)と式(17)が等しいと仮定して、e1〜4を求めると、式(18−1)〜式(18−4)が得られる。
(In the formula, V std (c 2 ) is a variable of the reference concentration calculation formula when the value obtained from the reference concentration calculation formula is the second concentration.)
Assuming that the formula (15) and the formula (17) are equal, e 1 to 4 are obtained, thereby obtaining the formula (18-1) to the formula (18-4).
式(18−1)〜式(18−4)を式(17)に代入すると、式(5)を得ることができる。 By substituting Equations (18-1) to (18-4) into Equation (17), Equation (5) can be obtained.
また、本実施形態に係るガス濃度測定装置において、ガス濃度測定装置は、光源からの光を受光し、光に応じた信号である参照出力を出力する参照用赤外線検出部をさらに備え、演算部が前記測定出力を前記参照出力で補正するものであっても良い。 Further, in the gas concentration measurement device according to the present embodiment, the gas concentration measurement device further includes a reference infrared detection unit that receives light from the light source and outputs a reference output that is a signal corresponding to the light, and an arithmetic unit May correct the measurement output with the reference output.
図2は、本発明に係るガス濃度測定装置の実施形態において、参照用赤外線検出部を追加した構成を説明するための図である。図中符号32は参照用赤外線検出部を示している。なお、図1に記載の構成要素と同じ機能を有する構成要素には同一の符号を付してある。なおここでは参考のため、ガスセル10を明示しているが、本発明においてガスセルは必須の構成ではなく、ガスセルの無い形態でも試験容器内等にガス濃度測定装置を配置することで下記と同様の2濃度検査を行うことが可能である。
測定出力を参照出力に基づいて補正することで、式(1)中のVout(0)(測定対象ガスによる吸収が無い場合の測定用赤外線検出部の出力)が経時的に変化したとしても、その変化分を補正できるため、従来よりも高精度なガス濃度測定が可能になるという効果を奏する。
補正の具体例としては、式(19)などがある。
FIG. 2 is a diagram for explaining a configuration in which a reference infrared detecting unit is added in the embodiment of the gas concentration measuring apparatus according to the present invention.
Even if V out (0) in Equation (1) (the output of the infrared detecting unit for measurement when there is no absorption by the measurement target gas) changes over time by correcting the measurement output based on the reference output Since the amount of change can be corrected, the gas concentration can be measured with higher accuracy than before.
A specific example of the correction is equation (19).
(式中、Vstd’は参照出力で補正された測定出力である。)
また、式(19)右辺の分母と分子が逆になっても良い。
また、本実施形態に係わるガス濃度測定装置において、演算部が、光源を点灯させた時の測定出力と参照出力の少なくとも一方を、光源を消灯させた時の測定出力と参照出力の少なくとも一方に基づいて補正するものであってもよい。
補正の具体例としては、式(20)、式(21)のように、光源を点灯させた時の測定出力および参照出力と、光源を消灯させた時の測定出力および参照出力の差分をとるなどがある。
(In the formula, V std ′ is a measurement output corrected with a reference output.)
Also, the denominator and numerator on the right side of Equation (19) may be reversed.
Further, in the gas concentration measurement apparatus according to the present embodiment, the calculation unit converts at least one of the measurement output and the reference output when the light source is turned on into at least one of the measurement output and the reference output when the light source is turned off. Corrections may be made based on this.
As a specific example of the correction, the difference between the measurement output and the reference output when the light source is turned on and the measurement output and the reference output when the light source is turned off is obtained as in Expression (20) and Expression (21). and so on.
(式中、DOUTは光源を点灯させた時の測定出力を光源を消灯させた時の測定出力で補正したもの、Drefは光源を点灯させた時の参照出力を光源を消灯させた時の参照出力で補正したもの、Vout_onは光源を点灯させた時の測定出力、Vout_offは光源を消灯させた時の測定出力、Vref_onは光源を点灯させた時の参照出力、Vref_offは光源を消灯させた時の参照出力である。
ここで、光源を点灯させた状態とは、光源が周囲環境から放射される赤外線量よりも多い赤外線を放射している状態をいう。
また、光源を消灯させた状態とは、完全に消灯している状態でなくてもよい。
光源への電力供給の有無に係わらず、光源が赤外線を放射している状態であっても、放射する赤外線量が光源点灯時に放射する赤外線量以下である場合、または周囲環境から放射される赤外線量と同等以下である場合には、光源は実質的に赤外線を放射しない状態であるため消灯状態と看做される。
(In the formula, D OUT is a value obtained by correcting the measurement output when the light source is turned on with the measurement output when the light source is turned off, and D ref is the reference output when the light source is turned on when the light source is turned off. those of the corrected reference output, V out_on measurement output when is lit light source, V out_off measurement output when turns off the light source, V ref_on reference output when is lit light source, V ref_off is This is a reference output when the light source is turned off.
Here, the state in which the light source is turned on refers to a state in which the light source emits more infrared rays than the amount of infrared rays emitted from the surrounding environment.
Moreover, the state where the light source is turned off may not be a state where the light source is completely turned off.
Regardless of whether or not power is supplied to the light source, even if the light source emits infrared rays, if the amount of infrared rays emitted is less than or equal to the amount of infrared rays emitted when the light source is turned on, or infrared rays emitted from the surrounding environment When the amount is equal to or less than the amount, the light source is considered to be in a light-off state because it is in a state of substantially not emitting infrared rays.
光源を消灯させた時の測定出力や参照出力に基づいて、光源を店頭させた時の測定出力や参照出力を補正することで、測定出力や参照出力に含まれる回路的オフセットを補正できるため、従来よりも高精度なガス濃度測定が可能になるという効果を奏する。
ここで、回路的オフセットとは、例えば測定用赤外線検出や参照用赤外線検出部に内蔵される増幅回路の出力オフセットなどである。
以下、本実施形態のガス濃度測定装置における各構成要件について説明する。各構成要件の具体例や技術的特徴は、本発明の技術思想を逸脱しない範囲で単独または組み合わせて適用可能である。
Based on the measurement output and reference output when the light source is turned off, the circuit offset included in the measurement output and reference output can be corrected by correcting the measurement output and reference output when turning on the light source. There is an effect that the gas concentration can be measured with higher accuracy than before.
Here, the circuit-like offset is, for example, an output offset of an amplifier circuit incorporated in a measurement infrared detection or reference infrared detection unit.
Hereinafter, each component in the gas concentration measuring apparatus of this embodiment is demonstrated. Specific examples and technical features of each constituent element can be applied alone or in combination without departing from the technical idea of the present invention.
(測定用赤外線検出部及び参照用赤外線検出部)
測定用赤外線検出部、参照用赤外線検出部は、光源が出力する赤外線に対する感度を有し、入射された赤外線に応じた信号を出力するものである。測定用赤外線検出部は参照用赤外線検出部よりも、測定対象ガスによる赤外線吸収帯域に対する感度の赤外線吸収帯域以外の帯域に対する感度に対する比が大きいものであれば特に制限されない。測定用赤外線検出部及び参照用赤外線検出部には、焦電センサ(Pyroelectric sensor)、サーモパイル(Thermopile:熱電堆)、ボロメータ(Bolometer)等の熱型赤外線センサや、量子型赤外線センサ等が好適である。
測定用赤外線検出部、参照用赤外線検出部は、測定対象ガスに併せて所望の光学特性を有する光学フィルタをさらに備えていてもよい。例えば、測定対象ガスが炭酸ガスの場合、測定用赤外線検出部には炭酸ガスによる赤外線吸収が多く生じる波長帯(代表的には4.3μm付近)の赤外線を濾波できるバンドパスフィルタを搭載し、参照用赤外線検出部には炭酸ガスによる赤外線吸収が生じない波長帯(代表的には3.9μm付近)の赤外線を濾波できるバンドパスフィルタを搭載する形態が例示される。
(Infrared detector for measurement and infrared detector for reference)
The infrared detecting unit for measurement and the infrared detecting unit for reference have sensitivity to the infrared rays output from the light source, and output signals corresponding to the incident infrared rays. The measurement infrared detection unit is not particularly limited as long as the ratio of the sensitivity to the infrared absorption band by the measurement target gas to the sensitivity to the band other than the infrared absorption band is larger than that of the reference infrared detection unit. Thermal infrared sensors such as pyroelectric sensors, thermopiles, bolometers, quantum infrared sensors, and the like are suitable for the measurement infrared detection unit and the reference infrared detection unit. is there.
The measurement infrared detection unit and the reference infrared detection unit may further include an optical filter having desired optical characteristics in addition to the measurement target gas. For example, when the measurement target gas is carbon dioxide, the measurement infrared detector is equipped with a bandpass filter capable of filtering infrared light in a wavelength band (typically around 4.3 μm) where infrared absorption by carbon dioxide occurs a lot. Examples of the reference infrared detection unit include a band-pass filter capable of filtering infrared light in a wavelength band (typically around 3.9 μm) in which infrared absorption by carbon dioxide gas does not occur.
(光源)
光源は、測定用赤外線検出部、参照用赤外線検出部が感度を有する赤外線帯域を出力できるものであれば特に制限されない。例えば、白熱電球やセラミックヒータ、MEMS(Micro Electro Mechanical Systems)ヒーターやLEDなどを用いることができる。
(演算部)
演算部は、ガス濃度算出における演算が可能なものであれば特に制限されず、例えば、アナログIC、ディジタルIC及びCPU(Central Processing Unit)等が好適である。演算部には、光源を制御するための機能が含まれていても構わない。
(light source)
The light source is not particularly limited as long as the measurement infrared detection unit and the reference infrared detection unit can output a sensitive infrared band. For example, an incandescent bulb, a ceramic heater, a MEMS (Micro Electro Mechanical Systems) heater, an LED, or the like can be used.
(Calculation unit)
The calculation unit is not particularly limited as long as it can perform calculation in gas concentration calculation. For example, an analog IC, a digital IC, and a CPU (Central Processing Unit) are suitable. The calculation unit may include a function for controlling the light source.
(ガスセル)
本実施形態のガス濃度測定装置は、内部に測定対象ガスを流入可能であり、内部に光源、測定用赤外線検出部、参照用赤外線検出部、演算部等を配置可能なガスセルをさらに備えても良い。ここで、流入可能とは光源から出力された赤外線が測定対象ガスの存在する空間を通って、測定用赤外線検出部に到達可能であることを示す。ガスセルをさらに備えることで、測定用赤外線検出部及び参照用赤外線検出部の出力する信号のSN比を高めることができ、より高精度なガス濃度測定装置が実現する。赤外線検出部に入射される赤外線の効率化の観点から、ガスセル内部が赤外線を反射する材料で形成されていることが好ましい。具体的にはアルミニウムや銅などの金属材料が挙げられる。
次に、本実施形態のガス濃度測定装置の実施例について説明する。
(Gas cell)
The gas concentration measurement apparatus of the present embodiment may further include a gas cell capable of flowing a measurement target gas therein and in which a light source, a measurement infrared detection unit, a reference infrared detection unit, a calculation unit, and the like can be disposed. good. Here, “inflowable” means that the infrared light output from the light source can reach the measurement infrared detection section through the space where the measurement target gas exists. By further providing a gas cell, the signal-to-noise ratio of signals output from the measurement infrared detection unit and the reference infrared detection unit can be increased, and a more accurate gas concentration measurement device is realized. From the viewpoint of increasing the efficiency of infrared rays incident on the infrared detection unit, the gas cell is preferably formed of a material that reflects infrared rays. Specifically, metal materials, such as aluminum and copper, are mentioned.
Next, examples of the gas concentration measuring apparatus according to this embodiment will be described.
タングステン光源、CO2による赤外線吸収のある4.2μm〜4.4μmの波長帯を選択的に濾波選別する光学フィルタを搭載した測定用赤外線検出部31としての量子型赤外線センサ「IR1011」(旭化成エレクトロニクス株式会社製)、CO2による赤外線吸収の無い3.7μm〜3.9μmの波長帯を選択的に濾波選別する光学フィルタを搭載した参照用赤外線検出部としての量子型赤外線センサ「IR1011」(旭化成エレクトロニクス株式会社製)、演算部として記憶部と処理部を備えたICを、リン青銅に金メッキを施したガスセル中に、配置した炭酸ガス濃度測定装置を準備した。
Quantum infrared sensor “IR1011” (Asahi Kasei Electronics) as an
次いで、濃度0ppmの炭酸ガスをガスセル中に充填した時の、光源が点灯および消灯している時の、それぞれアンプにより増幅された測定用赤外線検出部と参照用赤外線検出部からの出力と、濃度986mの炭酸ガスをガスセル中に充填した時の、光源が点灯および消灯している時の、それぞれアンプにより増幅された測定用赤外線検出部と参照用赤外線検出部からの出力とを用いて、上述した実施形態の濃度演算を行った。
具体的な演算は下記の通りである。
以下、本実施例で述べる測定出力とは、光源を点灯している時の測定出力と光源を消灯している時の測定出力との差分であり、参照出力とは、光源を点灯している時の参照出力と光源を消灯している時の参照出力との差分である。
Next, when the light source is turned on and off when carbon dioxide with a concentration of 0 ppm is filled in the gas cell, the output from the measurement infrared detection unit and the reference infrared detection unit amplified by the amplifier, and the concentration Using the output from the measurement infrared detector and the reference infrared detector amplified by the amplifier when the light source is turned on and off when 986 m of carbon dioxide gas is filled in the gas cell, The concentration calculation of the embodiment was performed.
The specific calculation is as follows.
Hereinafter, the measurement output described in this embodiment is the difference between the measurement output when the light source is turned on and the measurement output when the light source is turned off, and the reference output is the light source turned on. The difference between the reference output at the time and the reference output when the light source is turned off.
まず、測定時の測定出力に対する参照出力の比(Dout’)、炭酸ガス濃度0ppm時の測定出力に対する参照出力の比(Dout(c1)’)、また、炭酸ガス濃度986ppm時の測定出力に対する参照出力の比(Dout(c2)’)、基準濃度算出式から求まる値が0である時の基準濃度算出式の変数の値(Vstd(c1))、基準濃度算出式から求まる値が986である時の基準濃度算出式の変数の値(Vstd(c2))を演算した。次いで、Vout(c1)=Dout(c1)’、Vout(c2)=Dout(c2)’とし、式(3)に必要な値を代入し、炭酸ガス濃度を演算した。 First, the ratio of the reference output to the measurement output at the time of measurement (D out '), the ratio of the reference output to the measurement output at the carbon dioxide concentration of 0 ppm (D out (c 1 )'), and the measurement at the carbon dioxide concentration of 986 ppm The ratio of the reference output to the output (D out (c 2 ) ′), the value of the variable of the reference concentration calculation formula when the value obtained from the reference concentration calculation formula is 0 (V std (c 1 )), the reference concentration calculation formula The value (V std (c 2 )) of the reference concentration calculation equation when the value obtained from 986 is 986 was calculated. Next, V out (c 1 ) = D out (c 1 ) ′ and V out (c 2 ) = D out (c 2 ) ′ are set, and a necessary value is substituted into equation (3) to calculate the carbon dioxide concentration. did.
基準濃度算出式とは、ここで用いているガス濃度測定装置と近いガス濃度特性を示す別個体のガス濃度測定装置(基準ガス濃度測定装置)の、炭酸ガス濃度と測定出力に対する参照出力の比の関係を、直接的あるいは近似的に表す数式である。ここでは、基準ガス濃度測定装置の0〜5000ppmの5点での濃度試験結果から、式(22)のような基準濃度算出式を導出した。 The reference concentration calculation formula is the ratio of the carbon dioxide concentration and the reference output to the measured output of a separate gas concentration measuring device (standard gas concentration measuring device) that exhibits gas concentration characteristics close to those of the gas concentration measuring device used here. Is a mathematical expression that directly or approximately represents the relationship. Here, the reference concentration calculation formula like Formula (22) was derived | led-out from the density | concentration test result in 0-5000 ppm of the reference gas concentration measuring apparatus.
ここで、f(Vstd)は基準濃度算出式、Vstdは基準濃度算出式の変数である。 Here, f (V std ) is a variable for the reference concentration calculation formula, and V std is a variable for the reference concentration calculation formula.
[比較例]
以下、本比較例で述べる測定出力とは、光源を点灯している時の測定出力と光源20をしている時の測定出力との差分であり、参照出力とは、光源を点灯している時の参照出力と光源を消灯している時の参照出力との差分である。
まず、式(23)のような、2次の係数が固定で、1次の係数(b1)と0次の係数(b0)が未定である濃度算出式を用意した。
[Comparative example]
Hereinafter, the measurement output described in this comparative example is the difference between the measurement output when the light source is turned on and the measurement output when the
First, a concentration calculation formula was prepared, in which the second-order coefficient is fixed and the first-order coefficient (b 1 ) and the zero-order coefficient (b 0 ) are undetermined, such as Expression (23).
ここで、g(Dout’)は比較例における濃度算出式、Dout’は測定時の測定用赤外線検出部の出力に対する参照用赤外線検出部の出力、f1は濃度算出式の1次の係数、f0は濃度算出式の0次の係数である。
濃度算出式(式(23))の2次の係数は、ここで用いているガス濃度測定装置と近いガス濃度特性を示す別個体のガス濃度測定装置の、炭酸ガス濃度と参照出力に対する測定出力の比との関係を表す、2次の近似式の2次の係数である。ここでは、実施例で用いた基準ガス濃度測定装置の0〜5000ppmの5点での濃度試験結果から、炭酸ガス濃度と参照出力に対する測定出力の比との関係を表す2次近似式を求め(式(22))、その2次関数の2次の係数を濃度算出式(式(23))中の2次の係数とした。
Here, g (D out ′) is the concentration calculation formula in the comparative example, D out ′ is the output of the reference infrared detection unit relative to the output of the measurement infrared detection unit at the time of measurement, and f 1 is the primary of the concentration calculation formula. coefficient, f 0 is the zero-order coefficient of the density calculating equation.
The second-order coefficient of the concentration calculation formula (formula (23)) is the measurement output for the carbon dioxide concentration and the reference output of a separate gas concentration measurement device that exhibits a gas concentration characteristic close to that of the gas concentration measurement device used here. Is a secondary coefficient of a quadratic approximate expression that represents the relationship with the ratio of. Here, a quadratic approximate expression representing the relationship between the carbon dioxide concentration and the ratio of the measured output to the reference output is obtained from the concentration test results at 5 points of 0 to 5000 ppm of the standard gas concentration measuring apparatus used in the example ( Formula (22)) and the quadratic coefficient of the quadratic function were used as the secondary coefficient in the concentration calculation formula (formula (23)).
次いで、式(22)の1次および0次の係数を、炭酸ガス濃度0ppm時の測定用赤外線検出部31の出力に対する参照用赤外線検出部の出力と、炭酸ガス濃度987ppm時の参照用赤外線検出部の出力に対する測定用赤外線検出部31の出力の比から求め、式(24)を得た。
Next, the first-order coefficient and the zero-order coefficient of the equation (22) are obtained by using the output of the reference infrared detection unit relative to the output of the measurement
次いで、式(12)に測定時の参照出力に対する測定出力の比を代入し、炭酸ガス濃度を演算した。
図3は、上述した実施例と比較例を対比した結果を示す図である。
図3の結果より、実施例の演算によると最大で−14ppmの誤差にとどまったが、比較例1の演算によると最大で+273ppmの誤差が生じた。
以上の結果より、本実施形態のガス濃度演算装置によれば、従来の濃度算出式よりも高精度な濃度演算が可能であることが理解される。
Next, the ratio of the measured output to the reference output at the time of measurement was substituted into Equation (12), and the carbon dioxide concentration was calculated.
FIG. 3 is a diagram showing a result of comparing the above-described example and comparative example.
From the results of FIG. 3, the maximum error was −14 ppm according to the calculation of the example, but the maximum +273 ppm error was generated according to the calculation of the comparative example 1.
From the above results, it is understood that the gas concentration calculation device of this embodiment can perform concentration calculation with higher accuracy than the conventional concentration calculation formula.
以上、本発明の実施形態について説明したが、本発明の技術的範囲は、上述した実施形態に記載の技術的範囲には限定されない。上述した実施形態に、多様な変更又は改良を加えることも可能であり、そのような変更又は改良を加えた形態も本発明の技術的範囲に含まれ得ることが、特許請求の範囲の記載から明らかである。 As mentioned above, although embodiment of this invention was described, the technical scope of this invention is not limited to the technical scope as described in embodiment mentioned above. It is possible to add various changes or improvements to the above-described embodiments, and it is possible to add such changes or improvements to the technical scope of the present invention. it is obvious.
本発明は、炭酸ガス等に代表される赤外線吸収を生じるガスのガス濃度測定装置として好適である。 The present invention is suitable as a gas concentration measuring device for gases that generate infrared absorption typified by carbon dioxide.
10 ガスセル
11 ガス導入口
12 ガス導出口
20 光源
31 測定用赤外線検出部
32 参照用赤外線検出部
40 演算部
DESCRIPTION OF
Claims (6)
前記光源からの光を受光し、光に応じた信号である測定出力を出力する測定用赤外線検出部と、
前記測定出力が入力される演算部と、
を備えたガス濃度測定装置であって、
前記演算部は、
第1の濃度の測定対象ガス中で前記光源を点灯させた時に前記測定用赤外線検出部が出力する第1の測定出力と、
前記第1の濃度と異なる第2の濃度の測定対象ガス中で前記光源を点灯させた時に前記測定用赤外線検出部が出力する第2の測定出力と、
基準濃度算出式から求まる濃度が前記第1の濃度であるときの変数の値である第1の解と、
前記基準濃度算出式から求まる濃度が前記第2の濃度であるときの変数の値である第2の解と、から得られる係数と、
前記基準濃度算出式を前記第1の解と前記第1の濃度で補正した式と、
前記第1の濃度と、
を含む濃度算出式に、測定時の測定出力を前記第1の測定出力で規格化して代入することで測定対象ガスの濃度を演算するガス濃度測定装置。 A light source;
An infrared detector for measurement that receives light from the light source and outputs a measurement output that is a signal corresponding to the light;
A calculation unit to which the measurement output is input;
A gas concentration measuring device comprising:
The computing unit is
A first measurement output that is output from the measurement infrared detection unit when the light source is turned on in a measurement gas having a first concentration;
A second measurement output output by the measurement infrared detection unit when the light source is turned on in a measurement target gas having a second concentration different from the first concentration;
A first solution which is a value of a variable when the concentration obtained from a reference concentration calculation formula is the first concentration;
A coefficient obtained from a second solution that is a value of a variable when the concentration obtained from the reference concentration calculation formula is the second concentration;
An equation in which the reference density calculation formula is corrected with the first solution and the first density;
The first concentration;
A gas concentration measuring device that calculates the concentration of the gas to be measured by substituting the measurement output at the time of measurement with the first measurement output into a concentration calculation formula including
前記第2の測定出力と前記第1の測定出力の比と、
前記第2の解と前記第1の解の比と、
から得られる請求項1に記載のガス濃度測定装置。 The coefficient is
A ratio of the second measurement output to the first measurement output;
The ratio of the second solution to the first solution;
The gas concentration measuring device according to claim 1 obtained from the above.
前記濃度算出式は、
前記基準濃度算出式の1次〜n次の係数を、前記第1の解で補正し、0次の係数を前記第1の濃度で補正した式に、前記係数をかけ、さらに前記第1の濃度を足し合わせた式である請求項1または請求項2に記載のガス濃度測定装置。 The reference concentration calculation formula is an nth order polynomial,
The concentration calculation formula is:
The first to nth order coefficients of the reference density calculation formula are corrected with the first solution, the zeroth order coefficient is corrected with the first density, the coefficient is multiplied, and the first The gas concentration measuring device according to claim 1 or 2, wherein the concentration is a formula obtained by adding the concentrations.
下記式(1)に基づいて測定対象ガスの濃度を演算する請求項1から請求項3のいずれか一項に記載のガス濃度測定装置。
The gas concentration measuring apparatus according to any one of claims 1 to 3, wherein the concentration of the measurement target gas is calculated based on the following equation (1).
前記光源からの光を受光し、光に応じた信号である参照出力を出力する参照用赤外線検出部をさらに備え、
前記演算部が
前記測定出力を前記参照出力で補正する請求項1から請求項4のいずれか一項に記載のガス濃度測定装置。 The gas concentration measuring device includes:
It further includes a reference infrared detection unit that receives light from the light source and outputs a reference output that is a signal corresponding to the light,
The gas concentration measuring device according to any one of claims 1 to 4, wherein the calculation unit corrects the measurement output with the reference output.
前記光源を点灯させた時の前記測定出力と前記参照出力の少なくとも一方を、
前記光源を消灯させた時の前記測定出力と前記参照出力の少なくとも一方に基づいて補正する請求項1から請求項5のいずれか一項に記載のガス濃度測定装置。 The computing unit is
At least one of the measurement output and the reference output when the light source is turned on,
The gas concentration measurement apparatus according to claim 1, wherein correction is performed based on at least one of the measurement output and the reference output when the light source is turned off.
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Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55109948A (en) * | 1979-02-15 | 1980-08-23 | Mazda Motor Corp | Measuring method for exhaust gas of internal combustion engine |
| JPH11304695A (en) * | 1998-04-18 | 1999-11-05 | Horiba Ltd | Method for preparing calibration curve for infrared gas analyzer |
| JP2004101416A (en) * | 2002-09-11 | 2004-04-02 | Horiba Ltd | Multi-component analysis apparatus |
| JP2006275754A (en) * | 2005-03-29 | 2006-10-12 | Horiba Ltd | Analyzer and calibration method |
| JP2010066209A (en) * | 2008-09-12 | 2010-03-25 | Yazaki Corp | Concentration measuring device |
| US20120330568A1 (en) * | 2010-02-16 | 2012-12-27 | Hamamatsu Photonics K.K. | Gas concentration calculation device, gas concentration measurement module, and light detector |
-
2015
- 2015-09-30 JP JP2015193898A patent/JP6571476B2/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55109948A (en) * | 1979-02-15 | 1980-08-23 | Mazda Motor Corp | Measuring method for exhaust gas of internal combustion engine |
| JPH11304695A (en) * | 1998-04-18 | 1999-11-05 | Horiba Ltd | Method for preparing calibration curve for infrared gas analyzer |
| JP2004101416A (en) * | 2002-09-11 | 2004-04-02 | Horiba Ltd | Multi-component analysis apparatus |
| JP2006275754A (en) * | 2005-03-29 | 2006-10-12 | Horiba Ltd | Analyzer and calibration method |
| JP2010066209A (en) * | 2008-09-12 | 2010-03-25 | Yazaki Corp | Concentration measuring device |
| US20120330568A1 (en) * | 2010-02-16 | 2012-12-27 | Hamamatsu Photonics K.K. | Gas concentration calculation device, gas concentration measurement module, and light detector |
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