[go: up one dir, main page]

JPS6136926Y2 - - Google Patents

Info

Publication number
JPS6136926Y2
JPS6136926Y2 JP3170480U JP3170480U JPS6136926Y2 JP S6136926 Y2 JPS6136926 Y2 JP S6136926Y2 JP 3170480 U JP3170480 U JP 3170480U JP 3170480 U JP3170480 U JP 3170480U JP S6136926 Y2 JPS6136926 Y2 JP S6136926Y2
Authority
JP
Japan
Prior art keywords
electrophoresis
output
grating
frequency
photomultiplier tube
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
JP3170480U
Other languages
Japanese (ja)
Other versions
JPS56133552U (en
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 filed Critical
Priority to JP3170480U priority Critical patent/JPS6136926Y2/ja
Publication of JPS56133552U publication Critical patent/JPS56133552U/ja
Application granted granted Critical
Publication of JPS6136926Y2 publication Critical patent/JPS6136926Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Description

【考案の詳細な説明】 本考案は溶液中における可視的な浮遊粒子の電
気泳動による移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 migration velocity of visible suspended particles in a solution.

白血球の浮遊液に電界を作用させて白血球に電
気泳動を行わせると、その泳動速度の差異から診
断上の情報が得られる。このような目的のために
可視的浮遊粒子の電気泳動速度を測定する装置が
既に提案されている。この既提案の位置の原理は
次のようなものである。
When an electric field is applied to a leukocyte suspension to cause the leukocytes to undergo electrophoresis, diagnostic information can be obtained from the difference in migration speed. For this purpose, an apparatus for measuring the electrophoretic velocity of visible suspended particles has already been proposed. The principle of this previously proposed position is as follows.

電気泳動管に目的の粒子の浮遊液を入れて目的
粒子に電気泳動を行わせ、電気泳動管を強い光で
照明し投影レンズで浮遊粒子の像を格子上に結像
させる。浮遊粒子の像は輝いた点状で格子上を電
気泳動による粒子移動に従つて移動する。従つて
格子背後で格子透過光を測光すると粒子像の光が
格子線の間を通過したり格子線にかくされたりす
るため測光出力が変動する。そこで測光出力の変
動成分の周波数分析をすれば浮遊粒子の電気泳動
速度が求まる。しかしこれだけでは電気泳動速度
は20μ/秒程度で測光出力の変動成分の周波数は
大へん低く、電気回路のドリフトの影響が強く現
われ信号処理が困難である。そこで格子を円板の
周辺に設けて円板を回転させることによつて格子
を移動させ格子と浮遊粒子像との相対速度を高め
て格子透過光の測光出力の変動成分の周波数を高
め信号処理を容易にしている。
A suspension of target particles is placed in an electrophoresis tube, the target particles are electrophoresed, the electrophoresis tube is illuminated with strong light, and an image of the suspended particles is formed on a grid using a projection lens. Images of suspended particles are bright dots that move on the grid as the particles move due to electrophoresis. Therefore, when the grating transmitted light is photometered behind the grating, the light of the particle image passes between the grating lines or is hidden by the grating lines, causing the photometric output to fluctuate. Therefore, by frequency analysis of the fluctuation component of the photometric output, the electrophoretic velocity of suspended particles can be determined. However, with this alone, the electrophoresis speed is about 20 μ/sec, and the frequency of the fluctuation component of the photometric output is very low, and the influence of drift in the electric circuit appears strongly, making signal processing difficult. Therefore, by setting a grating around the disk and rotating the disk, the grating is moved and the relative speed between the grating and the floating particle image is increased, thereby increasing the frequency of the fluctuating component of the photometric output of the light transmitted through the grating and processing the signal. is facilitated.

上述した所が既提案装置の原理であるが、この
既提案装置は上述したように格子を回転させると
云う機械的運動部分を含んでいるため構造が複雑
であり、振動、耐久性、信頼性等種々な点で純電
気的な構成に比し不利である。
The above is the principle of the previously proposed device, but this proposed device has a complicated structure because it includes a mechanically moving part that rotates the lattice, and has problems with vibration, durability, and reliability. It is disadvantageous in various respects compared to a purely electrical configuration.

従つて本考案は純電気的な構成を有する可視的
浮遊粒子の電気泳動速度を測定する装置を提供す
ることを目的としてなされた。
SUMMARY OF THE INVENTION It is therefore an object of the present invention to provide an apparatus for measuring the electrophoretic velocity of visible suspended particles having a purely electrical configuration.

本考案は静止した格子上に浮遊粒子像を形成
し、上記格子を透過した光を光電変換し、適宜周
波数の交流を上記光電変換出力で変調し、この変
調された交流信号を周波数分析し、得られた成分
周波数ともとの交流周波数との差によつて光電変
換出力の周波数を求めるようにした電気泳動測定
装置を提供する。以下実施例によつて本考案を説
明する。
The present invention forms a floating particle image on a stationary grating, photoelectrically converts the light transmitted through the grating, modulates an alternating current of an appropriate frequency with the photoelectric conversion output, and analyzes the frequency of this modulated alternating current signal. An electrophoresis measurement device is provided that determines the frequency of a photoelectric conversion output based on the difference between the obtained component frequency and the original AC frequency. The present invention will be explained below with reference to Examples.

第1図は本考案の一実施例装置の構成を示し、
第2図は同じく回路を示す。第1図で1は電気泳
動管で目的粒子を浮遊させた粒子を満たし、両端
に電極2,3が挿入してあり、電極2,3間に電
圧を印加するようになつている。4はレーザ光源
で電気泳動管1の上方に配置され集光レンズ系5
によつて電気泳動管1内の適所を強く照明する。
6は電気泳動管1の側方に配置された投影レンズ
で電気泳動管1で上記レーザ光により強く照明さ
れている浮遊粒子の像を格子7上に形成する。格
子7は固定されている。格子7は格子線が目的粒
子の電気泳動の方向(水平方向)と直交する方向
に延びており、格子線を浮遊粒子の電気泳動の方
向に多数平行に並べたものである。8は上記格子
7の背後に配置された光電子増倍管で格子7を透
過した浮遊粒子像の光を受光するようになつてお
り、その出力が信号処理回路9に送られる。
FIG. 1 shows the configuration of an apparatus according to an embodiment of the present invention,
FIG. 2 also shows the circuit. In FIG. 1, reference numeral 1 denotes an electrophoresis tube filled with suspended target particles, with electrodes 2 and 3 inserted at both ends, so that a voltage is applied between the electrodes 2 and 3. 4 is a laser light source placed above the electrophoresis tube 1, and a condensing lens system 5
A suitable location within the electrophoresis tube 1 is strongly illuminated.
Reference numeral 6 denotes a projection lens disposed on the side of the electrophoresis tube 1, which forms an image of the floating particles in the electrophoresis tube 1, which are strongly illuminated by the laser beam, on the grid 7. The grid 7 is fixed. The grid 7 has grid lines extending in a direction perpendicular to the direction of electrophoresis (horizontal direction) of target particles, and a large number of grid lines are arranged parallel to the direction of electrophoresis of suspended particles. A photomultiplier tube 8 is arranged behind the grating 7 and is adapted to receive the light of the floating particle image transmitted through the grating 7, and its output is sent to the signal processing circuit 9.

第2図は信号処理回路9の構成を示す。この実
施例は光電子増倍管8のダイノードに交流信号を
印加し、その交流を光電子増倍管8の入力によつ
て変調するようにしたものである。Gは水晶発振
器であり、その出力はカウントダウンカウンタC
で計数される。カウンタCは周波数選択回路Sに
よつて任意の計数値がプリセツトされる。従つて
カウンタCは発振器Gの出力波形をプリセツト数
だけ計数する毎に信号を出し、その出力でトリガ
フリツプフロツプTRをトリガする。同フリツプ
フロツプの出力はバンドパスフイルタFを通して
基本波だけが取出され増幅器Wに印加される。増
幅器Wの出力は正弦波であつて光電子増倍管8の
第1と第2のダイノードd1とd2との間に印加
される。このため光電子増倍管8の感度は増幅器
Wの出力周波数と同じ周波数で変動する。Aは光
電子増倍管8の出力を増幅するプリアンプであ
り、その出力が周波数解析回路FFTに印加され
る。周波数解析回路FFTは一定期間の光電子増
倍管8の出力を記憶し、同出力のスペクトル分布
を算出する。このスペクトル分布はダイノードd
1,d2間に印加した交流の周波数を中心に
第3図のような分布を示し、側帯波のピークの周
波数ととの差が格子7の透過光の変動周波
数の平均を示し、浮遊粒子の電気泳動速度をv、
レンズ6の投影倍率をm、格子7の格子線ピツチ
をnとすると格子上の粒子像の移動速度はmvで
=mv/nにより目的粒子の電気泳動速
度が求められる。
FIG. 2 shows the configuration of the signal processing circuit 9. As shown in FIG. In this embodiment, an alternating current signal is applied to the dynode of the photomultiplier tube 8, and the alternating current signal is modulated by the input of the photomultiplier tube 8. G is a crystal oscillator whose output is a countdown counter C
is counted. The counter C is preset to an arbitrary count value by the frequency selection circuit S. Therefore, the counter C outputs a signal every time it counts the output waveform of the oscillator G by a preset number, and uses the output to trigger the trigger flip-flop TR. From the output of the flip-flop, only the fundamental wave is taken out through a bandpass filter F and applied to an amplifier W. The output of the amplifier W is a sine wave and is applied between the first and second dynodes d1 and d2 of the photomultiplier tube 8. Therefore, the sensitivity of the photomultiplier tube 8 varies at the same frequency as the output frequency of the amplifier W. A is a preamplifier that amplifies the output of the photomultiplier tube 8, and its output is applied to the frequency analysis circuit FFT. The frequency analysis circuit FFT stores the output of the photomultiplier tube 8 for a certain period of time and calculates the spectral distribution of the same output. This spectral distribution is the dynode d
The distribution shown in Figure 3 is centered around the frequency 0 of the alternating current applied between 1 and d2, and the difference between the peak frequency of the sideband and 0 indicates the average fluctuating frequency of the light transmitted through the grating 7, and the floating The electrophoretic velocity of the particles is v,
When the projection magnification of the lens 6 is m and the grid line pitch of the grating 7 is n, the moving speed of the particle image on the grating is mv, and the electrophoretic speed of the target particle is determined by -0 =mv/n.

本考案電気泳動測定装置は上述したような構成
で機械的に運動する部分を全く含まず信号の交流
化がなされているので信号処理が安定して行われ
る。
The electrophoresis measuring device of the present invention has the above-described configuration and does not include any mechanically moving parts and converts signals into alternating current, so that signal processing can be performed stably.

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

第1図は本考案の一実施例装置の構造的部分の
斜視図、第2図は同じく信号処理部の回路図、第
3図は上記回路の光電子増倍管出力のスペクトル
分布図である。 1……電気泳動管、2,3……電極、4……レ
ーザ光源、6……投影レンズ、7……格子、8…
…光電子増倍管、9……信号処理回路、d1,d
2……第1及び第2ダイノード、W……アンプ、
F……フイルタ、TR……トリガフリツプフロツ
プ、C……カウンタ、G……水晶発振器、FFT
……周波数解析回路。
FIG. 1 is a perspective view of a structural part of an apparatus according to an embodiment of the present invention, FIG. 2 is a circuit diagram of the signal processing section, and FIG. 3 is a spectral distribution diagram of the photomultiplier tube output of the circuit. 1... Electrophoresis tube, 2, 3... Electrode, 4... Laser light source, 6... Projection lens, 7... Grid, 8...
...Photomultiplier tube, 9...Signal processing circuit, d1, d
2...first and second dynodes, W...amplifier,
F...Filter, TR...Trigger flip-flop, C...Counter, G...Crystal oscillator, FFT
...Frequency analysis circuit.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 電気泳動管中の浮遊粒子の像を固定格子上に形
成する構成を有し、上記格子を透過した光を光電
子増倍管に入射させ、同光電子増倍管のダイノー
ドに交流信号を印加し、同光電子増倍管の出力を
周波数解折回路に印加するようにした電気泳動測
定装置。
It has a configuration in which an image of floating particles in an electrophoresis tube is formed on a fixed grid, the light transmitted through the grid is incident on a photomultiplier tube, and an alternating current signal is applied to a dynode of the photomultiplier tube, An electrophoresis measurement device that applies the output of the photomultiplier tube to a frequency decomposition circuit.
JP3170480U 1980-03-10 1980-03-10 Expired JPS6136926Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3170480U JPS6136926Y2 (en) 1980-03-10 1980-03-10

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3170480U JPS6136926Y2 (en) 1980-03-10 1980-03-10

Publications (2)

Publication Number Publication Date
JPS56133552U JPS56133552U (en) 1981-10-09
JPS6136926Y2 true JPS6136926Y2 (en) 1986-10-25

Family

ID=29627550

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3170480U Expired JPS6136926Y2 (en) 1980-03-10 1980-03-10

Country Status (1)

Country Link
JP (1) JPS6136926Y2 (en)

Also Published As

Publication number Publication date
JPS56133552U (en) 1981-10-09

Similar Documents

Publication Publication Date Title
US4786815A (en) Non-contact sensor with particular utility for measurement of road profile
US4961643A (en) Method of and apparatus for measuring speed
JPS6136926Y2 (en)
JPS623727Y2 (en)
SU570818A1 (en) Device for measuring dust concentration in the air
SU972379A1 (en) Method of and device for measuring suspension particle electrokinetic parameters
JPS6211295B2 (en)
JPS59128449A (en) Method for detecting moving speed of object
Richards et al. Optical multichannel analyzer as a scanner for the ultracentrifuge: I. Single beam operation
SU798553A1 (en) Photoelectric dispersed-material particle counter
SU1173264A1 (en) Method of measuring particle size
SU855440A1 (en) Device for local measuring of aerosol particle dimensions and mass flow
JPS6213002Y2 (en)
JPS61196104A (en) Position detecting method and its photo-receiving device by means of laser beam
JPS6239702B2 (en)
SU1539527A1 (en) Method and apparatus for measuring distance to reflecting surface
JPS643541A (en) Instrument for measuring fine particle in fluid
SU645086A1 (en) Carrier tape speed measuring device
SU1571508A1 (en) Apparatus for measuring the speed of movement of an object
JPS625648Y2 (en)
SU993017A1 (en) Photoelectric device for measuring object geometric dimensions
RU1804608C (en) Method of determining speed and dimensions of particles in moving medium
RU2018116C1 (en) Method and device for determining light scattering (diffusion) coefficient in liquid media
SU576840A1 (en) Nephelometer
SU750344A1 (en) Device for determining charge value and sign of charge of aerosol particles