JPS6218862B2 - - Google Patents
Info
- Publication number
- JPS6218862B2 JPS6218862B2 JP56144712A JP14471281A JPS6218862B2 JP S6218862 B2 JPS6218862 B2 JP S6218862B2 JP 56144712 A JP56144712 A JP 56144712A JP 14471281 A JP14471281 A JP 14471281A JP S6218862 B2 JPS6218862 B2 JP S6218862B2
- Authority
- JP
- Japan
- Prior art keywords
- component
- time
- approximation
- components
- light
- 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.)
- Expired
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N2021/6417—Spectrofluorimetric devices
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/6445—Measuring fluorescence polarisation
Landscapes
- Health & Medical Sciences (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
Description
【発明の詳細な説明】
本発明は、螢光偏光測定装置に係り、特に反応
の経時変化を測定し、該測定値より一定時間後の
値を外挿するのに好適な機能を有する装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a fluorescence polarization measuring device, and more particularly to a device having a function suitable for measuring changes in a reaction over time and extrapolating a value after a certain period of time from the measured value. .
経時的に変化する反応においては、目的とする
測定時間において直接測定値が得られない場合が
ある。 In reactions that change over time, direct measurement values may not be obtained at the intended measurement time.
例えば、反応停止直前の測定値を求めたいが、
反応を停止させるために試料を測定部から取り出
さなければならない場合、同一試料にて、二つ以
上の現象を同一時刻に測定しなければならない場
合、反応液中のある成分を過するが、過の中
間時間における測定値を必要とする場合等があ
る。これらの測定においては、ある限られた時間
の測定値から近似を行い、目的とする測定時間で
の値を算出することが一般的に行われている。 For example, if you want to find the measured value just before the reaction stops,
When the sample must be removed from the measuring section to stop the reaction, or when two or more phenomena must be measured at the same time on the same sample, certain components in the reaction solution may be lost, but There are cases where measured values at intermediate times are required. In these measurements, it is common practice to make approximations from measured values over a limited period of time to calculate values at the intended measurement time.
特に本発明に係る螢光偏光測定の場合には、同
一試料に対して垂直偏光成分と水平偏光成分を別
別に測定しなければならず、目的とする時間に両
者の成分を同時に測定することはできない。従つ
て測定値による近似(外挿)を行い目的とする時
間での値を求めなければならない。 In particular, in the case of fluorescence polarization measurement according to the present invention, the vertical polarization component and the horizontal polarization component must be measured separately for the same sample, and it is impossible to measure both components at the same time at the desired time. Can not. Therefore, it is necessary to approximate (extrapolate) the measured values to find the value at the desired time.
従来一般的に行われていた方法は、アナログ記
録計に記録されたデータに直線定規を外挿し、直
線近似を行つていた。ところが物質の経時変化特
に生体関連物質の変化は単一の物質の直線的な変
化よりも、複数の物質の総合された変化が生じる
ため、観測される反応過程は、曲線的に反応が進
行する場合が多い。 The conventional method has been to extrapolate a straight line ruler to the data recorded on an analog recorder to make a straight line approximation. However, changes in substances over time, especially changes in biologically related substances, involve integrated changes in multiple substances rather than linear changes in a single substance, so the observed reaction process progresses in a curved manner. There are many cases.
曲線的に反応が進行している場合に、直線近似
を行うことは、誤差の原因となる。また曲線定規
を使用したとしても、反応曲線の曲率と定規を合
致させることは、非常に困難である。また測定者
がマニユアルに近似を行うことは、個人者が伴い
近似値のバラツキが生じ不正確である。 When the reaction progresses in a curved manner, linear approximation causes errors. Furthermore, even if a curve ruler is used, it is very difficult to match the curvature of the reaction curve with the ruler. Furthermore, manual approximation by a measurer is inaccurate because the approximations vary depending on the individual.
本発明は上述した従来技術のもつ欠点を解決し
反応に即した近似を行い、かつ近似によつて得ら
れた値から、螢光偏光測定における偏光度を求め
ようとするものである。 The present invention solves the above-mentioned drawbacks of the prior art, performs an approximation based on the reaction, and determines the degree of polarization in fluorescence polarization measurement from the value obtained by the approximation.
本発明の目的は、生体関連物質の反応過程の近
似を効果的に行うことにより、該近似によつて得
られた外挿値から、誤差を僅少にした螢光偏光度
を得る装置を提供するにある。 An object of the present invention is to provide an apparatus that effectively approximates the reaction process of biologically related substances and obtains a degree of fluorescence polarization with minimal error from the extrapolated value obtained by the approximation. It is in.
本発明は、生体関連物質の反応が直線的または
曲線的に進行することを実験的に確認し、この反
応に即した近似を行い、かつ曲線近似のみの場合
曲率が強調され誤差が拡大されることを、解消す
るために、直線近似と曲線近似の組み合わせを行
うようにしたことにある。こうした近似により、
目的とする螢光偏光度を求める。 The present invention experimentally confirms that reactions of biological substances proceed in a linear or curved manner, and performs approximations based on this reaction, and in the case of only curve approximation, curvature is emphasized and errors are magnified. In order to solve this problem, we combined linear approximation and curve approximation. With these approximations,
Find the desired degree of fluorescence polarization.
第1図に本発明による実施例の機能系統図を示
す。 FIG. 1 shows a functional system diagram of an embodiment according to the present invention.
光源1から発した白色光は励起側分光器2によ
つて、単色光に分光されたのち励起側偏光子3で
偏光され、測定キユベツト4に照射される。測定
キユベツト内の試料は、励起されて螢光を発す
る。該螢光は、螢光側偏光子7を通過し螢光側分
光器8に導びかれる。螢光側分光器に入射した光
は、指定の螢光波長の単色光に分光され、該単色
光のみ光検知器9に到達する。 White light emitted from a light source 1 is separated into monochromatic light by an excitation side spectrometer 2, polarized by an excitation side polarizer 3, and irradiated onto a measurement cuvette 4. The sample in the measurement cuvette is excited and emits fluorescence. The fluorescent light passes through a fluorescent polarizer 7 and is guided to a fluorescent spectroscope 8. The light incident on the fluorescence-side spectroscope is split into monochromatic light having a designated fluorescence wavelength, and only this monochromatic light reaches the photodetector 9.
試料を測定キユベツトに入れ、該キユベツトを
測光位置にセツトし、測定を開始すると制御部1
2からの制御信号により、パルスモータ13が動
作し、励起側偏光子は垂直成分の励起光のみ通過
させるようにセツトされる。 When the sample is placed in the measurement cuvette, the cuvette is set at the photometry position, and the measurement is started, the controller 1
The pulse motor 13 is operated by the control signal from the pump 2, and the excitation side polarizer is set so as to pass only the vertical component of the excitation light.
他方、螢光側偏光子は制御部からの指令信号に
より、パルスモータ14が動作し、これによつて
駆動される。この駆動は、一定時間間隔にて90゜
回転が、間欠的に繰り返し行われる。 On the other hand, the fluorescent side polarizer is driven by the pulse motor 14 operated by a command signal from the control section. In this drive, 90° rotation is intermittently repeated at regular time intervals.
すなわち励起された試料から発した螢光は、偏
光励起光に対して、直交する成分の光と、平行な
成分の光に分別されて、光検知器に到達する。 That is, the fluorescent light emitted from the excited sample is separated into a light component orthogonal to the polarized excitation light and a light component parallel to the polarized excitation light before reaching the photodetector.
光検知器で検知された光信号は、電気信号に変
換され、前置増幅器10を経て、A/D変換器1
1によりデイジタル信号に変換される。 The optical signal detected by the photodetector is converted into an electrical signal, passed through a preamplifier 10, and then sent to an A/D converter 1.
1 is converted into a digital signal.
垂直な成分の光及び平行な成分の光は、それぞ
れA/D変換器により、デイジタル信号に変換さ
れた後、メモリー部15に記憶される。一定時間
測定が行われると、制御部の指令により過が行
われる。測定キユベツト4に収容されていた試料
は、過部6を通り、ここで粒子等の成分は別
され、溶液のみが測定キユベツト5に回収され
る。過液が収容された測光キユベツト2が、前
記測光キユベツト1に代つて測光位置に移動し、
過液の螢光強度の測定が行われる。 The perpendicular component light and the parallel component light are each converted into digital signals by an A/D converter and then stored in the memory section 15. After the measurement has been carried out for a certain period of time, the measurement is carried out according to a command from the control section. The sample contained in the measurement cuvette 4 passes through a filter section 6, where components such as particles are separated, and only the solution is collected in the measurement cuvette 5. The photometric cuvette 2 containing the liquid is moved to the photometric position in place of the photometric cuvette 1,
A measurement of the fluorescence intensity of the superfluous liquid is made.
ここで、過を行つている時間の中間の時刻
(第2図、第3図に示すTf)までは反応が進行し
ていたと考えられる。しかしながら時刻Tfにお
いて、実際に測定を行うことは不可能である。従
つて本発明請求範囲に述べる通り、ある限られた
時間内の測定値に基づいて近似を行い、時刻Tf
に対する外挿を行う。 Here, the reaction is considered to have progressed until the middle time (T f shown in FIGS. 2 and 3). However, it is impossible to actually perform measurements at time T f . Therefore, as stated in the claims of the present invention, approximation is performed based on measured values within a certain limited time, and the time T f
Perform extrapolation for .
具体的には、メモリー部に記憶された垂直成分
の光信号のデータ及び平行成分の光信号のデータ
を用いて、演算部14により近似式の作成を行
う。 Specifically, the arithmetic unit 14 creates an approximate expression using the vertical component optical signal data and the parallel component optical signal data stored in the memory unit.
本測定における測定例を第2図、第3図に示
す。実線で示したものが、実際に測定されたデー
タであり、点線で示したものが近似式によつて得
られた直線または曲線である。 Measurement examples in this measurement are shown in FIGS. 2 and 3. The solid line indicates actually measured data, and the dotted line indicates a straight line or curve obtained by an approximate formula.
反応は必ずしも直線的に進行する場合だけでな
く、曲線を描く場合が多い。従つて本発明におい
ては、垂直成分、平行成分の両成分ともに、直線
近似を行う場合と曲線近似を行う場合及び一方の
成分は直線近似を行い、他方の成分は曲線近似を
行う三者を実施し、実測に即した近似を行わせる
ようにした。特に第3図に示すように、平行成分
の光信号が直線近似にフイツトし、垂直成分の光
信号が曲線近似にフイツトすることは、実測デー
タとして観測される。こうした実測例において、
両成分ともに直線近似または、曲線近似のみを行
なうことは、外挿値の誤差を拡大することにな
る。 Reactions do not necessarily proceed linearly, but often follow a curve. Therefore, in the present invention, both vertical and parallel components are subjected to linear approximation, curve approximation is performed, and linear approximation is performed for one component, and curve approximation is performed for the other component. The approximation was made based on actual measurements. In particular, as shown in FIG. 3, it is observed as actual measurement data that the parallel component optical signal fits into a straight line approximation, and the perpendicular component optical signal fits into a curved line approximation. In these actual measurement examples,
Performing only linear approximation or curve approximation for both components will increase the error in the extrapolated value.
更に本発明においては、下記の演算式により螢
光偏光度:Pの演算を行う。 Furthermore, in the present invention, the fluorescence polarization degree: P is calculated using the following calculation formula.
P=(I⊥(T)−I⊥(F))−(I(T)−I(F))×G/(I⊥(T)−I⊥(F))+(I(T)−I
(F))×G
ここで
I⊥(T):垂直成分のTfにおける近似値
I(T):平行成分のTfにおける近似値
I⊥(F):過溶液の垂直成分の螢光偏光強度
I(F):過溶液の平行成分の螢光偏光強度
G:励起側偏光子を水平にした時に得られる装置
定数である。 P=(I⊥(T)-I⊥(F))-(I(T)-I(F))×G/(I⊥(T)-I⊥(F))+(I(T)- I
(F))×G where I⊥(T): Approximate value of vertical component at T f I(T): Approximate value of parallel component at T f I⊥(F): Fluorescence polarization of perpendicular component of supersolution Intensity I(F): Fluorescent polarization intensity of parallel component of hypersolution G: Device constant obtained when the excitation side polarizer is horizontal.
上式によつて求められる螢光偏光度:Pは、I
⊥(T)及びI(T)が誤差をもつ場合は、当
然誤差を生じる。また外挿近似値、I⊥(T)及
びT(T)が実際の反応から、かけはなれた値
を近似した場合には、Pの値も実際の反応に即さ
ないものとなる。 The degree of fluorescence polarization determined by the above formula: P is I
If ⊥(T) and I(T) have an error, an error will naturally occur. Furthermore, if the extrapolation approximations, I⊥(T) and T(T), approximate values that are far from the actual reaction, the value of P will also not correspond to the actual reaction.
本発明における表示部17には、得られた3種
類の近似値及び、各々の螢光偏光度Pが印字され
る。 The three types of approximate values obtained and the degree of fluorescence polarization P for each are printed on the display section 17 in the present invention.
本発明により下記の効果が得られる。 The present invention provides the following effects.
1 従来行われていた用手法による近似(直線定
規による直線外挿)のもつ特長を生かし、かつ
曲線を描く反応曲線を直線近似した場合の誤差
を低減し、外挿値の精度の向上をはかる。1. Take advantage of the advantages of conventional manual approximation (linear extrapolation using a straight line ruler), reduce errors when linearly approximating a curved reaction curve, and improve the accuracy of extrapolated values. .
2 直線近似のみによる外挿近似だけでなく、曲
線近似及び、直線近似と曲線近似の組み合わせ
による近似を行うことにより、実際の反応に即
応した近似が可能となる。2. By performing not only extrapolation approximation using only linear approximation, but also approximation using curve approximation and a combination of linear approximation and curve approximation, approximation that immediately responds to the actual reaction becomes possible.
3 いちいち測定者が、手で近似を行う煩雑さが
解消され、測定者による個人差がなくなる。3. The complexity of having to make approximations by hand for each measurer is eliminated, and individual differences among measurers are eliminated.
4 本発明における実施例で述べたように、一方
の成分が直線的に変化し、他方の成分が曲線的
に変化する場合には、本発明は極めて有効であ
る。4. As described in the embodiments of the present invention, the present invention is extremely effective when one component changes linearly and the other component changes curved.
5 直線近似、曲線近似及び両者の組み合わせに
よつて得られた外挿値から、螢光偏光度:Pの
値を演算、表示することにより研究者に、反応
の過程を数値的に情報として提供することが、
可能となる。5 Calculate and display the value of the degree of fluorescence polarization: P from the extrapolated values obtained by linear approximation, curve approximation, and a combination of both to provide researchers with numerical information on the reaction process. What you can do is
It becomes possible.
第1図は、本発明の一実施例の機能系統図であ
り、第2図および第3図は、本発明の一実施例の
近似法の説明図である。
1……光源、3,7……偏光子、4,5……キ
ユベツト、9……検知器、16……演算部。
FIG. 1 is a functional system diagram of an embodiment of the present invention, and FIGS. 2 and 3 are explanatory diagrams of an approximation method of an embodiment of the present invention. 1... Light source, 3, 7... Polarizer, 4, 5... Cubeette, 9... Detector, 16... Arithmetic unit.
Claims (1)
入れ、該キユベツトの懸濁状態の試料液と該試料
液のろ液に偏光した励起光を照射して、前記物質
が放射する螢光を、平行偏光成分と垂直偏光成分
とに分けて、両成分の光強度を計測する装置にお
いて、両成分のある限られた時間内の測定値よ
り、一方の成分においては近似直線を作成し、他
方の成分においては近似曲線を作成し、一定時間
後の値を読み出す機能とを備え、上記試料液の上
記両成分に関する上記一定時間後の値および上記
ろ液の上記両成分の光強度から螢光偏光度を求め
ることを特徴とした螢光偏光測定装置。1. A time-varying substance is placed in a photometric cuvette, and polarized excitation light is irradiated onto the suspended sample solution in the cuvette and the filtrate of the sample solution, so that the fluorescent light emitted by the substance is collimated. In a device that separates the polarized light component and the vertically polarized light component and measures the light intensity of both components, an approximate straight line is created for one component from the measured values of both components within a certain limited time, and an approximate straight line is created for the other component. is equipped with a function to create an approximate curve and read out the values after a certain period of time, and calculates the degree of fluorescence polarization from the values after the certain period of time for both components of the sample solution and the light intensity of both components of the filtrate. A fluorescence polarization measuring device characterized by determining the .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56144712A JPS5847238A (en) | 1981-09-16 | 1981-09-16 | Fluorescence polarization measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56144712A JPS5847238A (en) | 1981-09-16 | 1981-09-16 | Fluorescence polarization measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5847238A JPS5847238A (en) | 1983-03-18 |
| JPS6218862B2 true JPS6218862B2 (en) | 1987-04-24 |
Family
ID=15368530
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56144712A Granted JPS5847238A (en) | 1981-09-16 | 1981-09-16 | Fluorescence polarization measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5847238A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55109950A (en) * | 1979-02-17 | 1980-08-23 | Japan Spectroscopic Co | Measuring instrument for polarized fluorescence |
-
1981
- 1981-09-16 JP JP56144712A patent/JPS5847238A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5847238A (en) | 1983-03-18 |
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