JPH0843301A - Method and device for measuring absorbance, component concentration or specific gravity of liquid sample - Google Patents
Method and device for measuring absorbance, component concentration or specific gravity of liquid sampleInfo
- Publication number
- JPH0843301A JPH0843301A JP13727795A JP13727795A JPH0843301A JP H0843301 A JPH0843301 A JP H0843301A JP 13727795 A JP13727795 A JP 13727795A JP 13727795 A JP13727795 A JP 13727795A JP H0843301 A JPH0843301 A JP H0843301A
- Authority
- JP
- Japan
- Prior art keywords
- refractive index
- measurement
- cell
- calculated
- sample
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000005484 gravity Effects 0.000 title claims abstract description 107
- 238000002835 absorbance Methods 0.000 title claims abstract description 69
- 239000007788 liquid Substances 0.000 title claims abstract description 26
- 238000000034 method Methods 0.000 title claims description 62
- 210000002700 urine Anatomy 0.000 claims abstract description 89
- 238000004364 calculation method Methods 0.000 claims abstract description 69
- 230000004907 flux Effects 0.000 claims abstract description 19
- 102000004169 proteins and genes Human genes 0.000 claims abstract description 17
- 108090000623 proteins and genes Proteins 0.000 claims abstract description 17
- 238000000491 multivariate analysis Methods 0.000 claims abstract description 14
- WQZGKKKJIJFFOK-GASJEMHNSA-N Glucose Natural products OC[C@H]1OC(O)[C@H](O)[C@@H](O)[C@@H]1O WQZGKKKJIJFFOK-GASJEMHNSA-N 0.000 claims abstract description 11
- 239000008103 glucose Substances 0.000 claims abstract description 11
- 238000001514 detection method Methods 0.000 claims abstract description 10
- 238000005259 measurement Methods 0.000 claims description 102
- 238000002834 transmittance Methods 0.000 claims description 29
- 230000003287 optical effect Effects 0.000 claims description 18
- 238000011088 calibration curve Methods 0.000 claims description 9
- 230000000694 effects Effects 0.000 claims description 7
- 238000000691 measurement method Methods 0.000 claims description 3
- 239000006193 liquid solution Substances 0.000 claims 1
- 230000005540 biological transmission Effects 0.000 abstract description 2
- 239000000523 sample Substances 0.000 description 43
- 239000000243 solution Substances 0.000 description 28
- XSQUKJJJFZCRTK-UHFFFAOYSA-N Urea Chemical compound NC(N)=O XSQUKJJJFZCRTK-UHFFFAOYSA-N 0.000 description 13
- 239000004202 carbamide Substances 0.000 description 13
- 238000012545 processing Methods 0.000 description 12
- 239000012488 sample solution Substances 0.000 description 10
- 238000012360 testing method Methods 0.000 description 10
- 238000006073 displacement reaction Methods 0.000 description 9
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 9
- 235000000346 sugar Nutrition 0.000 description 8
- 238000010521 absorption reaction Methods 0.000 description 6
- 238000012937 correction Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 230000007170 pathology Effects 0.000 description 5
- 239000013558 reference substance Substances 0.000 description 5
- FAPWRFPIFSIZLT-UHFFFAOYSA-M Sodium chloride Chemical compound [Na+].[Cl-] FAPWRFPIFSIZLT-UHFFFAOYSA-M 0.000 description 4
- 238000012314 multivariate regression analysis Methods 0.000 description 4
- 239000000126 substance Substances 0.000 description 4
- 238000004458 analytical method Methods 0.000 description 3
- 230000001419 dependent effect Effects 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 238000012628 principal component regression Methods 0.000 description 3
- 238000004445 quantitative analysis Methods 0.000 description 3
- 238000000611 regression analysis Methods 0.000 description 3
- 150000008163 sugars Chemical class 0.000 description 3
- CIWBSHSKHKDKBQ-JLAZNSOCSA-N Ascorbic acid Chemical compound OC[C@H](O)[C@H]1OC(=O)C(O)=C1O CIWBSHSKHKDKBQ-JLAZNSOCSA-N 0.000 description 2
- DDRJAANPRJIHGJ-UHFFFAOYSA-N creatinine Chemical compound CN1CC(=O)NC1=N DDRJAANPRJIHGJ-UHFFFAOYSA-N 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 230000001575 pathological effect Effects 0.000 description 2
- 239000011780 sodium chloride Substances 0.000 description 2
- LPXPTNMVRIOKMN-UHFFFAOYSA-M sodium nitrite Chemical compound [Na+].[O-]N=O LPXPTNMVRIOKMN-UHFFFAOYSA-M 0.000 description 2
- 230000002485 urinary effect Effects 0.000 description 2
- 102000009027 Albumins Human genes 0.000 description 1
- 108010088751 Albumins Proteins 0.000 description 1
- 102000001554 Hemoglobins Human genes 0.000 description 1
- 108010054147 Hemoglobins Proteins 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 235000010323 ascorbic acid Nutrition 0.000 description 1
- 229960005070 ascorbic acid Drugs 0.000 description 1
- 239000011668 ascorbic acid Substances 0.000 description 1
- 230000008033 biological extinction Effects 0.000 description 1
- 239000008280 blood Substances 0.000 description 1
- 210000004369 blood Anatomy 0.000 description 1
- 238000009535 clinical urine test Methods 0.000 description 1
- 229940109239 creatinine Drugs 0.000 description 1
- 238000007405 data analysis Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 239000003814 drug Substances 0.000 description 1
- 229940079593 drug Drugs 0.000 description 1
- 229910052736 halogen Inorganic materials 0.000 description 1
- 150000002367 halogens Chemical class 0.000 description 1
- GPRLSGONYQIRFK-UHFFFAOYSA-N hydron Chemical compound [H+] GPRLSGONYQIRFK-UHFFFAOYSA-N 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- 210000003734 kidney Anatomy 0.000 description 1
- UTLRZTUJSMCBHB-UHFFFAOYSA-M lithium;3-oxobutanoate Chemical compound [Li+].CC(=O)CC([O-])=O UTLRZTUJSMCBHB-UHFFFAOYSA-M 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000001556 precipitation Methods 0.000 description 1
- 238000011002 quantification Methods 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 238000012216 screening Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 235000010288 sodium nitrite Nutrition 0.000 description 1
- 239000002904 solvent Substances 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は尿や血液を初めとして各
種液体試料の吸光度、成分濃度又は比重を測定する方法
とそれらの測定装置に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring the absorbance, component concentration or specific gravity of various liquid samples including urine and blood, and a measuring device therefor.
【0002】[0002]
【従来の技術】吸光度測定にはランバート・ベアの法則
が用いられる。理想的な状態のランバートベア法則の吸
収方程式は次の(1)式のように記される。 log{Io(λ)/I(λ)}=ε(λ)×C×L ……(1) Io(λ):セルへの入射光強度 I(λ) :セルを透過した測定光の強度 ε(λ) :成分の吸光係数(波長に依存する) C :溶液中の成分濃度 L :セル長 (1)式から、波長走査の間中、溶液の濃度Cと光路長
Lが変らなければ、IoとIを測定することにより、そ
の物質に固有の吸光係数に比例した形のスペクトルを得
ることができる。Lambert-Beer's law is used for measuring absorbance. The absorption equation of the Lambert-Beer law in an ideal state is expressed by the following equation (1). log {Io (λ) / I (λ)} = ε (λ) × C × L (1) Io (λ): incident light intensity on the cell I (λ): intensity of the measurement light transmitted through the cell ε (λ): Extinction coefficient of component (depending on wavelength) C: Concentration of component in solution L: Cell length From formula (1), if concentration C of solution and optical path length L do not change during wavelength scanning. , Io and I can be measured to obtain a spectrum in a form proportional to the absorption coefficient peculiar to the substance.
【0003】尿の比重値は尿中に溶けている全溶質の濃
度を示す指標であり、腎臓により調節される尿量と、最
終的に尿中に排泄される溶質量により決定される。尿比
重の検査法としては、大きく分けると次の5方式が行な
われている。 重量法……同一温度、同一圧力下における純水と同体
積の尿との重量比から尿比重を求める。 超音波法……溶液密度差による超音波音速の差を測定
して尿比重を求める。 試験紙法……イオン強度を測定して尿比重を求める。 液滴落下法……水と混ざり合わない溶媒、例えばオイ
ル中に滴下した尿の沈澱速度から比重を求める。 屈折率法……屈折率は光学物性の1つであって液体の
純度や溶液の濃度と深い相関を有している。また、溶液
においては、その屈折率の精密な測定が可能である。特
に、尿の屈折率は尿比重とほぼ比例することから、日本
臨床病理学会標準化委員会が1979年に作成した図
2,図3の日本臨床病理学会ノモグラムを用いて屈折率
との対応から尿比重を求める。この場合、屈折率は屈折
率計を用いて測定している。The specific gravity of urine is an index showing the concentration of total solutes dissolved in urine, and is determined by the amount of urine regulated by the kidney and the amount of solute finally excreted in urine. The urine specific gravity is roughly divided into the following five methods. Gravimetric method: Calculate the specific gravity of urine from the weight ratio of pure water and the same volume of urine at the same temperature and pressure. Ultrasonic method: Determine the specific gravity of urine by measuring the difference in ultrasonic velocity due to the difference in solution density. Test strip method: Determine urine specific gravity by measuring ionic strength. Droplet drop method: Determine the specific gravity from the precipitation rate of urine dropped in a solvent that does not mix with water, such as oil. Refractive index method: Refractive index is one of optical properties and has a deep correlation with the purity of liquid and the concentration of solution. In addition, the refractive index of a solution can be precisely measured. In particular, since the refractive index of urine is almost proportional to the specific gravity of urine, the urine refractive index is used in correspondence with the refractive index using the Japanese Society for Clinical Pathology nomograms of FIGS. 2 and 3 created in 1979 by the Japanese Society for Clinical Pathology Standardization Committee. Calculate the specific gravity. In this case, the refractive index is measured using a refractometer.
【0004】日常検査の中では、屈折率法と試験紙法が
よく用いられている。試験紙法で用いる試験紙は水素イ
オン濃度に応じて青緑色から黄緑色の色調を呈するの
で、尿比重は試験紙の色調を比色することにより、1.
000〜1.030の範囲で0.005幅の7段階で示
される。試験紙法は蛋白や糖の影響を受けにくいという
利点をもっている。しかし、比重提示の精度が屈折率法
では0.001幅であるのに対し、試験紙法では0.0
05幅と粗い。また、試験紙法は目視判定で行なう測定
方法であるのに対し、屈折率法は測定装置を構築しやす
く、高速、かつ高精度に自動測定を行なうことができ
る。In the routine inspection, the refractive index method and the test strip method are often used. Since the test paper used in the test paper method has a blue-green to yellow-green color tone depending on the hydrogen ion concentration, the urine specific gravity is 1.
It is shown in seven steps of 0.005 width in the range of 000 to 1.030. The test strip method has the advantage that it is less susceptible to proteins and sugars. However, the accuracy of the specific gravity presentation is 0.001 in the refractive index method, while it is 0.0 in the test strip method.
05 width and coarse. Further, while the test strip method is a measurement method that is performed by visual judgment, the refractive index method is easy to construct a measurement device, and automatic measurement can be performed at high speed and with high accuracy.
【0005】屈折率法によるメーカー間のばらつきの改
善と、溶質成分の構成比の変動に基づく重量法との差を
補正し、国内での統一基準化が行なわれた。そこで、検
討されたのは以下の2項目である。 (1)尿中に存在する主な溶質は塩化ナトリウム、尿素
などであり、これらは生理的又は病的状態で変動して尿
比重に影響を与える作用をする。 (2)病的条件では、蛋白や糖などの濃度の増加や薬剤
の投与などは、尿比重の変動に、より大きな影響を与え
る。[0005] By improving the variation among manufacturers by the refractive index method and by compensating for the difference between the gravimetric method based on the change in the composition ratio of solute components, a unified standard in Japan has been made. Therefore, the following two items were examined. (1) The main solutes present in urine are sodium chloride, urea, etc., which act depending on the physiological or pathological state to affect the specific gravity of urine. (2) Under pathological conditions, an increase in the concentration of proteins and sugars and the administration of drugs have a greater effect on changes in the specific gravity of urine.
【0006】これらの点を勘案してブドウ糖及び蛋白の
尿比重への影響は、 (1)ブドウ糖の濃度1%当り、尿比重は0.004上
昇する (2)蛋白の濃度1%当り、尿比重は0.003上昇す
る として補正されることとなっている。そこで、屈折率法
による尿比重測定は、尿中の蛋白及び糖を測定するため
の汎用の試験紙法と組み合わせて行われており、屈折率
計を用いて求められた比重を、試験紙を用いて求めた糖
と蛋白の濃度に応じて補正している。Considering these points, the influence of glucose and protein on the specific gravity of urine is as follows: (1) The specific gravity of glucose is increased by 1% and the specific gravity of urine is increased by 0.004. The specific gravity is supposed to be corrected by increasing 0.003. Therefore, the measurement of urine specific gravity by the refractive index method is performed in combination with a general-purpose test strip method for measuring proteins and sugars in urine, and the specific gravity obtained using a refractometer is measured with a test strip. It is corrected according to the sugar and protein concentrations obtained by using.
【0007】尿素濃度と尿比重との関係を用いて尿比重
を求める方法も提案されている(特開平5−18084
6号公報参照)。その提案された方法では、尿試験紙の
ような尿中の尿素濃度を呈色変化で示すようにした尿素
濃度測定用呈色試験具を使用して尿素濃度を測定し、そ
の結果を、予め作成されている尿素濃度と尿比重の関係
を示す標準色調表に当て嵌めて尿比重を求める。尿素濃
度に基づく発色と尿比重の関係を示した標準色調表は、
尿素濃度と尿比重との関係が 尿比重=尿素濃度(mg/dl)×1.43×10-5+
1.008 で示されることに基づいており、通常測定される尿比重
の範囲1.000〜1.030の間を0.005刻みに7
等分し、各範囲の中心値に対する尿素濃度を示す尿素濃
度測定用呈色試験紙の色調を決定して作成されている。A method for determining the urine specific gravity by using the relationship between the urea concentration and the urine specific gravity has also been proposed (Japanese Patent Laid-Open No. 5-18084).
No. 6 publication). In the proposed method, the urea concentration is measured by using a urea concentration measuring color tester that shows the urea concentration in urine as a color change, such as a urine test strip, and the result is previously calculated. The urine specific gravity is calculated by fitting it to a standard color chart showing the relationship between the urea concentration and the urine specific gravity. The standard color chart showing the relationship between color development based on urea concentration and urine specific gravity is
The relationship between the urea concentration and the specific gravity of urine is: Specific gravity of urine = Concentration of urea (mg / dl) x 1.43 x 10 -5 +
It is based on what is shown in 1.008, and the urine specific gravity range normally measured between 1.000 and 1.030 is 7 in 0.005 steps.
It is created by equally dividing the color tone of the urea concentration measuring color test paper showing the urea concentration with respect to the center value of each range.
【0008】[0008]
【発明が解決しようとする課題】吸収測定において、試
料を入れる容器としてガラスなどのセルを用いる場合、
セルと空気、及びセルと溶液界面で光が反射し、透過光
強度に影響が現われる。セルと空気との間での反射は空
気とセルの屈折率だけに関係し、溶液の濃度には依存し
ない。しかし、セルと溶液界面での反射は溶液の屈折率
に関係し、溶液の濃度が異なると変化する。そのため、
屈折が透過率変化を介して透過光強度へ与える影響を修
正する必要がある。When a cell such as glass is used as a container for a sample in absorption measurement,
Light is reflected at the cell-air interface and the cell-solution interface, and the transmitted light intensity is affected. The reflection between the cell and the air is related only to the refractive index of the air and the cell and not to the concentration of the solution. However, the reflection at the cell-solution interface is related to the refractive index of the solution and changes with different solution concentrations. for that reason,
It is necessary to correct the effect of refraction on the transmitted light intensity via the change in transmittance.
【0009】そこで、屈折による透過率変化を介して透
過光強度が変化する点を考慮すると、透過光強度Iは、
ランバート・ベアの吸収方程式から次の(2)式のよう
に表わされる。 I=Iot(no,nc,n)exp(−ΣαiCiL) (2) αi:溶液中のi成分の吸収係数(波長に依存する) Ci:溶液中のi成分濃度 t(no,nc,n):透過率 no;大気の屈折率 n ;溶液の屈折率(波長に依存する) nc;セルの屈折率 つまり、大気、セル及び溶液の間で屈折率が相違するた
め、波長によって透過率tが変化して透過光強度Iが変
化し、それが吸光度に影響する結果、成分濃度の測定結
果には透過率変化に起因する誤差が入り込む。Therefore, considering that the transmitted light intensity changes due to the change in transmittance due to refraction, the transmitted light intensity I is
From the Lambert-Bear absorption equation, it is expressed as the following equation (2). I = Iot (no, nc, n) exp (-ΣαiCiL) (2) αi: absorption coefficient of i component in solution (dependent on wavelength) Ci: i component concentration in solution t (no, nc, n) : Transmittance no; refractive index of air n; refractive index of solution (dependent on wavelength) nc; refractive index of cell In other words, since the refractive index differs between the atmosphere, the cell and the solution, the transmittance t depends on the wavelength. As a result of the change, the transmitted light intensity I changes, which affects the absorbance. As a result, an error resulting from the change in transmittance is introduced into the measurement result of the component concentration.
【0010】入射光強度Ioを補正する方法は各種考案
されている。例えば、(1)同一セルに水などの参照物
質を入れて測定する、(2)光源光の一部をセルを通さ
ずにモニタする、などが行なわれているが、屈折率の相
違による誤差までは補償されていない。Various methods for correcting the incident light intensity Io have been devised. For example, (1) a reference substance such as water is put in the same cell for measurement, and (2) a part of light source light is monitored without passing through the cell. Not up to.
【0011】また、屈折による透過率変化の透過光強度
への影響は、セル長Lを長くすると相対的に小さくな
り、吸収測定の精度を高くすることができる。しかし、
セル長を長くすると、高散乱物質などの測定を行なった
場合に透過光強度が小さくなり、S/N比が悪くなる。
尿比重を求める従来の屈折率法では、屈折率と成分濃度
をそれぞれ異なる手段により測定するため、高価な装置
を必要とし、測定の手間や煩雑さが加わる問題がある。Further, the influence of the change in transmittance due to refraction on the intensity of transmitted light becomes relatively small when the cell length L is increased, and the accuracy of absorption measurement can be improved. But,
When the cell length is increased, the intensity of transmitted light becomes smaller and the S / N ratio becomes worse when a highly scattering substance or the like is measured.
In the conventional refractive index method for obtaining the specific gravity of urine, since the refractive index and the component concentration are measured by different means, an expensive device is required, and there is a problem that the measurement labor and complexity are added.
【0012】尿素濃度と尿比重との関係を用いる上記引
用例の方法では、日本臨床病理学会ノモグラムに示す分
解能を得ることは不可能であり、装置を使用して精密な
尿比重を検査する前のスクリーニングにしか利用するこ
とができない。そのため異常値が出た場合は別の方法で
再測定が必要になる。また、尿素濃度を測定して現われ
た呈色状態を、呈色試験具に現われた同じ色又は近似し
た色を目視で判定するため、測定者の個人差を含むこと
になる。It is impossible to obtain the resolution shown in the nomogram of the Japanese Society for Clinical Pathology by the method of the above-mentioned reference that uses the relationship between the urea concentration and the urine specific gravity. Can only be used for screening. Therefore, if an abnormal value appears, it is necessary to re-measure with another method. In addition, since the same or similar color that appears in the color tester is visually determined for the coloration state that appears by measuring the urea concentration, the individual differences of the measurers are included.
【0013】本発明の第1の目的は、高散乱物質にも適
用でき、セル長を長くすることなく、空気、セル、被測
定物質の屈折率の相違に起因する誤差をも補償して吸光
度を測定する簡便な方法及び装置を提供することであ
る。本発明の第2の目的は、その吸光度をもとにして成
分濃度を求める方法及び装置を提供することである。本
発明の第3の目的は、尿試料に限らず、溶液試料一般に
ついて、吸光度をもとにして成分濃度を求め、それを用
いてさらに比重を算出する方法と装置を提供することで
ある。本発明の第4の目的は、1台の測定装置で、尿試
料の屈折率と成分濃度を同時に測定し、屈折率と比重の
関係から尿の比重を求め、尿比重の補正因子である蛋白
と糖の濃度値による補正も行なうことにより、高精度で
精密な尿比重測定を簡易に行なう方法と装置を提供する
ことである。The first object of the present invention can also be applied to a highly scattering substance, and without compensating the cell length, it compensates for an error caused by a difference in refractive index between air, a cell and a substance to be measured, and absorbs light. The object is to provide a simple method and device for measuring. A second object of the present invention is to provide a method and apparatus for determining the component concentration based on its absorbance. A third object of the present invention is to provide a method and an apparatus for calculating not only urine samples but also solution samples in general, the component concentration based on the absorbance and further calculating the specific gravity using the concentration. A fourth object of the present invention is to measure the refractive index and the component concentration of a urine sample at the same time with a single measuring device, determine the specific gravity of urine from the relationship between the refractive index and the specific gravity, and determine the protein that is a correction factor for the specific gravity of urine. It is an object of the present invention to provide a method and a device for easily performing highly accurate and precise urine specific gravity measurement by also performing correction based on the concentration value of sugar.
【0014】[0014]
【課題を解決するための手段】本発明による吸光度測定
方法は、測定光束の入射面に対し出射面が傾斜している
三角セルに液体試料を収容し、測定光束を前記入射面に
垂直な方向に入射させ、その出射面から出射する測定光
束を光の強度と位置をともに検出できるリニアセンサで
受光し、測定光束の複数の測定波長の各波長ごとに透過
光強度を検出するとともに、そのリニアセンサ上での測
定光束位置から試料の屈折率を算出し、その算出された
屈折率、既知の大気屈折率及び既知のセル屈折率を用い
て三角セルでの透過率変化を介して透過光強度へ与える
影響を補正して吸光度を求める。According to the absorbance measuring method of the present invention, a liquid sample is accommodated in a triangular cell whose exit surface is inclined with respect to the incident surface of the measuring light beam, and the measuring light beam is directed in a direction perpendicular to the incident surface. The measurement light flux emitted from the output surface is received by a linear sensor that can detect both the intensity and position of the light, and the transmitted light intensity is detected for each of the multiple measurement wavelengths of the measurement light flux. The refractive index of the sample is calculated from the position of the measurement light beam on the sensor, and the transmitted light intensity is obtained through the change in the transmittance in the triangular cell using the calculated refractive index, the known atmospheric refractive index, and the known cell refractive index. Absorbance is calculated by correcting the effect on
【0015】本発明による成分濃度測定方法は、上記の
方法により求められた各測定波長ごとの吸光度を用い、
多変量解析演算を行なって各成分濃度を算出する。本発
明による液体試料の比重測定方法は、上記の方法により
算出された各成分濃度を加算して密度を算出し、それを
もとに比重を算出する。本発明による尿比重測定方法
は、尿の屈折率と比重との関係を示す既知のデータを用
い、上記の方法により求められた尿試料の屈折率をその
データにあてはめてその尿試料の比重を求め、かつ上記
の方法により算出された成分濃度のうちのブドウ糖と蛋
白の濃度に対応する尿比重上昇分を補正する。The component concentration measuring method according to the present invention uses the absorbance for each measurement wavelength obtained by the above method,
A multivariate analysis calculation is performed to calculate the concentration of each component. In the method of measuring the specific gravity of a liquid sample according to the present invention, the density of each component calculated by the above method is added to calculate the density, and the specific gravity is calculated based on the density. The urine specific gravity measuring method according to the present invention uses known data showing the relationship between the refractive index and the specific gravity of urine, and applies the refractive index of the urine sample obtained by the above method to the data to determine the specific gravity of the urine sample. The urine specific gravity increase corresponding to the glucose and protein concentrations of the component concentrations obtained and calculated by the above method is corrected.
【0016】本発明の方法を実現する装置を図1に示
す。2は液体試料を収容し、測定光束の入射面に対し出
射面が傾斜した三角セルであり、測定光束が三角セル2
の入射面に対して垂直方向に入射するように測定光路が
設定された測定光学系と組み合わされている。3は三角
セル2の出射面から出射する測定光束を受光する位置に
設けられ、光の強度と位置をともに検出できるリニアセ
ンサである。30は屈折率算出部であり、三角セル2に
屈折率が既知の液体を入れて測定したときの三角セル2
からの出射光をリニアセンサ3で受光したときの検出位
置を基準とし、三角セル2に屈折率が未知の試料を入れ
て測定したときの三角セル2からの出射光を前記リニア
センサ3で受光したときの検出位置の変位置量を検出
し、その変位置量に対応する試料の屈折率を検量線又は
計算により算出する。31は吸光度算出部であり、三角
セル2からの出射光をリニアセンサ3で受光したときの
透過光強度、大気の屈折率及びセルの屈折率、並びに屈
折率算出部30で算出された試料の屈折率を用いて三角
セル2での透過率変化の影響を補正した成分濃度に依存
する吸光度を算出する。32は成分濃度算出部であり、
吸光度算出部31で算出された複数測定波長での成分濃
度に依存する吸光度をもとに多変量解析演算を行なって
各成分濃度を算出する。33は比重算出部であり、成分
濃度算出部32で算出された各成分濃度を加算して密度
を算出し、それをもとに比重を算出する。35は尿比重
算出部であり、尿の屈折率と比重との関係を示す既知の
データを用い、屈折率算出部30で求められた尿試料の
屈折率をそのデータにあてはめてその尿試料の比重を求
め、成分濃度算出部32で算出された成分濃度のうちの
ブドウ糖と蛋白の濃度に対応する尿比重上昇分を補正す
る。34は各部で算出された吸光度、成分濃度、液体試
料の比重、又は尿試料の比重を出力するレコーダやCR
Tなどの出力部である。An apparatus for implementing the method of the present invention is shown in FIG. Reference numeral 2 denotes a triangular cell that contains a liquid sample and has an exit surface inclined with respect to an incident surface of the measurement light beam.
Is combined with a measurement optical system in which the measurement optical path is set so as to be incident in a direction perpendicular to the incident surface of. Reference numeral 3 denotes a linear sensor which is provided at a position for receiving the measurement light flux emitted from the emission surface of the triangular cell 2 and which can detect both the intensity and the position of the light. Reference numeral 30 denotes a refractive index calculation unit, which is used when the liquid having a known refractive index is put into the triangular cell 2 for measurement.
The linear sensor 3 receives the light emitted from the triangular cell 2 when a sample with an unknown refractive index is put into the triangular cell 2 for measurement with reference to the detection position when the light emitted from the linear sensor 3 is received. The variable position amount of the detected position at that time is detected, and the refractive index of the sample corresponding to the variable position amount is calculated by a calibration curve or calculation. Reference numeral 31 denotes an absorbance calculator, which is the transmitted light intensity when the light emitted from the triangular cell 2 is received by the linear sensor 3, the refractive index of the atmosphere and the refractive index of the cell, and the sample of the sample calculated by the refractive index calculator 30. The refractive index is used to calculate the absorbance depending on the component concentration in which the influence of the transmittance change in the triangular cell 2 is corrected. 32 is a component concentration calculation unit,
Each component concentration is calculated by performing a multivariate analysis calculation based on the absorbances that are calculated by the absorbance calculation unit 31 and that depend on the component concentrations at a plurality of measurement wavelengths. Reference numeral 33 denotes a specific gravity calculating unit, which adds the component concentrations calculated by the component concentration calculating unit 32 to calculate the density and calculates the specific gravity based on the density. Reference numeral 35 denotes a urine specific gravity calculation unit, which uses known data showing the relationship between the refractive index and specific gravity of urine, and applies the refractive index of the urine sample obtained by the refractive index calculation unit 30 to the data to obtain the urine sample The specific gravity is calculated, and the increase in urine specific gravity corresponding to the glucose and protein concentrations in the component concentration calculated by the component concentration calculating unit 32 is corrected. 34 is a recorder or CR for outputting the absorbance, the component concentration, the specific gravity of the liquid sample, or the specific gravity of the urine sample calculated in each part.
An output unit such as T.
【0017】本発明における三角セルは外形が三角形で
あるものだけでなく、測定に用いる光束が通過する一対
のガラス面が互いに平行でなく、その一対のガラス面が
直接又は延長線上で交差するものであればよい。すなわ
ち、測定光束の入射面に対し出射面が傾斜しているもの
を三角セルと呼ぶ。The triangular cell according to the present invention is not limited to one having a triangular outer shape, but a pair of glass surfaces through which a light beam used for measurement passes are not parallel to each other, and the pair of glass surfaces intersect directly or on an extension line. If That is, a cell whose output surface is inclined with respect to the incident surface of the measurement light beam is called a triangular cell.
【0018】[0018]
【作用】屈折率算出部30と吸光度算出部31における
動作を説明する。屈折率及び吸光度算出 屈折率の透過率への影響を考慮した理論式は、式(2)
に示した通りであるが、ここで、式(2)から透過率I
o/Iは次のように変形される。 Io/I=(1/t)exp(ΣαiCiL) (3)The operation of the refractive index calculator 30 and the absorbance calculator 31 will be described. Refractive Index and Absorbance Calculation The theoretical formula considering the effect of refractive index on transmittance is given by the formula (2)
However, here, the transmittance I is calculated from the equation (2).
o / I is transformed as follows. Io / I = (1 / t) exp (ΣαiCiL) (3)
【0019】式(3)から、吸光度Aを求めると次のよ
うになる。 A=log(Io/I) =log{(1/t)exp(ΣαiCiL)} =−logt+ΣαiCiL =An+Ac (4) Ac:成分濃度Ciに依存する吸光度 An:反射の影響を受けた吸光度The absorbance A is obtained from the equation (3) as follows. A = log (Io / I) = log {(1 / t) exp (ΣαiCiL)} = − logt + ΣαiCiL = An + Ac (4) Ac: Absorbance dependent on component concentration Ci An: Absorbance affected by reflection
【0020】式(4)から、成分濃度Ciに依存する吸
光度Acは次のように求められる。 Ac=A−An (5) 吸光度AはIoとIの測定値を用い、式(4)から求め
ることができる。Iは、三角セル2を用いて透過光強度
と溶液の屈折率nを同時に測定するようにした図4に示
すように、セル2を透過してリニアセンサ3で捉えられ
た波形のピーク位置の出力値から求められる。Ioは装
置固有の値であり、光学系設定時に測定しておく。t
は、図5に模式的に示されるセル2の各界面1,2,
3,4での透過率から、 t=t1t2t3t4 (6) t1:界面1での透過率 t2:界面2での透過率 t3:界面3での透過率 t4:界面4での透過率 となる。空気とセル2との界面での透過率においてはt
1=t4、セル2と溶液2aの界面での透過率においては
t2=t3であるから、フレネルの式を利用して t1=t4=4n0nc/(n0+nc)2 (7) t2=t3=4n0n/(nc+n)2 (8) となる。式(6)は、式(7)と式(8)から、 t=256n0 4n2nc2/(n0+nc)4(nc+n)4 (9)From equation (4), the absorbance Ac depending on the component concentration Ci can be obtained as follows. Ac = A-An (5) The absorbance A can be obtained from the equation (4) using the measured values of Io and I. I is the peak position of the waveform captured by the linear sensor 3 after passing through the cell 2 as shown in FIG. 4 in which the transmitted light intensity and the refractive index n of the solution are simultaneously measured using the triangular cell 2. Calculated from the output value. Io is a value peculiar to the apparatus and is measured at the time of setting the optical system. t
Are each interface 1, 2 ,, of the cell 2 shown schematically in FIG.
From the transmittances at 3 and 4, t = t 1 t 2 t 3 t 4 (6) t 1 : the transmittance at the interface 1 t 2 : the transmittance at the interface 2 t 3 : the transmittance at the interface 3 t 4 : It is the transmittance at interface 4. The transmittance at the interface between air and cell 2 is t
1 = t 4 , and t 2 = t 3 at the transmittance at the interface between the cell 2 and the solution 2a. Therefore, using the Fresnel equation, t 1 = t 4 = 4n 0 nc / (n 0 + nc) 2 (7) t 2 = t 3 = 4n 0 n / (nc + n) 2 (8) From the equation (7) and the equation (8), the equation (6) is t = 256n 0 4 n 2 nc 2 / (n 0 + nc) 4 (nc + n) 4 (9)
【0021】式(9)において、空気の屈折率n0を1
とし、セルの屈折率をncとして材質により決定される
既知の値を用い、溶液の屈折率nとして図4に示す装置
から測定した値を用いると、tを算出することができ、
吸光度Anはその算出値tを用いて、An=−logtに
より算出できる。In the equation (9), the refractive index n 0 of air is 1
Using the known value determined by the material as the refractive index nc of the cell and the value measured from the device shown in FIG. 4 as the refractive index n of the solution, t can be calculated,
The absorbance An can be calculated by An = −logt using the calculated value t.
【0022】ここで、図4の装置を用いて溶液の屈折率
nを測定する原理を説明する。屈折率算出部30は屈折
率の絶対値を直接求めるのではなく、図4において、参
照物質(例えば水)を測定した場合の光軸のリニアセン
サ3の受光面上の照射位置と、尿試料を測定した場合の
光軸のリニアセンサ3の受光面上の照射位置との差(こ
れを変位置量と定義する)を測定して屈折率に換算す
る。Here, the principle of measuring the refractive index n of the solution using the apparatus of FIG. 4 will be described. The refractive index calculation unit 30 does not directly obtain the absolute value of the refractive index, but in FIG. 4, the irradiation position on the light receiving surface of the linear sensor 3 of the optical axis when the reference substance (for example, water) is measured, and the urine sample. The difference between the optical axis and the irradiation position on the light-receiving surface of the linear sensor 3 (this is defined as a variable position amount) is measured and converted into a refractive index.
【0023】図4において、三角セル2の入射面に直角
に入射した測定光は屈折して空気層へ出射され、リニア
センサ3へ入射する。セル2、溶液及び空気における屈
折の関係を、 θ1:溶液からセル界面への入射角 θ2:溶液側セル界面からセル層への屈折角 θ3:セル層から空気層への出射角 n0:空気の屈折率 nc:セルの屈折率 n:溶液の屈折率(波長に依存する) とすると、 n・sinθ1=nc・sinθ2 (10) nc・sinθ2=n0・sinθ3 (11) となる。式(10)と式(11)から、 n・sinθ1=n0・sinθ3 となり、溶液の屈折率nは、 n=n0・sinθ3/sinθ1 (12) となる。式(12)は、sinθ1=sinαであることから
次のように変形される。 n=n0・sinθ3/sinα (13) 空気の屈折率n0=1、αが三角セル2の頂角であるこ
とから、屈折角θ3を測定することにより溶液の屈折率
nを計算で求めることができる。In FIG. 4, the measurement light that has entered the entrance surface of the triangular cell 2 at a right angle is refracted, emitted to the air layer, and enters the linear sensor 3. The refraction relationship between the cell 2, the solution and the air is as follows: θ 1 : incident angle from solution to cell interface θ 2 : refraction angle from solution side cell interface to cell layer θ 3 : exit angle from cell layer to air layer n 0 : refractive index of air nc: refractive index of cell n: refractive index of solution (depending on wavelength), n · sin θ 1 = nc · sin θ 2 (10) nc · sin θ 2 = n 0 · sin θ 3 ( 11) becomes. From the equations (10) and (11), n · sin θ 1 = n 0 · sin θ 3 and the refractive index n of the solution is n = n 0 · sin θ 3 / sin θ 1 (12). Expression (12) is modified as follows because sin θ 1 = sin α. n = n 0 · sin θ 3 / sin α (13) Since the refractive index n 0 = 1 of air and α is the apex angle of the triangular cell 2, the refractive index n of the solution is calculated by measuring the refractive angle θ 3. Can be found at.
【0024】ここでは、屈折角θ3を測定するのではな
く、屈折率の変化(例えば、水の場合と試料溶液の場合
との変化)による測定光束の変位置量Dを測定し、それ
をもとに屈折率を計算する。変位置量Dは、リニアセン
サ3で捉えた波形のピーク位置を検出し、基準物質(例
えば水)を測定したときの波形のピーク位置D0を基準
として、試料溶液を測定したときの波形のピーク位置ま
での距離Dを測定することにより求める。セル層から空
気層への出射角θ3が、基準物質を測定したときと試料
溶液を測定したときとでdθ3だけ変化したとすれば、
変位置量Dは D=M・dθ3 である。Mは三角セルの光出射点からリニアセンサ3ま
での距離である。一方、式(13)から、 dn=(n0・cosθ3/sinα)・dθ3 であるので、この2つの式から dn=D・n0・cosθ3/M・sinα (14) となる。ここで、cosθ3は装置固有の値で、光学系設定
時に測定しておく。(14)式によれば、試料溶液の屈
折率nと基準物質の屈折率nsとの差dnは変位置量D
に比例する。 n=ns+dn であるので、(14)式を用いると、変位置量Dの測定
から計算のみによって試料溶液の屈折率nを求めること
もできる。Here, instead of measuring the refraction angle θ 3 , the displacement amount D of the measurement light flux due to the change in the refractive index (for example, the change between water and the sample solution) is measured, and it is Calculate the refractive index based on it. The amount of displacement D is the peak position of the waveform detected by the linear sensor 3, and the peak position D 0 of the waveform when the reference substance (for example, water) is measured is used as a reference to measure the waveform of the sample solution. It is determined by measuring the distance D to the peak position. If the emission angle θ 3 from the cell layer to the air layer changes by dθ 3 between when the reference substance is measured and when the sample solution is measured,
The variable position amount D is D = M · dθ 3 . M is the distance from the light emitting point of the triangular cell to the linear sensor 3. On the other hand, from equation (13), since it is dn = (n 0 · cosθ 3 / sinα) · dθ 3, become the two equations dn = D · n 0 · cosθ 3 / M · sinα (14). Here, cos θ 3 is a value peculiar to the apparatus and is measured at the time of setting the optical system. According to the equation (14), the difference dn between the refractive index n of the sample solution and the refractive index ns of the reference substance is the displacement amount D.
Is proportional to Since n = ns + dn, the refractive index n of the sample solution can be obtained only by calculation from the measurement of the displacement amount D by using the equation (14).
【0025】実用的で高精度に屈折率を求めることので
きる方法は、検量線を用いる方法である。検量線法で
は、ある比重範囲(例えば1.000〜1.050)の試
料を用い、各試料について、本発明での方法により測定
した変位置量Dのデータと、別に屈折率計を用いて得た
屈折率データとから検量線式を導いておく。そして、試
料溶液の測定にあたっては、本発明により変位置量値D
を測定して検量線を用いて屈折率nを算出する。A practical method for obtaining the refractive index with high accuracy is to use a calibration curve. In the calibration curve method, a sample having a specific gravity range (for example, 1.000 to 1.050) is used, and for each sample, data of the displacement amount D measured by the method of the present invention and a refractometer are separately used. A calibration curve formula is derived from the obtained refractive index data. In measuring the sample solution, the displacement amount value D
Is measured and the refractive index n is calculated using a calibration curve.
【0026】本発明によれば、測定した吸光度Aと算出
したAnを用い、式(5)によりAc(=A−An)を
算出することにより、屈折が透過率変化を介して透過光
強度へ与える影響を補正することができ、成分濃度Ci
に依存する吸光度Acを正確に求めることができる。According to the present invention, the measured absorbance A and the calculated An are used to calculate Ac (= A-An) by the equation (5), whereby the refraction changes to the transmitted light intensity through the change in the transmittance. The influence given can be corrected, and the component concentration Ci
It is possible to accurately obtain the absorbance Ac depending on
【0027】成分濃度算出 成分濃度に依存する吸光度Acをもとにして成分濃度を
算出する成分濃度算出部32の動作を説明する。(4)
式から、成分濃度に依存する吸光度Acは Ac=ΣαiCiL であり、未知変数はCi(i=1,2,……K;Kは成
分数)であるので、K個の独立な波長で吸光度を測定
し、連立方程式を解けば各成分の濃度を算出することが
できる。主成分回帰分析法(PCR法)や部分最小二乗
法(PLS法)などの多変量回帰分析法を用いてデータ
解析を行なえば、濃度をより高精度に求めることができ
る。 Calculation of Component Concentration The operation of the component concentration calculating unit 32 for calculating the component concentration based on the absorbance Ac depending on the component concentration will be described. (4)
From the formula, the absorbance Ac depending on the component concentration is Ac = ΣαiCiL, and the unknown variable is Ci (i = 1, 2, ... K; K is the number of components), so the absorbance at K independent wavelengths is The concentration of each component can be calculated by measuring and solving the simultaneous equations. The concentration can be obtained with higher accuracy by performing data analysis using a multivariate regression analysis method such as a principal component regression analysis method (PCR method) or a partial least squares method (PLS method).
【0028】多変量回帰分析法では、一度に多くの吸光
度情報を用いて回帰分析することができるので、単回帰
分析に比べて高い精度の定量分析が可能である。重回帰
分析は最も多用されているが、多数の試料が必要であ
り、各波長の吸光度値どうしの相関が高い場合にはその
定量分析精度は非常に低くなる。一方、多変量回帰分析
法である主成分回帰分析法は多波長の吸光度情報を互い
に無相関な主成分に集約させることができ、さらに不必
要なノイズデータを削除することができるので、高い定
量分析精度が得られる。また部分最小二乗法は主成分の
抽出の際に試料濃度のデータも利用することができるの
で、主成分回帰分析法と同様に高い定量分析精度を得る
ことができる。In the multivariate regression analysis method, since regression analysis can be performed using a large amount of absorbance information at one time, quantitative analysis can be performed with higher accuracy than single regression analysis. The multiple regression analysis is most frequently used, but a large number of samples are required, and when the correlation between the absorbance values at each wavelength is high, the accuracy of the quantitative analysis becomes very low. On the other hand, the principal component regression analysis method, which is a multivariate regression analysis method, can aggregate the multi-wavelength absorbance information into principal components that are uncorrelated with each other, and can also eliminate unnecessary noise data, thus achieving high quantification. Analytical accuracy can be obtained. Further, since the partial least squares method can also use the data of the sample concentration when extracting the main component, it is possible to obtain a high quantitative analysis accuracy as in the principal component regression analysis method.
【0029】例えば、測定しようとする各試料成分につ
いてその単成分水溶液の可視又は近赤外の波長領域での
濃度と吸光度との間の相関係数の絶対値が0.5以上、
好ましくは0.9以上の波長をその成分固有の測定波長
として選択し、試料溶液に対し可視光又は近赤外光を照
射し、測定しようとする複数の各成分についてそれぞれ
前記の条件で選択された測定波長での吸光度を測定する
ことにより、多変量回帰分析法により複数の試料成分を
同時に定量分析することができる。波長λjでの吸光度
Aと濃度との相関係数Rjは次の式により与えられる。For example, for each sample component to be measured, the absolute value of the correlation coefficient between the concentration of the single component aqueous solution in the visible or near infrared wavelength region and the absorbance is 0.5 or more,
Preferably, a wavelength of 0.9 or more is selected as a measurement wavelength peculiar to the component, the sample solution is irradiated with visible light or near infrared light, and each of the plurality of components to be measured is selected under the above conditions. By measuring the absorbance at different measurement wavelengths, a plurality of sample components can be simultaneously quantitatively analyzed by the multivariate regression analysis method. The correlation coefficient Rj between the absorbance A and the concentration at the wavelength λj is given by the following equation.
【0030】[0030]
【数1】 [Equation 1]
【0031】上記の式中で、Aijはi番目のサンプル
でのその成分の波長λjでの吸光度、Ciはi番目のサ
ンプルでのその成分の濃度である。試料が尿試料の場合
には、各尿中成分の測定波長として、水に対して強い吸
収をもつ波長領域を避け、水に対して透過率の高い25
000〜5280cm-1又は4980〜4000cm-1
の波数領域から選択する。In the above equation, Aij is the absorbance of the component at the wavelength λj in the i-th sample, and Ci is the concentration of the component in the i-th sample. When the sample is a urine sample, the measurement wavelength of each urinary component should be a wavelength range that strongly absorbs water, and has a high transmittance for water.
000-5280 cm -1 or 4980-4000 cm -1
Select from the wavenumber region of.
【0032】各尿中成分の好ましい測定波長は、波数で
表わして、グルコースに対しては11380〜9720
cm-1、9430〜9400cm-1、9340〜932
0cm-1、9260〜6560cm-1、6510〜55
40cm-1、5530〜5280cm-1、4980〜4
850cm-1、4830〜4480cm-1、4440〜
4330cm-1又は4300〜4010cm-1から選択
し、ヘモグロビンに対しては25000〜7250cm
-1、7220〜6430cm-1、6190〜5690c
m-1、5660〜5280cm-1又は4900〜408
0cm-1から選択し、アルブミンに対しては7280〜
6350cm-1、5910〜5880cm-1、5790
〜5740cm-1、5630〜5300cm-1、490
0〜4720cm-1、4670〜4280cm-1又は4
230〜4070cm-1から選択し、アセト酢酸リチウ
ムに対しては8490〜6360cm-1、6040〜5
610cm-1、5430〜5300cm-1、4900〜
4760cm-1、4680〜4510cm-1又は447
0〜4320cm-1から選択し、アスコルビン酸に対し
ては7270〜6520cm-1、6430〜5290c
m-1、4950〜4860cm-1又は4810〜409
0cm-1から選択し、クレアチニンに対しては9370
〜5870cm-1、5810〜5280cm-1、498
0〜4730cm-1、4690〜4320cm-1又は4
290〜4090cm-1から選択し、塩化ナトリウムに
対しては7640〜5280cm-1又は4980〜40
80cm-1から選択し、亜硝酸ナトリウムに対しては8
680〜5300cm-1、4980〜4210cm-1又
は4160〜4100cm-1から選択する。The preferred measurement wavelength of each urinary component is represented by wave number, and is 11380-9720 for glucose.
cm -1, 9430~9400cm -1, 9340~932
0cm -1, 9260~6560cm -1, 6510~55
40cm -1, 5530~5280cm -1, 4980~4
850cm -1, 4830~4480cm -1, 4440~
Select from 4330cm -1 or 4300~4010cm -1, relative to the hemoglobin 25000~7250cm
-1 , 7220-6430 cm -1 , 6190-5690c
m -1 , 5660-5280 cm -1 or 4900-408
It is selected from 0 cm -1 and for albumin 7280-
6350 cm -1 , 5910-5880 cm -1 , 5790
~ 5740 cm -1 , 5630-5300 cm -1 , 490
0-4720 cm -1 , 4670-4280 cm -1 or 4
230-4070 cm -1 , selected from lithium acetoacetate 8490-6360 cm -1 , 6040-5
610 cm -1 , 5430-5300 cm -1 , 4900-
4760 cm -1 , 4680-4510 cm -1 or 447
It is selected from 0 to 4320 cm -1 , and 7270 to 6520 cm -1 and 6430 to 5290 c for ascorbic acid.
m -1 , 4950-4860 cm -1 or 4810-409
Select from 0 cm -1 and 9370 for creatinine
~ 5870 cm -1 , 5810-5280 cm -1 , 498
0-4730 cm -1 , 4690-4320 cm -1 or 4
Selected from 290 to 4090 cm -1, and 7640 to 5280 cm -1 or 4980 to 40 for sodium chloride
Choose from 80 cm -1 and 8 for sodium nitrite
It is selected from 680 to 5300 cm -1 , 4980 to 4210 cm -1 or 4160 to 4100 cm -1 .
【0033】比重算出 比重算出部33の動作を説明する。比重算出部33では
成分濃度算出部32で求められた試料溶液中の全ての成
分濃度から比重を算出する。密度ρは、 ρ=m/V (15) m:全成分の重量 V:試料溶液の体積 で定義される。各成分の重量をmiとすると、各成分の
体積濃度Ciは、 Ci=mi/V (16) である。m=Σmiであるので、式(15)と式(1
6)から、 ρ=m/V =Σmi/V =ΣCi (17) となる。式(17)で求める密度と水の密度(常数)か
ら比重を求めることができ、成分の重量を測らなくて
も、成分濃度から比重を計算により求めることができ
る。試料溶液の比重を計算で求めるこの方法は、尿試料
に適用できることは勿論であるが、その他の溶液試料に
ついても一般的に適用することができる。 Specific gravity calculation The operation of the specific gravity calculator 33 will be described. The specific gravity calculating unit 33 calculates the specific gravity from all the component concentrations in the sample solution obtained by the component concentration calculating unit 32. The density ρ is defined by ρ = m / V (15) m: weight of all components, V: volume of sample solution. When the weight of each component is mi, the volume concentration Ci of each component is Ci = mi / V (16). Since m = Σmi, the formula (15) and the formula (1
From 6), ρ = m / V = Σmi / V = ΣCi (17) The specific gravity can be calculated from the density calculated by the equation (17) and the density of water (constant number), and the specific gravity can be calculated from the component concentration without measuring the weight of the component. This method of calculating the specific gravity of the sample solution by calculation can, of course, be applied to a urine sample, but can also be generally applied to other solution samples.
【0034】尿比重測定 試料が尿試料である場合に、屈折率算出部30で尿試料
の屈折率を算出し、比重算出部35で尿の比重を算出す
る方法を説明する。この方法だけは尿試料に特有の方法
であり、尿以外の溶液試料に適用することはできない。A method of calculating the refractive index of the urine sample by the refractive index calculating unit 30 and calculating the specific gravity of urine by the specific gravity calculating unit 35 when the urine specific gravity measurement sample is the urine sample will be described. This method alone is unique to urine samples and cannot be applied to solution samples other than urine.
【0035】比重算出部35は、屈折率算出部30で求
められた屈折率を用い、例えば図2及び図3に示される
ノモグラムから比重を算出する。比重範囲が1.035
を越える範囲については図2及び図3に示されたもの以
外のノモグラムを用いて比重を算出する。さらに、吸光
度算出部31と成分濃度算出部32により、屈折が透過
率変化を介して透過光強度へ与える影響を補正して算出
された成分濃度のうちのブドウ糖と蛋白の濃度を用い、 ブドウ糖……濃度1%あたり、尿比重は0.004上昇 蛋白 ……濃度1%あたり、尿比重は0.003上昇 という事実に基づき、図2及び図3のノモグラムから求
めた比重値を補正する。The specific gravity calculating unit 35 uses the refractive index obtained by the refractive index calculating unit 30 to calculate the specific gravity from the nomograms shown in FIGS. 2 and 3, for example. Specific gravity range is 1.035
For the range exceeding, the specific gravity is calculated using a nomogram other than those shown in FIGS. Further, the absorbance calculation unit 31 and the component concentration calculation unit 32 use the glucose and protein concentrations among the component concentrations calculated by correcting the influence of refraction on the transmitted light intensity through the change in transmittance, and the glucose ... … The specific gravity of urine increased by 0.004 per concentration of 1% protein .... Based on the fact that the specific gravity of urine increased by 0.003 per concentration of 1%, the specific gravity values obtained from the nomograms of FIGS. 2 and 3 are corrected.
【0036】すなわち、屈折率と吸光度の同時測定によ
り、吸光度測定から比重の補正因子であるブドウ糖及び
蛋白の濃度を求め、それをもとに尿比重の補正を行なう
ことにより、単一の方法及び単一の装置で、簡易で精密
な尿比重測定を行なうことができるようになる。That is, by simultaneously measuring the refractive index and the absorbance, the concentrations of glucose and protein, which are the correction factors of the specific gravity, are obtained from the measurement of the absorbance, and the urine specific gravity is corrected on the basis of the obtained concentrations to obtain a single method and It becomes possible to perform simple and precise urine specific gravity measurement with a single device.
【0037】[0037]
【実施例】図6は第1の実施例を表わす。光源1は複数
の波長の測定光束を選択的に放出できる光源であり、例
えばレーザダイオードアレイ、可変波長レーザ、又は多
波長を発生する光源と分光器を組み合わせたものなどで
ある。光源1からの測定光束は三角セル2の入射面に対
し直角に入射するように光源とセル2が配置されてい
る。セル2を透過し、屈折した測定光束はリニアセンサ
3で受光される。リニアセンサ3は入射光の強度と位置
をともに電気信号に変換して出力できるものであり、こ
のようなリニアセンサとしてはフォトダイオードアレイ
やCCDセンサを用いることができる。データ処理部4
はリニアセンサ3からの電気信号を各波長ごとの信号に
分離し、A/D変換してデジタル信号に変換する入出力
ポート10、CPU6、ROM7、RAM8、磁気記憶
装置などの記憶媒体9を含んでいる。5は出力部として
のレコーダである。図1における屈折率算出部30、吸
光度算出部31、成分濃度算出部32、比重算出部3
3,35はデータ処理部4により実現されている。FIG. 6 shows a first embodiment. The light source 1 is a light source capable of selectively emitting measurement light beams of a plurality of wavelengths, and is, for example, a laser diode array, a variable wavelength laser, or a combination of a light source that generates multiple wavelengths and a spectroscope. The light source and the cell 2 are arranged so that the measurement light beam from the light source 1 is incident on the entrance surface of the triangular cell 2 at a right angle. The measurement light beam that has passed through the cell 2 and is refracted is received by the linear sensor 3. The linear sensor 3 is capable of converting both the intensity and position of incident light into an electric signal and outputting the electric signal. As such a linear sensor, a photodiode array or a CCD sensor can be used. Data processing unit 4
Includes a storage medium 9 such as an input / output port 10 for separating an electric signal from the linear sensor 3 into a signal for each wavelength, and A / D converting the signal into a digital signal, a CPU 6, a ROM 7, a RAM 8, and a magnetic storage device. I'm out. Reference numeral 5 is a recorder as an output unit. The refractive index calculation unit 30, the absorbance calculation unit 31, the component concentration calculation unit 32, and the specific gravity calculation unit 3 in FIG.
3, 35 are realized by the data processing unit 4.
【0038】図7は第2の実施例を表わす。光源1aは
ハロゲンランプのように複数の波長を同時に発生する光
源である。セル2を透過した後の測定光が分光装置11
を経てリニアセンサ3に受光される。分光装置11は回
折格子ではなく、複数の干渉フィルタを備え、光路上へ
のフィルタを切り換えることにより分光するフィルタロ
ータである。図6では測定光束の入射光が波長の選択さ
れたものであるのに対し、図7では入射光は複数の波長
を含んでおり、透過光が分光されて波長が選択される点
で異なっている。データ処理部4の構成は図6のものと
同じである。FIG. 7 shows a second embodiment. The light source 1a is a light source that simultaneously generates a plurality of wavelengths, such as a halogen lamp. The measurement light after passing through the cell 2 is spectroscopic device 11
The light is received by the linear sensor 3 after passing through. The spectroscopic device 11 is not a diffraction grating, but is a filter rotor that includes a plurality of interference filters and performs spectral separation by switching filters on the optical path. In FIG. 6, the incident light of the measurement light beam has a selected wavelength, whereas in FIG. 7, the incident light includes a plurality of wavelengths, and the transmitted light is spectrally separated to select the wavelength. There is. The configuration of the data processing unit 4 is the same as that of FIG.
【0039】図8は図6及び図7におけるデータ処理部
4をさらに具体的に示したものである。図6,7での入
出力ポート10は、センサ3の出力を増幅するアンプ1
2、デジタル信号に変換するA/D変換器13、入力ポ
ート14、入力データバッファ15、入力ポート22、
出力ポート23、センサ制御部19、I/O制御部20
及び光源制御部21を含んでいる。データ処理部4には
さらに表示部16、操作部17、外部入出力インターフ
ェース18が備えられている。FIG. 8 shows the data processing unit 4 in FIGS. 6 and 7 more specifically. The input / output port 10 in FIGS. 6 and 7 is an amplifier 1 that amplifies the output of the sensor 3.
2. A / D converter 13 for converting into a digital signal, input port 14, input data buffer 15, input port 22,
Output port 23, sensor control unit 19, I / O control unit 20
And a light source controller 21. The data processing unit 4 further includes a display unit 16, an operation unit 17, and an external input / output interface 18.
【0040】図6又は図7の実施例を用い、成分濃度を
求める処理の流れを図9のフローチャートにより説明す
る。データ処理部4の電源をオンにすると、全体の制御
部の電源がオンになり、データ処理部4にあるマイクロ
コンピュータ部分が初期化され、CPU6やRAM8な
どが初期設定される。マイクロコンピュータ動作が可能
になった後、記憶媒体9から測定と装置動作に関する初
期値データが読み込まれてRAM8へ書き込まれる。こ
のデータをもとに装置の初期設定作業が行なわれ、測定
の開始の指示を待つ。The flow of the process for obtaining the component concentration will be described with reference to the flowchart of FIG. 9 using the embodiment of FIG. 6 or 7. When the power supply of the data processing unit 4 is turned on, the power supply of the entire control unit is turned on, the microcomputer portion in the data processing unit 4 is initialized, and the CPU 6 and the RAM 8 are initialized. After the microcomputer operation becomes possible, the initial value data regarding the measurement and the device operation is read from the storage medium 9 and written in the RAM 8. Initialization work of the device is performed based on this data, and an instruction to start measurement is awaited.
【0041】試料が三角セル2に注入され、所定の場所
にセットされる。スタートボタンが押されると測定動作
を開始する。光源1又は1aからの測定光束が三角セル
2の入射面に対して垂直に入射し、三角セル2を透過し
た測定光がリニアセンサ3で受光される。リニアセンサ
3では光信号が電気信号に変換される。データ処理部4
では1つの測定波長に対するリニアセンサ3からの電気
信号をA/D変換してデジタル信号として取り込む。リ
ニアセンサ3からの電気信号から透過光強度Iと変位置
量Dを検出する。The sample is injected into the triangular cell 2 and set in a predetermined place. When the start button is pressed, the measurement operation starts. The measurement light beam from the light source 1 or 1a is incident perpendicularly on the incident surface of the triangular cell 2, and the measurement light transmitted through the triangular cell 2 is received by the linear sensor 3. The linear sensor 3 converts an optical signal into an electric signal. Data processing unit 4
Then, the electric signal from the linear sensor 3 for one measurement wavelength is A / D converted and taken in as a digital signal. The transmitted light intensity I and the displacement amount D are detected from the electric signal from the linear sensor 3.
【0042】次の測定波長に測定光を切り替える。測定
波長の切替えは、図6の実施例では光源1での点灯LD
素子の切替え、可変波長レーザの波長切替え又は分光器
の走査により行なわれ、図7の実施例では分光装置11
でのフィルタ切替えにより行なわれる。その切り換えた
測定波長でのリニアセンサ3からの電気信号を同じよう
にA/D変換して取り込む。このように、各測定波長ご
とにセル2を透過した光の強度Iと変位置量Dが検出さ
れて取り込まれる。The measurement light is switched to the next measurement wavelength. In the embodiment of FIG. 6, the switching of the measurement wavelength is performed by the lighting LD in the light source 1.
This is performed by switching the elements, switching the wavelength of the variable wavelength laser, or scanning the spectroscope. In the embodiment of FIG.
This is done by switching the filter at. The electric signal from the linear sensor 3 at the switched measurement wavelength is similarly A / D converted and captured. In this way, the intensity I and the displacement amount D of the light transmitted through the cell 2 are detected and captured for each measurement wavelength.
【0043】予定の波長でのリニアセンサ3からの電気
信号の取り込みを終了すると、変位置量Dから屈折率を
求め、この屈折率を用いて透過光強度を修正して吸光度
を求める。複数の測定波長での吸光度を用い、多変量解
析演算を行なって成分濃度を求める。その結果はレコー
ダ5などに出力する。最後にデータ処理部装置の電源を
オフにして測定を終了する。When the acquisition of the electric signal from the linear sensor 3 at the predetermined wavelength is completed, the refractive index is obtained from the displacement amount D, and the transmitted light intensity is corrected using this refractive index to obtain the absorbance. Using the absorbances at a plurality of measurement wavelengths, multivariate analysis calculation is performed to obtain the component concentration. The result is output to the recorder 5 or the like. Finally, the power of the data processing unit device is turned off to end the measurement.
【0044】図6又は図7の実施例を用い、各成分濃度
から比重を求める動作を図10のフローチャートにより
説明する。データ処理部装置の電源をオンにした後、試
料をセットして測定を始め、データの取込みを完了する
までの手順は図9のものと同じである。図10では屈折
率を求め、その屈折率を用いて透過光強度を修正して吸
光度を求め、その吸光度から多変量解析演算により成分
濃度を求める。尿試料に限らず、一般の溶液試料に対し
ては、各成分濃度が求まると、その全ての成分濃度の和
によって密度を求め、試料の比重を求める。The operation of obtaining the specific gravity from the concentration of each component will be described with reference to the flowchart of FIG. 10 using the embodiment of FIG. 6 or 7. The procedure from turning on the power of the data processing unit to setting the sample, starting the measurement, and completing the data acquisition is the same as in FIG. In FIG. 10, the refractive index is obtained, the transmitted light intensity is corrected using the refractive index to obtain the absorbance, and the component concentration is obtained from the absorbance by a multivariate analysis calculation. For not only urine samples but also general solution samples, when the concentration of each component is obtained, the density is obtained by the sum of the concentrations of all the components, and the specific gravity of the sample is obtained.
【0045】図6又は図7の実施例を用い、試料として
尿を測定する場合の尿の比重を求める動作を図11のフ
ローチャートにより説明する。この場合もデータ処理部
装値の電源をオンにし、試料をセットし、光源の波長を
切り換えて各波長でのリニアセンサ3からの電気信号を
デジタル値に変換して取り込むまでは図9及び図10の
動作と同じである。The operation of obtaining the specific gravity of urine when measuring urine as a sample will be described with reference to the flowchart of FIG. 11 using the embodiment of FIG. 6 or 7. In this case as well, the power supply of the data processing unit is turned on, the sample is set, the wavelength of the light source is switched, and the electric signal from the linear sensor 3 at each wavelength is converted into a digital value and fetched as shown in FIG. 9 and FIG. This is the same as the operation of 10.
【0046】図11では屈折率を求めて透過光強度を修
正して吸光度を求め、それをもとに多変量解析演算によ
り糖と蛋白の濃度を求める。一方、屈折率と比重の関係
を示す既知のデータを用い、それに測定により求めた屈
折率を適用してその尿試料の比重値を求める。一方、多
変量解析演算により求められた糖と蛋白の濃度により比
重値の補正を行なって結果を出力する。In FIG. 11, the refractive index is calculated, the transmitted light intensity is corrected, and the absorbance is calculated. Based on this, the sugar and protein concentrations are calculated by a multivariate analysis calculation. On the other hand, known data showing the relationship between the refractive index and the specific gravity is used, and the refractive index obtained by the measurement is applied to it to obtain the specific gravity value of the urine sample. On the other hand, the specific gravity value is corrected based on the sugar and protein concentrations obtained by the multivariate analysis calculation, and the result is output.
【0047】[0047]
【発明の効果】本発明では三角セルとリニアセンサを用
いることにより、セルを透過した測定光の透過光強度
と、リニアセンサ上での透過光の位置とを検出すること
により、透過光強度と液体試料の屈折率を同時に測定す
ることができるようになり、これにより屈折が透過率変
化を介して透過光強度へ与える影響を補正して吸光度を
高精度に測定することができるようになる。しかも、透
過光強度と屈折率を1台の測定装置で同時に測定できる
ので、装置の構成も簡単であり、操作も簡単ですむ。本
発明ではまた、このように液体試料の吸光度を各測定波
長ごとに正確に測定することができるので、多変量解析
演算により各成分濃度を高精度に算出することができ
る。本発明で尿試料に限らず一般の液体試料について
も、各成分濃度が正確に求まるので、それらを加算する
ことにより密度が計算でき、ひいては比重を求めること
ができる。本発明を尿試料の比重測定方法に適用すると
きは、その尿試料の屈折率と成分濃度が同時に測定でき
るので、屈折率から既知のデータを用いて比重を計算
し、その比重値に対し、同時に求めた糖と蛋白の濃度に
よる補正を行なうことによって尿比重を単一の測定装置
で精密に、かつ簡単に求めることができる。According to the present invention, by using the triangular cell and the linear sensor, the transmitted light intensity of the measuring light transmitted through the cell and the position of the transmitted light on the linear sensor are detected to obtain the transmitted light intensity. It becomes possible to measure the refractive index of the liquid sample at the same time, whereby the influence of refraction on the intensity of transmitted light through the change in transmittance can be corrected and the absorbance can be measured with high accuracy. Moreover, since the transmitted light intensity and the refractive index can be measured simultaneously by one measuring device, the device configuration is simple and the operation is simple. Further, in the present invention, since the absorbance of the liquid sample can be accurately measured for each measurement wavelength as described above, the concentration of each component can be calculated with high accuracy by the multivariate analysis calculation. In the present invention, not only the urine sample but also the general liquid sample can accurately determine the concentration of each component, so that by adding them, the density can be calculated, and thus the specific gravity can be determined. When the present invention is applied to the method for measuring the specific gravity of a urine sample, since the refractive index and the component concentration of the urine sample can be measured at the same time, the specific gravity is calculated using known data from the refractive index, and its specific gravity value, By performing correction based on the sugar and protein concentrations obtained at the same time, the specific gravity of urine can be accurately and easily obtained with a single measuring device.
【図1】本発明の装置を示すブロック図である。FIG. 1 is a block diagram showing an apparatus of the present invention.
【図2】屈折率と尿比重の標準基準を示す日本臨床病理
学会の提唱するノモグラムの表である。FIG. 2 is a nomogram table advocated by the Japanese Society of Clinical Pathology showing standard criteria for refractive index and urine specific gravity.
【図3】同ノモグラムのグラフである。FIG. 3 is a graph of the same nomogram.
【図4】本発明で三角セルを用いて透過光強度と屈折率
を同時に測定する原理を説明する図であり、(A)はセ
ルとリニアセンサを示す平面図、(B)はリニアセンサ
とリニアセンサが受光するセル透過光強度を示す図であ
る。4A and 4B are diagrams illustrating the principle of simultaneously measuring transmitted light intensity and refractive index using a triangular cell in the present invention, FIG. 4A is a plan view showing a cell and a linear sensor, and FIG. 4B is a linear sensor. It is a figure which shows the cell transmitted light intensity which a linear sensor receives.
【図5】セルへ照射された光の各界面での透過を模式的
に示すセルの断面図である。FIG. 5 is a cross-sectional view of a cell schematically showing transmission of light irradiated on the cell at each interface.
【図6】一実施例の全体の構成を示す概略ブロック図で
ある。FIG. 6 is a schematic block diagram showing the overall configuration of an embodiment.
【図7】他の実施例の全体の構成を示す概略ブロック図
である。FIG. 7 is a schematic block diagram showing the overall configuration of another embodiment.
【図8】一実施例におけるデータ処理部を示すブロック
図である。FIG. 8 is a block diagram illustrating a data processing unit according to an embodiment.
【図9】成分濃度を求める動作を示すフローチャート図
である。FIG. 9 is a flowchart showing an operation for obtaining a component concentration.
【図10】成分濃度から比重値を求める動作を示すフロ
ーチャート図である。FIG. 10 is a flowchart showing an operation for obtaining a specific gravity value from a component concentration.
【図11】尿試料の比重値を求める動作を示すフローチ
ャート図である。FIG. 11 is a flowchart showing an operation for obtaining a specific gravity value of a urine sample.
2 三角セル 3 リニアセンサ 30 屈折率算出部 31 吸光度算出部 32 成分濃度算出部 33 比重算出部 35 尿比重算出部 2 triangular cell 3 linear sensor 30 refractive index calculation unit 31 absorbance calculation unit 32 component concentration calculation unit 33 specific gravity calculation unit 35 urine specific gravity calculation unit
─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───
【手続補正書】[Procedure amendment]
【提出日】平成7年7月28日[Submission date] July 28, 1995
【手続補正1】[Procedure Amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】図2[Name of item to be corrected] Figure 2
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【図2】屈折率と尿比重の標準基準を示す日本臨床病理
学会の提唱するノモグラムの図表である。FIG. 2 is a nomogram chart advocated by the Japanese Society of Clinical Pathology showing standard criteria for refractive index and urine specific gravity.
Claims (8)
ている三角セルに液体試料を収容し、測定光束を前記入
射面に垂直な方向に入射させ、前記出射面から出射する
測定光束を光の強度と位置をともに検出できるリニアセ
ンサで受光し、測定光束の複数の測定波長の各波長ごと
に透過光強度を検出するとともに、そのリニアセンサ上
での測定光束位置から試料の屈折率を算出し、その算出
された屈折率、既知の大気屈折率及び既知のセル屈折率
を用いて三角セルでの透過率変化を介して透過光強度へ
与える影響を補正することを特徴とする吸光度測定方
法。1. A measurement light beam, in which a liquid sample is housed in a triangular cell whose emission surface is inclined with respect to the incident surface of the measurement light beam, the measurement light beam is made incident in a direction perpendicular to the incidence surface, and is emitted from the emission surface. Is received by a linear sensor that can detect both the intensity and position of the light, the transmitted light intensity is detected for each of the multiple measurement wavelengths of the measurement light beam, and the refractive index of the sample is measured from the position of the measurement light beam on the linear sensor. Is calculated, and the calculated refractive index, known atmospheric refractive index, and known cell refractive index are used to correct the influence on the transmitted light intensity through the change in transmittance in the triangular cell, and the absorbance is characterized by Measuring method.
ている三角セルに液体試料を収容し、測定光束を前記入
射面に垂直な方向に入射させ、前記出射面から出射する
測定光束を光の強度と位置をともに検出できるリニアセ
ンサで受光し、測定光束の複数の測定波長の各波長ごと
に透過光強度を検出するとともに、そのリニアセンサ上
での測定光束位置から試料の屈折率を算出し、その算出
された屈折率、既知の大気屈折率及び既知のセル屈折率
を用いて三角セルでの透過率変化を介して透過光強度へ
与える影響を補正して各測定波長ごとの吸光度を算出
し、多変量解析演算を行なって各成分濃度を算出する液
体試料の成分濃度測定方法。2. A measurement light flux, in which a liquid sample is housed in a triangular cell whose emission surface is inclined with respect to the incidence surface of the measurement light flux, the measurement light flux is made incident in a direction perpendicular to the incidence surface, and which is emitted from the emission surface. Is received by a linear sensor that can detect both the intensity and position of the light, the transmitted light intensity is detected for each of the multiple measurement wavelengths of the measurement light beam, and the refractive index of the sample is measured from the position of the measurement light beam on the linear sensor. The calculated refractive index, the known atmospheric refractive index and the known cell refractive index are used to correct the effect on the transmitted light intensity via the transmittance change in the triangular cell for each measurement wavelength. A method for measuring the component concentration of a liquid sample, which calculates the absorbance and performs multivariate analysis calculation to calculate the concentration of each component.
ている三角セルに液体試料を収容し、測定光束を前記入
射面に垂直な方向に入射させ、前記出射面から出射する
測定光束を光の強度と位置をともに検出できるリニアセ
ンサで受光し、測定光束の複数の測定波長の各波長ごと
に透過光強度を検出するとともに、そのリニアセンサ上
での測定光束位置から試料の屈折率を算出し、その算出
された屈折率、既知の大気屈折率及び既知のセル屈折率
を用いて三角セルでの透過率変化を介して透過光強度へ
与える影響を補正して各測定波長ごとの吸光度を算出
し、多変量解析演算を行なって各成分濃度を算出し、算
出された各成分濃度を加算して密度を算出し、それをも
とに比重を算出することを特徴とする液体試料の比重測
定方法。3. A measurement light flux, in which a liquid sample is housed in a triangular cell whose emission surface is inclined with respect to the incident surface of the measurement light flux, the measurement light flux is incident in a direction perpendicular to the incidence surface, and the measurement light flux is emitted from the emission surface. Is received by a linear sensor that can detect both the intensity and position of the light, the transmitted light intensity is detected for each of the multiple measurement wavelengths of the measurement light beam, and the refractive index of the sample is measured from the position of the measurement light beam on the linear sensor. The calculated refractive index, the known atmospheric refractive index and the known cell refractive index are used to correct the effect on the transmitted light intensity via the transmittance change in the triangular cell for each measurement wavelength. A liquid sample characterized by calculating the absorbance, performing multivariate analysis calculation to calculate the concentration of each component, adding the calculated concentration of each component to calculate the density, and then calculating the specific gravity based on it. Specific gravity measurement method.
に対し出射面が傾斜している三角セルに液体試料を収容
し、測定光束を前記入射面に垂直な方向に入射させ、前
記出射面から出射する測定光束を光の強度と位置をとも
に検出できるリニアセンサで受光し、測定光束の複数の
測定波長の各波長ごとに透過光強度を検出するととも
に、そのリニアセンサ上での測定光束位置から試料の屈
折率を算出し、 その算出された屈折率、既知の大気屈折率及び既知のセ
ル屈折率を用いて三角セルでの透過率変化を介して透過
光強度へ与える影響を補正して各測定波長ごとの吸光度
を算出し、多変量解析演算を行なって各成分濃度を算出
し、 尿の屈折率と比重との関係を示す既知のデータを用い、
前記で求められた試料屈折率をそのデータにあてはめて
その尿試料の比重を求め、 前記で算出された成分濃度のうちのブドウ糖と蛋白の濃
度に対応する尿比重上昇分を補正することを特徴とする
尿比重測定方法。4. The liquid solution is urine, and the liquid sample is housed in a triangular cell whose output surface is inclined with respect to the incident surface of the measurement light beam, and the measurement light beam is made incident in a direction perpendicular to the incident surface. The measurement light flux emitted from the exit surface is received by a linear sensor that can detect both the intensity and position of the light, the transmitted light intensity is detected for each of the multiple measurement wavelengths of the measurement light flux, and the measurement is performed on the linear sensor. The refractive index of the sample is calculated from the position of the light beam, and the calculated refractive index, known atmospheric refractive index, and known cell refractive index are used to correct the effect on the transmitted light intensity through the change in transmittance in the triangular cell. Then calculate the absorbance for each measurement wavelength, calculate the concentration of each component by performing a multivariate analysis calculation, using known data showing the relationship between the refractive index and specific gravity of urine,
The sample refractive index obtained above is applied to the data to obtain the specific gravity of the urine sample, and the increase in urine specific gravity corresponding to the glucose and protein concentrations of the component concentrations calculated above is corrected. Urine specific gravity measurement method.
対し出射面が傾斜した三角セル(2)と、 測定光束が三角セル(2)の入射面に対して垂直方向に
入射するように測定光路が設定された測定光学系と、 三角セル(2)の出射面から出射する測定光束を受光す
る位置に設けられ、光の強度と位置をともに検出できる
リニアセンサ(3)と、 三角セル(2)に屈折率が既知の液体を入れて測定した
ときの三角セル(2)からの出射光を前記リニアセンサ
(3)で受光したときの検出位置を基準とし、三角セル
(2)に屈折率が未知の試料を入れて測定したときの三
角セル(2)からの出射光を前記リニアセンサ(3)で
受光したときの検出位置の変位置量を検出し、その変位
置量に対応する試料の屈折率を検量線又は計算により算
出する屈折率算出部(30)と、 三角セル(2)からの出射光を前記リニアセンサ(3)
で受光したときの透過光強度、大気の屈折率及びセルの
屈折率、並びに屈折率算出部(30)で算出された試料
の屈折率を用いて三角セル(2)での透過率変化の影響
を補正した成分濃度に依存する吸光度を算出する吸光度
算出部(31)と、を備えたことを特徴とする吸光度測
定装置。5. A triangular cell (2) for accommodating a liquid sample, the exit surface of which is inclined with respect to the incident surface of the measuring light beam, and the measuring light beam so as to enter in a direction perpendicular to the incident surface of the triangular cell (2). A measurement optical system having a measurement optical path set in, a linear sensor (3) provided at a position for receiving the measurement light flux emitted from the emission surface of the triangular cell (2), and capable of detecting both the intensity and the position of the light; The triangular cell (2) is based on the detection position when the light emitted from the triangular cell (2) when the liquid having a known refractive index is put into the cell (2) and measured is received by the linear sensor (3). The variable amount of the detection position when the light emitted from the triangular cell (2) when the sample having an unknown refractive index is put into the measurement is received by the linear sensor (3) is detected, and the variable amount is detected. The refractive index of the corresponding sample is calculated using a calibration curve or calculation. Light output from the folding rate calculation unit (30) and the triangular cell (2) is input to the linear sensor (3).
Influence of the transmittance change in the triangular cell (2) by using the transmitted light intensity when received by the device, the atmospheric refractive index and the cell refractive index, and the sample refractive index calculated by the refractive index calculation unit (30) An absorbance measuring device comprising: an absorbance calculating unit (31) for calculating the absorbance depending on the corrected component concentration.
対し出射面が傾斜した三角セル(2)と、 測定光束が三角セル(2)の入射面に対して垂直方向に
入射するように測定光路が設定された測定光学系と、 三角セル(2)の出射面から出射する測定光束を受光す
る位置に設けられ、光の強度と位置をともに検出できる
リニアセンサ(3)と、 三角セル(2)に屈折率が既知の液体を入れて測定した
ときの三角セル(2)からの出射光を前記リニアセンサ
(3)で受光したときの検出位置を基準とし、三角セル
(2)に屈折率が未知の試料を入れて測定したときの三
角セル(2)からの出射光を前記リニアセンサ(3)で
受光したときの検出位置の変位置量を検出し、その変位
置量に対応する試料の屈折率を検量線又は計算により算
出する屈折率算出部(30)と、 三角セル(2)からの出射光を前記リニアセンサ(3)
で受光したときの透過光強度、大気の屈折率及びセルの
屈折率、並びに屈折率算出部(30)で算出された試料
の屈折率を用いて三角セル(2)での透過率変化の影響
を補正した成分濃度に依存する吸光度を算出する吸光度
算出部(31)と、 吸光度算出部(31)で算出された複数測定波長での成
分濃度に依存する吸光度をもとに多変量解析演算を行な
って各成分濃度を算出する成分濃度算出部(32)と、
を備えたことを特徴とする成分濃度測定装置。6. A triangular cell (2) containing a liquid sample and having an exit surface inclined with respect to the incident surface of the measuring light beam, and a measuring light beam incident on the incident surface of the triangular cell (2) in a direction perpendicular thereto. A measurement optical system having a measurement optical path set in, a linear sensor (3) provided at a position for receiving the measurement light flux emitted from the emission surface of the triangular cell (2), and capable of detecting both the intensity and the position of the light; The triangular cell (2) is based on the detection position when the light emitted from the triangular cell (2) when the liquid having a known refractive index is put into the cell (2) and measured is received by the linear sensor (3). The variable amount of the detection position when the light emitted from the triangular cell (2) when the sample having an unknown refractive index is put into the measurement is received by the linear sensor (3) is detected, and the variable amount is detected. The refractive index of the corresponding sample is calculated using a calibration curve or calculation. Light output from the folding rate calculation unit (30) and the triangular cell (2) is input to the linear sensor (3).
Influence of the transmittance change in the triangular cell (2) by using the transmitted light intensity when received by the device, the atmospheric refractive index and the cell refractive index, and the sample refractive index calculated by the refractive index calculation unit (30) A multivariate analysis calculation is performed based on the absorbance calculation unit (31) that calculates the absorbance that depends on the component concentration corrected for and the absorbance that is calculated by the absorbance calculation unit (31) that depends on the component concentrations at multiple measurement wavelengths. And a component concentration calculation unit (32) for calculating each component concentration.
A component concentration measuring device comprising:
対し出射面が傾斜した三角セル(2)と、 測定光束が三角セル(2)の入射面に対して垂直方向に
入射するように測定光路が設定された測定光学系と、 三角セル(2)の出射面から出射する測定光束を受光す
る位置に設けられ、光の強度と位置をともに検出できる
リニアセンサ(3)と、 三角セル(2)に屈折率が既知の液体を入れて測定した
ときの三角セル(2)からの出射光を前記リニアセンサ
(3)で受光したときの検出位置を基準とし、三角セル
(2)に屈折率が未知の試料を入れて測定したときの三
角セル(2)からの出射光を前記リニアセンサ(3)で
受光したときの検出位置の変位置量を検出し、その変位
置量に対応する試料の屈折率を検量線又は計算により算
出する屈折率算出部(30)と、 三角セル(2)からの出射光を前記リニアセンサ(3)
で受光したときの透過光強度、大気の屈折率及びセルの
屈折率、並びに屈折率算出部(30)で算出された試料
の屈折率を用いて三角セル(2)での透過率変化の影響
を補正した成分濃度に依存する吸光度を算出する吸光度
算出部(31)と、 吸光度算出部(31)で算出された複数測定波長での成
分濃度に依存する吸光度をもとに多変量解析演算を行な
って各成分濃度を算出する成分濃度算出部(32)と、 成分濃度算出部(32)で算出された各成分濃度を加算
して密度を算出し、それをもとに比重を算出する比重算
出部(33)と、を備えたことを特徴とする比重測定装
置。7. A triangular cell (2) for accommodating a liquid sample, the exit surface of which is inclined with respect to the incident surface of the measuring light beam, and the measuring light beam so as to enter in a direction perpendicular to the incident surface of the triangular cell (2). A measurement optical system having a measurement optical path set in, a linear sensor (3) provided at a position for receiving the measurement light flux emitted from the emission surface of the triangular cell (2), and capable of detecting both the intensity and the position of the light; The triangular cell (2) is based on the detection position when the light emitted from the triangular cell (2) when the liquid having a known refractive index is put into the cell (2) and measured is received by the linear sensor (3). The variable amount of the detection position when the light emitted from the triangular cell (2) when the sample having an unknown refractive index is put into the measurement is received by the linear sensor (3) is detected, and the variable amount is detected. The refractive index of the corresponding sample is calculated using a calibration curve or calculation. Light output from the folding rate calculation unit (30) and the triangular cell (2) is input to the linear sensor (3).
Influence of the transmittance change in the triangular cell (2) by using the transmitted light intensity when received by the device, the atmospheric refractive index and the cell refractive index, and the sample refractive index calculated by the refractive index calculation unit (30) A multivariate analysis calculation is performed based on the absorbance calculation unit (31) that calculates the absorbance that depends on the component concentration corrected for and the absorbance that is calculated by the absorbance calculation unit (31) that depends on the component concentrations at multiple measurement wavelengths. The specific gravity for calculating the density by adding each component concentration calculated by the component concentration calculating unit (32) which calculates the component concentration and the component concentration calculating unit (32). A specific gravity measuring device comprising: a calculator (33).
対し出射面が傾斜した三角セル(2)と、 測定光束が三角セル(2)の入射面に対して垂直方向に
入射するように測定光路が設定された測定光学系と、 三角セル(2)の出射面から出射する測定光束を受光す
る位置に設けられ、光の強度と位置をともに検出できる
リニアセンサ(3)と、 三角セル(2)に屈折率が既知の液体を入れて測定した
ときの三角セル(2)からの出射光を前記リニアセンサ
(3)で受光したときの検出位置を基準とし、三角セル
(2)に屈折率が未知の試料を入れて測定したときの三
角セル(2)からの出射光を前記リニアセンサ(3)で
受光したときの検出位置の変位置量を検出し、その変位
置量に対応する試料の屈折率を検量線又は計算により算
出する屈折率算出部(30)と、 三角セル(2)からの出射光を前記リニアセンサ(3)
で受光したときの透過光強度、大気の屈折率及びセルの
屈折率、並びに屈折率算出部(30)で算出された試料
の屈折率を用いて三角セル(2)での透過率変化の影響
を補正した成分濃度に依存する吸光度を算出する吸光度
算出部(31)と、 吸光度算出部(31)で算出された複数測定波長での成
分濃度に依存する吸光度をもとに多変量解析演算を行な
って各成分濃度を算出する成分濃度算出部(32)と、 尿の屈折率と比重との関係を示す既知のデータを用い、
屈折率算出部(30)で求められた試料屈折率をそのデ
ータにあてはめてその尿試料の比重を求め、成分濃度算
出部(32)で算出された成分濃度のうちのブドウ糖と
蛋白の濃度に対応する尿比重上昇分を補正する尿比重算
出部(35)と、を備えたことを特徴とする尿比重測定
装置。8. A triangular cell (2) containing a liquid sample and having an exit surface inclined with respect to the incident surface of the measuring light beam, and a measuring light beam so as to enter in a direction perpendicular to the incident surface of the triangular cell (2). A measurement optical system having a measurement optical path set in, a linear sensor (3) provided at a position for receiving the measurement light flux emitted from the emission surface of the triangular cell (2), and capable of detecting both the intensity and the position of the light; The triangular cell (2) is based on the detection position when the light emitted from the triangular cell (2) when the liquid having a known refractive index is put into the cell (2) and measured is received by the linear sensor (3). The variable amount of the detection position when the light emitted from the triangular cell (2) when the sample having an unknown refractive index is put into the measurement is received by the linear sensor (3) is detected, and the variable amount is detected. The refractive index of the corresponding sample is calculated using a calibration curve or calculation. Light output from the folding rate calculation unit (30) and the triangular cell (2) is input to the linear sensor (3).
Influence of the transmittance change in the triangular cell (2) by using the transmitted light intensity when received by the device, the atmospheric refractive index and the cell refractive index, and the sample refractive index calculated by the refractive index calculation unit (30) A multivariate analysis calculation is performed based on the absorbance calculation unit (31) that calculates the absorbance that depends on the component concentration corrected for and the absorbance that is calculated by the absorbance calculation unit (31) that depends on the component concentrations at multiple measurement wavelengths. Using the component concentration calculation unit (32) that calculates the concentration of each component and known data indicating the relationship between the refractive index and specific gravity of urine,
The specific refractive index of the urine sample is calculated by applying the sample refractive index obtained by the refractive index calculation unit (30) to the data, and the specific concentration of glucose and protein in the component concentrations calculated by the component concentration calculation unit (32) is calculated. A urine specific gravity measuring device comprising: a urine specific gravity calculating section (35) for correcting a corresponding increase in urine specific gravity.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13727795A JPH0843301A (en) | 1994-05-11 | 1995-05-10 | Method and device for measuring absorbance, component concentration or specific gravity of liquid sample |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6-123053 | 1994-05-11 | ||
| JP12305394 | 1994-05-11 | ||
| JP13727795A JPH0843301A (en) | 1994-05-11 | 1995-05-10 | Method and device for measuring absorbance, component concentration or specific gravity of liquid sample |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0843301A true JPH0843301A (en) | 1996-02-16 |
Family
ID=26460069
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13727795A Pending JPH0843301A (en) | 1994-05-11 | 1995-05-10 | Method and device for measuring absorbance, component concentration or specific gravity of liquid sample |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0843301A (en) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006105998A (en) * | 2004-10-07 | 2006-04-20 | Wyatt Technol Corp | Upgraded differential refractometer and measuring method for measuring differential refractive index |
| WO2008133281A1 (en) * | 2007-04-24 | 2008-11-06 | Canon Semiconductor Equipment Inc. | Concentration measuring method and system using refractivity distribution in flowing state |
| CN114270169A (en) * | 2019-09-18 | 2022-04-01 | 株式会社富士金 | Concentration measuring device |
| CN116559115A (en) * | 2023-01-15 | 2023-08-08 | 杭州齐威仪器有限公司 | Method for measuring solution concentration by using refractometer |
| JP2024035829A (en) * | 2022-09-02 | 2024-03-14 | アウトセンス ダイアグノスティクス リミテッド | urine analysis |
| CN120522112A (en) * | 2025-07-25 | 2025-08-22 | 深圳市安帕尔科技有限公司 | Gas identification and concentration detection method and system based on machine learning |
-
1995
- 1995-05-10 JP JP13727795A patent/JPH0843301A/en active Pending
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006105998A (en) * | 2004-10-07 | 2006-04-20 | Wyatt Technol Corp | Upgraded differential refractometer and measuring method for measuring differential refractive index |
| WO2008133281A1 (en) * | 2007-04-24 | 2008-11-06 | Canon Semiconductor Equipment Inc. | Concentration measuring method and system using refractivity distribution in flowing state |
| CN114270169A (en) * | 2019-09-18 | 2022-04-01 | 株式会社富士金 | Concentration measuring device |
| JP2024035829A (en) * | 2022-09-02 | 2024-03-14 | アウトセンス ダイアグノスティクス リミテッド | urine analysis |
| CN116559115A (en) * | 2023-01-15 | 2023-08-08 | 杭州齐威仪器有限公司 | Method for measuring solution concentration by using refractometer |
| CN120522112A (en) * | 2025-07-25 | 2025-08-22 | 深圳市安帕尔科技有限公司 | Gas identification and concentration detection method and system based on machine learning |
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