JPS6353499B2 - - Google Patents
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- Publication number
- JPS6353499B2 JPS6353499B2 JP56009799A JP979981A JPS6353499B2 JP S6353499 B2 JPS6353499 B2 JP S6353499B2 JP 56009799 A JP56009799 A JP 56009799A JP 979981 A JP979981 A JP 979981A JP S6353499 B2 JPS6353499 B2 JP S6353499B2
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- sample
- power supply
- measuring
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Classifications
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- 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
- G01N27/44713—Particularly adapted electric power supply
-
- 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
- G01N27/28—Electrolytic cell components
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- Molecular Biology (AREA)
- Physics & Mathematics (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Power Engineering (AREA)
- Engineering & Computer Science (AREA)
- Investigating Or Analyzing Materials Using Thermal Means (AREA)
- Investigating Or Analysing Biological Materials (AREA)
Description
【発明の詳細な説明】
本発明は、電気泳動、電気浸透等の界面動電現
象の測定方法および測定装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method and apparatus for measuring electrokinetic phenomena such as electrophoresis and electroosmosis.
すなわち、固液界面あるいは、液液界面に沿つ
て電場を加えた場合拡散二重層内のイオンが移動
し、これに伴い溶媒が運ばれることにより生ずる
液体の流動度を測定する電気浸透現象の測定、あ
るいはコロイド粒子が電場内で移動する速度(移
動度)を測定する電気泳動現象の測定に関する。 In other words, when an electric field is applied along the solid-liquid interface or the liquid-liquid interface, ions in the diffusion double layer move, and the solvent is carried along with this, and the electroosmotic phenomenon is measured by measuring the fluidity of the liquid. , or the measurement of electrophoretic phenomena, which measures the speed at which colloidal particles move in an electric field (mobility).
上記界面動電現象の測定装置としてたとえば、
コロイド荷電粒子の動きを観察する電気泳動測定
装置は、微小表面荷電物質を扱う分野では良く知
られている。 For example, as a measuring device for the above-mentioned electrokinetic phenomenon,
Electrophoretic measurement devices that observe the movement of colloidal charged particles are well known in the field of dealing with microscopic surface-charged substances.
上記電気泳動装置は、測定セルに直流電流を流
して電場を発生させ、その電場に応じて粒子が移
動する速度を測定して粒子の電荷等を算定する機
能を有するもので、かかる電気泳動装置の基本的
な操作手順は以下の通りである。 The electrophoresis device described above has a function of generating an electric field by passing a direct current through a measurement cell, and measuring the speed at which particles move according to the electric field to calculate the charge of the particles. The basic operating procedure is as follows.
1 試料検体を測定セルに導入する。1. Introduce the sample specimen into the measurement cell.
2 測定セル内の検体粒子の変動が安定するのを
待つて顕微鏡により試料検体を観察し、測定す
べき粒子を決定する。2. Wait until the fluctuations in the sample particles in the measurement cell become stable, observe the sample using a microscope, and determine the particles to be measured.
3 直流電流を印加し、粒子の移動を開始させ
る。3 Apply direct current to start particle movement.
4 印加後、粒子の流れが定常状態になつてから
粒子の移動度、すなわち単位時間当りに移動す
る距離を測定する。4 After the application, the particle mobility, that is, the distance traveled per unit time, is measured after the particle flow reaches a steady state.
5 測定終了後、直流電流の極性を逆転させ3項
及び4項と同様の操作を行い、逆方向の粒子の
移動度を測定する。5. After the measurement is completed, reverse the polarity of the DC current and perform the same operations as in Sections 3 and 4 to measure the mobility of particles in the opposite direction.
6 4及び5項で測定した移動度の平均をもつ
て、その粒子の1回の移動度とする。6 The average of the mobilities measured in Sections 4 and 5 is taken as the one-time mobility of the particle.
以下、2項乃至6項の操作を数十〜数百回繰返
し、その平均値をもつて、試料検体の粒子の平均
移動度とする。 Hereinafter, the operations in sections 2 to 6 are repeated several dozen to several hundred times, and the average value is taken as the average mobility of the particles of the sample specimen.
この電気泳動装置による測定で求められる電気
泳動度は電場強さ当りの各粒子の移動度(ボル
ト/センチメートル当りのミクロン/秒)で表わ
される。 The electrophoretic mobility determined by measurement using this electrophoresis device is expressed as the mobility of each particle per electric field strength (microns/second per volt/centimeter).
電気泳動による粒子の移動度は温度依存性が大
きい為、測定において正確な情報を得るには、測
定温度の管理に充分注意を払う必要があり、これ
が最も大きな課題となつている。 The mobility of particles due to electrophoresis is highly temperature dependent, so in order to obtain accurate information during measurement, it is necessary to pay sufficient attention to the management of the measurement temperature, which is the most important issue.
一般に測定セル内の温度を一定にするために、
測定セルの外部に媒体を循環させ、その媒体の温
度を一定に保つ方法が採られている。しかしこの
方法では、測定用の直流電流による測定セル内の
検体試料の発熱に対し、迅速な応答ができず、依
然として、上記課題は解決され得ない。 Generally, in order to keep the temperature inside the measurement cell constant,
A method is adopted in which a medium is circulated outside the measurement cell and the temperature of the medium is kept constant. However, with this method, it is not possible to quickly respond to the heat generation of the specimen sample in the measurement cell due to the direct current for measurement, and the above problem still cannot be solved.
ところで第4項において粒子の流れが安定する
までの時間は、およそ0.1〜0.2秒である。しかし
ながら測定用の直流電流を供給することにより発
生するジユール熱によつて、測定セル内の試料検
体の温度は上昇し、この温度を安定化する時間
は、セルの構造により異なるが一般に十数〜数百
秒である。従つて実際の移動度の測定時間は1回
あたり1〜3秒であるにもかかわらず、温度が、
安定したのちに測定を開始しようとすれば、1回
あたり十数〜数百秒の時間を要することになり、
多大な時間の労費である。 By the way, the time it takes for the flow of particles to stabilize in the fourth term is approximately 0.1 to 0.2 seconds. However, the temperature of the sample in the measurement cell rises due to the Joule heat generated by supplying the DC current for measurement, and the time required to stabilize this temperature varies depending on the structure of the cell, but generally it takes about 10 to 30 minutes. Several hundred seconds. Therefore, even though the actual mobility measurement time is 1 to 3 seconds per measurement, the temperature is
If you try to start measurement after it has stabilized, it will take tens to hundreds of seconds each time.
It costs a lot of time and labor.
また、測定用の直流電流を流した状態で温度の
安定するのを待つ間に、測定すべき粒子は、一方
向へ移動を続け、例えば、顕微鏡による電気泳動
測定方法では、大半の粒子が視野をはずれる結果
となつたり、粒子が一方向に移動してしまつたり
する為、温度一定のもとで、精度の高い測定を行
なうことは不可能であつた。 In addition, while waiting for the temperature to stabilize while a direct current is flowing for measurement, the particles to be measured continue to move in one direction. For example, in electrophoresis measurement using a microscope, most particles are visible It has been impossible to perform highly accurate measurements at a constant temperature because the particles may move in one direction.
従つて、界面動電現象の測定において、短時間
でかつ温度一定条件のもとで精度の高い測定値を
得ることは大きな課題となつている。 Therefore, in the measurement of electrokinetic phenomena, it is a major challenge to obtain highly accurate measured values in a short time and under constant temperature conditions.
上記の課題を解決すべく、本発明は、測定セル
内試料検体に交流電場を供給し、加熱することに
より、観察上は粒子を停止状態に保持しつつ直流
電場をかけた際と同一温度を保持することができ
る点に着目してなされたもので、測定精度の向上
および測定時間の短縮を目的とするものである。 In order to solve the above problems, the present invention supplies an AC electric field to the sample specimen in the measurement cell and heats it, thereby maintaining the particles at the same temperature as when applying a DC electric field while keeping the particles in a stopped state in observation. This was developed with the focus on the ability to maintain the measurement accuracy, and the purpose is to improve measurement accuracy and shorten measurement time.
本発明は、試料検体に測定用直流電場を供給す
る前に、測定用直流電場を供給した際に、試料検
体中で消費される電力と同じ程度の電力を試料検
体中で消費する交流電力を試料検体に供給するこ
とを特徴とする界面動電現象の測定方法、および
試料検体に電場をかける為の電源装置が、直流電
源と交流電源と両者のうちいずれかを選択する為
の出力選択回路とを有してなることを特徴とする
界面動電現象測定装置を提供する。 Before supplying the measurement DC electric field to the sample specimen, the present invention reduces the AC power consumed in the sample specimen to the same degree as the power consumed in the sample specimen when the measurement DC electric field is supplied. A method for measuring an electrokinetic phenomenon characterized by supplying an electric field to a sample specimen, and an output selection circuit for selecting either a DC power supply or an AC power supply as a power supply device for applying an electric field to the sample specimen. Provided is an electrokinetic phenomenon measuring device comprising:
すなわち、本発明はたとえば粒子の移動度の測
定に際し、電気泳動測定用の直流電流を試料検体
に供給していない時、つまり測定と測定の間に
は、測定用の直流電流が測定セル内で消費する電
力値と同じ値の電力を試料検体中で消費するよう
な交流電流を供給し続けることにより、試料検体
の温度を測定時と同じ状態に保つことを可能にす
るものである。 That is, when measuring the mobility of particles, for example, the present invention provides that when the DC current for electrophoresis measurement is not being supplied to the sample specimen, that is, between measurements, the DC current for measurement is not supplied to the sample in the measurement cell. By continuing to supply an alternating current that consumes the same amount of power in the sample as the consumed power, it is possible to maintain the temperature of the sample in the same state as during measurement.
ところで、本発明の電気泳動の測定で用いる交
流電力としては、測定すべき粒子を決定すること
の容易さから、粒子の運動が停止状態とみなし得
る周波数の使用が好ましく、通常10サイクル以上
が適当である。 By the way, for the AC power used in the electrophoresis measurement of the present invention, it is preferable to use a frequency at which the movement of the particles can be considered to be in a stopped state, from the viewpoint of ease of determining the particles to be measured, and usually 10 cycles or more is suitable. It is.
次に、本発明で用いる電源装置について、第1
図および第2図に示すブロツク図を参照しつつ説
明する。矩形波発振器Aによつて発せられた矩形
波は電力制御器Bによつて出力の調整が行われ、
さらにその次に接続された出力選択回路Cの指示
により、整流回路Dを通り、直流に変換されるか
あるいは、交流電流そのままであるかが決定さ
れ、負荷E(試料検体)に電場を供給するように
構成されている。 Next, regarding the power supply device used in the present invention, the first
This will be explained with reference to the block diagram shown in FIG. The output of the rectangular wave emitted by the rectangular wave oscillator A is adjusted by the power controller B,
Furthermore, according to the instructions of the output selection circuit C connected next, it is determined whether the current is converted to direct current or remains as alternating current through the rectifier circuit D, and an electric field is supplied to the load E (sample specimen). It is configured as follows.
この矩形波発振器は、商用交流電源によつて置
換え得るものである。 This square wave oscillator can be replaced by a commercial AC power source.
あるいは、第2図に示すごとく、第1図の発振
器Aの代りに、直流電源A1交流電源A2の2つか
ら構成され、それぞれが出力調整回路B1,B2を
経て、出力選択回路Cに接続されていてもよい。 Alternatively, as shown in Fig. 2, instead of the oscillator A in Fig. 1, it is composed of two DC power supplies A 1 and AC power supplies A 2 , each passing through output adjustment circuits B 1 and B 2 and connected to an output selection circuit. It may be connected to C.
本発明の測定方法および装置を用いることによ
り、温度一定のもとで移動度の測定が行われる
為、温度変化に起因する誤差の発生もなく、測定
精度を大きく向上させることができる。 By using the measuring method and apparatus of the present invention, mobility is measured under a constant temperature, so there is no error caused by temperature changes, and measurement accuracy can be greatly improved.
さらには、通常繰り返し測定が行なわれるが、
この場合も、交流を印加した状態で、測定粒子を
決定し、直ちに直流に切り換えを行ない、粒子の
移動度を測定するという操作を繰り返せばよく、
従来装置におけるごとく、温度の安定化のための
時間を必要とせず測定時間を大巾に短縮し得る。
次に、本発明に基づく顕微鏡を用いた電気泳動測
定装置の一実施例を説明する。 Furthermore, although repeated measurements are usually performed,
In this case as well, it is sufficient to repeat the operation of determining the particle to be measured while applying alternating current, immediately switching to direct current, and measuring the mobility of the particle.
Unlike conventional devices, no time is required for temperature stabilization, and the measurement time can be greatly shortened.
Next, an embodiment of an electrophoresis measuring device using a microscope based on the present invention will be described.
第3図に示すごとく、かかる電気泳動測定装置
は恒温槽1内に配置され、泳動室をなすU字型ガ
ラス管2と、このU字型ガラス管2の底部に50mm
の間隔で相対向して設置された1対の電極3,
3′と、これらの電極に電流を供給する電源7と
よりなるものである。 As shown in FIG. 3, this electrophoresis measuring device is placed in a thermostatic chamber 1, and has a U-shaped glass tube 2 forming a migration chamber, and a 50 mm
a pair of electrodes 3 placed opposite each other with an interval of
3', and a power source 7 that supplies current to these electrodes.
前記U字型ガラス管2は、試料検体21の満さ
れた内径2mmのU字管であり、その内部中央に
は、ポリエチレンチユーブで被覆された外径0.25
mmのシース熱電対32が設置されており、温度指
示器33により、U字型ガラス管内の温度が観測
される。 The U-shaped glass tube 2 is a U-shaped tube with an inner diameter of 2 mm filled with a sample specimen 21, and a tube with an outer diameter of 0.25 mm in the center thereof is covered with a polyethylene tube.
A mm sheathed thermocouple 32 is installed, and a temperature indicator 33 monitors the temperature inside the U-shaped glass tube.
電源7は、電気泳動を起す為の電場を試料にか
ける為の10mmAの直流定電流電源71と、商用周
波数の交流電源72に接続され、出力測定用の交
流電圧計74を具備する可変トランス73が出力
変換換回路17を介して並列接続されて構成され
ており、電極3,3′への電力供給を行なうしく
みとなつている。 The power source 7 includes a 10 mmA DC constant current power source 71 for applying an electric field to the sample to cause electrophoresis, and a variable transformer 73 connected to a commercial frequency AC power source 72 and equipped with an AC voltmeter 74 for output measurement. are connected in parallel via an output conversion circuit 17 to supply power to the electrodes 3 and 3'.
出力切換回路17は、閉じた時、直流正極性電
圧が通電電極3,3′に、印加されるように接続
された、直流正極性リレースイツチ18と、逆に
閉じた時、直流負極性電圧が、通常電極に印加さ
れるように接続された、直流負極性リレースイツ
チ19とよりなつており、両方共、開かれている
時は、交流電源72に接続されているような回路
である。 The output switching circuit 17 is connected to a DC positive polarity relay switch 18 which is connected so that when closed, a DC positive polarity voltage is applied to the current-carrying electrodes 3, 3', and conversely, when it is closed, a DC negative polarity voltage is applied. The circuit consists of a direct current negative polarity relay switch 19 which is connected so that the voltage is normally applied to the electrode, and when both are open, the circuit is connected to an alternating current power source 72.
一方、恒温槽1は温度調節装置4とヒータ15
とにより20℃±0.1℃に設定されている。 On the other hand, the constant temperature bath 1 has a temperature control device 4 and a heater 15.
The temperature is set at 20℃±0.1℃.
次に、この電気泳動測定装置を用いた測定の実
験例1について述べる。 Next, Experimental Example 1 of measurement using this electrophoresis measuring device will be described.
まず、試料として生理的食塩水の注入されたU
字型ガラス管2を、恒温槽1内に設置する。次に
交流電源72をONにし、可変トランス73によ
つて出力を電圧計74の値が108Vとなるように
調整しつつ、約10分間にわたり通電電極3,3′
への交流電流の供給を行なう。(このとき直流正
極性リレースイツチ18および直流負極性リレー
スイツチ19はOFF状態に保持しておく。)
このようにして、温度指示器33の指示値が一
定となり、安定状態となつたところで、直流正極
性リレースイツチ18を押してON状態にし、供
給する電流を交流から直流に切換える。 First, U injected with physiological saline as a sample.
A letter-shaped glass tube 2 is placed in a constant temperature bath 1. Next, the AC power supply 72 is turned on, and while the output is adjusted by the variable transformer 73 so that the value on the voltmeter 74 becomes 108V, the current-carrying electrodes 3, 3'
supplies alternating current to the (At this time, the DC positive polarity relay switch 18 and the DC negative polarity relay switch 19 are kept in the OFF state.) In this way, when the indicated value of the temperature indicator 33 becomes constant and stable, the DC Push the positive polarity relay switch 18 to turn it on and switch the supplied current from alternating current to direct current.
このとき、U字型ガラス管2内の温度は温度指
示器33の指示値によると、交流から直流に切換
えた場合の温度変化も0.1℃以下となつている。 At this time, according to the indicated value of the temperature indicator 33, the temperature inside the U-shaped glass tube 2 changes by 0.1° C. or less when switching from alternating current to direct current.
ちなみに、従来のごとく測定時のみ直流電流
を、通電電極に供給した場合のU字型ガラス管内
の温度の時間的変化は第4図に示すごとくなつて
いる。第4図において、たて軸は温度T(℃)横
軸は時刻t(sec)とした。 Incidentally, when direct current is supplied to the current-carrying electrode only during measurement as in the conventional case, the temperature within the U-shaped glass tube changes over time as shown in FIG. 4. In FIG. 4, the vertical axis represents temperature T (° C.), and the horizontal axis represents time t (sec).
第4図を参照することによつても、本発明の装
置および方法を測定に用いることにより、温度条
件一定のもとで、測定を行なうことができ、測定
精度が大幅に向上することが立証される。 Referring to FIG. 4, it is proved that by using the apparatus and method of the present invention for measurement, it is possible to perform measurements under constant temperature conditions, and the measurement accuracy is greatly improved. be done.
実際の粒子の移動度の測定にあたつては、次の
様な操作を行なう。観察上粒子が停止状態にある
交流電流供給時に、測定すべき粒子を決定し、試
料検体内の温度が充分に安定したところで、直流
正極性リレースイツチ18をONにし、粒子の移
動する速度を測定する。次に、直流負極性リレー
スイツチ19をONにし、前記の粒子の逆方向へ
移動する速度を測定し、正、負両方向の速度の平
均値をとり1つの粒子の移動度とする。 When measuring the actual mobility of particles, the following operations are performed. Determine the particles to be measured when AC current is supplied when the particles are in a stopped state for observation, and when the temperature inside the sample becomes sufficiently stable, turn on the DC positive polarity relay switch 18 and measure the speed at which the particles move. do. Next, the direct current negative polarity relay switch 19 is turned on, the velocity of the particles moving in the opposite direction is measured, and the average value of the velocity in both the positive and negative directions is taken as the mobility of one particle.
そしてさらに又、正方向、負方向というふうに
数十ないし数百回程度の繰り返し測定を行ない、
平均値が移動度とされるのである。 Then, repeat measurements several tens to hundreds of times in the positive and negative directions.
The average value is considered the mobility.
さらに、本発明についての第2の実施例の電気
泳動測定装置および測定方法について第5図およ
び第6図を参照しつつ説明する。 Furthermore, an electrophoresis measuring device and a measuring method according to a second embodiment of the present invention will be described with reference to FIGS. 5 and 6.
かかる電気泳動測定装置は、外側に冷却水の循
環槽10を有する厚さ0.7mm、高さ7mmの角型測
定セル20と、その両端に設定された通電電極
3,3′とこれらに電力供給を行なう電源装置8
0とより構成されている。 This electrophoresis measuring device includes a rectangular measuring cell 20 with a thickness of 0.7 mm and a height of 7 mm having a cooling water circulation tank 10 on the outside, energized electrodes 3 and 3' set at both ends of the cell, and power supplied to these. A power supply device 8 that performs
0.
循環槽10は温度調節装置4とヒータ15とに
よつて20℃±0.1℃に設定されている。 The circulation tank 10 is set at 20° C.±0.1° C. by the temperature controller 4 and the heater 15.
セル20内には、試料検体である培養液イー
グルに羊の赤血球を浮遊させたものが満たされ、
さらに通電電極3,3′の内側に、電圧測定用電
極12,12′が設置され、これに接続された直
流電圧計45により電圧の測定が行なえるように
なつている。又、電源装置80は第6図に示され
るごとく矩形波発振器81と、発振器81からの
矩形波信号を増幅する増幅器82と、増幅器82
からの矩形波電圧を昇圧するパルストランス83
と、トランス83からの交流矩形波電力を整流す
る整流器群84と、制御回路85とからなり整流
器群84は、ダイオード86〜89を有してい
る。制御回路85は、直流正極性指示用のリレー
スイツチ90及び直流負極性指示用のリレースイ
ツチ91と常閉接点92を有するリレー93と、
常開接点94,95を有するリレー96と、常閉
接点97,98及び常開接点99とを有するリレ
ー100とを有しており、リレー93,96,1
00には、交流電源101からの電圧が印加され
ている。 The cell 20 is filled with culture solution Eagle, which is a sample specimen, in which sheep red blood cells are suspended.
Further, voltage measuring electrodes 12, 12' are installed inside the current-carrying electrodes 3, 3', and voltage can be measured by a DC voltmeter 45 connected thereto. Further, as shown in FIG. 6, the power supply device 80 includes a rectangular wave oscillator 81, an amplifier 82 for amplifying the rectangular wave signal from the oscillator 81, and an amplifier 82.
A pulse transformer 83 that boosts the rectangular wave voltage from
, a rectifier group 84 that rectifies the AC rectangular wave power from the transformer 83, and a control circuit 85, and the rectifier group 84 has diodes 86 to 89. The control circuit 85 includes a relay switch 90 for direct current positive polarity instruction, a relay switch 91 for direct current negative polarity instruction, and a relay 93 having a normally closed contact 92;
It has a relay 96 having normally open contacts 94 and 95, and a relay 100 having normally closed contacts 97 and 98 and a normally open contact 99.
A voltage from the AC power supply 101 is applied to 00.
リレースイツチ90,91はそれぞれ常開接点
102,103及び104,105を有してお
り、交流電源101からリレー93,96,10
0へ供給される電流を制御する構成となつてい
る。 Relay switches 90, 91 have normally open contacts 102, 103 and 104, 105, respectively, and relays 93, 96, 10 are connected to AC power supply 101.
It is configured to control the current supplied to zero.
電源装置80において出力端子107,108
は、通電電極3,3′に接続されているが、この
出力端子108は、トランス83の2次側巻線の
中点からそのままとり出されたものであり、出力
端子107は、制御回路の出力に接続されてい
る。増幅器82はその増幅度を外部から任意に調
節できるようになつている。 Output terminals 107 and 108 in the power supply device 80
is connected to the current-carrying electrodes 3 and 3', but this output terminal 108 is directly taken out from the middle point of the secondary winding of the transformer 83, and the output terminal 107 is connected to the control circuit. connected to the output. The amplification degree of the amplifier 82 can be arbitrarily adjusted from the outside.
リレースイツチ90及び91が作動されない際
には、リレー93,96,100のいずれも励磁
されないため、ダイオード88,89には電流が
流れず、ダイオード86,87には交互に交流電
流が流れ、出力端子107,108には、発振器
81から発生される矩形波信号に対応した交流電
圧が出力され、通電電極3,3′には交流電圧が
印加される。 When relay switches 90 and 91 are not activated, none of relays 93, 96, and 100 are energized, so no current flows through diodes 88 and 89, and alternating current flows alternately through diodes 86 and 87, resulting in output An AC voltage corresponding to a rectangular wave signal generated from the oscillator 81 is output to the terminals 107 and 108, and an AC voltage is applied to the current-carrying electrodes 3 and 3'.
直流正極性のリレースイツチ90がシーケンス
回路(図示せず)により作動されると、接点10
2,103がONとなり、リレー93,96が励
磁され接点92はOFF、接点94,95がONと
なる為、ダイオード87,89に交互に、同一極
性の電流が流れ出力端子107,108には、直
流電圧が出力され、通電電圧3,3′には直流正
極性電圧が印加される。 When the DC positive polarity relay switch 90 is activated by a sequence circuit (not shown), the contact 10
2 and 103 are turned on, relays 93 and 96 are energized, contact 92 is turned off, and contacts 94 and 95 are turned on, so currents of the same polarity alternately flow through diodes 87 and 89 to output terminals 107 and 108. , a DC voltage is output, and a DC positive polarity voltage is applied to the energizing voltages 3, 3'.
逆に、直流負極性のリレースイツチ91がシー
ケンス回路(図示せず)により作動されると接点
104,105がONとなり、リレー96,10
0が励磁され、接点97,98はOFF、94,
95,99はONとなり、ダイオード86および
88に、交互に前述の場合とは逆方向で同一極性
の電流が流れ、出力端子107,108には直流
電圧が出力され、通電電極3,3′には直流負極
性の電圧が印加される。 Conversely, when DC negative polarity relay switch 91 is activated by a sequence circuit (not shown), contacts 104 and 105 turn ON, and relays 96 and 10
0 is excited, contacts 97 and 98 are OFF, 94,
95 and 99 are turned on, currents of the same polarity alternately flow through diodes 86 and 88 in the opposite direction to that in the above case, and a DC voltage is output to output terminals 107 and 108, and current is applied to current-carrying electrodes 3 and 3'. A negative DC voltage is applied.
かかる測定装置を用いた場合の電気泳動測定の
操作は、第1の実施例で述べたのと同様に行なわ
れるが、シーケンス回路(図示せず)により、正
極性リレースイツチ90および負極性リレースイ
ツチ91の操作電圧が供給され、交流、直流(正
極性、負極性)の操作は進められる。 The operation of electrophoresis measurement using such a measuring device is performed in the same manner as described in the first embodiment, but a sequence circuit (not shown) controls the positive polarity relay switch 90 and the negative polarity relay switch. 91 operating voltage is supplied, and AC and DC (positive polarity, negative polarity) operations proceed.
上述の電源装置を用いた場合、交、直流切換時
の温度変化は0.1℃以下、電圧変動は0.5V以下と
なつた。ちなみに従来の電源装置を用い測定時の
み10mAの直流電流を流した場合は、通電開始時
71.5Vであつた電圧は70Vとなり、温度変化は第
7図のごとくであつた。第7図においてたて軸は
温度T(℃)、横軸は時刻t(sec)とした。 When using the above power supply device, the temperature change when switching between AC and DC was less than 0.1°C, and the voltage fluctuation was less than 0.5V. By the way, if you use a conventional power supply and apply a 10mA DC current only during measurement, the
The voltage that was 71.5V became 70V, and the temperature change was as shown in Figure 7. In FIG. 7, the vertical axis is temperature T (° C.), and the horizontal axis is time t (sec).
これらの測定結果から明らかなように、かかる
装置を用い、本発明の測定方法によれば、非常に
精度のよい測定が可能でありしかも、温度の安定
化に時間を浪費することなく、短時間で測定を行
うことができる。 As is clear from these measurement results, using such an apparatus and the measurement method of the present invention, it is possible to perform measurements with very high precision, and also in a short period of time without wasting time in stabilizing the temperature. Measurements can be made with
なお、実施例においては顕微鏡による電気泳動
測定についてのみ説明してきたが、これに限らず
デイテクタードプラー法等による電気泳動の測定
あるいは、電気浸透現象の測定においても適用で
きることは言うまでもない。 In the examples, only electrophoresis measurements using a microscope have been described, but it goes without saying that the present invention is not limited to this and can also be applied to electrophoresis measurements using a detector Doppler method or the like, or to measurements of electroosmotic phenomena.
以上説明してきたように、本発明の界面動電現
象測定方法および装置は供給電流によるジユール
熱等の影響も受けることなく、精度良い測定値を
得ることができるものである。 As described above, the electrokinetic phenomenon measuring method and apparatus of the present invention can obtain highly accurate measured values without being affected by Joule heat or the like caused by the supplied current.
第1図及び第2図は、本発明の電源装置を示す
ブロツク図、第3図は、本発明第1の実施例の電
気泳動測定装置の概要図、第4図は、従来の測定
装置を用いた場合のU字型ガラス管内の温度変化
を示す説明図、第5図は、本発明第2の実施例の
電気泳動測定装置の概略図、第6図は、同電源装
置の回路図、第7図は、従来の測定装置を用いた
場合の測定セル内の温度変化を示す説明図であ
る。
1……恒温槽、2……U字型ガラス管、3,
3′……通電電極、4……温度調節装置、7……
電源装置、10……循環槽、12,12′……電
圧測定用電極、15……ヒータ、17……出力選
択回路、18……正極性リレースイツチ、19…
…負極性リレースイツチ、20……角型測定セ
ル、21……試料検体、32……シース熱電対、
33……温度指示器、45……直流電圧計、71
……直流電源、72……交流電源、73……可変
トランス、74……電圧計、80……電源装置、
81……発振器、82……増幅器、83……パル
ストランス、84……整流器群、85……制御回
路、86〜89……ダイオード、90,91……
リレースイツチ、92,97,98……常閉接
点、93,96,100……リレー、94,9
5,99,102,103,104,105……
常開接点、101……交流電源、107,108
……出力端子。
1 and 2 are block diagrams showing a power supply device of the present invention, FIG. 3 is a schematic diagram of an electrophoresis measuring device according to a first embodiment of the present invention, and FIG. 4 is a diagram showing a conventional measuring device. FIG. 5 is a schematic diagram of the electrophoresis measuring device according to the second embodiment of the present invention, FIG. 6 is a circuit diagram of the same power supply device, FIG. 7 is an explanatory diagram showing temperature changes within a measurement cell when a conventional measurement device is used. 1... Constant temperature chamber, 2... U-shaped glass tube, 3,
3'... Current-carrying electrode, 4... Temperature control device, 7...
Power supply device, 10... Circulation tank, 12, 12'... Voltage measurement electrode, 15... Heater, 17... Output selection circuit, 18... Positive polarity relay switch, 19...
... Negative polarity relay switch, 20 ... Square measurement cell, 21 ... Sample specimen, 32 ... Sheathed thermocouple,
33...Temperature indicator, 45...DC voltmeter, 71
... DC power supply, 72 ... AC power supply, 73 ... Variable transformer, 74 ... Voltmeter, 80 ... Power supply device,
81... Oscillator, 82... Amplifier, 83... Pulse transformer, 84... Rectifier group, 85... Control circuit, 86-89... Diode, 90, 91...
Relay switch, 92, 97, 98... Normally closed contact, 93, 96, 100... Relay, 94, 9
5,99,102,103,104,105...
Normally open contact, 101...AC power supply, 107, 108
...Output terminal.
Claims (1)
検体中で消費される電力と同程度の電力を、測定
用直流電場をかける前に試料検体中で消費させる
べく、交流電流を試料検体に供給することを特徴
とする界面動電現象の測定方法。 2 前記試料検体が泳動室内に収容された懸濁液
であり、この懸濁液中のコロイド粒子の電気泳動
度を測定するにあたり、前記交流電流が、その移
動度を測定すべきコロイド粒子を停止状態とみな
し得る程度の周波数を有することを特徴とする特
許請求の範囲第1項に記載の界面動電現象測定方
法。 3 試料検体に電場をかける為の電源装置を有し
てなり、試料検体中の界面動電現象を測定する装
置において、前記電源装置が、試料検体に測定用
電場をかける為の直流電源と、測定用電場をかけ
る前に、交流電流を試料検体に流す為の交流電源
と、それらのいずれかを選択する為の出力選択回
路を有していることを特徴とする界面動電現象測
定装置。 4 前記試料検体が泳動室内に収容された懸濁液
でありこの懸濁液中のコロイド粒子の電気泳動度
を測定する装置であつて、交流電源が、移動度を
測定すべきコロイド粒子を停止状態とみなし得る
程度の周波数を有するものであることを特徴とす
る特許請求の範囲第3項に記載の界面動電現象測
定装置。[Scope of Claims] 1. In order to consume the same amount of power in the sample specimen before applying the measurement DC electric field to the sample specimen as the power consumed in the sample specimen when applying the measurement DC electric field to the sample specimen, A method for measuring electrokinetic phenomena characterized by supplying a current to a sample specimen. 2. The sample specimen is a suspension contained in an electrophoresis chamber, and when measuring the electrophoretic mobility of colloidal particles in this suspension, the alternating current stops the colloidal particles whose mobility is to be measured. The electrokinetic phenomenon measuring method according to claim 1, characterized in that the electrokinetic phenomenon measurement method has a frequency that can be considered as a state. 3. An apparatus for measuring an electrokinetic phenomenon in a sample, comprising a power supply for applying an electric field to a sample, the power supply having a DC power supply for applying a measurement electric field to the sample; An electrokinetic phenomenon measuring device characterized by having an AC power supply for passing an AC current through a sample specimen and an output selection circuit for selecting one of them before applying an electric field for measurement. 4. An apparatus for measuring the electrophoretic mobility of colloidal particles in the suspension in which the sample specimen is a suspension contained in an electrophoresis chamber, wherein the AC power supply stops the colloidal particles whose mobility is to be measured. The electrokinetic phenomenon measuring device according to claim 3, wherein the electrokinetic phenomenon measuring device has a frequency that can be considered as a state.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56009799A JPS57124249A (en) | 1981-01-26 | 1981-01-26 | Method and apparatus for measuring interfacial dynamic electricity phenomenon |
| US06/238,822 US4433299A (en) | 1980-03-07 | 1981-02-27 | Method and apparatus for measuring interfacial electrokinetic phenomena |
| DE8181300931T DE3171972D1 (en) | 1980-03-07 | 1981-03-05 | Method and apparatus for measuring interfacial electrokinetic phenomena |
| EP81300931A EP0035878B1 (en) | 1980-03-07 | 1981-03-05 | Method and apparatus for measuring interfacial electrokinetic phenomena |
| DD81228148A DD156846A5 (en) | 1980-03-07 | 1981-03-09 | METHOD AND DEVICE FOR MEASURING ELECTRKINETIC APPEARANCE ON BORDERS |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56009799A JPS57124249A (en) | 1981-01-26 | 1981-01-26 | Method and apparatus for measuring interfacial dynamic electricity phenomenon |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57124249A JPS57124249A (en) | 1982-08-03 |
| JPS6353499B2 true JPS6353499B2 (en) | 1988-10-24 |
Family
ID=11730236
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56009799A Granted JPS57124249A (en) | 1980-03-07 | 1981-01-26 | Method and apparatus for measuring interfacial dynamic electricity phenomenon |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57124249A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104122316B (en) * | 2014-06-30 | 2016-05-25 | 中国科学院化学研究所 | Utilize distributed DC electric field to measure the mobility of particle and the method for dielectric mobility simultaneously |
| CN108896630B (en) * | 2018-06-11 | 2020-05-12 | 杨韫瑜 | Multifunctional temperature-controllable electrolytic cell for biological and chemical analysis |
-
1981
- 1981-01-26 JP JP56009799A patent/JPS57124249A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57124249A (en) | 1982-08-03 |
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