JP2003035662A - Quantitative analysis calibration method - Google Patents
Quantitative analysis calibration methodInfo
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- JP2003035662A JP2003035662A JP2001220518A JP2001220518A JP2003035662A JP 2003035662 A JP2003035662 A JP 2003035662A JP 2001220518 A JP2001220518 A JP 2001220518A JP 2001220518 A JP2001220518 A JP 2001220518A JP 2003035662 A JP2003035662 A JP 2003035662A
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- 238000000034 method Methods 0.000 title claims abstract description 77
- 238000004445 quantitative analysis Methods 0.000 title claims abstract description 21
- 239000000126 substance Substances 0.000 claims abstract description 177
- 238000001228 spectrum Methods 0.000 claims abstract description 143
- 238000012545 processing Methods 0.000 claims abstract description 65
- 238000002835 absorbance Methods 0.000 claims abstract description 62
- 238000011088 calibration curve Methods 0.000 claims abstract description 56
- 238000005259 measurement Methods 0.000 claims abstract description 45
- 230000008033 biological extinction Effects 0.000 claims abstract description 10
- 238000002834 transmittance Methods 0.000 claims abstract description 8
- 239000000203 mixture Substances 0.000 claims description 43
- 238000010521 absorption reaction Methods 0.000 claims description 32
- 238000012417 linear regression Methods 0.000 claims description 14
- 238000000491 multivariate analysis Methods 0.000 claims description 13
- 238000010586 diagram Methods 0.000 description 15
- 238000000862 absorption spectrum Methods 0.000 description 12
- 238000004458 analytical method Methods 0.000 description 7
- 238000004364 calculation method Methods 0.000 description 7
- 238000012937 correction Methods 0.000 description 4
- 229920006395 saturated elastomer Polymers 0.000 description 4
- 230000003287 optical effect Effects 0.000 description 3
- 238000004611 spectroscopical analysis Methods 0.000 description 3
- 238000004422 calculation algorithm Methods 0.000 description 2
- 238000013528 artificial neural network Methods 0.000 description 1
- 230000009194 climbing Effects 0.000 description 1
- 238000012790 confirmation Methods 0.000 description 1
- 230000004069 differentiation Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 238000012821 model calculation Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 238000012628 principal component regression Methods 0.000 description 1
- 238000011002 quantification Methods 0.000 description 1
- 238000000611 regression analysis Methods 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
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Abstract
(57)【要約】
【課題】 ノイズ成分を校正して混合物質中の所定物質
を定量する。
【解決手段】 ノイズ成分量を校正段階によって算出
し、且つ混合物質中の所定物質の濃度を算出する定量分
析校正方法であって、校正段階は、ゼロスペクトルと標
準スペクトルとを採取し、標準スペクトルの所定濃度
と、理想的な吸光係数とにより透過率を算出してノイズ
成分量を求め、所定波長を他の所定波長に変えて同様の
処理を繰り返し、各波長のノイズ成分量を集積し、通常
計測段階は、混合物質の計測スペクトルを採取し、計測
スペクトル及びゼロスペクトルからノイズ成分量を夫々
引いて吸光度を算出し、所定波長を他の所定波長に変え
て同様の処理を繰り返し、他の所定波長の吸光度を算出
して各波長の吸光度を集積し、予め求められた検量線に
より、混合物質中の所定物質の濃度を算出する。(57) [Problem] To quantify a predetermined substance in a mixed substance by calibrating a noise component. SOLUTION: This is a quantitative analysis calibration method for calculating a noise component amount in a calibration step and calculating a concentration of a predetermined substance in a mixed substance, wherein the calibration step collects a zero spectrum and a standard spectrum, and Calculate the transmittance based on the predetermined concentration and the ideal extinction coefficient to obtain the noise component amount, change the predetermined wavelength to another predetermined wavelength, repeat the same process, accumulate the noise component amount of each wavelength, In the normal measurement step, the measurement spectrum of the mixed substance is collected, the amount of noise component is subtracted from the measurement spectrum and the zero spectrum, the absorbance is calculated, the same processing is repeated by changing the predetermined wavelength to another predetermined wavelength, and the other processing is repeated. The absorbance at a predetermined wavelength is calculated, the absorbance at each wavelength is integrated, and the concentration of the predetermined substance in the mixed substance is calculated based on a previously determined calibration curve.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、混合物質中の所定
物質を定量する定量分析校正方法に関するものである。TECHNICAL FIELD The present invention relates to a quantitative analysis and calibration method for quantifying a predetermined substance in a mixed substance.
【0002】[0002]
【従来の技術】一般に、吸収スペクトルを用いて物質の
定量分析を行う際には、ランベルトベールの法則により
濃度と吸光度が比例することから、予め各所定濃度にお
ける受光スペクトル(受光強度もしくは受光面積)を測
定して各吸光度を求め、各所定濃度と各吸光度により検
量線を作成し、濃度が不明な物質の場合には吸光度を測
定することにより検量線に当てはめて定量している。2. Description of the Related Art Generally, when quantitatively analyzing a substance using an absorption spectrum, the concentration and the absorbance are proportional to each other according to Lambert-Beer's law. Is measured to obtain each absorbance, a calibration curve is created from each predetermined concentration and each absorbance, and in the case of a substance whose concentration is unknown, the absorbance is measured and applied to the calibration curve for quantification.
【0003】実際にガスの吸収分析における波長210
nmのSO2の検量線を例に示すと、検量線は、図19
に示す如く、高濃度部分で検量線の傾きが水平方向にな
るよう飽和し、ランベルトベールの法則に従わないよう
になっている。The wavelength 210 in actual gas absorption analysis
19 shows an example of a calibration curve of SO 2 in nm, the calibration curve is shown in FIG.
As shown in, the slope of the calibration curve is saturated in the high-concentration portion in the horizontal direction, and the Lambert-Beer law is not obeyed.
【0004】このランベルトベールの法則に従わない原
因の一つはノイズ成分によるものと考えられており、ノ
イズ成分には検出器に不要の迷光が入り込む迷光ノイズ
があり、図20に示す如く、分光器を使用しない分光分
析例の場合には、迷光1は光源2より筐体からの反射
光、散乱光等の原因によって生じ、サンプル3を通過す
ることなく検出器4に入り込んで測定に影響を与えてい
る。又、図21に示す如く、サンプル6の後側に分光器
7を備えた場合には、迷光8は光源9より分光器7の中
での散乱により生じ、目的波長の光とは別に検出器10
に入り込んで測定に影響を与えている。ここで、図2
0、図21中、5,11は光路、12は回折格子を夫々
示している。It is considered that one of the causes of not complying with the Lambert-Beer's law is due to a noise component. There is stray light noise in which unwanted stray light enters the detector in the noise component, and as shown in FIG. In the case of a spectroscopic analysis example that does not use a detector, the stray light 1 is generated by the light source 2 such as reflected light from the housing, scattered light, etc., and enters the detector 4 without passing through the sample 3 to affect the measurement. I'm giving. Further, as shown in FIG. 21, when the spectroscope 7 is provided on the rear side of the sample 6, the stray light 8 is generated by the scattering in the spectroscope 7 from the light source 9, and the stray light 8 is detected separately from the light of the target wavelength. 10
It gets in and affects the measurement. Here, FIG.
In FIG. 0, in FIG. 21, 5 and 11 are optical paths, and 12 is a diffraction grating.
【0005】このため、定量分析において検量線を使用
する際には、直線上の狭い部分のみを使用したり、検量
線範囲を分割する種々の方法が採用されている。Therefore, when a calibration curve is used in quantitative analysis, only a narrow portion on a straight line is used or various methods of dividing the calibration curve range are adopted.
【0006】[0006]
【発明が解決しようとする課題】しかしながら、混合ガ
ス等の混合物質においては、同様にノイズ成分が存在す
ると共に、所定物質の吸収スペクトル上に他の物質の吸
収スペクトルが重なるため、所定物質の吸収スペクトル
のみを測定することができず、混合物質中に含まれる所
定物質の濃度を測定することができないという問題があ
った。However, in a mixed substance such as a mixed gas, a noise component is also present, and the absorption spectrum of another substance overlaps with the absorption spectrum of the predetermined substance. There is a problem that it is not possible to measure only the spectrum, and it is not possible to measure the concentration of the predetermined substance contained in the mixed substance.
【0007】本発明は上述した実情に鑑みてなしたもの
で、ノイズ成分を校正して混合物質中の所定物質を定量
する定量分析校正方法を提供することを目的としてい
る。The present invention has been made in view of the above-mentioned circumstances, and an object thereof is to provide a quantitative analysis calibration method for calibrating a noise component to quantify a predetermined substance in a mixed substance.
【0008】[0008]
【課題を解決するための手段】本発明の請求項1は、時
間の経過により変化するノイズ成分量Pm(d)を校正
段階によって算出し、且つ組成比が不明である混合物質
より所定物質の濃度を通常計測段階によって算出する定
量分析校正方法であって、前記校正段階は、標準物質の
濃度ゼロのゼロスペクトルPz(d)と所定濃度の標準
スペクトルPr(d)とを採取し、校正用波長設定段階
として各受光スペクトルPz(d)、Pr(d)の処理
波長を所定波長に設定し、前記標準スペクトルPr
(d)の所定濃度と、予め求められたノイズ成分のない
理想的な吸光係数とにより透過率Trs(d)を計算
し、ノイズ成分量Pm(d)をAccording to a first aspect of the present invention, a noise component amount Pm (d) which changes with the passage of time is calculated in a calibration step, and a predetermined substance is selected from a mixed substance whose composition ratio is unknown. A quantitative analysis calibration method for calculating a concentration by a normal measurement step, wherein the calibration step collects a zero spectrum Pz (d) of zero concentration of a standard substance and a standard spectrum Pr (d) of a predetermined concentration for calibration. As the wavelength setting step, the processing wavelength of each of the received light spectra Pz (d) and Pr (d) is set to a predetermined wavelength, and the standard spectrum Pr is set.
The transmittance Trs (d) is calculated from the predetermined concentration of (d) and an ideal extinction coefficient without a noise component, which is obtained in advance, and the noise component amount Pm (d) is calculated.
【数4】Pm(d)=(Pr(d)−Trs(d)・P
z(d))/(1−Trs(d))
より求め、前記所定波長を他の所定波長に変えて処理手
順を校正用波長設定段階に戻すことにより同様の処理を
繰り返し、他の所定波長のノイズ成分量Pm(d)を算
出して各波長のノイズ成分量を集積し、前記通常計測段
階は、組成比が不明である混合物質より計測スペクトル
を採取し、計測用波長設定段階として各受光スペクトル
の処理波長を所定波長に設定し、前記計測スペクトル及
びゼロスペクトルPz(d)からノイズ成分量Pm
(d)を夫々引いて吸光度を算出し、前記所定波長を他
の所定波長に変えて処理手順を前記計測用波長設定段階
に戻すことにより同様の処理を繰り返し、他の所定波長
の吸光度を算出して各波長の吸光度を集積し、予め混合
物質から求められた検量線により、混合物質中の所定物
質の濃度を算出することを特徴とする定量分析校正方
法、に係るものである。## EQU00004 ## Pm (d) = (Pr (d) -Trs (d) .P
z (d)) / (1-Trs (d)), and the same process is repeated by changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the calibration wavelength setting step, thereby repeating another predetermined wavelength. The noise component amount Pm (d) is calculated and the noise component amounts of the respective wavelengths are integrated. In the normal measurement step, a measurement spectrum is collected from a mixed substance whose composition ratio is unknown, and each measurement wavelength setting step is performed. The processing wavelength of the received spectrum is set to a predetermined wavelength, and the noise component amount Pm is calculated from the measurement spectrum and the zero spectrum Pz (d).
(D) is subtracted to calculate the absorbance, and the same procedure is repeated by changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the measurement wavelength setting step to calculate the absorbance of another predetermined wavelength. Then, the absorbance of each wavelength is accumulated, and the concentration of the predetermined substance in the mixed substance is calculated from the calibration curve obtained from the mixed substance in advance.
【0009】本発明の請求項2は、組成比が不明である
混合物質より所定物質の濃度を算出し且つ連続的に次の
所定物質の濃度を算出する際に、前の所定物質の濃度を
算出してから次の所定物質の濃度を算出するまでの時間
間隔が所定時間を経過している場合には処理手順を校正
段階に戻し、前記時間間隔が所定時間の経過する前の場
合には処理手順を通常計測段階に戻す請求項1記載の定
量分析校正方法、に係るものである。According to a second aspect of the present invention, when the concentration of a predetermined substance is calculated from a mixed substance whose composition ratio is unknown and the concentration of the next predetermined substance is continuously calculated, the concentration of the previous predetermined substance is calculated. If the time interval from the calculation to the calculation of the concentration of the next predetermined substance has passed the predetermined time, the processing procedure is returned to the calibration step, and if the time interval is before the predetermined time has passed, The quantitative analysis calibration method according to claim 1, wherein the processing procedure is returned to the normal measurement stage.
【0010】本発明の請求項3は、単一物質の濃度ゼロ
から各所定濃度までの各受光スペクトルを採取し、単一
物質用波長設定段階として各受光スペクトルの処理波長
を所定波長に設定し、ノイズ成分量設定段階として前記
ノイズ成分を濃度ゼロの受光スペクトル又は所定濃度の
受光スペクトルより小さい任意の仮ノイズ成分量に仮設
定し、前記仮ノイズ成分量を濃度ゼロの受光スペクトル
及び所定濃度の受光スペクトルから夫々引いて各所定濃
度の吸光度を算出し、各所定濃度と吸光度の関係が直線
に従うとしてAccording to a third aspect of the present invention, each received spectrum from zero concentration of a single substance to each predetermined concentration is sampled, and a processing wavelength of each received spectrum is set to a predetermined wavelength as a wavelength setting step for a single substance. As a noise component amount setting step, the noise component is temporarily set to a light-receiving spectrum of zero density or an arbitrary temporary noise component amount smaller than a light-receiving spectrum of a predetermined density, and the temporary noise component amount is set to a light-receiving spectrum of zero density and a predetermined density. It is assumed that the absorbance at each specified concentration is calculated by subtracting it from the received light spectrum, and that the relationship between each specified concentration and the absorption follows a straight line.
【数5】Y=aX+b
a:傾き
b:切片
よりXに濃度、Yに吸光度を代入して線形回帰法により
相関係数を求め、続いて仮ノイズ成分量を他の仮ノイズ
成分量に変えて処理手順を前記ノイズ成分量設定段階に
戻すことにより同様の処理を繰り返して他の相関係数を
求め、各仮ノイズ成分量における複数の相関係数から最
も大きいものを選択することにより、選択された相関係
数に対応する傾きを所定波長の吸光係数と決定すると共
にノイズ成分量を決定し、更に前記所定波長を他の所定
波長に変えて処理手順を前記単一物質用波長設定段階に
戻すことにより同様の処理を繰り返して他の所定波長の
吸光係数及びノイズ成分量を夫々決定し、単一物質の受
光スペクトル中に含まれる各波長の吸光係数及び各波長
のノイズ成分量を集積する請求項1又は2記載の定量分
析校正方法、に係るものである。## EQU00005 ## Y = aX + b a: Slope b: From the intercept, the concentration is substituted for X and the absorbance is substituted for Y to obtain the correlation coefficient by the linear regression method, and then the temporary noise component amount is changed to another temporary noise component amount. The same procedure is repeated by returning the processing procedure to the noise component amount setting step to obtain another correlation coefficient, and by selecting the largest one from the plurality of correlation coefficients in each temporary noise component amount, the selection is performed. The slope corresponding to the correlation coefficient determined is determined as the absorption coefficient of the predetermined wavelength and the amount of noise component is determined, and the predetermined wavelength is changed to another predetermined wavelength to change the processing procedure to the single substance wavelength setting step. By returning, the same processing is repeated to determine the extinction coefficient and the noise component amount of other predetermined wavelengths respectively, and the extinction coefficient of each wavelength and the noise component amount of each wavelength included in the received spectrum of a single substance are integrated. Claim The present invention relates to the quantitative analysis calibration method described in 1 or 2.
【0011】本発明の請求項4は、単一物質の濃度ゼロ
から各所定濃度までの各受光スペクトルを採取し、単一
物質用波長設定段階として各受光スペクトルの処理波長
を所定波長に設定し、ノイズ成分量設定段階として前記
ノイズ成分を濃度ゼロの受光スペクトル又は所定濃度の
受光スペクトルより小さい任意の仮ノイズ成分量に仮設
定し、前記仮ノイズ成分量を濃度ゼロの受光スペクトル
及び所定濃度の受光スペクトルから夫々引いて各所定濃
度の吸光度を算出し、各所定濃度と吸光度の関係が直線
に従うとしてAccording to a fourth aspect of the present invention, each received light spectrum from zero concentration of a single substance to each predetermined concentration is sampled, and a processing wavelength of each received light spectrum is set to a predetermined wavelength as a wavelength setting step for a single substance. As a noise component amount setting step, the noise component is temporarily set to a light-receiving spectrum of zero density or an arbitrary temporary noise component amount smaller than a light-receiving spectrum of a predetermined density, and the temporary noise component amount is set to a light-receiving spectrum of zero density and a predetermined density. It is assumed that the absorbance at each specified concentration is calculated by subtracting it from the received light spectrum, and that the relationship between each specified concentration and the absorption follows a straight line.
【数6】Y=aX+b
a:傾き
b:切片
よりXに濃度、Yに吸光度を代入して線形回帰法により
切片を求め、続いて仮ノイズ成分量を他の仮ノイズ成分
量に変えて処理手順を前記ノイズ成分量設定段階に戻す
ことにより同様の処理を繰り返して他の切片を求め、各
仮ノイズ成分量における複数の切片から最もゼロに近い
ものを選択することにより、選択された切片に対応する
傾きを所定波長の吸光係数と決定すると共にノイズ成分
量を決定し、更に前記所定波長を他の所定波長に変えて
処理手順を前記単一物質用波長設定段階に戻すことによ
り同様の処理を繰り返して他の所定波長の吸光係数及び
ノイズ成分量を夫々決定し、単一物質の受光スペクトル
中に含まれる各波長の吸光係数及び各波長のノイズ成分
量を集積する請求項1又は2記載の定量分析校正方法、
に係るものである。[Formula 6] Y = aX + b a: Slope b: From the intercept, the concentration is substituted for X and the absorbance is substituted for Y to obtain the intercept by the linear regression method, and then the temporary noise component amount is changed to another temporary noise component amount for processing. The same processing is repeated by returning the procedure to the noise component amount setting step to obtain another intercept, and by selecting the intercept closest to zero from the plurality of intercepts in each provisional noise component amount, the selected intercept is obtained. Similar processing is performed by determining the corresponding slope as the absorption coefficient of a predetermined wavelength and determining the amount of noise component, and further changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the wavelength setting step for the single substance. 3. The absorption coefficient of another predetermined wavelength and the amount of noise component are respectively determined by repeating the above, and the absorption coefficient of each wavelength and the amount of noise component of each wavelength contained in the received spectrum of a single substance are integrated. Quantitative analysis calibration method of
It is related to.
【0012】本発明の請求項5は、混合物質の濃度ゼロ
の受光スペクトル及び組成比を変えた複数の受光スペク
トルを採取し、混合物質用波長設定段階として各受光ス
ペクトルの処理波長を所定波長に設定し、予め単一物質
より算出した所定波長のノイズ成分量を濃度ゼロの受光
スペクトル及び各組成比の受光スペクトルから夫々引く
ことにより各組成比での所定波長の吸光度を算出し、前
記所定波長を他の所定波長に変えて処理手順を前記混合
物質用波長設定段階に戻すことにより同様の処理を繰り
返して各組成比での他の所定波長の吸光度を夫々算出
し、各波長での吸光度及び各組成比のデータを用いて多
変量解析することにより混合物質中の所定物質の検量線
を作成することを特徴とする請求項1、2、3又は4記
載の定量分析校正方法、に係るものである。According to a fifth aspect of the present invention, a light-receiving spectrum of a mixed substance having a zero concentration and a plurality of light-receiving spectra having different composition ratios are sampled, and a processing wavelength of each light-receiving spectrum is set to a predetermined wavelength as a wavelength setting step for the mixed substance. Calculate the absorbance of the predetermined wavelength at each composition ratio by subtracting the noise component amount of the predetermined wavelength calculated in advance from a single substance from the reception spectrum of zero concentration and the reception spectrum of each composition ratio. Is changed to another predetermined wavelength and the same procedure is repeated by returning the treatment procedure to the wavelength setting step for the mixed substance to calculate the absorbance at each other predetermined wavelength at each composition ratio, and the absorbance at each wavelength and The calibration curve for quantitative analysis according to claim 1, 2, 3 or 4, wherein a calibration curve of a predetermined substance in a mixed substance is created by performing a multivariate analysis using data of each composition ratio. , It is those related to.
【0013】このように、請求項1によれば、校正段階
において経過時間により変化するノイズ成分量を校正
し、且つ校正したノイズ成分量及び予め準備した検量線
を用いることによって、組成比が不明である混合物質か
ら所定物質の濃度を算出するので、ノイズ成分量が変化
した場合であっても再度検量線を作成することなく、容
易に混合物質中の所定物質の濃度を算出することができ
る。As described above, according to the first aspect, the composition ratio is unknown by calibrating the noise component amount which changes with the passage of time in the calibration stage and using the calibrated noise component amount and the calibration curve prepared in advance. Since the concentration of the predetermined substance is calculated from the mixed substance, it is possible to easily calculate the concentration of the predetermined substance in the mixed substance without recreating a calibration curve even when the amount of noise components changes. .
【0014】請求項2によれば、連続的に混合物質中の
所定物質の濃度を算出する際に、前の所定物質の濃度を
算出した時から次の所定物質の濃度を算出する時までの
時間経過に対応して処理手順を変更するので、時間経過
により変化するノイズ成分量を時間経過に対応して校正
し、結果的に物質の濃度を連続的に測定する連続分析を
確実且つ精密に行うことができる。According to the second aspect, in continuously calculating the concentration of the predetermined substance in the mixed substance, from the time when the concentration of the previous predetermined substance is calculated to the time when the concentration of the next predetermined substance is calculated. Since the processing procedure is changed according to the passage of time, the amount of noise components that changes with the passage of time is calibrated according to the passage of time, and as a result, continuous analysis for continuously measuring the concentration of a substance can be performed reliably and accurately. It can be carried out.
【0015】請求項3又は4によれば、仮ノイズ成分量
を介して線形回帰法から算出された複数の相関係数もし
くは複数の切片により最適なものを選択して単一物質に
おける所定波長の吸光係数及びノイズ成分量を求め、且
つ所定波長を変えて同様に処理することにより他の所定
波長の吸光係数及びノイズ成分量を求め、各波長の吸光
係数及びノイズ成分量を集積するので、単一物質におけ
る各波長の吸光係数及びノイズ成分量を適確に求めるこ
とができる。According to the third or fourth aspect, the optimum one is selected from a plurality of correlation coefficients or a plurality of intercepts calculated by the linear regression method via the amount of the temporary noise component, and the optimum wavelength of a single substance is selected. Since the absorption coefficient and the noise component amount are obtained, and the same processing is performed by changing the predetermined wavelength, the absorption coefficient and the noise component amount at other predetermined wavelengths are obtained, and the absorption coefficient and the noise component amount at each wavelength are integrated. It is possible to accurately obtain the absorption coefficient and the amount of noise component of each wavelength in one substance.
【0016】請求項5によれば、単一物質より算出した
各波長のノイズ成分量を用いることにより混合物質から
ノイズ成分量を除いて各組成比での吸光度を算出し、且
つ各データを用いて多変量解析することにより混合物質
中の所定物質の吸光度等のデータを算出するので、所定
物質における各波長での複数の検量線を作成することが
できる。又、受光スペクトルからノイズ成分量を取り除
くので、高濃度で飽和した検量線を修正し、高精度な直
線で且つ再現性の高い検量線を作成することができる。According to the present invention, the absorbance at each composition ratio is calculated by removing the noise component amount from the mixed substance by using the noise component amount of each wavelength calculated from a single substance, and using each data. Since the data such as the absorbance of the predetermined substance in the mixed substance is calculated by performing the multivariate analysis by using the multivariate analysis, it is possible to create a plurality of calibration curves for the predetermined substance at each wavelength. Further, since the amount of noise components is removed from the received light spectrum, it is possible to correct a calibration curve saturated at high concentration and create a highly accurate calibration curve with high reproducibility.
【0017】[0017]
【発明の実施の形態】以下本発明の実施の形態を図面を
参照しつつ説明する。BEST MODE FOR CARRYING OUT THE INVENTION Embodiments of the present invention will be described below with reference to the drawings.
【0018】図1〜図4は本発明の定量分析校正方法を
実施する形態例のフローを示し、A,B,C,Dは夫々
のフローの接続点を示している。1 to 4 show a flow of an embodiment for carrying out the quantitative analysis / calibration method of the present invention, and A, B, C and D show connection points of the respective flows.
【0019】本発明の定量分析校正方法を実施する際に
は、ノイズ成分量及び吸光係数を求める段階と、検量線
を作成する段階と、時間経過により変化するノイズ成分
量を校正する校正段階と、混組成比が不明である混合物
質より所定物質の濃度を算出する段階とに分かれてい
る。When carrying out the quantitative analysis calibration method of the present invention, there are a step of obtaining a noise component amount and an extinction coefficient, a stage of creating a calibration curve, and a calibration stage of calibrating a noise component amount which changes with the passage of time. , The step of calculating the concentration of a predetermined substance from a mixed substance whose mixture composition ratio is unknown.
【0020】ノイズ成分のない理想の吸光係数を求める
段階を説明すると、初めに、一般の検量線を作成する場
合と同様に、単一物質(単一ガス)の濃度ゼロの場合、
及び濃度をn1,n2,n3…(少なくとも3個以上)
に変化させた場合の受光スペクトルP(d)(受光強
度、受光面積)を測定する。The step of obtaining an ideal extinction coefficient free from noise components will be described. First, as in the case of creating a general calibration curve, when the concentration of a single substance (single gas) is zero,
And the concentrations are n1, n2, n3 ... (at least 3 or more)
The light-receiving spectrum P (d) (light-receiving intensity, light-receiving area) when the value is changed to is measured.
【0021】次に複数の受光スペクトルP(d)を測定
した後には、各受光スペクトルを処理する波長を選択す
るよう単一物質用波長処理段階として初期波長dを設定
する。Next, after measuring a plurality of received light spectra P (d), the initial wavelength d is set as a single substance wavelength processing step so as to select a wavelength for processing each received light spectrum.
【0022】ここで、測定した各波長の受光スペクトル
には、ノイズ成分の迷光ノイズが含まれており、Here, the measured light reception spectrum of each wavelength contains stray light noise of a noise component,
【数7】P(d)=Ps(d)+Pm(d) P(d):測定した受光スペクトル(計測スペクトル) Ps(d):物質の受光スペクトル Pm(d):迷光ノイズの受光スペクトル となる。(7) P (d) = Ps (d) + Pm (d) P (d): Measured received light spectrum (measured spectrum) Ps (d): received light spectrum of substance Pm (d): Stray light noise received spectrum Becomes
【0023】このため、一般に各波長における吸光度を
求める式、Therefore, in general, an expression for obtaining the absorbance at each wavelength,
【数8】A(d)=log(Pz(d)/P(d))
A(d):吸光度
Pz(d):ゼロスペクトル(物質の濃度ゼロの場合の
受光スペクトル)
P(d):測定した受光スペクトル(計測スペクトル)
より、迷光ノイズの受光スペクトルを引き、## EQU8 ## A (d) = log (Pz (d) / P (d)) A (d): Absorbance Pz (d): Zero spectrum (reception spectrum when the concentration of the substance is zero) P (d): From the measured received spectrum (measured spectrum), subtract the received spectrum of stray light noise,
【数9】As(d)=log((Pz(d)−nPm
(d))/(P(d)−nPm(d)))
As(d):修正した吸光度
Pz(d):ゼロスペクトル(物質の濃度ゼロの場合の
受光スペクトル)
P(d):測定した受光スペクトル(計測スペクトル)
nPm(d):仮の迷光ノイズの受光スペクトル(仮ノ
イズ成分量)
に変形し、迷光ノイズのノイズ成分を数量化するようノ
イズ成分量設定段階として迷光ノイズをゼロの仮ノイズ
成分量(仮迷光)nPm(d)と仮設定する。## EQU9 ## As (d) = log ((Pz (d) -nPm
(D)) / (P (d) -nPm (d))) As (d): corrected absorbance Pz (d): zero spectrum (light-receiving spectrum when the concentration of the substance is zero) P (d): measured Light reception spectrum (measurement spectrum) nPm (d): Temporary stray light noise is set as a noise component amount setting step so as to quantify the noise component of stray light noise by transforming it into a light reception spectrum of temporary stray light noise (temporary noise component amount). A noise component amount (temporary stray light) nPm (d) is provisionally set.
【0024】続いて、仮ノイズ成分量nPm(d)が、
濃度ゼロの受光スペクトルPz(d)又は所定濃度の受
光スペクトルP(d)より小さい値であることを確認
し、[数9]に対して、仮ノイズ成分量nPm(d)の
ゼロの仮設定値、初期波長dにおける各所定濃度(n
1,n2,n3…)の受光スペクトルP(d)の測定
値、初期波長dにおける濃度ゼロでのゼロスペクトル
(受光スペクトル)Pz(d)の測定値を夫々代入し、
各所定濃度に対応する吸光度As(d)を算出する。Subsequently, the temporary noise component amount nPm (d) is
It is confirmed that the received light spectrum Pz (d) of zero density is smaller than the received light spectrum P (d) of a predetermined density, and the temporary noise component amount nPm (d) is temporarily set to zero with respect to [Equation 9]. Value, each predetermined concentration at the initial wavelength d (n
1, n2, n3 ...) and the measured value of the zero spectrum (received spectrum) Pz (d) at zero density at the initial wavelength d are substituted,
The absorbance As (d) corresponding to each predetermined concentration is calculated.
【0025】算出された各吸光度と、各所定濃度との関
係はランベルトベールの式The relationship between each calculated absorbance and each predetermined concentration is represented by the Lambert-Beer equation.
【数10】A=αn A:吸光度 α:吸光係数 n:濃度 に従い、直線の検量線となるので、(10) A = αn A: Absorbance α: extinction coefficient n: concentration According to, a linear calibration curve is obtained, so
【数11】Y=aX+b
a:傾き
b:切片
の式に、Xに各所定濃度(n1,n2,n3…)の値、
Yに各吸光度As(d)の算出値を代入し、最小二乗法
等の線形回帰法により処理して相関係数r(R2)、切
片b、傾きaを求める。[Formula 11] Y = aX + b a: slope b: in the equation of intercept, X is a value of each predetermined concentration (n1, n2, n3 ...),
The calculated value of each absorbance As (d) is substituted for Y and processed by a linear regression method such as the least square method to obtain the correlation coefficient r (R 2 ), the intercept b, and the slope a.
【0026】ここで、線形回帰法による処理を[表1]
に示すと、線形回帰法は、採取及び算出した濃度Xと吸
光度Yの複数組(少くとも三組以上)をK個として考え
る。Here, the processing by the linear regression method is shown in [Table 1].
In the linear regression method, a plurality of sets (at least three sets or more) of the collected and calculated concentration X and absorbance Y are considered as K.
【0027】[0027]
【表1】 [Table 1]
【0028】又、XとYの共分散SxyはThe covariance Sxy of X and Y is
【数12】 Sxy=(1/k)Σxy−avg_x×avg_y このとき、[Equation 12] Sxy = (1 / k) Σxy−avg_x × avg_y At this time,
【数13】a=Sxy/Sxx(13) a = Sxy / Sxx
【数14】b=avg_y−Sxy×avg_y/SxxB = avg_y−Sxy × avg_y / Sxx
【0029】又、相関係数rの二乗R2はFurther, the square R 2 of the correlation coefficient r is
【数15】R2=Sxy2/(Sxx・Syy)
であり、この計算値によりr(R2)が最も大きくなっ
た場合(1に近づいた場合)に濃度Xと吸光度Yの複数
組が直線上に位置すると判断する。又、r(R2)が最
も大きくなったときにはb=0になる(ゼロに最も近く
なる)のでbを基準にしてもよい。なお、線形回帰法に
おいて誤差の二乗和が最小になるnPmを求める場合に
はR2が最大になるとは限らず、b=0にもならないの
で適用できない。[Equation 15] R 2 = Sxy 2 / (Sxx · Syy), and when the calculated value of r (R 2 ) is the largest (close to 1), a plurality of pairs of concentration X and absorbance Y are obtained. Judge that it is located on a straight line. Further, when r (R 2 ) becomes the largest, b = 0 (closest to zero), so b may be used as a reference. In the linear regression method, when nPm that minimizes the sum of squares of the errors is obtained, R 2 does not always become the maximum, and b = 0 does not hold, so that it cannot be applied.
【0030】このような線形回帰法により仮ノイズ成分
量nPmがゼロの場合の相関係数r、切片b、傾きaを
求めた後には、傾きaと共に、相関係数r及び切片bの
少くとも一方を仮記憶する。After obtaining the correlation coefficient r, the intercept b, and the slope a when the provisional noise component amount nPm is zero by such a linear regression method, after the slope a, at least the correlation coefficient r and the intercept b are obtained. One is temporarily stored.
【0031】次に、ゼロの仮ノイズ成分量nPm(d)
に所定の増加量ΔnPmを加えて、図1に示す如く、処
理手順をノイズ成分量設定段階に戻すことによりノイズ
成分を他の仮ノイズ成分量nPm(d)と仮設定し、他
の仮ノイズ成分量nPm(d)が、濃度ゼロの受光スペ
クトル(ゼロスペクトル)Pz(d)又は所定濃度の受
光スペクトル(計測スペクトル)P(d)より小さい値
であることを確認する。Next, the zero temporary noise component amount nPm (d)
To the noise component amount setting step, the noise component is temporarily set to another temporary noise component amount nPm (d) by adding a predetermined increase amount ΔnPm to It is confirmed that the component amount nPm (d) is smaller than the light-receiving spectrum (zero spectrum) Pz (d) of zero concentration or the light-receiving spectrum (measurement spectrum) P (d) of a predetermined concentration.
【0032】確認した後には、初めに吸光度As(d)
を求めた処理と略同様に、[数9]に対して、他の仮ノ
イズ成分量nPm(d)の仮設定値、初期波長dにおけ
る各所定濃度(n1,n2,n3…)の受光スペクトル
P(d)の測定値、初期波長dにおける濃度ゼロのゼロ
スペクトルPzの測定値を夫々代入することにより、初
期波長dでの各所定濃度に対応する吸光度As(d)を
算出し、且つ、先の線形回帰法により相関係数等を算出
した処理と同様に、他の仮ノイズ成分量nPm(d)に
おける他の相関係数r、他の切片b、他の傾きaを求
め、同様に仮記憶する。After confirmation, firstly the absorbance As (d)
In the same manner as the processing for obtaining the above, for [Equation 9], a temporary setting value of other temporary noise component amount nPm (d) and a received light spectrum of each predetermined density (n1, n2, n3 ...) At the initial wavelength d. The absorbance As (d) corresponding to each predetermined concentration at the initial wavelength d is calculated by substituting the measured value of P (d) and the measured value of the zero spectrum Pz of zero concentration at the initial wavelength d, respectively, and Similar to the above-described process of calculating the correlation coefficient and the like by the linear regression method, another correlation coefficient r, another intercept b, and another slope a in another temporary noise component amount nPm (d) are obtained, and similarly. Temporarily store.
【0033】続いて、他の仮ノイズ成分量nPm(d)
に更に所定の増加量ΔnPmを加えて処理手順をノイズ
成分量設定段階に戻すことにより別の仮ノイズ成分量n
Pm(d)と仮設定し、同じ処理を繰り返して、別の仮
ノイズ成分量nPm(d)における別の相関係数r、別
の切片b、別の傾きaを求め、同様に仮記憶する。Next, another temporary noise component amount nPm (d)
To the noise component amount setting step by adding a predetermined increase amount ΔnPm to
Pm (d) is temporarily set and the same process is repeated to obtain another correlation coefficient r, another intercept b, and another slope a for another temporary noise component amount nPm (d), and similarly temporarily store them. .
【0034】このように仮ノイズ成分量nPm(d)に
徐々に増加量ΔnPmを加える処理は、初期波長dにお
ける複数の傾きaと初期波長dにおける複数の相関係数
r及び切片bとを求めて蓄積するものである。As described above, in the process of gradually increasing the increase amount ΔnPm to the temporary noise component amount nPm (d), a plurality of slopes a at the initial wavelength d, a plurality of correlation coefficients r and the intercept b at the initial wavelength d are obtained. It is what is accumulated.
【0035】更に、増加する仮ノイズ成分量nPm
(d)が、濃度ゼロの受光スペクトル(ゼロスペクト
ル)Pz(d)又は所定濃度の受光スペクトル(計測ス
ペクトル)P(d)を超えた時点で処理を停止する。こ
こで、処理を停止する場合は、相関係数rの蓄積数もし
くは切片bの蓄積数が所定以上になった場合でもよい。Further, the increasing amount of temporary noise component nPm
The process is stopped when (d) exceeds the received light spectrum (zero spectrum) Pz (d) of zero concentration or the received light spectrum (measured spectrum) P (d) of a predetermined concentration. Here, the processing may be stopped when the accumulated number of the correlation coefficient r or the accumulated number of the intercept b exceeds a predetermined value.
【0036】処理を停止した後、各仮ノイズ成分量nP
m(d)における複数の相関係数rの中より相関係数r
が最も大きいもの(最も1に近づいたもの)を選択する
と共に、各仮ノイズ成分量nPm(d)における複数の
切片bの中から切片bが最もゼロに近いものを選択す
る。ここで、相関係数r及び切片bを選択する場合は相
関係数rもしくは切片bのどちらか一方の処理でもよ
い。又、相関係数rが最も大きいものを選択する場合
は、R2の極大値を求めるものであり、微分法や山登り
法でも求めることができる。更に、極大になるポイント
部分を詳細に探索するよう極大値近傍の区間のみΔnP
mを小さくしてもよい。更に又、相関係数r及び切片b
を選択する場合は、多くの相関係数r及び切片bを蓄積
せずに、所定の仮ノイズ成分量nPm(d)における相
関係数r及び切片bを求めた時点で、前に仮記憶した相
関係数r及び切片bと比較し、常に相関係数rが最も大
きいもの、及び切片bが最もゼロに近いものを残すよう
にしてもよい。After the processing is stopped, each temporary noise component amount nP
Correlation coefficient r from among a plurality of correlation coefficients r in m (d)
Is selected, the one having the largest (closest to 1) is selected, and the one having the intercept b closest to zero is selected from the plurality of intercepts b in each temporary noise component amount nPm (d). Here, when selecting the correlation coefficient r and the intercept b, either the correlation coefficient r or the intercept b may be processed. Further, when the one having the largest correlation coefficient r is selected, the maximum value of R 2 is obtained, and it can be obtained by the differential method or the hill climbing method. In addition, ΔnP is set only for the section near the maximum value so that the point that becomes the maximum is searched in detail.
You may make m small. Furthermore, the correlation coefficient r and the intercept b
In the case of selecting, the correlation coefficient r and the intercept b in the predetermined temporary noise component amount nPm (d) are calculated without accumulating a large number of the correlation coefficient r and the intercept b, and are temporarily stored before. It is also possible to compare the correlation coefficient r and the intercept b, and always leave the one having the largest correlation coefficient r and the one having the intercept b closest to zero.
【0037】次いで、選択した相関係数r及び切片bの
少くとも一方の情報から実際のノイズ成分量Pm(d)
を決定すると共に、線形回帰法により算出された対応の
傾きaを決定し、決定された傾きaを初期波長dでの絶
対的な吸光係数αとする。Next, from the information of at least one of the selected correlation coefficient r and intercept b, the actual noise component amount Pm (d)
And the corresponding slope a calculated by the linear regression method are determined, and the determined slope a is used as the absolute absorption coefficient α at the initial wavelength d.
【0038】初期波長dでの実際のノイズ成分量Pm
(d)を求めた後には、初期波長dに所定の波長幅Δd
を加えて他の所定波長dと設定し、且つ他の所定波長d
が所定の範囲内であることを確認し、図1に示す如く、
処理手順を単一物質用波長設定段階に戻すことにより、
以下、迷光ノイズを仮ノイズ成分量(仮迷光)nPm
(d)に仮設定する等の同様な処理を行い、相関係数r
及び切片bを選択し、他の所定波長dにおける実際のノ
イズ成分量Pm(d)を決定すると共に、線形回帰法に
より算出された対応の傾きaを決定し、決定された傾き
aを他の所定波長dでの絶対的な吸光係数αとする。Actual noise component amount Pm at initial wavelength d
After obtaining (d), a predetermined wavelength width Δd is added to the initial wavelength d.
Is set to another predetermined wavelength d, and another predetermined wavelength d is set.
Is within the specified range, and as shown in Fig. 1,
By returning the processing procedure to the single substance wavelength setting stage,
Below, the stray light noise is calculated as the temporary noise component amount (temporary stray light) nPm.
Similar processing such as provisional setting in (d) is performed, and the correlation coefficient r
And the intercept b, the actual noise component amount Pm (d) at another predetermined wavelength d is determined, and the corresponding slope a calculated by the linear regression method is determined. The absolute absorption coefficient α at the predetermined wavelength d is set.
【0039】このように、所定波長dに徐々に所定の波
長幅Δdを加えて同様な処理を行うことにより各波長に
おける実際のノイズ成分量Pm(d)と絶対的な吸光係
数αを集積し、増加する所定波長dが所定の範囲を超え
た時点で処理を停止し、各波長における絶対的な吸光係
数スペクトルを求める。In this way, by gradually adding the predetermined wavelength width Δd to the predetermined wavelength d and performing the same processing, the actual noise component amount Pm (d) and the absolute absorption coefficient α at each wavelength are integrated. When the increasing predetermined wavelength d exceeds a predetermined range, the processing is stopped and the absolute absorption coefficient spectrum at each wavelength is obtained.
【0040】各波長における実際のノイズ成分量Pm
(d)を決定した後には、検量線を作成する段階に移行
し、検量線を作成する段階は、図2に示す如く、混合物
質(混合ガス)Pz(d)の濃度ゼロの場合、及び各成
分の組成比(濃度比)を変化させた場合の複数の受光ス
ペクトル(受光強度、受光面積)P(d)を測定する。
ここで、測定する混合物質(混合ガス)は単一物質(単
一ガス)を含んでいてもよいし、含んでなくてもよい。Actual noise component amount Pm at each wavelength
After the determination of (d), the process proceeds to the step of creating a calibration curve, and the step of creating the calibration curve is as shown in FIG. 2 when the concentration of the mixed substance (mixed gas) Pz (d) is zero, and A plurality of light receiving spectra (light receiving intensity, light receiving area) P (d) when the composition ratio (concentration ratio) of each component is changed is measured.
Here, the mixed substance (mixed gas) to be measured may or may not contain a single substance (single gas).
【0041】次に各受光スペクトルPz(d)、P
(d)を処理する波長を選択するよう混合物質用波長処
理段階として初期波長dを設定し、初期波長dが所定範
囲内であることを確認する。続いて、先の段階で求めた
各波長における実際のノイズ成分量Pm(d)より初期
波長dの場合のノイズ成分量Pm(d)を選択して準備
し、下記の[数16]に対して、初期波長dにおけるノ
イズ成分量Pm(d)の値、初期波長dにおける各組成
比の受光スペクトルP(d)の測定値、初期波長dにお
ける濃度ゼロでのゼロスペクトル(受光スペクトル)P
z(d)の測定値を夫々代入し、各組成比(濃度)での
混合物質の吸光度As(d)を算出する。Next, each received spectrum Pz (d), P
The initial wavelength d is set as the wavelength processing step for the mixed substance so as to select the wavelength for processing (d), and it is confirmed that the initial wavelength d is within the predetermined range. Subsequently, the noise component amount Pm (d) in the case of the initial wavelength d is selected and prepared from the actual noise component amount Pm (d) at each wavelength obtained in the previous step, and the following [Formula 16] is satisfied. The value of the noise component amount Pm (d) at the initial wavelength d, the measured value of the received light spectrum P (d) of each composition ratio at the initial wavelength d, and the zero spectrum (received light spectrum) P at zero concentration at the initial wavelength d.
The absorbance As (d) of the mixed substance at each composition ratio (concentration) is calculated by substituting the measured values of z (d).
【0042】[0042]
【数16】As(d)=log((Pz(d)−Pm
(d))/(P(d)−Pm(d)))
As(d):混合物質の修正した吸光度
Pz(d):混合物質のゼロスペクトル(物質の濃度ゼ
ロの場合の受光スペクトル)
P(d):測定した混合物質の受光スペクトル(計測ス
ペクトル)
Pm(d):単一物質より算出した実際の迷光ノイズの
受光スペクトル(実際のノイズ成分量)## EQU16 ## As (d) = log ((Pz (d) -Pm
(D)) / (P (d) -Pm (d))) As (d): modified absorbance Pz (d) of the mixed substance: zero spectrum of the mixed substance (light-receiving spectrum when the concentration of the substance is zero) P (D): Measured light-receiving spectrum of the mixed substance (measurement spectrum) Pm (d): Actual light-receiving spectrum of stray light noise calculated from a single substance (actual noise component amount)
【0043】ここで、単一物質及び混合物質の測定は、
同じ測定装置を用いることにより、単一物質に含まれる
各波長のノイズ成分量と、混合物質に含まれる各波長の
ノイズ成分量とが略同じである。又、単一物質の吸収ス
ペクトルの測定と混合物質の吸収スペクトルの測定との
測定間隔はノイズ成分量が変化しない時間である。Here, the measurement of a single substance and a mixed substance is
By using the same measuring device, the noise component amount of each wavelength contained in the single substance and the noise component amount of each wavelength contained in the mixed substance are substantially the same. The measurement interval between the measurement of the absorption spectrum of a single substance and the measurement of the absorption spectrum of a mixed substance is the time during which the amount of noise components does not change.
【0044】初期波長dでの吸光度As(d)を算出し
た後には、初期波長dに所定の波長幅Δdを加えて他の
所定波長dと設定し、図2に示す如く、処理手順を混合
物質用波長設定段階に戻し、以下、同様な処理を行な
い、各組成比での他の所定波長dでの吸光度As(d)
を求める。After calculating the absorbance As (d) at the initial wavelength d, a predetermined wavelength width Δd is added to the initial wavelength d to set another predetermined wavelength d, and the processing procedure is mixed as shown in FIG. After returning to the wavelength setting step for the substance, the same process is performed thereafter, and the absorbance As (d) at another predetermined wavelength d at each composition ratio is obtained.
Ask for.
【0045】このように、所定波長dに徐々に所定の波
長幅Δdを加えて同様な処理を行うことにより各波長に
おける各組成比の吸光度As(d)を集積し、増加する
所定波長dが所定の範囲を超えた時点で処理を停止し、
吸光度As(d)及び各組成比等のデータを用いて多変
量解析を行う。As described above, by gradually adding the predetermined wavelength width Δd to the predetermined wavelength d and performing the same process, the absorbance As (d) of each composition ratio at each wavelength is accumulated, and the increasing predetermined wavelength d is increased. Processing is stopped when the specified range is exceeded,
Multivariate analysis is performed using the data such as the absorbance As (d) and each composition ratio.
【0046】ここで、多変量解析について説明すると、
多変量解析は、重回帰分析、主成分回帰分析、PLS、
CLS、ニューラルネット等があり、下記にはPLS
(Partial Least Squares )モデルの計算理論を用いた
場合の例を説明する。The multivariate analysis will be described below.
Multivariate analysis includes multiple regression analysis, principal component regression analysis, PLS,
There are CLS, neural network, etc.
(Partial Least Squares) An example of using the calculation theory of the model will be described.
【0047】(PLSモデルの計算理論)Xを説明変
数、yを目的変数とする。(PLS model calculation theory) X is an explanatory variable and y is an objective variable.
【0048】[0048]
【数17】 [Equation 17]
【0049】吸光度スペクトル波形解析による濃度推定
モデルの場合、[数17]における、x(n,d)は、
波長d、計測番号nのときの吸光度であり、y(n)
は、計測番号nのとき濃度である。Nは計測数(サンプ
ル数)、Dは波長の分割数(説明変数の数)である。In the case of the concentration estimation model based on the absorbance spectrum waveform analysis, x (n, d) in [Equation 17] is
Absorbance at wavelength d and measurement number n, y (n)
Is the concentration when the measurement number is n. N is the number of measurements (the number of samples), and D is the number of wavelength divisions (the number of explanatory variables).
【0050】PLS法では、説明変数Xと目的変数yを
[数18]、[数19]の二つの基本式で求める。In the PLS method, the explanatory variable X and the objective variable y are obtained by the two basic equations [Equation 18] and [Equation 19].
【0051】[0051]
【数18】X=TPT+E T:潜在変数 P:ローディング E:説明変数Xの残差 上添え字のT:転置行列X = TP T + E T: Latent variable P: Loading E: Residual of explanatory variable X Superscript T: Transposed matrix
【0052】[0052]
【数19】y=Tq+f q:係数 f:目的変数yの残差Y = Tq + f q: coefficient f: residual of the objective variable y
【0053】又、潜在変数T、ローディングP及び係数
qは[数20]、[数21]、[数22]のように示さ
れる。Further, the latent variable T, the loading P and the coefficient q are shown as [Equation 20], [Equation 21] and [Equation 22].
【0054】[0054]
【数20】 t(n,a):a成分目の計測番号nの潜在変数 A:成分数(1〜Nの範囲内を選択可能) ta :潜在変数Tのa成分目の潜在変数ベクトル[Equation 20] t (n, a): a component th measurement number n of latent variables A: Number of component (a range of 1~N selectable) t a: latent variable vector of a component th latent variables T
【0055】[0055]
【数21】
p(a,d):a成分目の波長dのローディング
A:成分数(1〜Nの範囲内を選択可能)
pa :ローディングPのa成分目のローディングベクト
ル[Equation 21] p (a, d): Loading of the wavelength d of the a-component A: Number of components (selectable within the range of 1 to N) p a : Loading vector of the a-component of the loading P
【0056】[0056]
【数22】q=(q(1),q(2),q(3),…,
q(a),…q(A))
qa=q(a)
q(a):a成分目の係数である。[Equation 22] q = (q (1), q (2), q (3), ...,
q (a), ... Q (A)) q a = q (a) q (a): Coefficient of the a-th component.
【0057】ここで、モデルの特徴を表すのは、上位6
番目くらい間での成分であり、それ以上は、予測誤差を
低下させる。最適な成分数Aの決定は、クロスバリエー
ションを行うことで決定する。Here, the features of the model are represented by the top 6
It is a component for the second time, and more than that reduces the prediction error. The optimum number of components A is determined by performing cross variation.
【0058】次に、PLS法では、説明変数Xの情報を
目的変数yのモデリングに直接用いるのではなく、説明
変数Xの情報の一部を潜在定数tに変換して潜在定数t
を用いて目的変数yをモデリングする。Next, in the PLS method, the information of the explanatory variable X is not directly used for modeling the objective variable y, but a part of the information of the explanatory variable X is converted into a latent constant t and the latent constant t.
Is used to model the objective variable y.
【0059】(潜在定数t)ta は、説明変数Xの線形
結合であるとすれば、[数23]で表される。[0059] (potential constant t) t a, if a is a linear combination of the explanatory variables X, represented by [Expression 23].
【0060】[0060]
【数23】ta=Xwa
wa は重みベクトルであり、[数24]のように表され
る。[Mathematical formula-see original document] t a = Xw a w a is a weight vector, which is expressed as [Equation 24].
【0061】[0061]
【数24】 w(d,a):a成分目の波長dの重み係数[Equation 24] w (d, a): Weighting coefficient of the wavelength d of the a-th component
【0062】(第1成分の計算)続いて、成分が一つの
場合(a=1)を計算して説明すると、成分aが一つの
場合、[数18]、[数19]は[数25]、[数2
6]の式で表される。(Calculation of the First Component) Next, the case where there is one component (a = 1) will be described. When there is one component a, [Equation 18] and [Equation 19] are converted into [Equation 25] ], [Equation 2
6].
【0063】[0063]
【数25】X=t1p1 T+E[Expression 25] X = t 1 p 1 T + E
【0064】[0064]
【数26】y=t1q1+f [数23]より潜在定数tを[数27]に変形する。Y = t 1 q 1 + f From [Equation 23], the latent constant t is transformed into [Equation 27].
【0065】[0065]
【数27】
wのノルムを1になるように設定すると[数28]にな
る。[Equation 27] If the norm of w is set to 1, [Equation 28] is obtained.
【0066】[0066]
【数28】 [Equation 28]
【0067】更に、PLSのモデルは、目的変数yと潜
在定数tとの相関を大きくすると同時にtの分散を大き
くすることであり、これを満たす条件は、[数29]の
目的変数yと潜在定数tの共分散Sが最大になるポイン
トである。Further, the PLS model is to increase the correlation between the objective variable y and the latent constant t and at the same time increase the variance of t. The condition that satisfies this is that the objective variable y of [Equation 29] and the latent constant t This is the point where the covariance S of the constant t is maximized.
【0068】[0068]
【数29】S=yTt(29) S = y T t
【0069】ここで、wのノルムを1とする制約条件で
Sが最大になる条件をLagrangeの未定乗数法を用いて
[数30]のように求める。Here, the condition that maximizes S under the constraint condition that the norm of w is 1 is obtained as shown in [Equation 30] using Lagrange's undetermined multiplier method.
【0070】[0070]
【数30】 [Equation 30]
【0071】関数Gは、変数wの関数なので、Gをw
(d,1)について偏微分して、[数31]、[数3
2]の関係を得る。Since the function G is a function of the variable w, G is replaced by w
Partial differentiation is performed on (d, 1) to obtain [Formula 31] and [Formula 3].
2] is obtained.
【0072】[0072]
【数31】 [Equation 31]
【0073】[0073]
【数32】
この[数32]の両辺にw(d,1)を掛けると[数3
3]になる。[Equation 32] Multiplying both sides of this [Equation 32] by w (d, 1), [Equation 3]
3].
【0074】[0074]
【数33】 さらにdについて総和を取ると[数34]となる。[Expression 33] Further, the sum of d is obtained as [Equation 34].
【0075】[0075]
【数34】 [Equation 34]
【0076】ここで、‖w1 ‖=0の制約条件より[数
35]となる。Here, from the constraint condition of ‖w 1 ‖ = 0, [Equation 35] is obtained.
【0077】[0077]
【数35】 [Equation 35]
【0078】[数31]の左辺は、[数29]のS=y
T tの定義であるので、2μはyTtの値となる。従っ
て、S=yT tが最大になる最大のwの値は[数36]
で与えられる。The left side of [Equation 31] is S = y in [Equation 29].
Since it is the definition of T t, 2μ is the value of y T t. Therefore, the maximum value of w that maximizes S = y T t is [Equation 36]
Given in.
【0079】[0079]
【数36】 w1 のノルムは1なので、wは[数37]となる。[Equation 36] Since the norm of w 1 is 1, w is [Equation 37].
【0080】[0080]
【数37】w1=XTy/‖XTy‖ ここで潜在変数tは[数38]によって求まる。W 1 = X T y / ‖X T y‖ where the latent variable t is obtained by [Formula 38].
【0081】[0081]
【数38】t1=Xw1 (38) t 1 = Xw 1
【0082】[数25]のローディングベクトルp
1 は、説明変数Xの残差Eの要素の二乗和が最小になる
ように[数39]で求める。The loading vector p of [Equation 25]
1 is obtained by [Equation 39] so that the sum of squares of the elements of the residual E of the explanatory variable X is minimized.
【0083】[0083]
【数39】p1=XTt1/t1 Tt1 P 1 = X T t 1 / t 1 T t 1
【0084】[数26]の係数qa は、目的変数yの残
差ベクトルfの要素の二乗和が最小になるように条件か
ら[数40]で求める。The coefficient q a of [Equation 26] is calculated by [Equation 40] from the condition so that the sum of squares of the elements of the residual vector f of the objective variable y is minimized.
【0085】[0085]
【数40】q1=yTt1/t1 Tt1 Q 1 = y T t 1 / t 1 T t 1
【0086】(第2成分以降の計算)第2成分のモデル
式は[数41]、[数42]で表される。(Calculation after Second Component) The model formula of the second component is expressed by [Formula 41] and [Formula 42].
【0087】[0087]
【数41】X=t1p1 T+t2p2 T+EX = t 1 p 1 T + t 2 p 2 T + E
【0088】[0088]
【数42】y=t1q1+t2q2+fY = t 1 q 1 + t 2 q 2 + f
【0089】ここで、成分数1のモデリングで、Xのう
ち[数41]のt1 p1 T が使われ、yのうちt1 q1
が説明に使われたので、残っている情報を[数43]、
[数44]と置き換えることができる。Here, in modeling with one component, t 1 p 1 T of [Formula 41] of X is used, and t 1 q 1 of y is used.
Was used for the explanation, the remaining information is [Numerical equation 43],
It can be replaced with [Equation 44].
【0090】[0090]
【数43】Xnew=X−t1p1 T X new = X−t 1 p 1 T
【0091】[0091]
【数44】ynew=y−t1q1 Y new = y−t 1 q 1
【0092】Xnew とynew を用いると、[数41]、
[数42]は、[数45]、[数46]となる。Using X new and y new , [Formula 41],
[Formula 42] becomes [Formula 45] and [Formula 46].
【0093】[0093]
【数45】Xnew=t2p2 T+EX new = t 2 p 2 T + E
【0094】[0094]
【数46】ynew=t2q2+fY new = t 2 q 2 + f
【0095】これは、成分番号が一つ増えた以外は、
[数25]、[数26]と同じ式である。This is except that the component number is increased by one.
This is the same formula as [Formula 25] and [Formula 26].
【0096】従って、第1成分と同様にt2 、p2 、q
2 を求めることができる。Therefore, similarly to the first component, t 2 , p 2 , q
You can ask for 2 .
【0097】このループを繰り返すことで、第3成分以
降の算出ができる。By repeating this loop, the third and subsequent components can be calculated.
【0098】(回帰ベクトルの算出)必要な成分数A回
繰り返し計算をしたモデル式は[数47]、[数48]
のように書ける。(Calculation of Regression Vector) The model formula in which the necessary number of components is repeated A times is [Equation 47], [Equation 48]
Can be written as
【0099】[0099]
【数47】 X=TPT=t1p1 T+…+tapa T+…+tApA T X = TP T = t 1 p 1 T + ... + t a p a T + ... + t A p A T
【0100】[0100]
【数48】y=Tq=t1q1+…+taqa+…+taqa Y = Tq = t 1 q 1 + ... + t a q a + ... + t a q a
【0101】[数48]の潜在変数tに[数23]のt
1 =Xw1 を代入すると、推定するモデル式は、[数4
9]となる。The latent variable t in [Equation 48] is t in [Equation 23].
Substituting 1 = Xw 1 , the model equation estimated is
9].
【0102】[0102]
【数49】y=Xw1q1+(X−t1p1 T)w2q2+… 変形すると、Y = Xw 1 q 1 + (X−t 1 p 1 T ) w 2 q 2 + ...
【数50】 y=Xw1q1+Xw2q2−t1p1 Tw2q2+…Y = Xw 1 q 1 + Xw 2 q 2 −t 1 p 1 T w 2 q 2 + ...
【0103】この[数50]に[数23]のt1 =Xw
1 を代入してXでまとめると、[数51]となる。In this [Equation 50], t 1 = Xw in [Equation 23]
Substituting 1 and putting together in X gives [Equation 51].
【0104】[0104]
【数51】 y=X(w1q1+w2q2−w1p1 Tw2q2…)[Number 51] y = X (w 1 q 1 + w 2 q 2 -w 1 p 1 T w 2 q 2 ...)
【0105】ここで、[数52]のように、ある説明す
るベクトルHere, a certain vector to be explained, as in [Equation 52]
【外1】 に対して、目的変数[Outer 1] For the objective variable
【外2】 を推定するモデル式に変換する。[Outside 2] Is converted into a model formula for estimating.
【0106】[0106]
【数52】 [Equation 52]
【0107】[数52]で、bは回帰ベクトル呼ばれる
もので、[数53]で示される。In [Equation 52], b is called a regression vector and is represented by [Equation 53].
【0108】[0108]
【数53】 [Equation 53]
【0109】回帰ベクトルbは、[数51]から[数5
4]のように求められる。The regression vector b is calculated from [Equation 51] to [Equation 5]
4] is required.
【0110】[0110]
【数54】b=W(PTW)-1 B = W (P T W) -1
【0111】以上のPLS法のアルゴリズムをまとめ
て、図5に示す。The above PLS algorithm is summarized in FIG.
【0112】初めにPLS法による計算の開始から、成
分をa=1に設定して第1成分を求め、次に[数37]
で説明した第1成分の重みベクトルwa を演算し、wa
をもとに[数37]の潜在変数tを演算し、[数39]
のローディングベクトルPaを演算し、[数40]の係
数qa を演算し、求めたローディングベクトルPa と係
数qa から[数43]、[数44]で説明した第2成分
のモデルを設定し、成分aをa=a+1とインクリメン
トし、step1で、次の成分の演算が必要かどうかを
判断し、必要であれば(Yes)、すなわち第2成分の
重みベクトルw a の演算に戻して、同様な演算を繰り返
した後、次の成分の設定を行うと共にインクリメント
し、step1で、成分の演算が必要数行い必要でない
とき(No)、[数54]で説明した回帰ベクトルbを
演算して終了する。From the beginning of the calculation by the PLS method,
The minute is set to a = 1 to obtain the first component, and then [Formula 37]
The weight vector w of the first component described inaTo calculate wa
The latent variable t of [Equation 37] is calculated based on
Loading vector PaAnd calculate the value of [Equation 40]
Number qaIs calculated to obtain the loading vector PaClerk
Number qaTo the second component described in [Formula 43] and [Formula 44]
The model is set and the component a is incremented as a = a + 1
And whether or not it is necessary to calculate the next component in step 1.
Judge, and if necessary (Yes), that is, the second component
Weight vector w aReturn to and repeat the same operation
After that, set the next component and increment
However, in step 1, the required number of components are calculated and not required.
When (No), the regression vector b described in [Equation 54] is
Calculate and finish.
【0113】多変量解析を終了すると、混合物質中に含
まれる所定物質の吸光度、組成比(濃度)等のデータを
算出し、所定物質における各波長での複数の検量線を作
成することができる。When the multivariate analysis is completed, data such as the absorbance and composition ratio (concentration) of the predetermined substance contained in the mixed substance can be calculated, and a plurality of calibration curves at each wavelength of the predetermined substance can be prepared. .
【0114】続いて、検量線を作成した後、連続計測を
開始するとしてノイズ成分量を校正する校正段階を説明
すると、校正段階は、図3に示す如く、濃度ゼロのゼロ
スペクトルPz(d)と、標準単一物質による所定濃度
nrの標準スペクトルPr(d)との二点を採取して測
定する。ここで、用いる標準単一物質は、吸収スペクト
ルが一定範囲において、濃度を求める所定物質の吸収ス
ペクトルと重ならないこと、及び安定な物質であること
が最低の必要条件である。Next, the calibration step for calibrating the noise component amount after starting the calibration curve after starting the calibration curve will be explained. As shown in FIG. 3, the calibration step is a zero spectrum Pz (d) of zero concentration. And a standard spectrum Pr (d) having a predetermined concentration nr of a standard single substance are sampled and measured. The standard single substance used here is the minimum requirement that the absorption spectrum does not overlap with the absorption spectrum of the predetermined substance for which the concentration is to be determined within a certain range, and that it is a stable substance.
【0115】次にゼロスペクトルPz(d)と標準スペ
クトルPr(d)を測定した後には、各受光スペクトル
Pz(d)、Pr(d)を処理する波長を選択するよう
校正用波長処理段階として初期波長dを設定し、先の段
階で求めたノイズ成分のない初期波長dにおける理想の
吸光係数α(d)及び標準スペクトルPr(d)の所定
濃度nrをNext, after measuring the zero spectrum Pz (d) and the standard spectrum Pr (d), as a calibration wavelength processing step, a wavelength for processing each of the received light spectra Pz (d) and Pr (d) is selected. The initial wavelength d is set, and the ideal absorption coefficient α (d) and the predetermined concentration nr of the standard spectrum Pr (d) at the initial wavelength d without the noise component obtained in the previous step are set.
【数55】Trs(d)=10−α(d)・nr
Trs(d):透過率
に代入し、迷光のノイズ成分量を含まない透過率Trs
(d)を算出する。[Mathematical formula-see original document] Trs (d) = 10- [ alpha] (d) * nr Trs (d): Substituted into the transmittance, the transmittance Trs does not include the noise component amount of stray light.
Calculate (d).
【0116】ここで、透過率Trs(d)は、濃度ゼロ
のゼロスペクトルPz(d)及び標準スペクトルPr
(d)から不明のノイズ成分量Pm(d)を夫々引くこ
とによりHere, the transmittance Trs (d) is the zero spectrum Pz (d) and the standard spectrum Pr at zero density.
By subtracting the unknown noise component amount Pm (d) from (d),
【数56】Trs(d)=(Pr(d)−Pm(d))
/(Pz(d)−Pm(d))
の関係式が成り立つので、この式を変形して(56) Trs (d) = (Pr (d) -Pm (d))
Since the relational expression of / (Pz (d) -Pm (d)) is established,
【数57】Trs(d)(Pz(d)−Pm(d))=
Pr(d)−Pm(d)(57) Trs (d) (Pz (d) -Pm (d)) =
Pr (d) -Pm (d)
【数58】Pm(d)=(Pr(d)−Trs(d)・
Pz(d))/(1−Trs(d))
とし、[数58]に対して、迷光のノイズ成分量を含ま
ない透過率Trs(d)の算出値、及び濃度ゼロのゼロ
スペクトルPz(d)の測定値及び標準スペクトルPr
(d)の測定値を夫々代入することにより、所定の時間
経過等により変化したノイズ成分量Pm(d)を求め、
校正する。(58) Pm (d) = (Pr (d) -Trs (d) ·
Pz (d)) / (1-Trs (d)), the calculated value of the transmittance Trs (d) that does not include the noise component amount of stray light and the zero spectrum Pz (0) of zero density with respect to [Equation 58]. d) Measured value and standard spectrum Pr
By substituting the measured values of (d) respectively, the noise component amount Pm (d) that has changed due to the passage of a predetermined time or the like is obtained,
Calibrate.
【0117】初期波長dでのノイズ成分量Pm(d)を
校正した後には、初期波長dに所定の波長幅Δdを加え
て他の所定波長dと設定し、図3に示す如く、処理手順
を校正用波長設定段階に戻し、以下、同様な処理を行な
い、他の所定波長dでのノイズ成分量Pm(d)を校正
する。After the noise component amount Pm (d) at the initial wavelength d is calibrated, a predetermined wavelength width Δd is added to the initial wavelength d to set another predetermined wavelength d, and as shown in FIG. Is returned to the calibration wavelength setting stage, and the same processing is performed thereafter to calibrate the noise component amount Pm (d) at another predetermined wavelength d.
【0118】このように、所定波長dに徐々に所定の波
長幅Δdを加えて同様な処理を行うことにより各波長に
おける校正したノイズ成分量Pm(d)を集積し、増加
する所定波長dが所定の範囲を超えた時点で処理を停止
し、通常計測段階に移行する。As described above, by gradually adding the predetermined wavelength width Δd to the predetermined wavelength d and performing the same processing, the calibrated noise component amount Pm (d) at each wavelength is integrated to increase the predetermined wavelength d. The processing is stopped at the time when the predetermined range is exceeded, and the process shifts to the normal measurement stage.
【0119】通常計測段階を説明すると、図4に示す如
く、組成比が不明である混合物質の計測スペクトルP
(d)を採取して測定する。ここで、混合物質を構成す
る組成物は、組成比が異なってもよいが、検量線を作成
した混合物質の組成物と略同じである必要がある。The normal measurement step will be described. As shown in FIG. 4, the measurement spectrum P of the mixed substance whose composition ratio is unknown is shown.
(D) is sampled and measured. Here, the composition of the mixed substance may be different in composition ratio, but it is necessary that the composition is substantially the same as the composition of the mixed substance for which the calibration curve is prepared.
【0120】計測スペクトルP(d)を測定した後に
は、各受光スペクトルP(d)、Pz(d)を処理する
波長を選択するよう計測用波長処理段階として初期波長
dを設定し、組成比が不明である混合物質の計測スペク
トルP(d)及びゼロスペクトルPz(d)から、校正
したノイズ成分量Pm(d)を夫々引くことによりAfter the measurement spectrum P (d) is measured, the initial wavelength d is set as the measurement wavelength processing step so that the wavelengths for processing the respective light reception spectra P (d) and Pz (d) are set, and the composition ratio is set. By subtracting the calibrated noise component amount Pm (d) from the measured spectrum P (d) and the zero spectrum Pz (d) of the mixed substance whose
【数59】As(d)=log((Pz(d)−Pm
(d))/(P−Pm(d)))
As(d):校正した吸光度
の式を作成し、[数59]に対して、校正したノイズ成
分量Pm(d)の算出値、ゼロスペクトルPz(d)の
測定値及び計測スペクトルPの測定値を夫々代入するこ
とにより、初期波長dでの校正した吸光度As(d)を
算出する。As (d) = log ((Pz (d) −Pm
(D)) / (P-Pm (d))) As (d): A calibrated absorbance formula is created, and the calculated value of the calibrated noise component amount Pm (d) is zero with respect to [Equation 59]. The calibrated absorbance As (d) at the initial wavelength d is calculated by substituting the measured value of the spectrum Pz (d) and the measured value of the measured spectrum P, respectively.
【0121】初期波長dでの校正した吸光度As(d)
を算出した後には、初期波長dに所定の波長幅Δdを加
えて他の所定波長dと設定し、図4に示す如く、処理手
順を計測用波長設定段階に戻し、以下、同様な処理を行
ない、他の所定波長dでの校正した吸光度As(d)を
算出する。Calibrated absorbance As (d) at initial wavelength d
After calculating, the predetermined wavelength width Δd is added to the initial wavelength d to set another predetermined wavelength d, and the processing procedure is returned to the measurement wavelength setting step as shown in FIG. Then, the calibrated absorbance As (d) at another predetermined wavelength d is calculated.
【0122】このように、所定波長dに徐々に所定の波
長幅Δdを加えて同様な処理を行うことにより各波長に
おける校正した吸光度As(d)を集積し、増加する所
定波長dが所定の範囲を超えた時点で処理を停止し、先
に求めた検量線を用いることによって、組成比が不明で
ある混合物質より所定物質の濃度nを算出する。As described above, the calibrated absorbance As (d) at each wavelength is accumulated by gradually adding the predetermined wavelength width Δd to the predetermined wavelength d and performing the same process, and the increasing predetermined wavelength d is set to the predetermined value. When the concentration exceeds the range, the treatment is stopped, and the concentration curve of the predetermined substance is calculated from the mixed substance whose composition ratio is unknown by using the previously obtained calibration curve.
【0123】ここで、検量線により混合物質中の所定物
質の濃度nを算出する過程を説明すると、所定物質の濃
度nは、検量線として[数54]で示す回帰ベクトルb
により、各波長における校正した吸光度As(d)から
[数52]と同様に下記の[数60]で求められる。Here, the process of calculating the concentration n of the predetermined substance in the mixed substance by the calibration curve will be described. The concentration n of the predetermined substance is the regression vector b shown in [Equation 54] as a calibration curve.
Thus, the calibrated absorbance As (d) at each wavelength can be obtained by the following [Equation 60] as in [Equation 52].
【0124】[0124]
【数60】 [Equation 60]
【0125】すなわち、下記の[数61]の如く、波長
の分割数Dとそれに対応した波長dの吸光度を回帰ベク
トルbから求めて演算することにより、組成比が不明で
ある混合物質より所定物質の濃度nを算出することがで
きる。That is, as shown in the following [Equation 61], the absorption number of the wavelength division number D and the wavelength d corresponding thereto is calculated from the regression vector b and calculated to calculate a predetermined substance from the mixed substance whose composition ratio is unknown. The concentration n of can be calculated.
【0126】[0126]
【数61】 [Equation 61]
【0127】混合物質の計測スペクトルP(d)より所
定物質の濃度nを求めた後には、連続分析として、組成
比が不明である混合物質を新たに採取して所定物質の濃
度を算出する段階に移行し、前の所定物質の濃度を算出
した時点から次の所定物質の濃度を算出した時点までの
経過時間を常に監視することよって、図3、図4に示す
如く、経過時間が、ノイズ成分量Pm(d)に変化を起
す所定時間の経過後ならば処理手順を校正段階へ戻し、
ノイズ成分量Pm(d)に変化を起す所定時間の経過前
ならば処理手順を通常計測段階へ戻す。更に、同様な処
理手順を繰り返して次の計測サンプルの濃度を算出し、
以後、未知の計測サンプルが無くなるまで同様の処理を
続ける。ここで、ノイズ成分量Pm(d)が変化する所
定時間は物質の種類等によって異なり、適宜設定する。After obtaining the concentration n of the predetermined substance from the measured spectrum P (d) of the mixed substance, a step of calculating a concentration of the predetermined substance by sampling a new mixed substance whose composition ratio is unknown as a continuous analysis By continuously monitoring the elapsed time from the time when the concentration of the previous predetermined substance is calculated to the time when the concentration of the next predetermined substance is calculated, as shown in FIGS. If a predetermined time that causes a change in the component amount Pm (d) has passed, the processing procedure is returned to the calibration stage,
If a predetermined time before the change in the noise component amount Pm (d) occurs, the processing procedure is returned to the normal measurement stage. Furthermore, the same processing procedure is repeated to calculate the concentration of the next measurement sample,
After that, the same processing is continued until there are no unknown measurement samples. Here, the predetermined time during which the noise component amount Pm (d) changes varies depending on the type of substance and the like, and is set appropriately.
【0128】以下、組成が不明である混合物質より所定
物質の濃度を算出する過程における種々の処理を実際に
示し、仮ノイズ成分量nPm(d)、相関係数R2、切
片b等を求めた例では、所定波長dを210nmとする
ことにより、仮ノイズ成分量nPm(d)をnPmと、
ノイズ成分量Pm(d)をPmと、ゼロスペクトルPz
(d)をPzと、受光スペクトル(計測スペクトル)P
(d)をPとして夫々示す。Hereinafter, various processes in the process of calculating the concentration of a predetermined substance from a mixed substance of which the composition is unknown will be actually shown, and the temporary noise component amount nPm (d), the correlation coefficient R 2 , the intercept b, etc. will be obtained. In the above example, by setting the predetermined wavelength d to 210 nm, the provisional noise component amount nPm (d) is nPm,
The noise component amount Pm (d) is Pm, and the zero spectrum Pz
(D) is Pz, and received light spectrum (measurement spectrum) P
(D) is shown as P, respectively.
【0129】(実施例1)SO2において迷光の仮ノイ
ズ成分量nPmを変えた場合を検量線により説明する
と、図6に示す如く、仮ノイズ成分量nPmを変化させ
た場合には、検量線の傾きが立ち上がり、ある値の仮ノ
イズ成分量nPmで検量線が略直線になることが明らか
である。又、この時の仮ノイズ成分量nPmを変化させ
た時の仮ノイズ成分量nPmと相関係数の二乗のR2と
の関係を示すと、図7、図8に示す如く、仮ノイズ成分
量nPmは所定位置(1560付近)に極大がある。こ
こで、図8は図7の極大値近傍の拡大図である。更に、
この時の仮ノイズ成分量nPmを変化させた時の切片b
の関係を示すと、図9に示す如く、bは所定位置でb=
0となる。従って、相関係数R2が極大値、bがゼロの
位置の場合に、仮ノイズ成分量nPmは実際のノイズ成
分量Pm(実際の迷光)になり、実際のノイズ成分量P
mを1560〜1570と推測し、且つ吸光係数αに相
当する傾きaを210nmで0.0149とする。更に
又、測定した受光スペクトルPにどの程度ノイズ成分量
Pmが含まれているかを示すと、図10に示す如く、各
波長においてゼロスペクトルPz及び受光スペクトルP
の下に所定量のノイズ成分量Pmが存在することが明ら
かである。(Embodiment 1) The case of changing the temporary noise component amount nPm of stray light in SO 2 will be described with reference to a calibration curve. As shown in FIG. 6, when the temporary noise component amount nPm is changed, the calibration curve is changed. It is clear that the slope of rises and the calibration curve becomes substantially linear with a certain value of the temporary noise component amount nPm. Further, when the relationship between the temporary noise component amount nPm when the temporary noise component amount nPm at this time is changed and the square of the correlation coefficient R 2 is shown, as shown in FIG. 7 and FIG. nPm has a maximum at a predetermined position (near 1560). Here, FIG. 8 is an enlarged view of the vicinity of the maximum value in FIG. Furthermore,
Intercept b when the temporary noise component amount nPm at this time is changed
As shown in FIG. 9, b is a predetermined position and b =
It becomes 0. Therefore, when the correlation coefficient R 2 is the maximum value and b is zero, the provisional noise component amount nPm becomes the actual noise component amount Pm (actual stray light), and the actual noise component amount P
It is assumed that m is 1560 to 1570, and the slope a corresponding to the extinction coefficient α is 0.0149 at 210 nm. Furthermore, when it is shown how much the noise component amount Pm is included in the measured light receiving spectrum P, as shown in FIG. 10, the zero spectrum Pz and the light receiving spectrum P are obtained at each wavelength.
It is clear that there is a predetermined amount of noise component amount Pm under.
【0130】(実施例2)同一の装置において意図的に
光学系の調整を行なって実際の迷光のノイズ成分量Pm
を変えた例を用いて説明すると、図11に示す如く、ノ
イズ成分量Pmを含む検量線は、迷光のノイズ成分量P
mの大きさに伴って湾曲が大きくなり、且つ傾きが変化
している。又、図11の検量線より各ノイズ成分量Pm
を取り除くと、図12の迷光大(ノイズ成分大)、図1
3の迷光中(ノイズ成分中)、図14の迷光小(ノイズ
成分小)に示す如く、検量線は、迷光の大きさ(ノイズ
成分量の大きさ)にかかわらず、略直線になり、傾きも
略一定になることが明らかである。(Embodiment 2) The noise component amount Pm of the actual stray light is adjusted by intentionally adjusting the optical system in the same device.
Using an example in which the difference is changed, as shown in FIG. 11, the calibration curve including the noise component amount Pm shows the noise component amount P of stray light.
The curvature increases and the inclination changes with the size of m. Also, from the calibration curve of FIG. 11, the noise component amount Pm
Is removed, stray light is large (noise component is large) in FIG.
3 stray light (in noise component) and small stray light (small noise component) in FIG. 14, the calibration curve becomes a substantially straight line regardless of the size of stray light (noise component amount) It is clear that also becomes almost constant.
【0131】(実施例3)SO2を含んだ混合物質(混
合ガス)において所定波長dに所定の波長幅Δdを加え
ることにより実際に200nmから350nmまで処理
し、SO2について多変量解析し、混合物質中のSO2
の吸光度等のデータを算出する。ここで[表2]は、複
数ある各組成比のうち3つ(濃度20ppm、60pp
m、100ppm)を示し、夫々の組成比には各波長の
うち3つ(200.52nm、200.77nm、20
1.02nm)を示す。Example 3 A mixed substance (mixed gas) containing SO 2 was actually processed from 200 nm to 350 nm by adding a predetermined wavelength width Δd to a predetermined wavelength d, and SO 2 was subjected to multivariate analysis, SO 2 in mixed substances
Calculate the data such as absorbance. Here, [Table 2] shows three of each composition ratio (concentration 20 ppm, 60 pp
m, 100 ppm), and each composition ratio has three wavelengths (200.52 nm, 20.77 nm, 20).
1.02 nm) is shown.
【0132】[0132]
【表2】 [Table 2]
【0133】この結果として、図15には、各波長にお
けるゼロスペクトルPz、ノイズ成分量Pm、受光スペ
クトル(計測スペクトル)Pを、図16には、各波長に
おける絶対的な吸光係数スペクトルを示す。又、多変量
解析により作成される検量線は各波長ごとに存在し、適
宜校正段階及び測定段階を介して図17に示す補正前の
吸光度スペクトルを、図18に示す補正後の吸光度スペ
クトルに修正する。As a result, FIG. 15 shows the zero spectrum Pz, the noise component amount Pm, and the received light spectrum (measurement spectrum) P at each wavelength, and FIG. 16 shows the absolute absorption coefficient spectrum at each wavelength. Further, the calibration curve created by the multivariate analysis exists for each wavelength, and the absorbance spectrum before correction shown in FIG. 17 is corrected to the absorbance spectrum after correction shown in FIG. 18 through the calibration step and the measurement step as appropriate. To do.
【0134】このように、校正段階において経過時間に
より変化するノイズ成分量を校正し、且つ校正したノイ
ズ成分量及び予め準備した検量線を用いることによっ
て、組成比が不明である混合物質から所定物質の濃度を
算出するので、ノイズ成分量が変化した場合であっても
再度検量線を作成することなく、容易に混合物質中の所
定物質の濃度を算出することができる。As described above, by calibrating the noise component amount which changes with the passage of time in the calibration stage and using the calibrated noise component amount and the calibration curve prepared in advance, a predetermined substance from a mixed substance whose composition ratio is unknown is calibrated. Since the concentration is calculated, it is possible to easily calculate the concentration of the predetermined substance in the mixed substance without creating a calibration curve again even when the amount of noise component changes.
【0135】又、連続的に混合物質中の所定物質の濃度
を算出する際に、前の所定物質の濃度を算出した時から
次の所定物質の濃度を算出する時までの時間経過に対応
して処理手順を変更するので、時間経過により変化する
ノイズ成分量を時間経過に対応して校正し、結果的に物
質の濃度を連続的に測定する連続分析を確実且つ精密に
行うことができる。In addition, when continuously calculating the concentration of a predetermined substance in a mixed substance, it corresponds to the passage of time from the time when the concentration of the previous predetermined substance is calculated to the time when the concentration of the next predetermined substance is calculated. Since the processing procedure is changed according to the passage of time, the amount of noise component that changes with the passage of time can be calibrated according to the passage of time, and as a result, continuous analysis for continuously measuring the concentration of the substance can be performed reliably and precisely.
【0136】更に、仮ノイズ成分量を介して線形回帰法
から算出された複数の相関係数もしくは複数の切片によ
り最適なものを選択して単一物質における所定波長の吸
光係数及びノイズ成分量を求め、且つ所定波長を変えて
同様に処理することにより他の所定波長の吸光係数及び
ノイズ成分量を求め、各波長の吸光係数及びノイズ成分
量を集積するので、単一物質における各波長の吸光係数
及びノイズ成分量を適確に求めることができる。Furthermore, an optimum one is selected from a plurality of correlation coefficients or a plurality of intercepts calculated from the linear regression method via the temporary noise component amount, and the absorption coefficient and the noise component amount of a predetermined wavelength in a single substance are selected. Obtain the absorption coefficient and the noise component amount of other predetermined wavelength by changing the predetermined wavelength and performing the same process, and accumulate the absorption coefficient and noise component amount of each wavelength. The coefficient and the amount of noise component can be accurately obtained.
【0137】更に又、単一物質より算出した各波長のノ
イズ成分量を用いることにより混合物質からノイズ成分
量を除いて各組成比での吸光度を算出し、且つ各データ
を用いて多変量解析することにより混合物質中の所定物
質の吸光度等のデータを算出するので、所定物質におけ
る各波長での複数の検量線を作成することができる。こ
こで、単一物質及び混合物質を測定する測定装置を同じ
にすることより単一物質に含まれる各波長のノイズ成分
量、及び混合物質に含まれる各波長のノイズ成分量が略
同じになるので、混合物質のノイズ成分量を単一物質の
ノイズ成分量により取り除くことができる。又、受光ス
ペクトルからノイズ成分量を取り除くので、高濃度で飽
和した検量線を修正し、高精度な直線で且つ再現性の高
い検量線を作成することができる。Furthermore, by using the noise component amount of each wavelength calculated from a single substance, the absorbance at each composition ratio is calculated by removing the noise component amount from the mixed substance, and the multivariate analysis is performed using each data. By doing so, the data such as the absorbance of the predetermined substance in the mixed substance is calculated, so that it is possible to create a plurality of calibration curves for each wavelength of the predetermined substance. Here, by using the same measuring device for measuring the single substance and the mixed substance, the amount of noise components of each wavelength contained in the single substance and the amount of noise component of each wavelength contained in the mixed substance become substantially the same. Therefore, the noise component amount of the mixed substance can be removed by the noise component amount of the single substance. Further, since the amount of noise components is removed from the received light spectrum, it is possible to correct a calibration curve saturated at high concentration and create a highly accurate calibration curve with high reproducibility.
【0138】なお、本発明の定量分析校正方法は上述し
た実施例のみに限定されるものではなく、本発明の要旨
を逸脱しない範囲内において種々変更を加え得ることは
勿論である。The quantitative analysis / calibration method of the present invention is not limited to the above-mentioned embodiment, and it goes without saying that various modifications can be made without departing from the scope of the present invention.
【0139】[0139]
【発明の効果】以上説明したように、本発明の定量分析
校正方法によれば、下記の如き、種々の優れた効果を奏
し得る。As described above, according to the quantitative analysis / calibration method of the present invention, various excellent effects as described below can be obtained.
【0140】I)請求項1によれば、校正段階において
経過時間により変化するノイズ成分量を校正し、且つ校
正したノイズ成分量及び予め準備した検量線を用いるこ
とによって、組成比が不明である混合物質から所定物質
の濃度を算出するので、ノイズ成分量が変化した場合で
あっても再度検量線を作成することなく、容易に混合物
質中の所定物質の濃度を算出することができる。I) According to claim 1, the composition ratio is unknown by calibrating the noise component amount which changes with the passage of time in the calibration stage and using the calibrated noise component amount and the calibration curve prepared in advance. Since the concentration of the predetermined substance is calculated from the mixed substance, even if the amount of the noise component changes, the concentration of the predetermined substance in the mixed substance can be easily calculated without creating a calibration curve again.
【0141】II)請求項2によれば、連続的に混合物
質中の所定物質の濃度を算出する際に、前の所定物質の
濃度を算出した時から次の所定物質の濃度を算出する時
までの時間経過に対応して処理手順を変更するので、時
間経過により変化するノイズ成分量を時間経過に対応し
て校正し、結果的に物質の濃度を連続的に測定する連続
分析を確実且つ精密に行うことができる。II) According to claim 2, when continuously calculating the concentration of the predetermined substance in the mixed substance, when calculating the concentration of the next predetermined substance from the time when the concentration of the previous predetermined substance is calculated Since the processing procedure is changed according to the passage of time, the amount of noise component that changes with the passage of time is calibrated according to the passage of time, and as a result, continuous analysis that continuously measures the concentration of the substance is ensured. Can be done with precision.
【0142】III)請求項3又は4によれば、仮ノイ
ズ成分量を介して線形回帰法から算出された複数の相関
係数もしくは複数の切片により最適なものを選択して単
一物質における所定波長の吸光係数及びノイズ成分量を
求め、且つ所定波長を変えて同様に処理することにより
他の所定波長の吸光係数及びノイズ成分量を求め、各波
長の吸光係数及びノイズ成分量を集積するので、単一物
質における各波長の吸光係数及びノイズ成分量を適確に
求めることができる。III) According to claim 3 or 4, the optimum one is selected from a plurality of correlation coefficients or a plurality of intercepts calculated from the linear regression method via the amount of temporary noise components, and a predetermined value in a single substance is selected. Since the absorption coefficient and the noise component amount of the wavelength are obtained and the predetermined wavelength is changed and the same processing is performed, the absorption coefficient and the noise component amount of the other predetermined wavelength are obtained, and the absorption coefficient and the noise component amount of each wavelength are integrated. The absorption coefficient and the amount of noise components of each wavelength in a single substance can be accurately obtained.
【0143】IV)請求項5によれば、単一物質より算
出した各波長のノイズ成分量を用いることにより混合物
質からノイズ成分量を除いて各組成比での吸光度を算出
し、且つ各データを用いて多変量解析することにより混
合物質中の所定物質の吸光度等のデータを算出するの
で、所定物質における各波長での複数の検量線を作成す
ることができる。又、受光スペクトルからノイズ成分量
を取り除くので、高濃度で飽和した検量線を修正し、高
精度な直線で且つ再現性の高い検量線を作成することが
できる。IV) According to claim 5, the absorbance at each composition ratio is calculated by removing the noise component amount from the mixed substance by using the noise component amount at each wavelength calculated from a single substance, and Since the data such as the absorbance of the predetermined substance in the mixed substance is calculated by performing a multivariate analysis using, it is possible to create a plurality of calibration curves for each wavelength of the predetermined substance. Further, since the amount of noise components is removed from the received light spectrum, it is possible to correct a calibration curve saturated at high concentration and create a highly accurate calibration curve with high reproducibility.
【図1】本発明の定量分析校正方法を実施する形態例を
示すフローである。FIG. 1 is a flow showing an example of an embodiment for carrying out the quantitative analysis calibration method of the present invention.
【図2】図1より連続するフローである。FIG. 2 is a continuous flow from FIG.
【図3】図2より連続して校正段階を示すフローであ
る。FIG. 3 is a flowchart showing a calibration step continuously from FIG.
【図4】図3より連続して通常計測段階を示すフローで
ある。FIG. 4 is a flowchart showing a normal measurement stage continuously from FIG.
【図5】多変量解析(PLS法)によるアルゴリズムを
示す図である。FIG. 5 is a diagram showing an algorithm based on multivariate analysis (PLS method).
【図6】SO2において迷光の仮ノイズ成分量を変えた
時の検量線を示す図である。FIG. 6 is a diagram showing a calibration curve when a temporary noise component amount of stray light is changed in SO 2 .
【図7】図6において仮ノイズ成分量を変化させた時の
仮ノイズ成分量と相関係数の二乗値との関係を示す図で
ある。7 is a diagram showing a relationship between the amount of temporary noise components and the square value of a correlation coefficient when the amount of temporary noise components is changed in FIG.
【図8】図7の極大値近傍を示す拡大図である。8 is an enlarged view showing the vicinity of the maximum value in FIG.
【図9】図6において仮ノイズ成分量を変化させた時の
切片の関係を示す図である。9 is a diagram showing a relation of intercepts when the amount of temporary noise components is changed in FIG.
【図10】測定した受光スペクトルにどの程度ノイズ成
分量が含まれているかを示す図である。FIG. 10 is a diagram showing to what extent a measured light reception spectrum includes a noise component amount.
【図11】同一の装置において意図的に光学系の調整を
行なって実際の迷光のノイズ成分量を変えた場合の検量
線の例を示す図である。FIG. 11 is a diagram showing an example of a calibration curve when the optical system is intentionally adjusted in the same device to change the actual noise component amount of stray light.
【図12】図11の迷光大(ノイズ成分大)の検量線に
おいて各ノイズ成分量を取り除いた時の検量線を示す図
である。12 is a diagram showing a calibration curve obtained by removing the amount of each noise component from the calibration curve of large stray light (large noise component) in FIG. 11;
【図13】図11の迷光中(ノイズ成分中)の検量線に
おいて各ノイズ成分量を取り除いた時の検量線を示す図
である。13 is a diagram showing a calibration curve when each noise component amount is removed from the calibration curve in stray light (in noise component) of FIG. 11;
【図14】図11の迷光小(ノイズ成分小)の検量線に
おいて各ノイズ成分量を取り除いた時の検量線を示す図
である。14 is a diagram showing a calibration curve when each noise component amount is removed from the calibration curve for small stray light (small noise component) in FIG. 11;
【図15】各波長におけるゼロスペクトル、ノイズ成分
量、受光スペクトル(計測スペクトル)を示す図であ
る。FIG. 15 is a diagram showing a zero spectrum, a noise component amount, and a light reception spectrum (measurement spectrum) at each wavelength.
【図16】各波長における絶対的な吸光係数スペクトル
を示す図である。FIG. 16 is a diagram showing an absolute absorption coefficient spectrum at each wavelength.
【図17】各波長における補正前の吸光度スペクトルを
示す図である。FIG. 17 is a diagram showing an absorbance spectrum before correction at each wavelength.
【図18】各波長における補正後の吸光度スペクトルを
示す図である。FIG. 18 is a diagram showing an absorbance spectrum after correction at each wavelength.
【図19】従来の波長210nmのSO2の検量線を示
す図である。FIG. 19 is a view showing a conventional calibration curve of SO 2 having a wavelength of 210 nm.
【図20】非分散分光分析の場合における迷光を示す概
略図である。FIG. 20 is a schematic diagram showing stray light in the case of non-dispersive spectroscopic analysis.
【図21】分光器使用の分光分析の場合における迷光を
示す概略図である。FIG. 21 is a schematic diagram showing stray light in the case of spectroscopic analysis using a spectroscope.
As(d) 吸光度 P(d) 受光スペクトル(計測スペクトル) Pm(d) 実際のノイズ成分量 nPm(d) 仮ノイズ成分量 Pr(d) 標準スペクトル Pz(d) ゼロスペクトル Trs(d) 透過率 α(d) 吸光係数 R2 相関係数 r 相関係数 a 傾き b 切片 d 所定波長(初期波長) n 濃度As (d) Absorbance P (d) Light receiving spectrum (measurement spectrum) Pm (d) Actual noise component amount nPm (d) Temporary noise component amount Pr (d) Standard spectrum Pz (d) Zero spectrum Trs (d) Transmittance α (d) extinction coefficient R 2 correlation coefficient r correlation coefficient a slope b intercept d predetermined wavelength (initial wavelength) n concentration
───────────────────────────────────────────────────── フロントページの続き (72)発明者 小林 健 東京都江東区豊洲三丁目1番15号 石川島 播磨重工業株式会社東京エンジニアリング センター内 (72)発明者 八木 武人 東京都江東区豊洲三丁目1番15号 石川島 播磨重工業株式会社東京エンジニアリング センター内 (72)発明者 小原 正孝 東京都千代田区大手町二丁目2番1号 石 川島播磨重工業株式会社本社内 Fターム(参考) 2G059 AA01 BB01 CC06 EE01 FF08 HH03 ─────────────────────────────────────────────────── ─── Continued front page (72) Inventor Ken Kobayashi 3-15 Toyosu, Koto-ku, Tokyo Ishikawajima Harima Heavy Industries Tokyo Engineering Co., Ltd. In the center (72) Inventor Takehito Yagi 3-15 Toyosu, Koto-ku, Tokyo Ishikawajima Harima Heavy Industries Tokyo Engineering Co., Ltd. In the center (72) Inventor Masataka Ohara 2-2-1 Otemachi, Chiyoda-ku, Tokyo Stone Kawashima Harima Heavy Industries Co., Ltd. F term (reference) 2G059 AA01 BB01 CC06 EE01 FF08 HH03
Claims (5)
Pm(d)を校正段階によって算出し、且つ組成比が不
明である混合物質より所定物質の濃度を通常計測段階に
よって算出する定量分析校正方法であって、 前記校正段階は、標準物質の濃度ゼロのゼロスペクトル
Pz(d)と所定濃度の標準スペクトルPr(d)とを
採取し、校正用波長設定段階として各受光スペクトルP
z(d)、Pr(d)の処理波長を所定波長に設定し、
前記標準スペクトルPr(d)の所定濃度と、予め求め
られたノイズ成分のない理想的な吸光係数とにより透過
率Trs(d)を計算し、ノイズ成分量Pm(d)を 【数1】 Pm(d)=(Pr(d)−Trs(d)・Pz(d))/(1−Trs(d) ) より求め、前記所定波長を他の所定波長に変えて処理手
順を校正用波長設定段階に戻すことにより同様の処理を
繰り返し、他の所定波長のノイズ成分量Pm(d)を算
出して各波長のノイズ成分量を集積し、 前記通常計測段階は、組成比が不明である混合物質より
計測スペクトルを採取し、計測用波長設定段階として各
受光スペクトルの処理波長を所定波長に設定し、前記計
測スペクトル及びゼロスペクトルPz(d)からノイズ
成分量Pm(d)を夫々引いて吸光度を算出し、前記所
定波長を他の所定波長に変えて処理手順を前記計測用波
長設定段階に戻すことにより同様の処理を繰り返し、他
の所定波長の吸光度を算出して各波長の吸光度を集積
し、予め混合物質から求められた検量線により、混合物
質中の所定物質の濃度を算出することを特徴とする定量
分析校正方法。1. A quantitative analysis calibration method for calculating a noise component amount Pm (d) that changes with the passage of time in a calibration step, and for calculating the concentration of a predetermined substance from a mixed substance whose composition ratio is unknown in a normal measurement step. In the calibration step, a zero spectrum Pz (d) of zero concentration of the standard substance and a standard spectrum Pr (d) of a predetermined concentration are sampled, and each received spectrum P is set as a calibration wavelength setting step.
Set the processing wavelengths of z (d) and Pr (d) to predetermined wavelengths,
The transmittance Trs (d) is calculated based on a predetermined concentration of the standard spectrum Pr (d) and an ideal extinction coefficient without a noise component obtained in advance, and the noise component amount Pm (d) is calculated as follows: (D) = (Pr (d) −Trs (d) · Pz (d)) / (1−Trs (d)), the predetermined wavelength is changed to another predetermined wavelength, and the processing procedure is set to the calibration wavelength. By repeating the same processing by returning to the stage, the noise component amount Pm (d) of another predetermined wavelength is calculated and the noise component amount of each wavelength is integrated, and in the normal measurement stage, the composition ratio is unknown. The measurement spectrum is sampled from the substance, the processing wavelength of each received spectrum is set to a predetermined wavelength as a measurement wavelength setting step, and the noise component amount Pm (d) is subtracted from the measurement spectrum and the zero spectrum Pz (d), respectively, to obtain the absorbance. And calculate By repeating the same process by changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the measurement wavelength setting step, the absorbances of other predetermined wavelengths are calculated and the absorbances of the respective wavelengths are accumulated, and the mixed substance is prepared in advance. A calibration method for quantitative analysis, characterized in that the concentration of a predetermined substance in a mixed substance is calculated from a calibration curve obtained from.
質の濃度を算出し且つ連続的に次の所定物質の濃度を算
出する際に、前の所定物質の濃度を算出してから次の所
定物質の濃度を算出するまでの時間間隔が所定時間を経
過している場合には処理手順を校正段階に戻し、前記時
間間隔が所定時間の経過する前の場合には処理手順を通
常計測段階に戻す請求項1記載の定量分析校正方法。2. When calculating the concentration of a predetermined substance from a mixed substance of which the composition ratio is unknown and continuously calculating the concentration of the next predetermined substance, after calculating the concentration of the previous predetermined substance, If the time interval until the concentration of the predetermined substance is calculated exceeds the predetermined time, the processing procedure is returned to the calibration step, and if the time interval is before the predetermined time has elapsed, the processing procedure is changed to the normal measurement step. The quantitative analysis calibration method according to claim 1.
の各受光スペクトルを採取し、単一物質用波長設定段階
として各受光スペクトルの処理波長を所定波長に設定
し、ノイズ成分量設定段階として前記ノイズ成分を濃度
ゼロの受光スペクトル又は所定濃度の受光スペクトルよ
り小さい任意の仮ノイズ成分量に仮設定し、前記仮ノイ
ズ成分量を濃度ゼロの受光スペクトル及び所定濃度の受
光スペクトルから夫々引いて各所定濃度の吸光度を算出
し、各所定濃度と吸光度の関係が直線に従うとして 【数2】Y=aX+b a:傾き b:切片 よりXに濃度、Yに吸光度を代入して線形回帰法により
相関係数を求め、続いて仮ノイズ成分量を他の仮ノイズ
成分量に変えて処理手順を前記ノイズ成分量設定段階に
戻すことにより同様の処理を繰り返して他の相関係数を
求め、各仮ノイズ成分量における複数の相関係数から最
も大きいものを選択することにより、選択された相関係
数に対応する傾きを所定波長の吸光係数と決定すると共
にノイズ成分量を決定し、更に前記所定波長を他の所定
波長に変えて処理手順を前記単一物質用波長設定段階に
戻すことにより同様の処理を繰り返して他の所定波長の
吸光係数及びノイズ成分量を夫々決定し、単一物質の受
光スペクトル中に含まれる各波長の吸光係数及び各波長
のノイズ成分量を集積する請求項1又は2記載の定量分
析校正方法。3. A light reception spectrum from zero concentration of a single substance to each predetermined concentration is sampled, and a processing wavelength of each light reception spectrum is set to a predetermined wavelength as a wavelength setting step for a single substance, and a noise component amount setting step is performed. As the noise component is temporarily set to a light-receiving spectrum of zero density or an arbitrary temporary noise component amount smaller than the light-receiving spectrum of a predetermined density, and the temporary noise component amount is subtracted from the light-receiving spectrum of zero density and the light-receiving spectrum of a predetermined density, respectively. The absorbance at each given concentration is calculated, and assuming that the relationship between each given concentration and the absorbance follows a straight line, Y = aX + b a: slope b: From the intercept, the concentration is substituted for X and the absorbance is substituted for Y to obtain a phase by linear regression method. The similar process is repeated by obtaining the relation number, then changing the temporary noise component amount to another temporary noise component amount, and returning the processing procedure to the noise component amount setting step. The correlation coefficient of is determined, and by selecting the largest one from the plurality of correlation coefficients in each temporary noise component amount, the slope corresponding to the selected correlation coefficient is determined as the absorption coefficient of the predetermined wavelength and the noise component The amount is determined, the same procedure is repeated by changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the wavelength setting step for the single substance, and the absorption coefficient and the noise component amount of the other predetermined wavelength are determined. The quantitative analysis calibration method according to claim 1 or 2, wherein the absorption coefficient of each wavelength and the amount of noise component of each wavelength included in the received light spectrum of a single substance are respectively determined and accumulated.
の各受光スペクトルを採取し、単一物質用波長設定段階
として各受光スペクトルの処理波長を所定波長に設定
し、ノイズ成分量設定段階として前記ノイズ成分を濃度
ゼロの受光スペクトル又は所定濃度の受光スペクトルよ
り小さい任意の仮ノイズ成分量に仮設定し、前記仮ノイ
ズ成分量を濃度ゼロの受光スペクトル及び所定濃度の受
光スペクトルから夫々引いて各所定濃度の吸光度を算出
し、各所定濃度と吸光度の関係が直線に従うとして 【数3】Y=aX+b a:傾き b:切片 よりXに濃度、Yに吸光度を代入して線形回帰法により
切片を求め、続いて仮ノイズ成分量を他の仮ノイズ成分
量に変えて処理手順を前記ノイズ成分量設定段階に戻す
ことにより同様の処理を繰り返して他の切片を求め、各
仮ノイズ成分量における複数の切片から最もゼロに近い
ものを選択することにより、選択された切片に対応する
傾きを所定波長の吸光係数と決定すると共にノイズ成分
量を決定し、更に前記所定波長を他の所定波長に変えて
処理手順を前記単一物質用波長設定段階に戻すことによ
り同様の処理を繰り返して他の所定波長の吸光係数及び
ノイズ成分量を夫々決定し、単一物質の受光スペクトル
中に含まれる各波長の吸光係数及び各波長のノイズ成分
量を集積する請求項1又は2記載の定量分析校正方法。4. A light receiving spectrum from zero concentration of a single substance to each predetermined concentration is sampled, and a processing wavelength of each light receiving spectrum is set to a predetermined wavelength as a wavelength setting step for a single substance, and a noise component amount setting step is performed. As the noise component is temporarily set to a light-receiving spectrum of zero density or an arbitrary temporary noise component amount smaller than the light-receiving spectrum of a predetermined density, and the temporary noise component amount is subtracted from the light-receiving spectrum of zero density and the light-receiving spectrum of a predetermined density, respectively. The absorbance at each given concentration is calculated, and assuming that the relationship between each given concentration and the absorbance follows a straight line, Y = aX + b a: slope b: From the intercept, the concentration is substituted for X and the absorbance is substituted for Y Then, the temporary noise component amount is changed to another temporary noise component amount, and the processing procedure is returned to the noise component amount setting step to repeat the same processing, Obtain the piece, by selecting the one that is closest to zero from the plurality of intercepts in each temporary noise component amount, determine the slope corresponding to the selected intercept as the absorption coefficient of the predetermined wavelength and determine the noise component amount, Further, by changing the predetermined wavelength to another predetermined wavelength and returning the processing procedure to the single substance wavelength setting step, the same processing is repeated to determine the absorption coefficient and the noise component amount of the other predetermined wavelength, respectively. 3. The quantitative analysis calibration method according to claim 1, wherein the absorption coefficient of each wavelength and the amount of noise components of each wavelength included in the received light spectrum of one substance are integrated.
び組成比を変えた複数の受光スペクトルを採取し、混合
物質用波長設定段階として各受光スペクトルの処理波長
を所定波長に設定し、予め単一物質より算出した所定波
長のノイズ成分量を濃度ゼロの受光スペクトル及び各組
成比の受光スペクトルから夫々引くことにより各組成比
での所定波長の吸光度を算出し、前記所定波長を他の所
定波長に変えて処理手順を前記混合物質用波長設定段階
に戻すことにより同様の処理を繰り返して各組成比での
他の所定波長の吸光度を夫々算出し、各波長での吸光度
及び各組成比のデータを用いて多変量解析することによ
り混合物質中の所定物質の検量線を作成することを特徴
とする請求項1、2、3又は4記載の定量分析校正方
法。5. A light-receiving spectrum of a mixed substance having a zero concentration and a plurality of light-receiving spectra having different composition ratios are sampled, and a processing wavelength of each light-receiving spectrum is set to a predetermined wavelength as a wavelength setting step for the mixed substance, and a single wavelength is set beforehand. Calculate the absorbance of the predetermined wavelength at each composition ratio by subtracting the amount of the noise component of the predetermined wavelength calculated from the substance from the received spectrum of zero concentration and the received spectrum of each composition ratio, and the predetermined wavelength to other predetermined wavelength By repeating the same procedure by returning the treatment procedure to the wavelength setting step for the mixed substance, the absorbance at each other predetermined wavelength at each composition ratio is calculated, and the absorbance at each wavelength and the data of each composition ratio are calculated. 5. The quantitative analysis calibration method according to claim 1, 2, 3 or 4, wherein a calibration curve of a predetermined substance in the mixed substance is created by performing multivariate analysis.
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| WO2016035626A1 (en) * | 2014-09-05 | 2016-03-10 | 株式会社分光科学研究所 | Spectroscopic quantification method, and spectroscopic quantification device and program |
| JP2016057065A (en) * | 2014-09-05 | 2016-04-21 | 株式会社分光科学研究所 | Spectral quantification method, spectral quantification apparatus and program |
| US9791373B2 (en) | 2014-09-05 | 2017-10-17 | Spectroscopic Science Laboratory Co., Ltd. | Method for quantitative spectrometry, quantitative spectrometry apparatus, and program |
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