JPS6148865B2 - - Google Patents
Info
- Publication number
- JPS6148865B2 JPS6148865B2 JP55099138A JP9913880A JPS6148865B2 JP S6148865 B2 JPS6148865 B2 JP S6148865B2 JP 55099138 A JP55099138 A JP 55099138A JP 9913880 A JP9913880 A JP 9913880A JP S6148865 B2 JPS6148865 B2 JP S6148865B2
- Authority
- JP
- Japan
- Prior art keywords
- particle
- measurement
- concentration
- sample
- particles
- 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
Links
- 239000002245 particle Substances 0.000 claims description 54
- 238000005259 measurement Methods 0.000 claims description 25
- 239000000725 suspension Substances 0.000 claims description 2
- 238000001962 electrophoresis Methods 0.000 description 12
- 230000015654 memory Effects 0.000 description 12
- 238000000034 method Methods 0.000 description 11
- 230000007423 decrease Effects 0.000 description 6
- 238000002347 injection Methods 0.000 description 3
- 239000007924 injection Substances 0.000 description 3
- 239000000243 solution Substances 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 2
- 238000009792 diffusion process Methods 0.000 description 2
- 238000004062 sedimentation Methods 0.000 description 2
- 238000002835 absorbance Methods 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
- 239000012905 visible particle Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
- G01N27/26—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating electrochemical variables; by using electrolysis or electrophoresis
- G01N27/416—Systems
- G01N27/447—Systems using electrophoresis
- G01N27/44704—Details; Accessories
- G01N27/44717—Arrangements for investigating the separated zones, e.g. localising zones
- G01N27/44721—Arrangements for investigating the separated zones, e.g. localising zones by optical means
Landscapes
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Molecular Biology (AREA)
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- Physics & Mathematics (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
本発明は生体細胞のような可視的粒子の溶液中
に浮遊した状態における電気泳動速度を測定する
装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for measuring the electrophoretic velocity of visible particles, such as biological cells, suspended in a solution.
可視的浮遊粒子の電気泳動速度を測定する方法
は既にいくつか提案されているが、夫々の方法に
ついて適当な浮遊粒子密度があり、それよりも濃
くても淡くても測定結果が不安定になつて測定の
信頼性が低下する。例えば格子方式では格子上に
浮遊粒子の像を形成し、粒子の電気泳動によつて
粒子像が格子線を横切る度に格子透過光の強度が
変るから多数の粒子像による光量変化の波の重畳
された格子透過光の測光波形から周波数分析によ
つて粒子の電気泳動速度の分布を計算するが、粒
子濃度が高過ぎると観測部分に達する光量が減少
して、粒子数の増大がかえつて散乱光強度を弱め
てしまい粒子の電気泳動速度の分布を算出できな
くなり、濃度が低過ぎると統計的ゆらぎが増大し
て同一試料であつても毎回の測定による速度分布
のプロフアイルが異なつたものになる。また個個
の粒子を追跡して電気泳動速度を測定することを
基本原理とした方法では浮遊粒子濃度は上述した
方法に比しかなり低い所が適当であり、反対に浮
遊粒子の初期の濃度分布形と一定時間電気泳動を
行つた後の濃度分布形との比較から電気泳動速度
分布を求めるものでは粒子濃度はかなり高い所が
適当となる。 Several methods have already been proposed for measuring the electrophoretic velocity of visible suspended particles, but each method has an appropriate suspended particle density, and the measurement results will become unstable if the density is higher or lighter than that. The reliability of the measurement decreases. For example, in the grid method, images of floating particles are formed on a grid, and the intensity of the light transmitted through the grid changes each time the particle image crosses the grid lines due to particle electrophoresis, so waves of changes in light intensity due to multiple particle images are superimposed. The electrophoretic velocity distribution of the particles is calculated by frequency analysis from the photometric waveform of the light transmitted through the grating. However, if the particle concentration is too high, the amount of light reaching the observation area will decrease, and the increase in the number of particles will instead cause scattering. If the light intensity is weakened, it becomes impossible to calculate the electrophoretic velocity distribution of particles, and if the concentration is too low, statistical fluctuations will increase, resulting in different velocity distribution profiles for each measurement even for the same sample. Become. Furthermore, in a method based on the basic principle of tracking individual particles and measuring their electrophoretic velocity, it is appropriate for the suspended particle concentration to be much lower than in the above-mentioned method; When the electrophoretic velocity distribution is determined by comparing the particle shape with the concentration distribution shape after electrophoresis for a certain period of time, it is appropriate that the particle concentration be quite high.
他方試料はそれが調製された段階では高粒子濃
度であり、これを注射器のようなもので電気泳動
測定装置の測定領域に注入すると、注入当初同領
域内の粒子濃度は甚だ高いが、粒子の拡散と沈降
により粒子濃度は次第に低下して行き、所望の粒
子濃度を保つた溶液で電気泳動測定を行うと云う
ことはできない。 On the other hand, the sample has a high particle concentration when it is prepared, and when it is injected into the measurement area of an electrophoresis measurement device with something like a syringe, the particle concentration in the same area is extremely high at the time of injection, but the particle concentration is very high. The particle concentration gradually decreases due to diffusion and sedimentation, and it cannot be said that electrophoretic measurements can be performed with a solution that maintains the desired particle concentration.
従来は測定を行う者が電気泳動測定装置に試料
を注入した後、適当な時間を見計らつて測定を行
つていたので、夫々の測定方式に適した粒子濃度
になつた時期に測定しているとは限らず、信頼性
の高い測定が困難であつた。 In the past, the person performing the measurement injected the sample into the electrophoresis measuring device and then took the measurement at an appropriate time, so the measurement was carried out at a time when the particle concentration suitable for each measurement method was reached. However, it was difficult to make reliable measurements.
本発明は試料を電気泳動装置に注入した後、そ
の測定装置に適した即ち測定結果が最も安定した
ものとなる浮遊粒子濃度になつた時期を検出し、
その時期に自動的に測定を行うようにした装置を
提供するものである。以下実施例によつて本発明
を説明する。 The present invention, after injecting a sample into an electrophoresis device, detects when the suspended particle concentration has reached a level suitable for the measurement device, that is, the measurement results are most stable.
The purpose of the present invention is to provide a device that automatically performs measurements at that time. The present invention will be explained below with reference to Examples.
図は本発明の一実施例装置を示す。1は電気泳
動管で試料粒子を浮遊させる溶液が充してあり、
図外両端に電極が挿入してあり、図外の試料注入
ポートから試料粒子の濃厚な浮遊液が注入され
る。図は電気泳動管1の測定領域の部分だけを示
しており、注入された試料粒子は拡散、沈降及び
電気泳動によつて図示測定領域に拡散して来て当
初急に粒子濃度が高まり、その後次第に濃度が低
下して行く。2は投影レンズ系であり、測定領域
にある浮遊粒子の像を撮像管3の受光面に形成す
る。投影レンズ系2の光軸と直交する方向図外に
照明光源が配置されて浮遊粒子像は暗い背景に輝
いた点となつて形成されている。撮像管3から出
力される映像信号はゲートGを介して信号処理回
路4に入力され、この回路において試料粒子の電
気泳動速度が検出される。撮像管3から出力され
る映像信号はまた積分回路5にも入力される。積
分回路5は積分用コンデンサとそれに並列の漏洩
抵抗とよりなつておりその出力は映像信号の平均
レベルを示す。粒子像は輝いた点であるからこの
平均レベルは試料粒子の濃度が高いと高く試料粒
子の濃度と一定の一価関数関係にある。従つて積
分回路5の出力をコンパレータ6,6′に印加し
て適当に設定した基準レベルと比較することによ
つて特定の試料粒子濃度の状態を検知することが
できる。そこで予め実験によつて最も安定した測
定結果が得られる試料粒子濃度を求め、そのとき
コンパレータ6から信号が出力されるように基準
レベルを設定しておく。適当な粒子濃度の値は幅
を有するから、コンパレータは6,6′の2個を
用意し、夫々に与える基準レベルにはこの幅に相
当するだけの差を設けておく。コンパレータ6は
6′より高い濃度のとき信号を出す。前述したよ
うに測定領域における試料粒子濃度は試料注入直
前には0で急に高濃度になり、その後漸減する。
従つて試料注入によつてまずコンパレータ6′が
信号を出し、短時間経てコンパレータ6が信号を
出しその後コンパレータ6の信号が消え(ローレ
ベルとなる)、しばらくしてコンパレータ6′の信
号が消える。そこでコンパレータ6のハイレベル
信号の立下りでセツトされ、コンパレータ6′の
ハイレベル信号の立下りでリセツトされるフリツ
プフロツプ7のセツト出力でゲートGを開くよう
にすると、粒子濃度が漸減して行く過程で最適粒
子濃度の期間だけ信号処理回路4に映像信号が入
力されて信頼性の高い電気泳動測定が行われるこ
とになる。 The figure shows an embodiment of the invention. 1 is an electrophoresis tube filled with a solution that suspends sample particles;
Electrodes are inserted at both ends (not shown), and a concentrated suspension of sample particles is injected from a sample injection port (not shown). The figure shows only the measurement area of the electrophoresis tube 1, and the injected sample particles diffuse into the measurement area shown by diffusion, sedimentation, and electrophoresis, and the particle concentration increases suddenly at first, and then The concentration gradually decreases. Reference numeral 2 denotes a projection lens system, which forms an image of floating particles in the measurement area on the light receiving surface of the image pickup tube 3. An illumination light source is disposed outside the direction perpendicular to the optical axis of the projection lens system 2, and the floating particle image is formed as a bright dot on a dark background. A video signal output from the image pickup tube 3 is inputted to a signal processing circuit 4 via a gate G, and the electrophoretic velocity of sample particles is detected in this circuit. The video signal output from the image pickup tube 3 is also input to the integrating circuit 5. The integrating circuit 5 consists of an integrating capacitor and a leakage resistor in parallel with the integrating capacitor, and its output indicates the average level of the video signal. Since the particle image is a bright spot, this average level is high when the concentration of sample particles is high, and has a constant monovalent function relationship with the concentration of sample particles. Therefore, by applying the output of the integrating circuit 5 to the comparators 6, 6' and comparing it with an appropriately set reference level, it is possible to detect a specific sample particle concentration state. Therefore, the sample particle concentration at which the most stable measurement result can be obtained is determined in advance through experiments, and the reference level is set so that a signal is output from the comparator 6 at that time. Since an appropriate particle concentration value has a range, two comparators, 6 and 6', are prepared, and the reference levels given to each are provided with a difference corresponding to this range. Comparator 6 gives a signal when the concentration is higher than 6'. As described above, the sample particle concentration in the measurement region is 0 immediately before sample injection, suddenly increases to a high concentration, and then gradually decreases.
Therefore, when the sample is injected, the comparator 6' first outputs a signal, after a short time the comparator 6 outputs a signal, and then the signal of the comparator 6 disappears (becomes low level), and after a while the signal of the comparator 6' disappears. Therefore, if the gate G is opened by the set output of the flip-flop 7, which is set at the fall of the high level signal of the comparator 6 and reset at the fall of the high level signal of the comparator 6', the particle concentration gradually decreases. A video signal is input to the signal processing circuit 4 only during the optimum particle concentration period, and highly reliable electrophoresis measurement is performed.
信号処理回路4の一例を説明する。撮像管3は
デイジタル方式で走査され、水平方向の座標(x
座標)指定情報の一定範囲において映像信号がハ
イレベルであるときはそのときのy座標指定情報
をアドレス指定情報として第1のメモリの指定ア
ドレスに1を加算する。このアドレス指定情報は
y座標指定情報の引続く幾つかを一つにまとめて
一つのアドレスを指定するようにする。この構成
によつて像面で或る横幅の領域を水平に幾つかに
区分してその各区分内の粒子が検出される。そこ
で粒子濃度を適当に稀薄にしておくと、一つの区
分に一つの粒子があつて、その粒子が区分の例え
ば左端から入つて電気泳動で右端から出て行くま
での間次の粒子がその区分内に入つて来ることが
ないようにすることができる。このような濃度状
態ではメモリの各アドレスはそのアドレスに対応
した区分に粒子像がある間は一垂直走査の間に記
憶数が1ずつ増加する(このためには粒子像の大
きさが水平走査線の一本分以下であることが必
要)。そこで上記第1のメモリの各アドレスを1
垂直走査毎に一回走査し、その二回の走査におい
て記憶数の増加のないアドレスについて、その記
憶数を第2のメモリのアドレス指定情報として第
2のメモリのそのアドレスに1を加算し、第1の
メモリのそのアドレスのメモリを0に戻す。この
とき第1のメモリのそのアドレスの記憶数は粒子
像が一つの区分を左端から右端まで通り抜けるの
に要した時間を垂直走査周期を単位として測つた
ものであるから、それを第2のメモリのアドレス
指定情報にすると、その動作をゲートGが開いて
いる間継続したときの第2のメモリの記憶は電気
泳動速度の分布を示したものとなる。 An example of the signal processing circuit 4 will be explained. The image pickup tube 3 is digitally scanned and horizontal coordinates (x
Coordinate) When the video signal is at a high level within a certain range of designation information, 1 is added to the designated address of the first memory using the y-coordinate designation information at that time as address designation information. This addressing information combines several pieces of y-coordinate designation information to designate one address. With this configuration, an area of a certain width is horizontally divided into several sections on the image plane, and particles within each section are detected. Therefore, if the particle concentration is diluted appropriately, one particle will be in one section, and the next particle will be in that section until it enters the section from the left end and exits from the right end by electrophoresis. You can prevent it from coming inside. In such a density state, each address in the memory increases by 1 during one vertical scan as long as there is a particle image in the section corresponding to that address. (must be less than one line). Therefore, each address of the first memory is set to 1.
Scan once for each vertical scan, and for an address whose number of memories does not increase in the two scans, add 1 to that address of the second memory as address designation information of the second memory, and The memory at that address in the first memory is reset to zero. At this time, the number of memories stored at that address in the first memory is the time required for the particle image to pass through one section from the left end to the right end, measured in units of vertical scanning periods, so it is stored in the second memory. When the addressing information is set to , the storage in the second memory when the operation is continued while the gate G is open will indicate the distribution of electrophoretic velocity.
上述した実施例は個々の粒子像の動きを追跡す
る方式に属するもので粒子濃度はかかなり低い所
が適当で濃度の適当範囲は低濃度域で広いもので
ある。しかし本発明は粒子の電気泳動速度の測定
方式そのものには直接関係はなく、如何なる測定
方式に対しても適用できかつ必要性の高いもので
ある。 The above-mentioned embodiment belongs to a method of tracking the movement of individual particle images, and the particle concentration is suitably quite low, and the appropriate concentration range is wide in the low concentration region. However, the present invention is not directly related to the method of measuring the electrophoretic velocity of particles, but is applicable to any method of measurement and is highly necessary.
また粒子の適当濃度の検出法は撮影管の映像信
号を処理するものに限定されず例えば一定領域の
粒子像(個々の粒子が分解されている必要はな
い)を測光素子の受光面に形成し、受光素子の出
力信号をコンパレータで基準レベルと比較するよ
うにするとか吸光度を測定する等任意のものでよ
い。 Furthermore, methods for detecting the appropriate concentration of particles are not limited to those that process video signals from a camera tube, but can also be used, for example, to form a particle image of a certain area (individual particles do not need to be separated) on the light-receiving surface of a photometric element. Any method may be used, such as comparing the output signal of the light receiving element with a reference level using a comparator or measuring absorbance.
本発明は上述したような構成で、適当な粒子濃
度を検出して自動的にその濃度範囲だけで測定を
行うので測定結果の安定、測定者の個人差の解消
によつて信頼性の高い電気泳動測定が可能とな
る。 The present invention has the above-mentioned configuration, detects an appropriate particle concentration, and automatically performs measurement only within that concentration range, thereby stabilizing measurement results and eliminating individual differences among measurement personnel, thereby providing highly reliable electrical power. Electrophoresis measurement becomes possible.
図面は本発明の一実施例装置の構成を示すブロ
ツク図である。
1……電気泳動管、2……投影レンズ系、3…
…撮像管、4……信号処理回路、5……積分回
路、6,6′……コンパレータ、7……フリツプ
フロツプ、G……ゲート。
The drawing is a block diagram showing the configuration of an apparatus according to an embodiment of the present invention. 1... Electrophoresis tube, 2... Projection lens system, 3...
...Image tube, 4...Signal processing circuit, 5...Integrator circuit, 6, 6'...Comparator, 7...Flip-flop, G...Gate.
Claims (1)
粒子濃度測定手段と、同手段の出力を予め設定し
たレベルと比較する手段と、この比較手段の出力
によつて所定の粒子濃度範囲で作動するように制
御される試料粒子の電気泳動測定手段とよりなる
電気泳動測定装置。1. A particle concentration measuring means in the electrophoretic measurement area of the sample particle suspension, a means for comparing the output of the same means with a preset level, and a means for operating within a predetermined particle concentration range based on the output of the comparing means. An electrophoretic measuring device comprising controlled electrophoretic measuring means for sample particles.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9913880A JPS5723852A (en) | 1980-07-18 | 1980-07-18 | Electrophoretic measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9913880A JPS5723852A (en) | 1980-07-18 | 1980-07-18 | Electrophoretic measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5723852A JPS5723852A (en) | 1982-02-08 |
| JPS6148865B2 true JPS6148865B2 (en) | 1986-10-27 |
Family
ID=14239349
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9913880A Granted JPS5723852A (en) | 1980-07-18 | 1980-07-18 | Electrophoretic measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5723852A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB8513538D0 (en) * | 1985-05-29 | 1985-07-03 | Mackay C D | Electrophoresis |
| US5938117A (en) * | 1991-04-24 | 1999-08-17 | Aerogen, Inc. | Methods and apparatus for dispensing liquids as an atomized spray |
| US6629646B1 (en) | 1991-04-24 | 2003-10-07 | Aerogen, Inc. | Droplet ejector with oscillating tapered aperture |
| US6427682B1 (en) | 1995-04-05 | 2002-08-06 | Aerogen, Inc. | Methods and apparatus for aerosolizing a substance |
-
1980
- 1980-07-18 JP JP9913880A patent/JPS5723852A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5723852A (en) | 1982-02-08 |
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