JP2007187594A - Correction method of calibration curve - Google Patents

Correction method of calibration curve Download PDF

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JP2007187594A
JP2007187594A JP2006006930A JP2006006930A JP2007187594A JP 2007187594 A JP2007187594 A JP 2007187594A JP 2006006930 A JP2006006930 A JP 2006006930A JP 2006006930 A JP2006006930 A JP 2006006930A JP 2007187594 A JP2007187594 A JP 2007187594A
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spectrum
optical path
path length
sample
calibration curve
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JP4974042B2 (en
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Masahiro Watari
正博 渡
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Yokogawa Electric Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a correction method of a calibration curve which fixes a reference spectrum to predict the optical path length from a sample spectrum and corrects the spectrum, using the predicted optical path length that can neglect the fluctuations due to the individual differences of vials. <P>SOLUTION: On the basis of the sample spectrum measured by the vial or cell known in its optical path length, the ratio of the specific wave number ranges of the reference spectrum, and the measured spectrum is calculated by the method of least squares to determine the measuring optical path length, while the measured spectrum is converted into a spectrum measured by using the same optical path length as the reference spectrum to form the calibration curve. The ratio of the specific wave number range of the spectrum of an unknown sample to that of the reference spectrum is calculated by the method of least squares, to deduce the optical path length; and after the optical path length has been converted into the spectrum of a reference optical path length, the concentration and properties of the sample are deduced by using a preliminarily produced calibration curve. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

本発明は、近赤外線分光分析計の検量線補正方法に関し、バイアル瓶に採取したサンプルから得たスペクトルを使用して検量線を作成し、次にバイアル瓶に採取した未知サンプルの濃度または性状値を予測するに際し、バイアル瓶の個体差によるスペクトルのばらつきにより検量線を用いた予測値のばらつきを補正する方法に関するものである。   The present invention relates to a calibration curve correction method for a near-infrared spectrometer, a calibration curve is created using a spectrum obtained from a sample collected in a vial, and then the concentration or property value of an unknown sample collected in a vial The present invention relates to a method for correcting the variation in the predicted value using the calibration curve due to the variation in the spectrum due to the individual difference of the vials.

近年、化学、石油、生化学又は製薬、さらには食品分野など多岐にわたりその製造プロセス管理や品質管理を従来の化学分析法に代り近赤外分光分析方式に導入又は移行するための検討がなされている。
従来、製造プロセス管理や品質管理は分析室内での化学分析(滴定法)によるオフライン管理により行われてきた。
In recent years, studies have been made to introduce or shift manufacturing process control and quality control to near-infrared spectroscopy instead of conventional chemical analysis methods in a wide variety of fields such as chemical, petroleum, biochemical or pharmaceutical, and even food. Yes.
Conventionally, manufacturing process management and quality control have been performed by off-line management by chemical analysis (titration method) in an analysis chamber.

しかし、滴定法による定量分析は前処理に時間がかかり、また要求精度が高いことから滴定者には熟練と経験が要求され、更に分析に試薬を使用するので環境汚染につながるという問題がある。   However, the quantitative analysis by the titration method has a problem that it takes time for pretreatment and requires high accuracy, so that the titrator requires skill and experience, and further uses a reagent for analysis, leading to environmental pollution.

使い捨てのバイアル瓶を使用した近赤外分光分析計のサンプル測定は、簡便、安価であり、サンプルを搬送することも容易であるため、サンプル測定の主流となる可能性を有している。
図16はバイアル瓶に採取したサンプルを近赤外分光分析計を用いてサンプルのスペクトルを測定するための一例を示す図である。
Sample measurement of a near-infrared spectrometer using a disposable vial is simple and inexpensive, and since it is easy to transport a sample, it has the possibility of becoming the mainstream of sample measurement.
FIG. 16 is a diagram showing an example for measuring the spectrum of a sample collected in a vial using a near-infrared spectrometer.

図において、1は測定用ホルダであり、このホルダの中央付近にはバイアル(ここでは測定サンプルを入れる小型のガラス瓶を意味している。以下単にバイアルという)を挿入するバイアル挿入孔1aが形成され、この孔にサンプルを入れたバイアルを挿入して測定を行う。なお、この孔1aの周囲には複数個(図では6個)の予熱用バイアルを挿入するための予熱用バイアル挿入孔1bが形成されている。   In the figure, reference numeral 1 denotes a measurement holder, and a vial insertion hole 1a for inserting a vial (herein, a small glass bottle into which a measurement sample is put; hereinafter simply referred to as a vial) is formed near the center of the holder. Then, a vial containing a sample is inserted into the hole to perform measurement. A preheating vial insertion hole 1b for inserting a plurality (six in the figure) of preheating vials is formed around the hole 1a.

2はホルダ1を所定の温度に維持するための温調器である。また、このホルダ1の側面には近赤外光(以下、単に光という)を透過するための光透過孔1cが形成されており、この孔1cから入射した光はバイアルの中央部を貫通して検出器3に達するように構成されている。   Reference numeral 2 denotes a temperature controller for maintaining the holder 1 at a predetermined temperature. Further, a light transmission hole 1c for transmitting near infrared light (hereinafter simply referred to as light) is formed on the side surface of the holder 1, and light incident from the hole 1c penetrates the central portion of the vial. And reaches the detector 3.

検出器3で光電変換された信号は信号変換器4に送られてA/D変換され、Ethenet等によりデータ処理部(パソコン)5に送られてスペクトル表示される。
図16(b)は上記バイアル挿入孔1aに挿入されるバイアル10の形状を示すもので、パイレックス(登録商標)ガラスにより外径(D)8,内径(d)約6,高さ40(mm)に形成されたポリプロピレン製蓋13付きのバイアルである。
The signal photoelectrically converted by the detector 3 is sent to the signal converter 4 for A / D conversion, and sent to the data processing unit (personal computer) 5 by Ethernet or the like for spectrum display.
FIG. 16 (b) shows the shape of the vial 10 inserted into the vial insertion hole 1a. The outer diameter (D) 8, the inner diameter (d) is about 6, and the height 40 (mm) is made of Pyrex (registered trademark) glass. ) Formed with a polypropylene lid 13.

このようなバイアルは試料11を少量採取してサンプルテストを行うためのもので、取り扱いが簡単であり、図16aに示すバイアル瓶挿入孔に挿入するだけでよいので、手分析の場合に比較して迅速、正確に測定できるという特徴がある。   Such a vial is for collecting a small amount of the sample 11 and conducting a sample test. It is easy to handle and only needs to be inserted into the vial insertion hole shown in FIG. 16a. It can be measured quickly and accurately.

ところで、このような測定装置においては、サンプルの測定に際し多数のバイアルを使用する。そのためバイアル瓶のばらつきにより、検量線出力が変動するという問題がある。図16cはバイアルの実効光路長を説明するための断面図である。先に示したバイアルの外径は8mm、内径は約6mmであるが実際に透過する光は所定の太さの径を有しており、6mmの実効光路長を有しているとはいえない。しかし、バイアルの実効長を機械的に測定することは困難である。   By the way, in such a measuring apparatus, a large number of vials are used for measuring a sample. Therefore, there is a problem that the calibration curve output fluctuates due to variations in vials. FIG. 16c is a cross-sectional view for explaining the effective optical path length of the vial. The vial shown above has an outer diameter of 8 mm and an inner diameter of about 6 mm, but the actually transmitted light has a diameter of a predetermined thickness and cannot be said to have an effective optical path length of 6 mm. . However, it is difficult to mechanically measure the effective length of the vial.

本発明ではバイアルのばらつきによって生じる検量線の変動を、基準スペクトルを固定することでサンプルスペクトルから光路長を予測し、その予測光路長を使用してスペクトルを補正することでバイアルの個体差による変動を無視できる検量線の補正方法を提供することを目的とする。   In the present invention, fluctuations in the calibration curve caused by variations in vials are predicted by estimating the optical path length from the sample spectrum by fixing the reference spectrum, and correcting the spectrum using the predicted optical path length, thereby causing fluctuations due to individual differences in vials. An object of the present invention is to provide a calibration curve correction method that can ignore the above.

バイアルを用いた器差補正方法に関する先行技術として、例えば下記のようなものがある。   For example, the followings are related to the instrumental error correction method using a vial.

特開2001−41879号公報JP 2001-41879 A

このような課題を達成するために、本発明のうち請求項1記載の発明は、
光路長が既知のバイアル又はセルで測定したサンプルスペクトルを基準とし、
前記基準スペクトルと測定スペクトルの特定波数範囲の比を最小自乗法で求めて測定光路長を決定し、測定スペクトルを基準スペクトルと同じ光路長で測定したスペクトルに変換した後検量線を作成し、未知サンプルのスペクトルと基準スペクトルの特定波数範囲の比を最小自乗法で求めて光路長を推定し、基準光路長のスペクトルに変換した後、予め作成した検量線を使用してサンプルの濃度および性状を推定することを特徴とする。
In order to achieve such a problem, the invention according to claim 1 of the present invention is:
Based on the sample spectrum measured in a vial or cell with a known optical path length,
Determine the optical path length by calculating the ratio of the specific spectrum of the reference spectrum and the measured spectrum using the least square method, convert the measured spectrum to a spectrum measured with the same optical path length as the reference spectrum, create a calibration curve, and Estimate the optical path length by calculating the ratio of the specific spectrum of the sample spectrum to the specific spectrum using the least square method, convert it to the reference optical path length spectrum, and then use the calibration curve created in advance to determine the concentration and properties of the sample. It is characterized by estimating.

請求項2においては、請求項1記載の検量線作成方法において、
前記基準スペクトルを採用し基準スペクトルと測定スペクトルの比から求めた測定光路長を推定し、表示および出力するようにしたことを特徴とする。
In claim 2, in the calibration curve creation method according to claim 1,
The measurement optical path length obtained from the ratio of the reference spectrum and the measured spectrum is estimated, displayed, and output by adopting the reference spectrum.

本発明によれば次のような効果がある。
請求項1,2に記載の発明によれば、
光路長が既知のバイアル又はセルで測定したサンプルスペクトルを基準とし、
前記基準スペクトルと測定スペクトルの特定波数範囲の比を最小自乗法で求めて測定光路長を決定し、測定スペクトルを基準スペクトルと同じ光路長で測定したスペクトルに変換した後検量線を作成し、未知サンプルのスペクトルと基準スペクトルの特定波数範囲の比を最小自乗法で求めて光路長を推定し、基準光路長のスペクトルに変換した後、予め作成した検量線を使用してサンプルの濃度および性状を推定したので、バイアル瓶の個体差による検量線の予測誤差のばらつきを補正し、再現性がよく安定した予測が可能である。
The present invention has the following effects.
According to invention of Claim 1, 2,
Based on the sample spectrum measured in a vial or cell with a known optical path length,
Determine the optical path length by calculating the ratio of the specific spectrum of the reference spectrum and the measured spectrum using the least square method, convert the measured spectrum to a spectrum measured with the same optical path length as the reference spectrum, create a calibration curve, and Estimate the optical path length by calculating the ratio of the specific spectrum of the sample spectrum to the specific spectrum using the least square method, convert it to the reference optical path length spectrum, and then use the calibration curve created in advance to determine the concentration and properties of the sample. Since the estimation is made, it is possible to correct the variation in the prediction error of the calibration curve due to the individual difference of the vials, and to make a stable prediction with good reproducibility.

図1は本発明の実施形態の一例を示す検量線補正方法のフローチャートである。
はじめに工程aにおいてサンプルのスペクトル測定を行う(測定結果はメモリに格納する)。
次に、工程bにおいて、標準光路長を持つバイアルに入れたサンプルのスペクトルと比較し、特定波数範囲で標準スペクトルと相関を取る。
FIG. 1 is a flowchart of a calibration curve correction method showing an example of an embodiment of the present invention.
First, in step a, the spectrum of the sample is measured (the measurement result is stored in a memory).
Next, in step b, the sample is compared with the spectrum of a sample placed in a vial having a standard optical path length, and is correlated with the standard spectrum in a specific wave number range.

次に工程cにおいて、工程2で求めた相関から実効光路長を計算する。
次に工程dにおいて、計算した実効光路長と予め定めていた所定の光路長と比較して正常/異常を判定する(一定の閾値より外れている場合は異常と判断し表示する)。
次に工程eにおいてスペクトルの光路長を補正する。
次に工程fにおいて、検量線の計算を行う。
次に工程gにおいて工程fで求めた検量線を用いて成分/性状の予測値を出力する。
Next, in step c, the effective optical path length is calculated from the correlation obtained in step 2.
Next, in step d, normality / abnormality is determined by comparing the calculated effective optical path length with a predetermined optical path length determined in advance (if it is outside a certain threshold, it is determined to be abnormal and displayed).
Next, in step e, the optical path length of the spectrum is corrected.
Next, in step f, a calibration curve is calculated.
Next, in step g, the predicted value of the component / property is output using the calibration curve obtained in step f.

図2は図16に示したような近赤外線分光分析装置を用い、光路長の異なる3種類(2,5,10mm)のキュベットおよび外径8mm,内径約6mm,長さ40mmのバイアルを用いて100%トルエンの吸光度を測定したものである。図において横軸は波数、縦軸は吸光度を示している。なお、図2(b)はキュベットの形状を示すもので、光路長としての厚さmを2,5,10mmと変化させたものを使用する。   FIG. 2 uses a near-infrared spectrometer as shown in FIG. 16, using three types (2, 5, 10 mm) of cuvettes having different optical path lengths, and a vial having an outer diameter of 8 mm, an inner diameter of about 6 mm, and a length of 40 mm. The absorbance of 100% toluene is measured. In the figure, the horizontal axis represents the wave number, and the vertical axis represents the absorbance. FIG. 2 (b) shows the shape of the cuvette, and the one with the thickness m as the optical path length changed to 2, 5, and 10 mm is used.

図2において、5650cm−1の波数に注目すると2mmのキュベットの吸光度はおよそ0.28となっており、5mmのキュベットの吸光度は2mmのキュベットの2.5倍のおよそ0.7となっている。また、10mmのキュベットの吸光度は2mmのキュベットの5倍のおよそ1.4となっており、直線的な比例関係にあることがわかる。そして、ここで用いた内径約6mmのバイアルの吸光度はおよそ0.8であることが分かる。
これらキュベットの吸光度の比例関係とバイアルの吸光度からバイアルの実効光路長を推定することができる。
In FIG. 2, when attention is paid to the wave number of 5650 cm −1 , the absorbance of the 2 mm cuvette is about 0.28, and the absorbance of the 5 mm cuvette is about 0.7, which is 2.5 times that of the 2 mm cuvette. . Further, the absorbance of the 10 mm cuvette is about 1.4, which is five times that of the 2 mm cuvette, and it can be seen that there is a linear proportional relationship. And it turns out that the light absorbency of the vial with an internal diameter of about 6 mm used here is about 0.8.
The effective optical path length of the vial can be estimated from the proportional relationship between the absorbance of the cuvette and the absorbance of the vial.

このように光路長が既知の一個のキュベット又はバイアルを用いてあるサンプルのスペクトルを測定し、特定波数あるいは特定波数範囲の吸光度から検量線を作成し、この検量線に基づいてサンプルの特性を測定すれば正確な分析結果を得ることができる。
しかしながら、実際のサンプル測定では数十から百を超えるサンプルを採取して検量線を作成するのでサンプルの出し入れに手間がかかり、また、コンタミが起きやすいという問題があった。
In this way, the spectrum of a sample is measured using a single cuvette or vial with a known optical path length, a calibration curve is created from the absorbance in a specific wavenumber or a specific wavenumber range, and the characteristics of the sample are measured based on this calibration curve. By doing so, accurate analysis results can be obtained.
However, in actual sample measurement, since a calibration curve is created by collecting several tens to a hundred samples, it takes time to put in and take out the sample, and there is a problem that contamination is likely to occur.

そのため価格の安いバイアルを用いて使い捨てでスペクトルを測定し検量線を作成できればよいが、バイアルの光路長には製作ロット毎のばらつきや同じロットでも個体差があり、同じサンプルを異なるバイアルで測定すると予測結果がばらつくという問題があった。   Therefore, it is only necessary to measure the spectrum in a disposable manner using cheap vials, but there are variations in the optical path length of each vial and individual differences even in the same lot, and the same sample is measured in different vials. There was a problem that the prediction results varied.

図3は図16に示す赤外線分光分析装置と、図2で用いた波数と吸光度の関係を用い、ロットの異なる5種類(A〜E)のバイアルの中からそれぞれ1個のバイアルを抜き取って、図3(b)に示すように4方からそれぞれ3回測定し光路長を推定する工程を2度行い相関を調べた結果である。2度の推定に相関があり、光路長の推定が再現されていることがわかる。
ロットや個体差によりばらつきがあるが点線で示す直線イに対して相関関係があることが分かる。
3 uses the infrared spectroscopic analysis apparatus shown in FIG. 16 and the relationship between the wave number and the absorbance used in FIG. 2, and extracts one vial from each of five types (A to E) of different lots, As shown in FIG. 3 (b), it is a result of performing a process of estimating the optical path length by measuring three times from four directions twice and examining the correlation. It can be seen that there is a correlation between the two estimations and the estimation of the optical path length is reproduced.
It can be seen that there is a correlation with the straight line i shown by the dotted line, although there are variations due to lots and individual differences.

図4はロットA〜Eのそれぞれから80個をランダムに抽出して3回ずつ測定し、光路長のばらつきがどれほどあるかの頻度を調べたものである。図によれば6.48mmに中心があり、±約0.2mmのばらつきがあることが分かる。   FIG. 4 shows 80 samples randomly extracted from each of the lots A to E, measured three times, and examined how often the optical path length varies. According to the figure, it can be seen that there is a center at 6.48 mm and there is a variation of ± about 0.2 mm.

図5はトルエン中に7%のイソプロピルアルコールをいれて図15に示す近赤外線分光分析装置を用いてスペクトル変化を測定したもので、イ,ロで示す部分はスペクトルの変化の大きなイ’,ロ’部分を拡大したものである。イソプロピルアルコールの濃度に応じてスペクトルの吸光度が変化していることがわかる(図5は図1で示すフローチャートの工程(a)のスペクトル測定に相当する)。   FIG. 5 shows a spectrum change measured by using 7% isopropyl alcohol in toluene and the near-infrared spectroscopic analyzer shown in FIG. 'The part is enlarged. It can be seen that the absorbance of the spectrum changes according to the concentration of isopropyl alcohol (FIG. 5 corresponds to the spectrum measurement in step (a) of the flowchart shown in FIG. 1).

図6はロットAを使用してそれぞれのバイアルを3回ずつ測定し検量線を作成した一例を示すもので、横軸はリファレンスIPA濃度、縦軸は予測IPA濃度である。
なお、リファレンスIPA濃度は重量%で、溶媒(トルエン)とIPAの重量比より算出したものである。
図7は図6に示す検量線を使用した他のロットを含むバイアル中のIPA濃度の予測結果を示すものである。図6と比較するとバイアル個体差による予測結果のばらつきがあることが分かる。
FIG. 6 shows an example in which a calibration curve was created by measuring each vial three times using lot A, where the horizontal axis represents the reference IPA concentration and the vertical axis represents the predicted IPA concentration.
The reference IPA concentration is% by weight and is calculated from the weight ratio of the solvent (toluene) and IPA.
FIG. 7 shows the predicted results of IPA concentration in vials containing other lots using the calibration curve shown in FIG. Compared to FIG. 6, it can be seen that there is a variation in the prediction result due to the individual vial difference.

図8(a〜d)は検量線作成に際し、前処理を施した場合と前処理を施さない場合の検量線予測結果とロット間のばらつきを示す図である。なお、検量線作成に使用したバイアルはロットAを用いた。   FIGS. 8A to 8D are diagrams showing the calibration curve prediction result and the variation between lots when pre-processing is performed and when pre-processing is not performed when creating a calibration curve. The lot A was used as the vial used for preparing the calibration curve.

図8(a)は前処理なしでSEPが0.0929の場合のばらつきの度合いを示す図である。横軸はイソプロピルアルコール濃度(%)のラボ値に対する検量線を使用した予測値のばらつき、縦軸は頻度(測定された回数)を示している。ここで、SEP(Standard Error Prediction)とは予測したサンプル濃度とラボ値の標準偏差である。   FIG. 8A is a diagram showing the degree of variation when the SEP is 0.0929 without preprocessing. The horizontal axis represents the variation of the predicted value using the calibration curve with respect to the laboratory value of isopropyl alcohol concentration (%), and the vertical axis represents the frequency (number of times measured). Here, SEP (Standard Error Prediction) is the standard deviation of the predicted sample concentration and laboratory value.

図8(a)によれば、ばらつきが大きく標準偏差は0.0783であった。ここで標準偏差とは、各サンプルの予測値の平均値を取り、それを各予測値から引いたデータの標準偏差を取ったものである。   According to Fig.8 (a), the dispersion | variation was large and the standard deviation was 0.0783. Here, the standard deviation is a value obtained by taking an average value of predicted values of each sample and taking a standard deviation of data obtained by subtracting the average value from each predicted value.

図8(b)は前処理として2次微分を施したもので、SEPが0.0929の場合のばらつきの度合いを示す図である。この場合の標準偏差は0.0727であった。
図8(c)は前処理としてMSC(Multi-Scattering−Correction・・・多重散乱補正・・・以下、単にMSCという)を施したもので、SEPが0.1143の場合のばらつきの度合いを示す図である。この場合の標準偏差は0.0317であった。
FIG. 8B is a diagram showing the degree of variation when the second differentiation is performed as the preprocessing and the SEP is 0.0929. The standard deviation in this case was 0.0727.
FIG. 8 (c) shows the degree of variation when the MSP (Multi-Scattering-Correction ... multiple scattering correction ... hereinafter simply referred to as MSC) is applied as pre-processing, and the SEP is 0.1143. FIG. The standard deviation in this case was 0.0317.

図8(d)は前処理として2次微分およびMSCを施したもので、SEPが0.0602の場合のばらつきの度合いを示す図である。この場合の標準偏差は0.0331であった。これらの図から、前処理として2次微分およびMSCを施したものがばらつきが小さくなることがわかる。   FIG. 8D is a diagram in which second order differentiation and MSC are performed as preprocessing, and the degree of variation when SEP is 0.0602. The standard deviation in this case was 0.0331. From these figures, it can be seen that the variation obtained by performing the second order differentiation and the MSC as the preprocessing is reduced.

図9,図10は2次微分検量線による他のロットのバイアルを含む予測結果の効果を示すもので、図9は図8(b)の2次微分を施した状態、図10は2次微分およびMSCを施した状態を示している。なお、横軸はリファレンスIPA濃度、縦軸は予測IPA濃度である。これらの図によれば、MSCを施したもの(図10)がばらつきが小さいことがわかる。   9 and 10 show the effect of the prediction result including the vials of other lots by the second-order differential calibration curve. FIG. 9 shows the state after the second-order differentiation of FIG. 8B, and FIG. The state which performed differentiation and MSC is shown. The horizontal axis represents the reference IPA concentration, and the vertical axis represents the predicted IPA concentration. According to these figures, it can be seen that the MSC (FIG. 10) has a small variation.

図11(a)は標準スペクトルの吸光度と各サンプルの吸光度比の関係を示すもので、図11(b)に示すようなIPAの濃度により大きく変化する波数範囲を用いたものである。図11(b)において横軸は波数、縦軸は吸光度を示している。   FIG. 11A shows the relationship between the absorbance of the standard spectrum and the absorbance ratio of each sample, and uses a wave number range that varies greatly depending on the concentration of IPA as shown in FIG. 11B. In FIG. 11B, the horizontal axis indicates the wave number, and the vertical axis indicates the absorbance.

図12(a)は図11と同様標準スペクトルの吸光度と各サンプルスペクトルの吸光度比の関係を示す図である。
図11と図12を比較すると図12の方がばらつきも少なく、相関もよいことがわかる。
図11に示す直線の式
y=0.9902x+0.0043
r(相関係数)=0.9994
および図12に示す直線の式
y=0.9986x+0.0033
r(相関係数)=0.9998
は最小自乗法を用いて求めたサンプルスペクトルと標準スペクトルの相関で、y=ax+bのaに相当する値は標準スペクトルとサンプルスペクトルの光路比を示している。
FIG. 12A shows the relationship between the absorbance of the standard spectrum and the absorbance ratio of each sample spectrum, as in FIG.
Comparing FIG. 11 and FIG. 12, it can be seen that FIG. 12 has less variation and good correlation.
Linear equation shown in FIG.
y = 0.9902x + 0.0043
r (correlation coefficient) = 0.9994
And the linear equation shown in FIG.
y = 0.9986x + 0.0033
r (correlation coefficient) = 0.9998
Is the correlation between the sample spectrum and the standard spectrum obtained using the least square method, and the value corresponding to a in y = ax + b represents the optical path ratio between the standard spectrum and the sample spectrum.

図12(b)に示すように、ここではIPAの濃度による変化が少ない波数範囲を使用した。図11に比較してばらつきが小さく相関も良好であることがわかる(図12は図1で示すフローチャートの工程(b)の標準スペクトル測定と相関を取る工程に相当する)。   As shown in FIG. 12B, a wave number range in which the change due to the concentration of IPA is small is used here. Compared to FIG. 11, it can be seen that the variation is small and the correlation is good (FIG. 12 corresponds to the step of correlating with the standard spectrum measurement in step (b) of the flowchart shown in FIG. 1).

図11と図12の比較からMSCを使って光路長を予測する場合、サンプル濃度の影響を受けないスペクトル範囲を使用したほうが予測の安定性がよい。MSCでは標準のスペクトルとして検量線作成時のサンプルスペクトルの平均を使用する。   From the comparison between FIG. 11 and FIG. 12, when the optical path length is predicted using MSC, the stability of the prediction is better when the spectral range that is not affected by the sample concentration is used. In MSC, the average of the sample spectrum at the time of preparing the calibration curve is used as a standard spectrum.

そのため、検量線作成毎に平均スペクトルは変化して推定光路長に継続性がないという欠点があった。
そこで、予めパス長の既知のサンプルスペクトルを基準としてパス長補正量を計算する変形MSC法を提案する。
For this reason, the average spectrum changes every time a calibration curve is created, and there is a drawback that the estimated optical path length is not continuous.
Therefore, a modified MSC method is proposed in which the path length correction amount is calculated based on a sample spectrum whose path length is known in advance.

図13は既知光路長6.526mmのバイアルに入ったトルエン中にIPA3.283%が入ったサンプルスペクトルを基準にして予測した光路長と図2に示す純トルエンスペクトルから推定した光路長の相関を示すものである。   FIG. 13 shows the correlation between the optical path length estimated on the basis of a sample spectrum containing 3.283% IPA in toluene contained in a vial having a known optical path length of 6.526 mm and the optical path length estimated from the pure toluene spectrum shown in FIG. It is shown.

図13は2つの方法で求めた光路長の相関を示すもので、横軸はIPA濃度により変化するスペクトルから求めた予測光路長(mm)、縦軸はトルエンスペクトルから求めた予測光路長(mm)である。
図13は最小自乗法を用いて求めたIPA濃度が変化するサンプルスペクトルから求めた光路長とトルエンスペクトルから求めた光路長の相関を示すもので、r=0.912は相関係数を示している。
図13の結果は、トルエンを使用せずにサンプルスペクトルから光路長の予測が可能なことを示している。
FIG. 13 shows the correlation between the optical path lengths obtained by the two methods. The horizontal axis represents the predicted optical path length (mm) obtained from the spectrum varying with the IPA concentration, and the vertical axis represents the predicted optical path length (mm) obtained from the toluene spectrum. ).
FIG. 13 shows the correlation between the optical path length obtained from the sample spectrum obtained by changing the IPA concentration obtained using the method of least squares and the optical path length obtained from the toluene spectrum, and r = 0.912 represents the correlation coefficient. Yes.
The result of FIG. 13 shows that the optical path length can be predicted from the sample spectrum without using toluene.

図14はサンプルスペクトルから求めた光路長を使用してスペクトルを補正し、予測した結果を示すもので、光路長補正後のスペクトルを使用し2次微分検量線を作成し、他のロットバイアルを含む光路長補正スペクトルを予測した結果である。SEP(予測誤差)が0.056とロットによるばらつきが大きく減少していることが分かる。   FIG. 14 shows the result of correcting the spectrum using the optical path length obtained from the sample spectrum and showing the predicted result. Using the spectrum after optical path length correction, a secondary differential calibration curve was created, and other lot vials were prepared. It is the result of having predicted the optical path length correction spectrum including. It can be seen that the SEP (prediction error) is 0.056 and the variation among lots is greatly reduced.

図15は変形MSCの効果を示す図である。即ち図15(a)の上側の(イ)で示す線はサンプルスペクトルから予測した光路長を示し、図15(a)の(ロ)、(ハ)で示す線は変形MSCを用いたものと用いない場合のIPA予測値のばらつきの比較を示している。(ロ)で示す線は光路長補正無のIPA濃度の予測値、(ハ)で示す線は実効光路長を使用してスペクトルの補正をした後、検量線に当てはめIPA(イソプロピルアルコール)の予測値を計算したときのばらつきを示すものである。ばらつきが少なくなっていることが分かる。   FIG. 15 is a diagram showing the effect of the modified MSC. That is, the line indicated by (A) in the upper part of FIG. 15A indicates the optical path length predicted from the sample spectrum, and the lines indicated by (B) and (C) in FIG. 15A use the modified MSC. The comparison of the dispersion | variation in the IPA prediction value when not using is shown. The line indicated by (B) is the predicted value of the IPA concentration without optical path length correction, and the line indicated by (C) is the IPA (isopropyl alcohol) prediction that is applied to the calibration curve after correcting the spectrum using the effective optical path length. It shows the variation when the value is calculated. It can be seen that the variation is reduced.

図15(b)は検量線予測値のばらつきの比較を頻度表(ヒストグラム)にしたもので、変形MSCを使用した場合には使用しない場合に比較してばらつきが半分以下(σ=0.051→0.025)になっていることが分かる(図15(a)は図1で示すフローチャートの工程(g)に相当する)。   FIG. 15B is a frequency table (histogram) for comparing the variation of the calibration curve predicted values. When the modified MSC is used, the variation is less than half compared to the case where it is not used (σ = 0.051). → 0.025) (FIG. 15A corresponds to step (g) in the flowchart shown in FIG. 1).

なお、以上の説明は、本発明の説明および例示を目的として特定の好適な実施例を示したに過ぎない。本実施例では従って本発明は、上記実施例に限定されることなく、その本質から逸脱しない範囲で更に多くの変更、変形を含むものである。   The above description merely shows a specific preferred embodiment for the purpose of explanation and illustration of the present invention. Therefore, in the present embodiment, the present invention is not limited to the above embodiment, and includes many changes and modifications without departing from the essence thereof.

本発明の検量線補正方法のフローチャートである。It is a flowchart of the calibration curve correction method of the present invention. 異なる光路長によるトルエンスペクトルと光路長測定校正直線を示す図である。It is a figure which shows the toluene spectrum and optical path length measurement calibration straight line by different optical path lengths. ロットの異なるバイアルの中からそれぞれ1個のバイアルを抜き取って4方からそれぞれ各3回測定し光路長を推定する工程を2回行い推定光路長の相関を調べた結果を示す図であるIt is a figure which shows the result of having extracted one vial each from the vial from which a lot differs, and measuring the correlation of the estimated optical path length twice by measuring twice each from 4 directions and estimating the optical path length twice. 実効光路長とばらつきの関係を示す図である。It is a figure which shows the relationship between effective optical path length and dispersion | variation. トルエン中に7%のイソプロピルアルコールをいれてスペクトル変化を測定した結果を示す図である。It is a figure which shows the result of having put 7% isopropyl alcohol in toluene and measuring a spectrum change. ロットAを使用してバイアルの中のスペクトルを3回ずつ測定し検量線を作成した一例を示す図である。It is a figure which shows an example which measured the spectrum in a vial 3 times using lot A, and created the calibration curve. 図6に示す検量線を使用した他のロットを含むバイアル中のIPA濃度の予測結果を示す図である。It is a figure which shows the prediction result of the IPA density | concentration in the vial containing the other lot using the calibration curve shown in FIG. 図8検量線作成に際し、前処理を施した場合と前処理を施さない場合の検量線予測結果を示す図である8 is a diagram showing a calibration curve prediction result when pre-processing is performed and when pre-processing is not performed when creating a calibration curve. 2次微分検量線による他のロットのバイアルを含むサンプルの予測結果を示す図である。It is a figure which shows the prediction result of the sample containing the vial of another lot by a secondary differential calibration curve. 2次微分およびMSCを施した状態を示す図である。It is a figure which shows the state which gave the secondary differentiation and MSC. 標準スペクトルの吸光度と各サンプルの吸光度比の関係を示す図である。It is a figure which shows the relationship between the light absorbency of a standard spectrum, and the light absorbency ratio of each sample. 標準スペクトルの吸光度と各サンプルスペクトルの吸光度比の関係を示す図である。It is a figure which shows the relationship between the light absorbency of a standard spectrum, and the light absorbency ratio of each sample spectrum. 2つの方法で求めた光路長の相関を示す図である。It is a figure which shows the correlation of the optical path length calculated | required by two methods. サンプルスペクトルから求めた光路長を使用してスペクトルを補正し、予測した結果を示す図である。It is a figure which shows the result of having corrected a spectrum using the optical path length calculated | required from the sample spectrum, and having estimated. 変形MSC法を使用した光路長の推定値と変形MSC法を使用して補正した場合としない場合の測定値のばらつきの比較結果を示す図である。It is a figure which shows the comparison result of the dispersion | variation in the measured value when not estimating with the estimated value of the optical path length using a deformation | transformation MSC method, and the correction | amendment using a deformation | transformation MSC method. バイアル瓶に採取したサンプルを近赤外分光分析計を用いてサンプルのスペクトルを測定するための一例を示す図である。It is a figure which shows an example for measuring the spectrum of a sample extract | collected to the vial bottle using a near-infrared spectrometer.

符号の説明Explanation of symbols

1 測定用ホルダ
2 温調器
3 検出器
4 信号変換器
5 パソコン
10 バイアル瓶
11 試料
1 Measurement Holder 2 Temperature Controller 3 Detector 4 Signal Converter 5 Personal Computer 10 Vial Bottle 11 Sample

Claims (2)

光路長が既知のバイアル又はセルで測定したサンプルスペクトルを基準とし、
前記基準スペクトルと測定スペクトルの特定波数範囲の比を最小自乗法で求めて測定光路長を決定し、測定スペクトルを基準スペクトルと同じ光路長で測定したスペクトルに変換した後検量線を作成し、未知サンプルのスペクトルと基準スペクトルの特定波数範囲の比を最小自乗法で求めて光路長を推定し、基準光路長のスペクトルに変換した後、予め作成した検量線を使用してサンプルの濃度および性状を推定することを特徴とする検量線補正方法。
Based on the sample spectrum measured in a vial or cell with a known optical path length,
Determine the optical path length by calculating the ratio of the specific spectrum of the reference spectrum and the measured spectrum using the least square method, convert the measured spectrum to a spectrum measured with the same optical path length as the reference spectrum, create a calibration curve, and Estimate the optical path length by calculating the ratio of the specific spectrum of the sample spectrum to the specific spectrum using the least square method, convert it to the reference optical path length spectrum, and then use the calibration curve created in advance to determine the concentration and properties of the sample. A calibration curve correction method characterized by estimating.
前記基準スペクトルを採用し基準スペクトルと測定スペクトルの比から求めた測定光路長を推定し、表示および出力するようにしたことを特徴とする請求項1記載の検量線補正方法。
2. The calibration curve correcting method according to claim 1, wherein the reference optical spectrum is adopted, the measurement optical path length obtained from the ratio of the reference spectrum and the measurement spectrum is estimated, displayed, and output.
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