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JPS6214779B2 - - Google Patents
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JPS6214779B2 - - Google Patents

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Publication number
JPS6214779B2
JPS6214779B2 JP55095492A JP9549280A JPS6214779B2 JP S6214779 B2 JPS6214779 B2 JP S6214779B2 JP 55095492 A JP55095492 A JP 55095492A JP 9549280 A JP9549280 A JP 9549280A JP S6214779 B2 JPS6214779 B2 JP S6214779B2
Authority
JP
Japan
Prior art keywords
output
light
particles
light receiving
particle
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
Application number
JP55095492A
Other languages
Japanese (ja)
Other versions
JPS5720655A (en
Inventor
Hidehiko Fujii
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP9549280A priority Critical patent/JPS5720655A/en
Publication of JPS5720655A publication Critical patent/JPS5720655A/en
Publication of JPS6214779B2 publication Critical patent/JPS6214779B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/26Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating electrochemical variables; by using electrolysis or electrophoresis
    • G01N27/416Systems
    • G01N27/447Systems using electrophoresis
    • G01N27/44704Details; Accessories
    • G01N27/44717Arrangements for investigating the separated zones, e.g. localising zones
    • G01N27/44721Arrangements 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 Materials By The Use Of Optical Means Adapted For Particular Applications (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浮遊粒子の電
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 suspended particles, such as biological cells.

上述した細胞浮遊粒子の電気泳動速度の測定は
生物学研究、臨床検査等で応用の広いものであり
既に種々な測定装置が提案されている。これらの
装置は、浮遊粒子の像を格子上に結像させ、格子
の背後で格子透過光を測光すると、輝いた浮遊粒
子像が格子線にかくれたり格子線間に現われたり
することにより、個々の粒子像による測光出力は
交流的変化をし、その周波数は浮遊粒子の泳動速
度に対応しているので、多数の浮遊粒子像による
種々な周波数の交流信号の重なつた測光出力から
種々な演算方式で多数浮遊粒子の電気泳動の速度
分布を求めるようになつている。所でこれら従来
装置では安定した測定結果を得るには或る程度高
濃度の粒子浮遊液を必要とする。例えば次のよう
な極端な場合を考えてみる。浮遊粒子が2個だけ
あつて両方の像が同時に格子線に重なりまた格子
線間に現われる場合、2個の浮遊粒子による測光
出力の交流成分は同相で重なるため交流出力は2
となる。反対に2個の粒子像が一方が格子線に重
なつているとき他方が格子線間にあると測光出力
においては2つの交流信号が反対位相で重なるた
め交流出力は0となる。実際には2個の粒子の電
気泳動速度が丁度同じと云うことは滅多にない
し、その位相関係が上のように極端な関係になる
こともないから、上述したような状態が起る確率
は小さい。しかし粒子数が増して来ると同じ速度
を持つた粒子対の存在する場合の数は増して来る
から、多数の粒子の夫々に基づく測光出力中の交
流成分が互に比較的強め合う場合或は相殺し合う
場合と云うのは比較的よく起るのであり、同じグ
ループの試料でありながら電気泳動速度の分布図
が測定毎に比較的シヤープになつたり、ブロード
になつたりする不安定が現われ、個々の粒子に由
来する交流成分が互に強め合う事例と相殺し合う
事例とが互に相殺し合う平均的事象が起り得る事
象の大部分を占め毎回の測定結果におけるゆらぎ
がなくなるためにはかなり多数の粒子が必要とな
る。
The above-mentioned measurement of the electrophoretic velocity of suspended particles in cells has a wide range of applications in biological research, clinical testing, etc., and various measuring devices have already been proposed. These devices focus images of suspended particles on a grating and measure the light transmitted through the grating behind the grating. The photometric output from the particle images changes in an alternating current manner, and the frequency corresponds to the electrophoretic speed of the suspended particles. Therefore, various calculations can be performed from the photometric output, which is the superimposition of alternating current signals of various frequencies due to a large number of suspended particle images. The electrophoretic velocity distribution of a large number of suspended particles can be determined using this method. However, in order to obtain stable measurement results with these conventional devices, a particle suspension liquid of a relatively high concentration is required. For example, consider the following extreme case. If there are only two suspended particles and both images overlap the grid lines at the same time and appear between the grid lines, the AC components of the photometric output from the two suspended particles will overlap in phase, so the AC output will be 2.
becomes. On the other hand, if two particle images, one of which overlaps the grid lines, and the other are located between the grid lines, the two AC signals will overlap with opposite phases in the photometric output, so the AC output will be 0. In reality, the electrophoretic speeds of two particles are rarely exactly the same, and the phase relationship between them is never as extreme as the one above, so the probability that the above situation will occur is small. However, as the number of particles increases, the number of pairs of particles with the same velocity increases. Cases in which they cancel each other out occur relatively often, and instability appears in which the electrophoretic velocity distribution diagram becomes relatively sharp or broad with each measurement even though the samples are from the same group. The average event in which the alternating current components originating from individual particles mutually strengthen and cancel each other accounts for most of the possible events, and it takes a considerable amount of time to eliminate fluctuations in the measurement results each time. A large number of particles are required.

しかし測定に必要な粒子数が少なくてよいと云
うことは測定上有利な事柄であり、特に生体試料
で試薬として特殊な抗体を用いると云つた場合、
多数の試料を処理するには個々に試料で測定に必
要な細胞数が少なくて済むと云うことは大へん重
要なことである。
However, the fact that only a small number of particles are required for measurement is an advantage in measurement, especially when using a special antibody as a reagent for biological samples.
When processing a large number of samples, it is very important that only a small number of cells are required for measurement in each individual sample.

本発明は比較的少数の粒子数によつて浮遊粒子
の電気泳動速度が安定に測定できる装置を提供す
ることを目的としてなされた。本発明に係る電気
泳動測定装置は複数の受光素子を浮遊粒子の電気
泳動の方向と平行に並べ、浮遊粒子の像をこの受
光素子の配列面に形成させ、粒子像が各受光素子
の受光面を通過する時間を測定し、その時間の分
布を表示するようにしたことを特徴とし、浮遊粒
子の濃度は各受光素子の一つおきに一時に一個の
粒子の像が投射される程度とする。受光素子一個
の幅を1mmとし投影倍率を10倍とし、焦点深度を
0.5mmとすると50個/m3程度の粒子濃度でよいこ
とになる。以下実施例によつて本発明を説明す
る。
The present invention was made with the object of providing an apparatus capable of stably measuring the electrophoretic velocity of suspended particles using a relatively small number of particles. The electrophoresis measuring device according to the present invention arranges a plurality of light receiving elements parallel to the direction of electrophoresis of floating particles, forms an image of the floating particles on the array surface of the light receiving elements, and forms a particle image on the light receiving surface of each light receiving element. The particle transit time is measured and the time distribution is displayed, and the concentration of suspended particles is such that an image of one particle is projected at a time from every other light-receiving element. . The width of each photodetector is 1 mm, the projection magnification is 10x, and the depth of focus is
If it is 0.5 mm, a particle concentration of about 50 particles/m 3 is sufficient. The present invention will be explained below with reference to Examples.

第1図は本発明の一実施例装置を示す。1は電
気泳動管で可視的粒子の浮遊した溶液が充してあ
り、図外両端に電極が挿入してあつて、粒子は矢
印方向に電気泳動を行つている。電気泳動管は図
の紙面の向う側から強く照明されている。2はレ
ンズで強く照明されている粒子の像を受光素子面
3上に形成する。P1〜Pnは受光素子で、この
実施例では全部で32個あり一列に並べられてお
り、その一例の全長は30mmである。1個の受光素
子の受光面は1辺が1mm弱の正方形で、32個の受
光素子が一つのパツケージ内に収められている。
これらの受光素子の配列方向は電気泳動管1の管
軸と平行である。レンズ2は浮遊粒子の像を10倍
に拡大して受光面3上に形成している。各受光素
子P1〜Pnの出力は夫々計時回路4に入力され
る。計時回路4からは各受光素子に対応した信号
が出力されてデータ処理回路5に入力され、デー
タ処理回路では、この入力に基いて試料粒子の電
気泳動速度の分布を算出する。
FIG. 1 shows an embodiment of the present invention. 1 is an electrophoresis tube filled with a solution in which visible particles are suspended, electrodes are inserted at both ends (not shown), and the particles are electrophoresed in the direction of the arrow. The electrophoresis tube is strongly illuminated from beyond the plane of the figure. 2 forms an image of the particles that are strongly illuminated by a lens on the light receiving element surface 3. P1 to Pn are light receiving elements, and in this embodiment, there are a total of 32 light receiving elements, and they are arranged in a row, and the total length of one example is 30 mm. The light-receiving surface of each light-receiving element is a square with sides of less than 1 mm, and 32 light-receiving elements are housed in one package.
The arrangement direction of these light receiving elements is parallel to the tube axis of the electrophoresis tube 1. The lens 2 magnifies the image of the floating particles ten times and forms it on the light receiving surface 3. The outputs of the light receiving elements P1 to Pn are respectively input to the clock circuit 4. The clock circuit 4 outputs a signal corresponding to each light receiving element and inputs it to the data processing circuit 5, and the data processing circuit calculates the electrophoretic velocity distribution of the sample particles based on this input.

第2図は上述した計時回路4の構成を示す。各
受光素子P1〜Pn-1の出力端子は夫々対応する
コンパレータC1〜Cn-1の(−)端子に接続さ
れる。各コンパレータC1〜Cn-1の(+)端子
には対応受光素子の右隣の受光素子の出力端子が
接続されている。各コンパレータC1〜Cn-1
出力端子は3端子アンドゲートA1〜An-2の一
入力端子に接続される。各アンドゲートの他の一
つの入力端子には対応コンパレータの右隣のコン
パレータの出力の反転信号が印加される。各アン
ドゲートの残りの一入力端子にはパルスジエネレ
ータCpの出力するクロツクパルスが印加されて
いる。各アンドゲートA1〜An-2の出力は夫々
カウンタK1〜Kn-2に入力されて計数される。
カウンタK1〜Kn-2の計数出力がデータ処理回
路5に入力される。
FIG. 2 shows the configuration of the clock circuit 4 described above. The output terminals of the respective light receiving elements P1 to Pn -1 are connected to the (-) terminals of the corresponding comparators C1 to Cn -1 , respectively. The output terminal of the light receiving element on the right side of the corresponding light receiving element is connected to the (+) terminal of each of the comparators C1 to Cn -1 . The output terminal of each comparator C1 to Cn -1 is connected to one input terminal of three-terminal AND gates A1 to An -2 . An inverted signal of the output of the comparator on the right of the corresponding comparator is applied to the other input terminal of each AND gate. A clock pulse output from a pulse generator Cp is applied to the remaining input terminal of each AND gate. The outputs of the AND gates A1 to An -2 are respectively input to counters K1 to Kn -2 and counted.
The count outputs of the counters K1 to Kn -2 are input to the data processing circuit 5.

計時回路4の動作を説明する。今例えば受光素
子P2に着目し、P2に一個の粒子の像が形成さ
れているとする。像は第2図で左から右へと移動
するものとする。P2に像が投映されている間コ
ンパレータC2の(−)端子入力はハイレベルで
あり、左右両隣P1,P3には粒子像が形成され
ていないとする。そうするとコンパレータC2の
(−)端子入力はハイ、(+)端子入力はローでC
2の出力はローである。またコンパレータC1の
(−)端子入力はロー、(+)端子入力はハイであ
るから、C1の出力はハイである。従つてアンド
ゲートA1の右側2つの入力端子は共に入力がハ
イとなつてA1が開となり、パルスジエネレータ
Cpの出力パルスがカウンタK1に入力されて計
数される。この計数は粒子像が受光素子P2を通
過し終るまで続けられる。従つてカウンタK1の
最終的な計数出力は一個の粒子像が受光素子P2
を横切るのに要した時間を表わす。データ処理装
置5は各カウンタK1〜Kn-2の出力及びコンパ
レータC2〜Cn-1の出力を繰返し走査してモニ
タしており、例えばカウンタK1について云えば
コンパレータP2の出力がローである間はK1の
出力を読込まず、P2の出力がハイであることを
検知するとK1の出力を読込むと共にK1をリセ
ツトする。データ処理装置ではこのようにして読
込んだ各カウンタの計数値をその計数値をメモリ
のアドレス指定数値として、メモリの指定された
アドレスに数1を加算する。即ちメモリ上の測定
された粒子速度の位置に1を積算して行く。一個
の粒子像は幾つかの受光素子を横切つて行く間に
粒子の沈降により受光面から上方に外れて行く。
他方新しい粒子が下方から受光面に入つて来る
(投影しているから上下逆になつているから)。従
つて上述した動作を或る時間続けていると103
のオーダの粒子についての電気泳動速度のデータ
がメモリに蓄積される。このデータは上述したよ
うに速度数値をアドレスとしてその速度が検出さ
れる度に1を積算したものであるから、そのまゝ
電気泳動速度の分布のプロフアイルのデイジタル
データになつている。或は上のようにして得られ
た各速度データから直ちに平均速度を求める演算
を行うようにしてもよい。
The operation of the clock circuit 4 will be explained. For example, let us now focus on the light receiving element P2 and assume that an image of one particle is formed on P2. The image is assumed to move from left to right in Figure 2. It is assumed that the (-) terminal input of the comparator C2 is at a high level while the image is being projected onto P2, and no particle images are formed on the left and right neighbors P1 and P3. Then, the (-) terminal input of comparator C2 is high and the (+) terminal input is low.
The output of 2 is low. Further, since the (-) terminal input of the comparator C1 is low and the (+) terminal input is high, the output of C1 is high. Therefore, the two input terminals on the right side of AND gate A1 are both high, and A1 is open, and the pulse generator
The output pulses of Cp are input to counter K1 and counted. This counting continues until the particle image finishes passing through the light receiving element P2. Therefore, the final count output of the counter K1 is that one particle image is detected by the light receiving element P2.
represents the time required to cross the The data processing device 5 repeatedly scans and monitors the outputs of the counters K1 to Kn -2 and the outputs of the comparators C2 to Cn -1 . For example, for counter K1, while the output of comparator P2 is low, K1 When it detects that the output of P2 is high without reading the output of P2, it reads the output of K1 and resets K1. In the data processing device, the count value of each counter read in this way is used as the address designation value of the memory, and the number 1 is added to the designated address of the memory. That is, 1 is added to the position of the measured particle velocity on the memory. While a single particle image crosses several light-receiving elements, it moves upward from the light-receiving surface due to sedimentation of the particles.
On the other hand, new particles enter the light-receiving surface from below (because it is projected upside down). Therefore, if the above-described operation is continued for a certain period of time, electrophoretic velocity data for particles on the order of 10 3 will be accumulated in the memory. As described above, this data is obtained by adding 1 each time the velocity is detected using the velocity numerical value as an address, so it becomes digital data of the profile of the electrophoretic velocity distribution. Alternatively, calculations may be made to immediately calculate the average speed from each speed data obtained as described above.

本発明電気泳動測定装置は上述したような構成
で一つの受光素子に同時に2個以上の粒子像が形
成されると却つて測定誤差が現われるので粒子密
度は低い方が良く、従来の格子を用いる方法では
格子ピツチは測定対象試料の粒子径の2倍程度が
望ましいので粒子の大きさによつて格子を変えね
ばならなかつたが、本発明は一個の受光素子の大
きさは幅1mm程度に限定されるのでなく、もつと
大きくてもよいのであり、粒子の大きさを問題に
しなくてもよいと云う利点を有する。
The electrophoresis measuring device of the present invention has the above-described configuration, and if two or more particle images are simultaneously formed on one light-receiving element, measurement errors will appear. In this method, the grid pitch is preferably about twice the particle diameter of the sample to be measured, so the grid had to be changed depending on the particle size, but in the present invention, the size of one photodetector is limited to about 1 mm in width. It has the advantage that the size of the particles does not have to be a problem because they can be large rather than being small.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例装置の全体構成を示
すブロツク図、第2図は上記における計時回路の
詳細を示す回路図である。 1……電気泳動管、2……レンズ、3……受光
面、4……計時回路、5……データ処理装置、P
1〜Pn……受光素子、C1〜Cn-1……コンパレ
ータ、Cp……パルスジエネレータ、K1〜Kn-2
……カウンタ。
FIG. 1 is a block diagram showing the overall configuration of an apparatus according to an embodiment of the present invention, and FIG. 2 is a circuit diagram showing details of the time measuring circuit described above. 1... Electrophoresis tube, 2... Lens, 3... Light receiving surface, 4... Timing circuit, 5... Data processing device, P
1~Pn...Photodetector, C1~Cn -1 ...Comparator, Cp...Pulse generator, K1~Kn -2
……counter.

Claims (1)

【特許請求の範囲】[Claims] 1 複数の受光素子を可視的粒子の電気泳動の方
向と平行に並べ、この受光素子列の受光面に浮遊
粒子像を形成する光学系を配置し、各受光素子に
浮遊粒子像が形成されていることによる出力が出
ている時間を測定する回路と、これらの各時間測
定回路の出力に出力の度数分布、平均の算出等の
適宜の演算を施すデータ処理装置を設けた電気泳
動測定装置。
1 A plurality of light-receiving elements are arranged parallel to the direction of electrophoresis of visible particles, an optical system for forming a floating particle image is arranged on the light-receiving surface of the array of light-receiving elements, and a floating particle image is formed on each light-receiving element. An electrophoresis measurement device that is equipped with a circuit that measures the time during which an output is produced due to the presence of a sensor, and a data processing device that performs appropriate calculations such as calculation of the frequency distribution and average of the output on the output of each of these time measurement circuits.
JP9549280A 1980-07-11 1980-07-11 Measuring apparatus of cataphoresis Granted JPS5720655A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9549280A JPS5720655A (en) 1980-07-11 1980-07-11 Measuring apparatus of cataphoresis

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9549280A JPS5720655A (en) 1980-07-11 1980-07-11 Measuring apparatus of cataphoresis

Publications (2)

Publication Number Publication Date
JPS5720655A JPS5720655A (en) 1982-02-03
JPS6214779B2 true JPS6214779B2 (en) 1987-04-03

Family

ID=14139090

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9549280A Granted JPS5720655A (en) 1980-07-11 1980-07-11 Measuring apparatus of cataphoresis

Country Status (1)

Country Link
JP (1) JPS5720655A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58189926U (en) * 1982-06-14 1983-12-16 石川島播磨重工業株式会社 Powder flow rate measuring device
GB9509410D0 (en) * 1995-05-10 1995-07-05 Imperial College Molecular imaging

Also Published As

Publication number Publication date
JPS5720655A (en) 1982-02-03

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