TW200523706A - Micro flow rate generator, pump and pump system - Google Patents

Micro flow rate generator, pump and pump system Download PDF

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Publication number
TW200523706A
TW200523706A TW093136330A TW93136330A TW200523706A TW 200523706 A TW200523706 A TW 200523706A TW 093136330 A TW093136330 A TW 093136330A TW 93136330 A TW93136330 A TW 93136330A TW 200523706 A TW200523706 A TW 200523706A
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TW
Taiwan
Prior art keywords
solution
pump
voltage
flow
aforementioned
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TW093136330A
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Chinese (zh)
Inventor
Tomiiti Hasegawa
Makoto Morita
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Niigata Tlo Corp
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Publication of TW200523706A publication Critical patent/TW200523706A/en

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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04BPOSITIVE-DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS
    • F04B17/00Pumps characterised by combination with, or adaptation to, specific driving engines or motors
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04BPOSITIVE-DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS
    • F04B19/00Machines or pumps having pertinent characteristics not provided for in, or of interest apart from, groups F04B1/00 - F04B17/00
    • F04B19/006Micropumps

Abstract

A micro flow rate generator comprising a porous thin film placed in a channel, a pair of electrodes arranged on the opposite sides of the porous thin film, a means for supplying solution to the channel, and a DC power supply for applying a DC voltage between the pair of electrodes, characterized in that the solution has been processed so as not to cause electrolysis and a flow of the solution passing through the porous thin film is generated by applying a DC voltage between the pair of electrodes.

Description

200523706 (1) 九、發明說明 [發明所屬之技術領域】 本發明係關於能夠控制液體的微少流量之方法、及 使用該方法之泵浦、以及使用該方法之泵浦系統,特別 係關於適合於使用在生物物質或藥品、食品等的分析之 微少流量產生裝置及泵浦以及泵浦系統。200523706 (1) IX. Description of the invention [Technical field to which the invention belongs] The present invention relates to a method capable of controlling a small flow rate of a liquid, a pump using the method, and a pump system using the method, and particularly to a method suitable for It is used for the analysis of biological substances, pharmaceuticals, food, etc., and a small flow generating device, a pump, and a pump system.

【先前技術】 通過管內的液體之流量控制係以往以來,使用機械 性閥改變張開度,或調整壓力之方法來進行。例如,在 專利文獻1,揭示有具備藥液供給泵浦之藥液供給裝置, 其中藥液供給泵浦係進行由藥液儲藏槽振動地送出藥液 的動作之隔膜泵浦。且,在專利文獻2,揭示有洗淨水噴 出裝置,該裝置係具備將氣泡混入至洗淨水之氣泡混入[Prior art] Control of the flow rate of the liquid in the tube has been performed by using a mechanical valve to change the opening degree or adjust the pressure. For example, Patent Document 1 discloses a medicinal solution supply device including a medicinal solution supply pump, wherein the medicinal solution supply pump is a diaphragm pump that performs an operation of vibratingly delivering a medicinal solution from a medicinal solution storage tank. Further, Patent Document 2 discloses a washing water spraying device including a bubble mixing device for mixing bubbles into the washing water.

手段,將多量的細微氣泡分散於洗淨水中之氣泡水流噴 出。 .、 但,由於這些方法會產生脈動流,故不適合於須要 精度良好地控制微少流量之用途上。 一方面,在專利文獻3,揭示有流體供給裝置,該裝 置係具備流體儲藏部、壓力傳送部、及將添加有作爲陰 離子移動的媒體之陰離子交換樹脂及導電劑的金屬氧化 物使用於陰極之電化學電池部。 又’爲了獲得無脈動流或低脈動流且低流量之泵浦 而根據細長的毛管體之電氣滲透流或利用電氣泳動( ~ 4 - 200523706 (2) migration )以產生微少流量之方法,被揭示於專利文獻 4。例如,揭示有:如其圖1所示,在由一端將試料溶液 導入至石英毛管後,在毛管量端施加高電壓,進行電氣 泳動,使電氣泳動分離成分移動之例。 且,不施加高電壓,而使電池等之較低的電壓,藉 由多孔質薄膜,以控制或產生溶液之微少流量的發明, 爲根據本發明的發明者們之硏究成果,如非專利文件i 所示。 若根據非專利文獻]的話,記載有:使用離子化程 度大的鈉水溶液或鉀水溶液作爲溶液,能夠適當地控制 微少流量。 專利文獻1 :日本特開2 0 0 0 - 2 6 5 9 4 5號公報 專利文獻2:國際公開WO99/09265 專利文獻3 :日本特開平9- 1 922 1 3號公報 專利文獻4 :日本特開平9 - 2 8 1 0 7 7號公報 非專利文獻]:杉谷、長谷川、鳴海:「通過電壓附 加時的多孔質薄片之流體的流動特性」;日本機械學會 北陸信越支部第39期總會、演講論文集[No〇27_1;)P93〜 94 ( 2002 年 3 月 8 曰) 【發明內容】 作爲進行微少流量之控制者,進行··例如,在微管 道內使包含血液、DNA或細胞等之溶液流動,藉由顯微 鏡擴大觀察對象物。在此情況時,當在泵浦流量具有變 -5 - 200523706 (3) 動或脈動等時,則已被擴大的對象物之像振動,無法進 行精確的觀察。因此,期望無脈動、變動之泵浦。又, 亦被要求不會有堵塞而可確保穩定的流量,並且處理性 良好或廉價者。 但,在現時間點,並無可充分地滿足如此要求之泵 浦。特別係在以往的泵浦,無法簡單地改變流動的正反 〇 例如,前述專利文獻4所記載之使用毛管體般之細 微管的電氣滲透流或利用電氣泳動以產生微少流量之方 法’係需要1 00 V以上之高電壓,其相反面,由於所獲得 的流量少,故不易進行微少流量之控制。 一方面,關於前述專利文獻1所記載之使用多孔質 薄膜的微少流量控制之發明,係硏究開發的過程之發明 ’在貫用化上存在有數個應解決之問題。其一,因使用 a有鈉或鉀之水溶液作爲作動流體,所以會有受到電壓 方也加而在內部產生氫或氣泡,而改變了流量特性。 本發明之目的係在於解決上述課題,提供在流體內 不會有氫或氣泡產生之無脈流或低脈流的微少流量產生 裝置及泵浦以及泵浦系統。 本發明之另~目的係在於提供以較低的電壓即足夠 且k里控制彳谷液之無脈流或低脈流的微少流量產生裝 置及泵浦以及泵浦系統。 又,本發明的另一目的係在於不會有堵塞,可確保 L疋的&夏,並且處理性良好而廉價之微少流量產生裝 ^ 6 - 200523706 (4) 置及泵浦以及泵浦系統。 [用以解決課題之手段] 本發明的微少流量產生裝置之特徵係在於:具備有 :配置於流通路之多孔質薄膜、設置於該多孔質薄膜的 兩側之一對電極、將溶液供給至前述流通路之手段、及 在前述一對電極間施加直流電壓之直流電源,前述溶液 爲處理成不會產生電氣分解之溶液,藉由在前述一對電 極間施加直流電壓’使過前述多孔質薄膜的前述溶液之 流動產生。 本發明的其他特徵係在於:作爲處理成不會產生前 述電氣分解之溶液’在前述溶液中添加氧化劑。 本發明的其他特徵係在於:作爲處理成不會產生前 述電氣分解之溶液,前述溶液爲使粒徑〇 (Πμηι〜〇 5_ 之微粒子浮游於媒體之液體。 本發明的其他特徵係在於:使用前述微少流量產生 裝置之泵浦或泵浦系統。 在本發日月之微少流量產生裝置、栗浦或栗浦系統, 在流遇路中女裝多孔質溥膜’在一對電極施加直流電壓 ’該電極係夾持多孔質溥膜而配置成溶液的流入側爲陽 極、而流出側爲陰極。在這之中,因根據溶液、電極、 膜的種類之組合、或溶液的離子化程度等之條件,使得 電壓對流量之關係有所不同,所以藉由該組合,能夠進 行微少W里之控制。藉由過且地設定上述諸條件,可獲 -Ί - 200523706 (5) ^ &得到與施加電壓大致成比例的流量之泵浦。Means, a large amount of fine bubbles are dispersed in the bubble water jet of the washing water to be ejected. However, because these methods generate pulsating flow, they are not suitable for applications that require precise control of small flows. On the other hand, Patent Document 3 discloses a fluid supply device including a fluid storage section, a pressure transmission section, and a metal oxide to which an anion exchange resin and a conductive agent added as a medium for anion movement are used. Electrochemical cell department. Also, in order to obtain a pump with no pulsating flow or low pulsating flow and low flow, a method of generating a small flow based on the electric permeation flow of a slender capillary body or the use of electrical swimming (~ 4-200523706 (2) migration) was revealed. In Patent Document 4. For example, as shown in FIG. 1, an example is shown in which a sample solution is introduced into a quartz capillary tube from one end, a high voltage is applied to the capillary end, and electrophoresis is performed to move the electrophoretic separation component. In addition, the invention that does not apply a high voltage and allows a lower voltage of a battery or the like to control or generate a small flow of a solution through a porous film is the research result of the inventors according to the present invention, such as a non-patent File i is shown. According to the non-patent literature], it is described that a small flow rate can be appropriately controlled using an aqueous solution of sodium or potassium having a large degree of ionization. Patent Document 1: Japanese Patent Laid-Open No. 2 0 0 0-2 6 5 9 4 5 Patent Document 2: International Publication WO99 / 09265 Patent Document 3: Japanese Patent Laid-Open No. 9- 1 922 1 Patent Document 4: Japanese Patent Kaiping 9-2 8 1 0 7 7 Non-Patent Documents]: Sugiya, Hasegawa, Naruto: "Flow characteristics of fluid through porous flakes when voltage is applied"; The 39th General Assembly of the Hokuriku Shin-Etsu Branch, Japan Mechanical Engineering Association, Proceedings [No〇27_1;) P93 ~ 94 (March 8, 2002) [Summary of the Invention] As a controller that performs a small amount of flow, perform ... For example, a microchannel containing blood, DNA, or cells The solution flows, and the observation object is enlarged with a microscope. In this case, when there is a change in the pump flow rate -5-200523706 (3) Vibration or pulsation, the image of the enlarged object cannot be accurately observed. Therefore, a pump without pulsation and fluctuation is desired. In addition, it is also required to have a stable flow rate without clogging, and to have good handling properties or low cost. However, at this point in time, there is no pump that can adequately meet such requirements. In particular, in conventional pumps, it is not possible to simply change the flow direction. For example, the electric permeation flow using a capillary tube-like capillary tube as described in the aforementioned Patent Document 4 or a method using electrophoresis to generate a small flow is required On the other hand, for high voltages above 1 00 V, it is not easy to control a small flow because the flow obtained is small. On the one hand, the invention of the minute flow rate control using a porous film described in the aforementioned Patent Document 1 is an invention that has been researched in the development process. First, since an aqueous solution containing sodium or potassium is used as the working fluid, a voltage receiving side is also applied to generate hydrogen or air bubbles inside, thereby changing the flow characteristics. An object of the present invention is to solve the above-mentioned problems and provide a minute flow rate generating device, a pump, and a pumping system that have no pulse flow or low pulse flow without generating hydrogen or bubbles in the fluid. Another object of the present invention is to provide a minute flow rate generating device, a pump, and a pumping system that control a pulseless flow or a low pulse flow of the barley fluid at a low voltage, which is sufficient and k mile. In addition, another object of the present invention is to prevent clogging, to ensure that L 疋 & summer is good, and that the processability is low and the flow rate generation device is inexpensive. 6-200523706 (4) Installation and pumping and pumping system . [Means for solving the problem] The minute flow generating device of the present invention is characterized by including a porous film disposed in a flow path, a pair of electrodes provided on one of both sides of the porous film, and supplying a solution to The means for the flow path, and a DC power source for applying a DC voltage between the pair of electrodes. The solution is a solution that does not cause electrical decomposition, and the porous material is passed through applying a DC voltage between the pair of electrodes. The flow of the aforementioned solution of the film is generated. Another feature of the present invention is that an oxidizing agent is added to the solution as a solution processed so as not to cause the aforementioned electrolysis. Another feature of the present invention is that it is a solution that is processed so as not to cause the aforementioned electrical decomposition, and the solution is a liquid in which fine particles having a particle size of 0 (Πμηι ~ 〇5_ float in the medium. Another feature of the present invention is that the aforementioned is used The pump or pump system of the micro-flow generating device. In the micro-flow generating device, Kuriura or Kuriura system of the current sun and the moon, the women's porous membrane in the flow path is 'applying a DC voltage to a pair of electrodes' The electrode is configured such that the inflow side of the solution is an anode and the outflow side is a cathode by sandwiching a porous rhenium membrane. Among them, the electrode is based on the combination of the type of the solution, the electrode, and the membrane, or the degree of ionization of the solution. The conditions make the voltage-flow relationship different, so with this combination, you can control a small amount of W. By setting the above conditions, you can get -Ί-200523706 (5) ^ & A pump that applies a voltage proportional to the flow rate.

例如,因鈉水溶液或鉀水溶液係離子化程度大,所 以將這些作爲溶液來使用的話,則能夠理想地控制微少 流量’但如前所述,會產生氣泡。發明者係精心硏究之 結果’可得知,即使爲鈉水溶液或鉀水溶液的電解質者 ’ S使用在水溶液中添加過氧化氫等的氧化劑之方法、 或作爲溶液使用將微粒子分散之膠體溶液時,則在液體 中不會產生氫氣或氣泡,能夠藉由微少的電壓來理想地 控制流量,而開發出本發明。 【發明效果】For example, since the degree of ionization of an aqueous sodium or potassium solution is large, if these are used as a solution, it is possible to ideally control a slight flow rate ', but as described above, bubbles may be generated. As a result of careful investigation, the inventor has found that even if it is an electrolyte of a sodium or potassium aqueous solution, it is a method of adding an oxidizing agent such as hydrogen peroxide to an aqueous solution, or a colloidal solution in which fine particles are dispersed as a solution. The present invention was developed by not generating hydrogen or bubbles in the liquid and ideally controlling the flow rate with a small voltage. [Inventive effect]

若根據本發明的話,可達到下述效果:微少流量產 生裝置係具備配置於溶液的流通路中之多孔質薄膜與一 對電極,藉由在此電極間施加較低的電壓、例如丨〇 v左 右的直流電壓,能夠產生無脈動之溶液的微少流量。此 流量係形成與施加電壓大致呈比例者,使得容易控制流 量,處理性良好而廉價。又,不會有堵塞,而可確保穩 定的流量,也就是在溶液的內部不會產生氫氣或氣泡, 即使〜直反復進行,流量特性也不會改變。 【實施方式】 以下,說明本發明的實施形態。首先,說明本發明 的微少流量產生裝置之基本結構。 _] A係顯示本發明的微少流量產生裝置之原理的示 冬 200523706 (6) 意圖。圖1 B係顯示本發明的微少流量產生裝置之局部的 斜視圖。在供溶液2 0流動之管路(流通路)1的途中, 於與此管路的軸線方向呈垂直的方向,經由支承體3安 裝多孔質薄膜2。又,在夾持著此多孔質薄膜2而上游側 及下游側設置一對電極4、5。支承體3的圓形開口部也 就是多孔質薄膜2面對流動之圓形區域、與設於一對電 極4、5的圓形開口部,實質上係具有相同半徑,各中心 位於管路的軸線上。 溶液20係被處理成不會產生電氣分解。因而在溶液 中添加氧化劑。亦可在陰極使用鉛電極,或亦可使用如 此溶液與鉛電極之組合。 又’作爲其他方法,溶液2 0亦可爲在媒體使粒徑爲 0.0 1 μΐΒ〜0 · 5 μηι的微粒子浮游之液體。在此情況,微粒 子係須要在液體中具有帶電之性質。例如,能夠使用在 溶液中使微粒子分離之膠體狀溶液。 夾持多孔質薄膜2配置的一對電極係以溶液的流入 側爲陽極4、流出側爲陰極5之方式,由直流電源6經由 開關7施加]00V以下的預定直流電壓。在圖示例,作成 左側爲陽極4、而右側爲陰極5之情況,溶液2 0朝箭號 方向流動。再者,當在一對電極間施加1 0V〜2 0V的電 壓時,流動於電極間之電流爲3 0 // Α〜1 〇 〇 μ Α左右的微 少電流,所消耗的電力極少,這是本發明的特徵之一。 再者,如後所詳述般,根據構成要素之溶液、電極 、及多孔質薄膜的種類或材料等的組合、或溶液的離子 -9 - 200523706 (7) 化程度等之各條件,施加電壓對流量之關係會有所不同 。藉此’以這些構成要素之組合,可獲得能進行期望的 流量之控制的泵浦。 圖2係顯示本發明的微少流量控制泵浦的一實施例 的結構之縱斷面圖。在第一管路丨內,經由支承體3保 持著多孔質薄膜2。第一管路1及支承體3係以具有電氣 絕緣性的材料所構成。作爲多孔質薄膜2之一例,爲厚 度1 1 μηι的鎳製者,在直徑8 mm的圓形區域內,規則性 地設有5 5 6 00個孔徑大致爲5μιη的孔。又,在多孔質薄 膜2的兩側設置陽極4及陰極5。如圖1 Β所示,保持多 孔質薄膜2的支承體3及一對電極爲平板狀,其間夾持 密封材固定於第一管路1。 如後所述,多孔質的孔徑係1 μ m〜1 0 μ m的範圍爲佳 。又,各電極與多孔質薄膜2之間隔係1 m m〜1 c m左右 的範圍爲佳。這些一對電極係經由切換開關7連接於直 流電源6。直流電源6係用來將1 〇〇 V左右以下的直流電 懕供給至一對電極之電源,能夠使用電池。或,作爲直 流電源6,亦可爲由交流電源經由轉換器以獲得直流電源 之電源裝置。又,作成具備可變阻抗器等的電壓調整手 段者。切換開關7係具有切換對於一對電極的電壓之極 性、或作成OFF之切換功能。第一管路1的流入側管27 係連接於溶液槽(未圖示)。溶液槽與第一管路1之高 度,基本上相同,即落差爲零。如在後的實施例所述, 藉由因應用途,改變此落差,能夠獲得因應了用途之期 -10- 200523706 (8) 望的流量特性。 再者,設置於一對電極4、5的圓形開口部係並非一 定須要與支承體3的圓形開口部之大小相同。例如,亦 可作成:設置於一對電極4、5的開口部係半徑較支承體 3的開口部大,且作爲具有複數個細微口之開口部的結構 〇 接連於第一管路1的流出側管2 6之第二管道1 0係 分成流入側管道部8與流出側管道部9,藉由細管22結 合著。流入側管道部8之下部係充滿溶液(驅動液)2 0 。一方面,在此細管22與流入側管道部8的上部、流出 側管道部9的上部充滿著中間媒體2 ;[。且,在成爲泵浦 之流出側的流出側管道部9內,充滿水或血液等的噴出 液2 3,連接於流出側管2 8。 圖3係顯示溶液、多孔質薄膜等的組合之一例。在 圖3的例子’作爲溶液(驅動液)2 〇,使用媒體爲水、 電解質水溶液爲氯化鈉或氯化鉀。多孔質薄膜2爲鎳製 ,電極係陽極4爲銀、陰極5爲鋅之組合。又,若採用 銀與氯化銀(AgCl )之組合的話,則能夠構成可切換陽 極、陰極之可逆電極。在溶液,添加作爲氧化劑之過氧 化氫水或二鉻酸鉀。 圖3的組合係僅爲一例,當然亦可組合同樣特性之 其他要素。例如’亦可在電極,使用鋅板(陰極)、銀 板(陽極)之組合。 又,圖4係顯示關於溶液、多孔質薄膜等的組合之 -11 - 200523706 (9) 其他例。在圖4的例子,作爲溶液(驅動液)2 0,使用 將微粒子分散之膠體溶液。即,作爲溶液之膠體溶液係 以水或藉由離子交換機除去了離子之離子交換水爲媒體 ,在其混入聚乙烯粒子或矽粒子等的微粒子。膠體溶液 亦可爲在油中混入微粒子者。 又,多孔質薄膜2係使用鎳或非金屬之聚碳酸酯。 作爲多孔質薄膜之材料,亦可適用非金屬丙烯樹脂。電 極之陽極、陰極均爲不銹鋼板。作爲聚碳酸酯製之多孔 質薄膜2的具體構成例,例如厚度爲1 1 μπα,在直徑 1 0 mm的圓內設置3 2 0 0 0 0個孔徑大約爲5 μηι之孔。 再者,膠體溶液,亦可爲在水中使微粒子懸浮者, 亦可爲在油或有機溶媒中使微粒子懸浮者。 能作爲溶液(驅動液)2 0來加以使用者係不限於膠 體溶液。例如,亦可爲以離子交換水爲媒體,在其中使 微粒子分散之懸浮液。 如此,在本發明的泵浦所能使用之溶液(驅動液) 2 〇,在媒體使粒徑〇 . 〇 1 μ m〜〇 . 5 μ m的微粒子浮游之液體 即可。在此情況下,微粒子係爲在液體中具有帶電之性 質之物的話,則不論金屬、非金屬均可利用。例如,亦 可使用氧化鋁的粉末作爲微粒子。 其次,說明圖2的實施例之動作。在溶液槽,將作 爲驅動液2 0之電解質水溶液(參照圖3 )、或使微粒子 (參照圖4 )分散之膠體溶液,充滿於第一管路1內與第 一管道】〇的流入側管道部8內部。然後,在成爲泵浦的 -12 - 200523706 (10) 流出側之流出側管道部9內下部,充滿污水或血液等的 噴出液23。 藉由對於陽極4與陰極5施加直流電壓,鈉水溶液 係流向第二管道的流入側,其會按壓中間媒體(矽油、 變壓器油)2 1,將噴出液(水、污水等)23朝流出側管 2 8壓出。若停止對於陽極4與陰極5施加電壓,則溶液 的流動也停止。藉由如此操作,能夠產生溶液的微少流 晕 ° 再者,溶液也就是電解質水溶液(例如鈉水溶液) 2 〇係受到施壓電壓,而會有氫或氣泡產生,因而影響流 量。但,若添加過氧化氫或二鉻酸鉀等的氧化劑的話, 能夠防止氫或氣泡之產生。當在實施如此對策後,使用 電解質強之溶液時,則能夠以施加更低之電壓,使流量 產生。 又,藉由使用以離子交換機除去了離子的膠體溶液 之方法,亦可不會產生氫。 圖5係顯示使用如圖2所示的微少流量控制泵浦, 根據圖3所示的要件之組合,進行實驗而獲得之泵浦的 流量特性之一結果的圖。測試液爲〇 . 9 %食鹽水、施加電 壓爲5 V、所使用的多孔質薄膜2爲鎳箔、其孔徑爲 5.0 ] μ m者。電極係分別爲鋅板(陰極)、銀板(陽極) 。又’溶液槽的局度(水柱)爲〇mm。在此’作爲電極 ,在陰極使用鋅板,在陽極使用銀板。由此圖可得知, 在施加電壓後立刻產生流動。當實驗開始時,在電壓爲 -13- 200523706 (11) 零之狀態起,經過3 0 0秒之時間點施加5 V之電壓。施加 電壓後,流量增加,在經過了 3 5 0秒之時間點,形成大 約爲2.0 ( Illm3/S )之流量,之後,持續獲得大致一定的 流量。 本發明的流體移送裝置係與利用隔膜或活塞之泵浦 不同’原堙上無脈動爲其特徵。在圖5之資料,在流量 上能見若午的脈動,但與在之後所進行的其他試驗結果 相較 '檢討之結果,可得知,資料上之脈動主要係使用 於流量 '測定之電子天秤的不穩定及程式上的問題所引起 者。這是由於即使在附加電壓之前(流量爲零)之狀態 亦能見相间的變動之故。因此,可知,泵浦所引起之脈 動係較圖$的資料値更小。又,在獲得穩定的一定流量 之間的時間,在資料上經過了 5 〇秒,但會有測定用程式 上的問體所引起之遲慢,實際上,在進行電壓施加後, 於5〜1 0秒程度可獲得穩定之一定流量。 發明們係反復進行數次實驗,確認不會產生氫或 氣泡。當在陰極使用鋅時,則能夠防止氫產生。又,在 陽極使用銀板時,則能防止因氯所引起之膜的腐蝕。且 ,當在陰極使用A g C1之可逆電極時,則更具效果。又, 當添加過氧化氫水、二鉻酸鉀作爲氧化劑時,可進一步 提高效果。 又,爲了進行比較,圖6係顯示當將電壓增加至8V 時之泵浦的流量特性的圖表。在電壓5 V,流量大約爲 2.0 ( mm3/s ),而在電壓8 V,流量大約爲4.0 ( m m 3 / s ) ~ 14- 200523706 (12) ,也就是當電壓增加時,流量也變大。 圖7係根據圖4所示的要件之組合,使用在離子交 換水中置入單分散聚乙烯粒子的膠體溶液作爲水溶液之 情況的結果。測試液係〇 . 〇 1 %之單分散聚乙烯膠體溶液 、附加電壓爲5 V、所使用的多孔質薄膜2爲鎳箔、其孔 徑大約爲5 μηι者。電極係陰極、陽極均爲不銹鋼板。在 已進行離子交換之膠體溶液,因不會產生氫或氯,所以 電極能夠使用不銹鋼板。 當實驗開始時,在電壓爲零之狀態起,經過3 0 0秒 之時間點施加電壓。由此圖可得知,施加電壓後,立刻 產生流動,而獲得大約爲1 .〇 ( mm3/s )之大致一定的流 量。藉由改變濃度或電壓可調整流量。 使用膠體溶液之優點係因不會電氣分解,所以能夠 無數次使用相同溶液、且不會產生氣泡或氫。這係在反 復進行測驗中已得到確認。 圖8係根據圖4所示的要件之組合,多孔質薄膜使 用聚碳酸酯膜的情況之結果。測試液係0.0 1 %之單分散 聚乙储膠體溶液、附加電壓爲5 V、所使用的多孔質薄膜 2爲聚碳酸酯膜、其孔徑大約爲5 μηι者。電極係陰極、 陽極均爲不銹鋼板。當實驗開始時,在電壓爲零之狀態 起,經過3 0 0秒之時間點施加電壓。由此圖可得知,施 加電壓後’立刻產生流動,而獲得大約爲( mm3/s ) 之大致一定的流量。在反復進行實驗下,確認了此實驗 之再現性。聚碳酸酯的優點係膜的腐蝕少,而可長期使 - 15- 200523706 (13) 用,且低成本。 在此,說明關於本發明的微少流量控制泵浦。首先 ,說明關於施加電壓與泵浦流量之關係。 當將附加於泵浦之電壓設爲V、電流設爲I時,則聚 浦輸入爲V X I。又,將泵浦的噴出壓力設爲P、流羹設 爲Q時,則泵浦輸出爲以P X Q。依此,將功率設爲P _ ,則如下。According to the present invention, the following effects can be achieved: the minute flow generating device is provided with a porous film and a pair of electrodes arranged in a flow path of a solution, and a lower voltage, such as 丨 0v, is applied between the electrodes. The left and right DC voltage can generate a small flow of the pulsation-free solution. This flow rate is formed approximately in proportion to the applied voltage, which makes it easy to control the flow rate, has good handling properties, and is inexpensive. In addition, there is no clogging, and a stable flow rate can be ensured, that is, no hydrogen gas or bubbles are generated inside the solution, and the flow rate characteristics will not change even if the process is repeated. [Embodiment] Hereinafter, an embodiment of the present invention will be described. First, the basic structure of the minute flow generating device of the present invention will be described. _] A shows the principle of the minute flow generating device of the present invention. Winter 200523706 (6) Intent. Fig. 1B is a perspective view showing a part of the minute flow generating device of the present invention. In the middle of the pipe (flow path) 1 through which the solution 20 flows, a porous film 2 is mounted via a support 3 in a direction perpendicular to the axis direction of the pipe. Further, a pair of electrodes 4 and 5 are provided on the upstream side and the downstream side of the porous thin film 2 therebetween. The circular opening of the support 3 is the circular area where the porous film 2 faces the flow, and the circular opening provided on the pair of electrodes 4 and 5 has substantially the same radius, and each center is located in the pipeline. On the axis. The solution 20 is processed so as not to cause electrical decomposition. Therefore, an oxidant is added to the solution. A lead electrode can also be used at the cathode, or a combination of this solution and a lead electrode can also be used. As another method, the solution 20 may be a liquid in which fine particles having a particle diameter of 0.0 1 μΐΒ to 0.5 μm are floated in the medium. In this case, the microparticle system needs to be charged in the liquid. For example, a colloidal solution in which fine particles are separated in a solution can be used. A pair of electrodes arranged with the porous film 2 are arranged such that the inflow side of the solution is the anode 4 and the outflow side is the cathode 5, and a predetermined DC voltage of 00 V or less is applied from the DC power source 6 through the switch 7. In the example shown in the figure, when the anode 4 is on the left and the cathode 5 is on the right, the solution 20 flows in the direction of the arrow. In addition, when a voltage of 10V to 20V is applied between a pair of electrodes, the current flowing between the electrodes is a small current of about 30 0 / Α ~ 1 〇μμ, which consumes very little power. This is One of the features of the present invention. In addition, as will be described in detail later, the voltage is applied according to various conditions such as the type of the constituent elements, the type of the electrode, and the type of the porous film, the material, or the ion-9 of the solution (7). The relationship to traffic will be different. In this way, a combination of these components enables a pump capable of controlling a desired flow rate. Fig. 2 is a longitudinal sectional view showing the structure of an embodiment of a minute flow control pump according to the present invention. A porous film 2 is held in a first pipe 丨 via a support 3. The first pipe 1 and the support body 3 are made of an electrically insulating material. An example of the porous film 2 is a nickel made with a thickness of 11 μm. In a circular region with a diameter of 8 mm, 5 5 6 00 holes having a pore size of approximately 5 μm are regularly provided. An anode 4 and a cathode 5 are provided on both sides of the porous film 2. As shown in FIG. 1B, the support body 3 and the pair of electrodes holding the porous film 2 are in a flat plate shape, and the sealing material is fixed to the first pipe 1 therebetween. As described later, the range of the porous pore diameter is preferably 1 μm to 10 μm. The distance between each electrode and the porous film 2 is preferably in the range of about 1 m to 1 cm. These pair of electrodes are connected to a DC power source 6 via a change-over switch 7. The DC power supply 6 is a power supply for supplying DC power of about 1000 V or less to a pair of electrodes, and a battery can be used. Alternatively, the DC power source 6 may be a power source device that obtains a DC power source from an AC power source through a converter. Moreover, a person who has prepared a voltage adjusting means such as a variable resistor. The change-over switch 7 has a switching function for changing the polarity of the voltage to a pair of electrodes or turning it OFF. The inflow-side pipe 27 of the first pipe 1 is connected to a solution tank (not shown). The height of the solution tank and the first pipeline 1 is basically the same, that is, the drop is zero. As described in the following examples, by changing the difference in accordance with the use, it is possible to obtain a desired flow rate characteristic according to the period of use -10- 200523706 (8). The circular openings provided in the pair of electrodes 4 and 5 do not necessarily have to be the same size as the circular openings of the support 3. For example, it is also possible to provide a structure in which the openings provided in the pair of electrodes 4 and 5 have a larger radius than the openings of the support 3 and are structured as openings having a plurality of fine openings. The second pipe 10 of the side pipe 26 is divided into an inflow-side pipe portion 8 and an outflow-side pipe portion 9 and is connected by a thin pipe 22. The lower portion of the inflow-side pipe portion 8 is filled with a solution (driving liquid) 2 0. On the one hand, here the thin tube 22 and the upper part of the inflow-side pipe part 8 and the upper part of the outflow-side pipe part 9 are filled with the intermediate medium 2; [. Further, the outflow-side pipe portion 9 serving as the outflow side of the pump is filled with a discharge liquid 2 3 such as water or blood, and is connected to the outflow-side tube 28. FIG. 3 shows an example of a combination of a solution and a porous film. In the example of FIG. 3, as the solution (driving solution) 20, the medium used is water, and the electrolyte solution is sodium chloride or potassium chloride. The porous thin film 2 is a combination of nickel, the electrode system anode 4 is silver, and the cathode 5 is zinc. In addition, if a combination of silver and silver chloride (AgCl) is used, a reversible electrode capable of switching anodes and cathodes can be formed. To the solution, hydrogen peroxide or potassium dichromate was added as an oxidant. The combination shown in FIG. 3 is only an example, and it is a matter of course that other elements having the same characteristics may be combined. For example, a combination of a zinc plate (cathode) and a silver plate (anode) may be used for the electrode. Fig. 4 shows another example of a combination of a solution, a porous film, and the like. In the example of FIG. 4, as the solution (driving liquid) 20, a colloidal solution in which fine particles are dispersed is used. That is, the colloidal solution as a solution is made of water or ion-exchanged water from which ions have been removed by an ion exchanger as a medium, and fine particles such as polyethylene particles or silicon particles are mixed therein. The colloidal solution may be a mixture of fine particles in oil. The porous film 2 is made of nickel or non-metallic polycarbonate. As the material of the porous film, a non-metallic acrylic resin can also be applied. The anode and cathode of the electrodes are stainless steel plates. As a specific configuration example of the porous film 2 made of polycarbonate, for example, a thickness of 11 μπα is provided, and 3 2 0 0 0 holes having a diameter of about 5 μm are provided in a circle with a diameter of 10 mm. The colloidal solution may be a suspension of fine particles in water, or a suspension of fine particles in oil or an organic solvent. The user that can be applied as a solution (driving fluid) 20 is not limited to a colloidal solution. For example, a suspension in which ion-exchanged water is used as a medium in which fine particles are dispersed. In this way, the solution (driving solution) 20 that can be used for the pump of the present invention can be a liquid in which fine particles having a particle size of 0.01 μm to 0.5 μm float in the medium. In this case, if the fine particles are charged in a liquid, they can be used regardless of metal or non-metal. For example, a powder of alumina may be used as the fine particles. Next, the operation of the embodiment of FIG. 2 will be described. In the solution tank, the inflow side pipe of the first pipe 1 and the first pipe is filled with an electrolyte aqueous solution (see FIG. 3) or a colloidal solution in which fine particles (see FIG. 4) are dispersed as the driving liquid. Department 8 inside. Then, in the lower part of the outflow-side pipe portion 9 which becomes the pump -12-200523706 (10) outflow side, the discharge liquid 23 such as sewage or blood is filled. By applying a DC voltage to the anode 4 and the cathode 5, an aqueous sodium solution flows to the inflow side of the second pipe, which presses the intermediate medium (silicone oil, transformer oil) 21, and directs the ejection liquid (water, sewage, etc.) 23 toward the outflow side. Tube 2 8 is pressed out. When the application of voltage to the anode 4 and the cathode 5 is stopped, the flow of the solution is also stopped. By doing so, a small flow of the solution can be generated. In addition, the solution, which is an aqueous electrolyte solution (such as an aqueous solution of sodium), is subjected to a voltage under pressure, and hydrogen or air bubbles are generated, thereby affecting the flow. However, if an oxidizing agent such as hydrogen peroxide or potassium dichromate is added, generation of hydrogen or bubbles can be prevented. When such a countermeasure is implemented, when a solution with a strong electrolyte is used, a lower voltage can be applied to generate a flow rate. In addition, by using a colloidal solution in which ions are removed by an ion exchanger, hydrogen is not generated. Fig. 5 is a graph showing one of the results of the flow characteristics of the pump obtained by performing an experiment based on the combination of the requirements shown in Fig. 3 using the minute flow control pump shown in Fig. 2. The test solution was 0.9% saline, the applied voltage was 5 V, and the porous film 2 used was a nickel foil with a pore diameter of 5.0 μm. The electrode systems are zinc plate (cathode) and silver plate (anode). The locality (water column) of the solution tank is 0 mm. Here, as the electrode, a zinc plate is used for the cathode and a silver plate is used for the anode. It can be seen from this figure that a flow occurs immediately after the voltage is applied. When the experiment started, a voltage of 5 V was applied at a time point of 300 seconds after the voltage was -13- 200523706 (11) zero. After the voltage was applied, the flow rate increased, and a flow rate of approximately 2.0 (Illm3 / S) was formed after a lapse of 350 seconds. After that, a substantially constant flow rate was continuously obtained. The fluid transfer device of the present invention is different from a pump using a diaphragm or a piston. In the data in Figure 5, the pulsation of Ruowu can be seen in the flow, but compared with the results of other tests performed later, it can be known that the pulsation in the data is mainly used in the electronic balance that measures the flow. Caused by instability and programming problems. This is because the interphase variation can be seen even in the state before the voltage is applied (the flow rate is zero). Therefore, it can be seen that the pulsation caused by the pump is smaller than the data shown in Figure $. In addition, the time between obtaining a constant constant flow rate has passed 50 seconds on the data, but there is a delay caused by the question on the measurement program. Actually, the voltage is A certain amount of flow can be obtained in about 10 seconds. The inventors repeated experiments several times to confirm that no hydrogen or bubbles were generated. When zinc is used in the cathode, hydrogen generation can be prevented. When a silver plate is used as the anode, corrosion of the film due to chlorine can be prevented. And, when the reversible electrode of Ag C1 is used in the cathode, it is more effective. When hydrogen peroxide water and potassium dichromate are added as oxidants, the effect can be further enhanced. For comparison, FIG. 6 is a graph showing the flow characteristics of the pump when the voltage is increased to 8V. At a voltage of 5 V, the flow is approximately 2.0 (mm3 / s), and at a voltage of 8 V, the flow is approximately 4.0 (mm3 / s) ~ 14- 200523706 (12), that is, when the voltage is increased, the flow becomes larger . Fig. 7 is a result of a case where a colloidal solution in which monodisperse polyethylene particles are placed in ion-exchanged water is used as an aqueous solution based on the combination of the requirements shown in Fig. 4. The test solution was a 0.01% monodisperse polyethylene colloid solution, the applied voltage was 5 V, and the porous film 2 used was a nickel foil with a pore diameter of about 5 μm. The electrode system cathode and anode are stainless steel plates. In the colloidal solution that has undergone ion exchange, since no hydrogen or chlorine is generated, stainless steel plates can be used as electrodes. When the experiment started, the voltage was applied at a time point of 300 seconds after the voltage was zero. It can be seen from the figure that immediately after the voltage is applied, a flow occurs, and a substantially constant flow rate of about 1.0 (mm3 / s) is obtained. The flow rate can be adjusted by changing the concentration or voltage. The advantage of using a colloidal solution is that it does not decompose electrically, so the same solution can be used numerous times without generating bubbles or hydrogen. This has been confirmed in repeated tests. Fig. 8 is a result of a case where a polycarbonate film is used for the porous film based on the combination of the requirements shown in Fig. 4. The test liquid was a monodisperse polyethylene colloid solution of 0.0 1%, the applied voltage was 5 V, and the porous film 2 was a polycarbonate film with a pore diameter of about 5 μm. The electrode system cathode and anode are stainless steel plates. When the experiment started, the voltage was applied at a time point of 300 seconds after the voltage was zero. It can be seen from this figure that immediately after the voltage is applied, a flow occurs, and a substantially constant flow rate of approximately (mm3 / s) is obtained. Repeated experiments confirmed the reproducibility of this experiment. Polycarbonate has the advantages of less corrosion of the film and long-term use-15- 200523706 (13) and low cost. Here, the minute flow control pump according to the present invention will be described. First, the relationship between the applied voltage and the pump flow rate will be described. When the voltage applied to the pump is set to V and the current is set to I, the pump input is V X I. When the pump discharge pressure is set to P and the flow rate is set to Q, the pump output is set to P X Q. According to this, the power is set to P_, as follows.

η =P Q/ ( VI) ...... ( 1 )η = P Q / (VI) ... (1)

圖9係將使用本發明的泵浦所獲得的泵浦輸出P q $ 於壓力 P加以顯示者。由此圖可得知,即使改變壓力, 泵浦輸出也大致爲一定。此時,負荷之電壓爲 5 V,根據 實驗,即使改變壓力P,電流I也呈3 X 1 (Γ5安培,大致 一定。即,可得知,當泵浦輸入 VI=1 ·5 X 1 0·4瓦特時, 泵浦輸出P Q大約爲1 8瓦特之一定値。因此,雖Ρ變 化,Q對應其也變化’但若輸入一定的話’會有P Q = π V I = —定關係’功率π係由式(1 )形成7? = 0.6 7 X 1 0 ·5。 一方面,將開口於厚度L的膜之半徑R的孔與長度L半 徑R的細管近似時’則流量Q之流體通過此孔之際的壓 力損失P爲如下式所求取(流動爲層流)。 P (2)FIG. 9 shows the pump output P q $ obtained by using the pump of the present invention as the pressure P. It can be seen from this figure that even if the pressure is changed, the pump output is approximately constant. At this time, the voltage of the load is 5 V. According to the experiment, even if the pressure P is changed, the current I is 3 X 1 (Γ5 amperes, which is approximately constant. That is, it can be seen that when the pump input VI = 1 · 5 X 1 0 · At 4 watts, the pump output PQ is about 18 watts. Therefore, although P changes, Q also changes accordingly. But if a certain input is entered, there will be PQ = π VI =-fixed relationship. Power π system 7? = 0.6 7 X 1 0 · 5 is formed by the formula (1). On the one hand, when a hole with a radius R of a film having a thickness L and a thin tube with a length L and a radius R are approximated, the fluid of the flow rate Q passes through the hole The pressure loss P at this time is obtained by the following formula (flow is laminar): P (2)

8/7 L -16 - 200523706 (14) 在此,//爲流體黏度。 圖1 〇係顯示式(2 )與實驗値之比較。該圖中所示 之泊肅葉流動的直線係顯示式(2 ),黑點係顯示實驗値 。由該圖可得知,兩者一致,開口於膜之孔與細管可一 4。由式(2 ) ’將根據裝置所決定之定數設爲C時,則 如下式。 (3 )8/7 L -16-200523706 (14) Here, // is fluid viscosity. Fig. 10 shows the comparison between formula (2) and experiment 値. The linear system of Poiseuille flow shown in the figure shows the formula (2), and the black dots show the experiment 値. It can be seen from the figure that the two are consistent, and the hole and the thin tube opening in the membrane can be aligned. When formula (2) 'is used to set the fixed number determined by the device to C, the formula is as follows. (3)

Q-CP 7?與C之値係根據實際的泵浦與流體片的組合而有 所不同,但預先將其在遞送時實驗性地決定的話,則期 望的流量Q係根據由式(1 ) ( 3 )所求取的式(4 ) ’藉 由賦予電力VI (實際上,因電流I爲一定,所以實質上 :爲電壓V )來求取。 (4) 在當々與C於遞送時設定成預定値,R也作爲一定 之情況時,由V = RI之關係,重寫式(4 )時則求得下式 (其中,k爲定數) -17 - 200523706 (15) 由式(5 )可得知,預先設定7?或C之條件的話,則 流量Q係與施加電壓V成比例。 圖1 1係顯示使用本發明的泵浦,測定對於施加電壓 之泵浦噴出量的結果的一例者。由此圖亦可得知,本發 明的泵浦之流量Q係除了流量Q少之區域以外,其餘與 施加電壓V呈比例。 一般而言,在微少流量泵浦,以流量計不易一邊直 接測量流量Q —邊使用。因此,爲了以微少流量泵浦確 保正確之設定流量,而期望:事先以實驗取得如圖1 1所 示之賦予施加電壓V與流量Q之關係的特性線圖,根據 此特性線圖調節電壓,以獲得預定的流量。 其次,說明關於以本發明的泵浦,獲得與施加電壓 v成比例之流量Q之點。 在本發明的泵浦,將溶液槽之負也就是落差亦可作 成零。將落差設爲零,而由+極朝-極產生流動之現象’ 主要係因電氣滲透流或電氣泳動所引起者。 因此,當調查僅將落差設爲零時的電壓之影響’則 可得知,在安裝了多孔質薄膜的狀態下即會產生流量。 這是由於在未安裝膜之狀態下不會產生流量,故爲微小 區域之流動特有的現象。在此,考察關於在設於多孔質 薄膜的細微孔前後之電極,以附加電壓來產生流量之原 理。 電氣滲透流係指在微細管等的流通內可作成電偶層 -18- 200523706 (16) (e 1 e c t r i c d o u b 1 e ] a y e r ),該偶層係藉由庫倫力朝負極 移動,於一方向產生流動之現象。 圖1 2係在本發明的泵浦,於使用電解質水溶液(氯 化鈉、氯化鉀)的情況之電氣滲透流的示意圖。如圖12 所示,細微管的流通路之壁面帶有負電,藉此’在壁面 附近,正離子聚集而形成電偶層。該電偶層係藉由庫倫 力朝負極移動。周圍的正離子係依次朝壁面移動’經常 形成電偶層。又,在電偶層的周圍,受到電偶層的正離 子所拉引,負離子亦產生移動。此時,由於靜電力等的 力也作動,故在負極全體產生流動。 這是由於根據本發明之使用圖3所示的電解質水溶 液的情況之泵浦效果、特別是噴出、吸入一定流量之效 果之故。 其次,在本發明的泵浦,藉由如圖4所示的膠體溶 液產生泵浦效果的理由係如下所述。 一般而言,浸漬於液體的物體,幾乎的情況係帶有 負電,溶液中的正離子受其所拉引(吸著)。膠體粒子 也帶負電,但在其周圍拉引吸著液體中的負離子’粒子 全體形成與帶有正離子的粒子同類。因此,爲了簡單化 ,而將吸著有正離子的膠體粒子如圖1 3般描繪。 膠體溶液的情況也大致與圖1 2相同。但,在膠體溶 液的情況,正離子緊密附著於負離子周圍,其全體看似 形成正粒子,該正粒子,在電氣滲透流或電氣泳動、吸 著等特別是微小的區域特有現象,產生流動。即,在膠 -19- 200523706 (17) 體溶液,不會有負離子,而在如圖1 4般狀態下產生流動 〇 其次,圖1 5係顯示在本發明的泵浦,使用0 . 1 μη:直 徑的膠體粒子,改變多孔質薄膜2的細微孔之(孔)徑 ,而其他條件相同之情況的流量特性。施加電壓爲5 V。 實驗的細微孔的徑係有2 μ m、5 μ m、1 2 μ m、及4 0 μ m的4 種類。確定了在徑爲2μηι與5μπι,可獲得大致相同之泵 浦效果。但,在徑爲12μηι,流量若干降低,而徑爲 4 0 μηι則不會產生泵浦效果。與此相關聯,當孔徑變得極 端大時則形成無膜(孔)之情況,在此情況下,發明者 們實驗性地確定了不會產生泵浦效果。相反地,在孔徑 變得極端小,也不會產生泵浦效果。由此可得知,細微 孔的徑係對於膠體粒子的(粒)徑須要適度的大小,但 過大或過小均不好。 發明者們係根據實驗確認了下述點。其一例,如圖 1 6所示,當膠體粒子的直徑R = 0 · 0 9 μ m,多孔質薄膜2的 局度Η = ] 3 m ni,孔數量=5 5 6 0 0個時,期望膜厚D = 1 0 μ m, 多孔質薄膜2的細微孔的徑E = 5 μ m。 又,反復進行實驗的結果,可得知,膜厚D係具有 與流量呈反比例之關係、及( 1 0〜2 0 0 ) R的範圍爲有 效,膜厚D係D= ( 1/5〜2 ) E的範圍爲有效。在實用上 ’期望多孔質薄膜的厚度係作爲5 μιΐι〜2 0 0 μηι。 又,一對電極與多孔質薄膜2之間隙也大大地影響 特性。當間隙過窄時,則一對電極間的電氣阻抗變小, - 20 - 200523706 (18) 造成過大的電流流動。相反地,當間隙過大時,則由於 對於多孔質薄膜2的前後之溶液,無法生成充分強度的 電場’故無法確保目標之流量。由此,期望一對電極與 多孔質薄膜2之間隙係在1 mm〜i cm的範圍。 再者,這些膜厚D、細微孔的徑、電極間間隔等的 數値範圍係即使在將微少粉末混合於懸浮液的溶液、或 電解質水溶液的情況,也具有同樣的效果。 圖1 7 A至圖丨7 C係簡單地顯示膠體粒子通過開口於 多孔質薄膜2的細微孔(以下僅稱爲孔)之情況。各圖 中的水平之直線部分係顯示開口於多孔質薄膜中的孔之 剖面,以-表示在與液體的徑界面帶負電。在此境界面, 吸著有吸附如圖1 3所示的正離子之膠體離子。在如此狀 態下,於膜的左右放置負、正電極。如圖】7 a所示,於 與膠體粒子的相對關係上,孔徑過小之情況時,膠體粒 子係欲朝負電極,但無法通過孔,而不會產生栗浦效果 〇 如圖1 7 B所示,在孔徑爲適當的情況時,膠體粒子 係通過孔’伴隨著周圍的液體朝負電極側移動。此日寺, 已經吸附於膜、孔與液體的境界面之膠體粒子係發揮阻 止已經通過孔的膠體粒子的逆流之作用(阻滯作用)。 如圖1 7 C所示,在孔徑過大的情況時,孔的中心附 近之膠體粒子係朝負電極方向移動,但由於孔大,故根 據位於境界面的膠體粒子之阻滯作用變得無效,在孔的 中心附近與境界面之間,產生膠體粒子的逆流,其結果 -21 - 200523706 (19) ,不會產生泵浦效果。 根據以上的泵浦效果產生的原因,而使用直徑大的 膠體粒子的話,則至大的孔徑之膜爲止會產生泵浦效果 ,此時所產生的流量也大。又,藉由選擇吸著程度強的 粒子與膜之組合,能夠改善泵浦效果。 其次,針對置入有粒子的膠體溶液,改變各種條件 ,確認具有通用性。以下顯示其結果。 圖]8係採用使用聚乙烯粒子的膠體溶液作爲驅動液 ,顯示改變電極的組合之情況時的流量特性。針對不銹 鋼(陽極)-不銹鋼(陰極)的情況、銀(陽極)-不銹鋼 (陰極)、銀(陽極)-鋅(陰極)的情況時進行實驗, 可得知流量特性幾乎相同。 圖1 9係採用使用聚乙烯粒子的膠體溶液作爲驅動液 ,將聚乙烯粒子的塡充率在 0 . 1 %〜0.0 0 0 1 %的範圍內加 以改變的情況之結果。在 0 · 0 0 0 1 %,若干流量減少,但 在其以上之塡充率,可獲得大致相同之流量。 圖2 0係將粒子變成矽粒子,進行與圖1 9相同實驗 的情況之結果。與圖1 9同樣地,在0.0 〇 〇 1 %,若干流量 減少,但在其以上之塡充率,可獲得大致相同之流量。 圖2 1係泵浦的第二管道1 〇的其他實施例之構成圖 ,在1支的管(玻璃管等)之中間部置入中間媒體2 1 , 將噴出液2 3 (在圖2 3 )由左朝右壓出使其流動者。在此 細的一支管2 6,不需考量根據落差之影響。如此,若將 根據電壓施加所引起的流動作爲動力源,則能夠達到各 -22- 200523706 (20) 種型式的泵浦。 圖2 2、圖2 3係本發明的泵浦之其他實施例的構成圖 。在此例,在圖2所示的微少流量產生裝置,切換施加 直流電壓之陽極、陰極,作成可使流體往復移動。在此 情況時’錯由以膠體溶液作爲使用於驅動部分之溶液, 能夠使流體往復動作。在圖2 2,由箭號方向也就是陽極 朝陰極側產生膠體的流動,將中間媒體2 1朝右側推壓, 將噴出液2 3由管2 8噴出。此時,藉由閥3 4,使噴出液 23不會朝供給槽33方向流動。一方面,在圖23,與其 完全相反之方向產生流動,拉引中間媒體2 1,將供給槽 3 3的噴出液2 3供給至連結管3丨內。此時,藉由閥3 5, 使噴出側的噴出液2 3不會由管2 8吸入。藉此,能夠進 行吸入、噴出,可長時間地連續使用。 其次’說明關於圖1 A、1 B或圖2所示的本發明之微 少流量泵浦的應用例。 首先’圖2 4係應用本發明的泵浦系統的一實施例之 平面圖,圖25係其A-A斷面圖。 泵浦系統2 0 0係台座2 0 1上搭載泵浦1 〇 〇。此泵浦 1 0 0係呈平板狀之結構。這是由於當在桌上的平面搭載平 面狀的台座2 0 1之情況時,泵浦]〇 〇呈平面狀結構的話 則容易進行組裝之故。泵浦! 〇 〇係由上框i 〇丨與下框1 〇 2 所構成,在上框1 0 1的上部搭載有外殻1 03。在外殼]03 內,內裝有圖1 A、】B或圖2所示的微少流量產生裝置 】0 6 °在此’知I:成上重要點’係預先將微少流量產生裝置 -23- 200523706 (21) 1 0 6內的多孔質薄膜2之平面與上框1 ο 1的平面配設於相 同相向。如此則容易製作裝置,能夠減少溶液的流通路 之彎折部產生。又,在上框1 〇 1的內面,設有通路1 1 〇, 以與連絡口 I 〇 9、連絡通路1 1 1相連。當在微少流量產生 裝置1 0 6的一對電極,施加直流電壓時,溶液係通過輸 入管1 04、擴大路徑1 0 7,經由微少流量產生裝置1 0 6通 過擴大路徑1 〇 8、連絡口 1 0 9、通路1 1 0、連絡通路Π 1 ,由出口管1 0 5排出至目的場所。通路1 1 〇係設於上框 1 0 1上,但亦可設置於下框1 02的上面。將上框1 0 1與下 框1 0 2作成切離之結構係由於爲了容易進行通路1 1 〇的 加工之故。當然,亦可將上框101與下框102作成一體 者。 如此構成之泵浦1 00係搭載於平板狀台座20】,而在 該台座2 0 1配置有電池1 1 7、電壓調整器(可變阻抗) ]1 6、導通關閉(ON · OFF )開關1 1 5及電池收納部蓋子 I 1 8。電壓調整器1 1 6係連接於控制器(未圖示)。在控 制器內,如前所述,根據預先設定的條件資料與式(4 ) 、式(5 )所示的關係,運算對於所需流量之施加電壓値 ’形成此電壓値地調整電壓調整器而確保預定流量地進 行控制。再者,利用者亦可參照圖1 1的特性,直接操作 電壓調整器1 1 6。 此微少流量產生裝置1 0 6係因具有藉由電池等的低 電壓電源,能輸送溶液之特徵,所以能夠以乾電池驅動 ’不需要另外設置大型的電源。因此,能夠將電池]]7、 -24- 200523706 (22) 阻抗Π 6、開關1 1 5所有內裝於台座2 0 ],而作成容易搬 運之結構。由電池1 1 7所產生的電壓係能夠使用導線Π 2 、1 1 3、1 1 4施加於微少流量產生裝置〗〇 6的電極(陽極 、陰極),此電壓係可藉由介裝於導線 1 1 4之阻抗 Π 6 加以調整,又能藉由開關1 1 5由電源切離。 圖2 6係本發明的泵浦系統之其他實施例的構成圖。 在此例,顯示作爲驅動液的溶液2 0與噴出液2 3之接觸 結合的一方法者。在泵浦 1 0 0的出口管 1 0 5之出口部設 有槽202,在其內部設有區隔壁220。以區隔壁220爲境 界,出口管1 05的出口端連接於左側的空間,在區隔壁 2 2 0的右側空間,經由管2 1 3、閥2 1 1、管2 1 2,連接著 具備伸縮管2 1 4之槽2 0 3。噴出液2 3進入至此槽2 0 3內 ,藉由按壓伸縮管2 1 4,該噴出液2 3係經由管2 ] 3、閥 211、管2]2,供給至槽202內,然後藉由關閉閥211, 能夠停止該供給動作。又,在該槽202的左側連接有管 2 0 7,經由閥2 0 8、管2 0 6 ,槽2 0 2內的噴出液2 3係噴出 至另外設置的槽2 0 5內。 當將電壓施加於設在泵浦100的外殻103內之微少 流量產生裝置1 06的一對電極時,則槽2 04內的驅動液 2 0係經由管2 1 7被吸起,通過上框1 0 1內的通路〗1 0, 進一步通過管105,進入至槽202內的左側之小室內。此 溶液(驅動液)係通過區隔壁2 2 0的小孔進入至右側的 小室內,將位在其上部之噴出液2 3推起。藉此,噴出液 2 3係通過管2 0 6噴出至槽2 0 5內。噴出液之比重較溶液 -25- 200523706 (23) 的比重小之情況時,如圖所示,使這些接觸於槽202 右側之小室即可。在溶液20的比重較噴出液23的比 小之情況時,在槽202的左側之小室使這些接觸即可 在溶液2 0與噴出液2 3相互混合之溶液的情況時,將 間媒體(例如矽油)2 1介裝在這些之界面即可。 圖2 7係本發明的泵浦1 〇 〇之其他實施例的構成圖 其係在圖2 5的實施例之通路1 1 〇置入中間媒體2 1,以 爲境界,在微少流量產生裝置1 06側置入驅動液20, 在其相反側置入噴出液2 3者,而作爲置入此噴出液 之方法,在上框1 0 1的上方部設置具有閥2 〇之粗狀的 Π9,在將噴出液23導入至此管119內後,在進行實 時關閉閥1 2 0。 圖2 8係本發明的泵浦〗〇 〇之其他實施例的構成圖 這是在相連於外殼103的管1〇4之上方部設置槽2〇4, 此槽2 0 4內塡充驅動液2 0,藉由重力將驅動液經由 1 〇4、微少流量產生裝置丨〇 6導入至通路丨〗〇。然後, 由中間媒體2 1由出口管1 〇5將噴出液23排出至目的 所。此流量係根據設在微少流量產生裝置丨〇 6的上方 之槽2 04的局度而有所改變,但作爲調節此時的流量 方法,調節施加於微少流量產生裝置1 的電極之電 的施加方式。當進一步增加流量時,施加正方向的電 ,增大其量即可。一方面,在欲減少流量時,施加反 向的但壓,使其作用於停止流量之方向即可。若增大 亀壓之大小,亦可安全地停止流動。 的 重 〇 中 其 而 23 管 驗 在 管 經 場 部 之 壓 壓 方 逆 -26 - (24) (24)200523706 圖2 9係本發明的泵浦〗〇 〇之其他實施例的構成圖。 這是在通路1 1 0的途中設置堵塞部1 0 1 -a,以此爲境界, 將管1 2 2與1 2 3設置於下框1 02,在這些之間設置長條管 1 2 1,構成關閉式環之結構。在成爲此關閉式環之長條管 1 2 1的一部分分歧連接有管1 2 4,經由閥1 2 5將噴出液2 3 塡充至內部。又,在管1 22的途中預先置入中間媒體2 1 。如此,即使經過長時間,也不會有流動停止之虞,而 可獲得期望之流量。在此實施例,即使設置圖2 6之具有 區隔壁220的槽2 02以代替長條管121,也可獲得同樣的 效果。 圖3 0係本發明的泵浦1 0 0之其他實施例的構成圖。 與圖29同樣地,在通路110的途中設置堵塞部l〇l-a, 以此爲境界,將管122與123設置於下框102而連結成 U字狀,在其內部塡充中間媒體2】者。在管〗2 2的一部 分設置閥1 2 6,經由該閥置入溶液(驅動液)2 0,~方面 ,在管1 2 3的一部分設置閥1 2 7,經由該閥置入噴出液 2 3。在此圖中,其結構爲閥]2 2、1 2 3的上端連接於上框 1 0 1的上部,而在這些的上端部連接有浮1 2 6、〗2 7 ,但 亦可在連接於下框1 02的U字狀之閥]22、] 23的一部分 設置分歧管,而將閥126、127加以連接者。 如上所述,本發明的泵浦或泵浦系統係可適用於使 用在生物物質或藥品、食品等的分析。 圖3 1係顯示將本發明的泵浦系統裝設於血液等的分 析系統之例子。圖3〗所示的分析系統係除了本發明之栗 -27- 200523706 (25) 浦系統外,尙具備:具有電腦之分析裝置3 〇 〇與其顯示 裝置3 0 2及顯微鏡3〇4。組合設於微少流量泵浦1〇〇的噴 出側之微管道與能見化功能部3 1 0,將包含有作爲分析對 象的血液、DNA或細胞等的溶液流入至微管道內,藉由 皆光等的操作將對象物加以能見化。然後藉由顯微鏡3 〇 4 擴大觀察。在此情況下’當泵浦流量產生變動或脈動時 ’則已被擴大的對象物之圖像振動,無法進行精確的觀 察。當使用本發明的泵浦時,則由於在泵浦流量不會產 生變動或脈動,故已被擴大的對象物之圖像不會振動, 而可進行高精確度之觀察。又,在以往的泵浦無法簡單 地改變流動的正反’但在本發明之泵浦,藉由改變電極 之正負,能夠簡單地使流動反轉。 本發明除了如上所述般之不會有變動或脈動產生、 或能夠簡單地使流動反轉外,本發明的泵浦進一步具有 以下的特徵。 (1) 藉由使電壓改變’能夠容易且自由地進行流量 控制。 (2) 由於能以低電壓作動,故安全性高。 (3) 廉價。 (4) 小型。 (5) 不會有堵塞,可確保穩定之流量。 藉此,本發明的泵浦係亦可進一步擴展應用至生物 關係之實驗、硏究的範圍。且能夠裝設於各種醫療機器 加以使用。 -28 - 200523706 (26) [圖式簡單說明】 ‘ 圖1 A係顯示本發明的微少流量產生裝置之原理的示 意圖;圖1 B係顯示本發明的微少流量產生裝置之局部的 斜視圖。 圖2係本發明的微少流量產生裝置之一實施例的構 成圖。 圖3係顯示在本發明的一實施例所使用的溶液、多 孔質薄膜等的組合之例的圖。^ 圖4係顯示在本發明的一實施例所使用的溶液、多 孔質薄膜等的其他組合之例的圖。 圖5係顯示本發明的流量特性的一例之圖。 圖6係顯示本發明的流量特性的其他例之圖。 圖7係顯示本發明的流量特性的其他例之圖。 圖8係顯示本發明的流量特性的其他例之圖。 圖9係將使用本發明的泵浦所獲得的泵浦輸出p q對 於壓力P加以顯示之圖。 圖1 〇係顯示式(2 )與實驗値的比較之圖。 圖1 1係顯示使用本發明的泵浦,對於施壓電壓測定 噴出星之結果的一例之圖。 圖1 2係在本發明的泵浦,使用電解質水溶液(氯化 鈉、氯化鉀)的情況之電氣滲透流的示意圖。 圖].3係顯示吸著有正離子的膠體粒子之圖。 圖]4係顯示在本發明的泵浦,使用了膠體溶液的情 況之流動的狀態之圖。 -29- 200523706 (27) 圖]5係顯示在本發明的泵浦,使用〇 . 1 μ1Ώ直徑的膠 體粒子,改變多孔質薄膜的細微孔的孔徑,其他條件則 相同的情況之流量特性的圖。 圖1 6係說明膠體粒子的直徑R與細微孔的孔徑Ε及 膜厚D的關係之圖。 圖1 7 Α係膠體粒子通過開口於多孔質薄膜的細微孔 之狀況的說明圖;圖1 7B係膠體粒子通過開口於多孔質 薄膜的細微孔之狀況的說明圖;圖1 7 C係膠體粒子通過 開口於多孔質薄膜的細微孔之狀況的說明圖。 圖1 8係顯示本發明的泵浦之流量特性的其他例之圖 〇 圖1 9係顯示本發明的泵浦之流量特性的其他例之圖 〇 圖2 0係顯示本發明的泵浦之流量特性的其他例之圖 〇 圖2 1係顯示本發明的泵浦之變形例的圖。 圖2 2係顯示本發明的泵浦的其他實施例之構成圖。 圖2 3係顯示在圖2 2所示的泵浦之一動作的圖。 圖2 4係顯示本發明的泵浦系統之一實施例的平面圖 〇 圖25係顯示圖24的A-A斷面圖。 圖2 6係顯示本發明的泵浦系統之其他實施例的構成 圖2 7係顯示本發明的泵湳系統內的泵浦部之其他實 -30- 200523706 (28) 施例的構成圖。 圖28係顯示本發明的泵浦系統內的泵浦部之其他實 施例的構成圖。 圖2 9係顯示本發明的泵浦系統內的泵浦部之其他實 施例的構成圖。 圖3 0係顯示本發明的泵浦系統內的泵浦部之其他實 施例的構成圖。 圖3 I係顯示本發明的泵浦系統之應用例的圖。 【主要元件符號說明】 1…第一管路 2···多孔質薄膜 3…支承體 4…電極(陽極) 5··.電極(陰極) 6···直流電源 7…開關 8…第二管路之流入側管道部 9…第二管路之流出側管道部 ]〇…第二管道 20…溶液(驅動液) 21…中間媒體 22…細管 2 3…噴出液 200523706 (29) 26···第一管路之流出側管 2 7…第一管路之流入側管 ]00…泵浦 1 0 ]…上框 1 0 1 - a…堵塞部 1 0 2…下框 103…外殼 1 0 4…輸入管 1 05…出口管 1 06···微少流量產生裝置 1 07…擴大路徑 1 08…擴大路徑 1 09…連絡口 ]1 2…導線 1 1 5…開關 1 1 6···阻抗 1 1 7…電池 2 0 0···泵浦系統The relationship between Q-CP 7? And C varies depending on the actual combination of the pump and the fluid sheet. However, if it is determined experimentally at the time of delivery, the expected flow rate Q is determined by equation (1). (3) The obtained formula (4) 'is obtained by applying electric power VI (actually, because the current I is constant, it is essentially a voltage V). (4) When 々 and C are set to predetermined 値 at the time of delivery, and R is also a certain case, the relationship of V = RI is obtained. When rewriting equation (4), the following equation is obtained (where k is a fixed number) ) -17-200523706 (15) It can be known from the formula (5) that if 7 or C is set in advance, the flow rate Q is proportional to the applied voltage V. Fig. 11 shows an example of a result of measuring the pump discharge amount with respect to an applied voltage using the pump of the present invention. It can also be seen from this figure that the flow rate Q of the pump of the present invention is proportional to the applied voltage V except for the area where the flow rate Q is small. Generally speaking, it is not easy to directly measure the flow rate Q while using a small flow pump. Therefore, in order to ensure the correct set flow rate by pumping with a small flow rate, it is expected that the characteristic line diagram of the relationship between the applied voltage V and the flow rate Q shown in FIG. To get a predetermined flow. Next, the point of obtaining the flow rate Q proportional to the applied voltage v with the pump of the present invention will be described. In the pump of the present invention, the negative, that is, the drop, of the solution tank can be made zero. The phenomenon that the drop is set to zero and flow from + pole to-pole is caused mainly by electric percolation flow or electric swimming. Therefore, when investigating the effect of voltage only when the drop is set to zero, it can be seen that a flow rate is generated when a porous film is installed. This is because the flow rate does not occur when the membrane is not installed, and it is a phenomenon unique to the flow in a small area. Here, the principle of generating a flow rate by applying a voltage to the electrodes provided before and after the pores of the porous film will be examined. Electrical permeation flow refers to the formation of galvanic layer in the circulation of microtubes, etc.-18- 200523706 (16) (e 1 ectricdoub 1 e] ayer), which is caused by the coulomb force to move toward the negative electrode in one direction The phenomenon of flow. Fig. 12 is a schematic diagram of the electric percolation flow in the case of using the electrolyte solution (sodium chloride, potassium chloride) in the pump of the present invention. As shown in Fig. 12, the wall surface of the flow path of the microtube is negatively charged, whereby positive ions gather near the wall surface to form a galvanic layer. The galvanic layer is moved toward the negative electrode by Coulomb force. The surrounding positive ions are sequentially moved toward the wall surface ', often forming a galvanic layer. In addition, around the galvanic layer, positive ions of the galvanic layer are pulled, and negative ions also move. At this time, since a force such as an electrostatic force is also actuated, a flow occurs in the entire negative electrode. This is due to the pumping effect in the case of using the electrolytic aqueous solution shown in Fig. 3, particularly the effect of ejecting and inhaling a certain flow rate according to the present invention. Next, the reason why the pump of the present invention produces a pumping effect with a colloidal solution as shown in Fig. 4 is as follows. Generally speaking, an object immersed in a liquid is almost negatively charged, and positive ions in the solution are pulled (adsorbed) by it. Colloidal particles are also negatively charged, but the anion particles attracted to the liquid are attracted around the particles, and the particles are similar to particles with positive ions. Therefore, for simplicity, colloidal particles adsorbed with positive ions are depicted as shown in Figure 13. The situation of the colloidal solution is also substantially the same as that of FIG. 12. However, in the case of a colloidal solution, positive ions closely adhere to the surrounding negative ions, and all of them appear to form positive particles. The positive particles have a phenomenon that is particularly small in areas such as electrical permeation flow, electrophoresis, and adsorption, and flow. That is, in the gel-19-200523706 (17) body solution, there will be no negative ions, and flow will occur in the state shown in Figure 14. Second, Figure 15 shows the pump of the present invention, using 0.1 μηι : Diameter of colloidal particles. Flow rate characteristics in the case where the diameter (pore) of the fine pores of the porous film 2 is changed, and other conditions are the same. The applied voltage is 5 V. The diameters of the experimental micropores were 4 types of 2 μm, 5 μm, 12 μm, and 40 μm. It is determined that the pumping effect is about the same when the diameter is 2μm and 5μm. However, at a diameter of 12 μηι, the flow rate is slightly reduced, while a diameter of 40 μηι does not produce a pumping effect. In connection with this, when the pore diameter becomes extremely large, no film (hole) is formed. In this case, the inventors have experimentally determined that no pumping effect will occur. On the contrary, the pore diameter becomes extremely small and no pumping effect is produced. It can be seen that the diameter of the fine pores needs to have a moderate size for the (grain) diameter of the colloidal particles, but it is not good to be too large or too small. The inventors confirmed the following points based on experiments. As an example, as shown in Fig. 16, when the diameter of the colloidal particles R = 0 · 0 9 μ m, the locality of the porous film 2] =] 3 m ni, and the number of pores = 5 5 6 0 0, it is expected The film thickness was D = 10 μm, and the diameter of the fine pores of the porous film 2 was E = 5 μm. As a result of repeated experiments, it can be seen that the film thickness D system has an inversely proportional relationship with the flow rate, and the range of (1 0 to 2 0 0) R is effective, and the film thickness D system D = (1/5 to 2) The range of E is valid. Practically, it is desirable that the thickness of the porous film is 5 μm to 200 μm. The gap between the pair of electrodes and the porous film 2 also greatly affects the characteristics. When the gap is too narrow, the electrical impedance between a pair of electrodes becomes small, and-20-200523706 (18) causes excessive current to flow. Conversely, when the gap is too large, a sufficient electric field cannot be generated for the solution before and after the porous thin film 2, and the target flow rate cannot be secured. Therefore, the gap between the pair of electrodes and the porous film 2 is desirably in a range of 1 mm to 1 cm. In addition, the range of these film thicknesses D, the diameter of the pores, and the distance between the electrodes is similar to that obtained when a small amount of powder is mixed with a suspension solution or an electrolyte aqueous solution. Figs. 17A to 7C show how colloidal particles pass through the fine pores (hereinafter simply referred to as pores) opened in the porous film 2. Figs. The horizontal straight line in each figure shows the cross section of the pores opened in the porous film. The negative line is negatively charged at the interface with the liquid. At this interface, colloidal ions that adsorb positive ions as shown in Figure 13 are adsorbed. In this state, the negative and positive electrodes are placed on the left and right of the film. As shown in Figure 7a, in the relative relationship with colloidal particles, when the pore size is too small, the colloidal particles are intended to face the negative electrode, but cannot pass through the pores without generating the Kuriura effect. It is shown that when the pore size is appropriate, the colloidal particles pass through the pores and move toward the negative electrode side with the surrounding liquid. At this temple, the colloidal particles that have been adsorbed at the interface between the membrane, the pores and the liquid play a role in blocking the countercurrent of the colloidal particles that have passed through the pores (blocking effect). As shown in Figure 17C, when the pore size is too large, the colloidal particles near the center of the pores move toward the negative electrode. However, because the pores are large, the blocking effect of the colloidal particles located at the boundary interface becomes invalid. A countercurrent of colloidal particles is generated near the center of the hole and the boundary interface. As a result, -21-200523706 (19) does not produce a pumping effect. According to the reasons for the above pumping effect, if a colloidal particle having a large diameter is used, the pumping effect will be produced until the film having a large pore size, and the flow rate generated at this time is also large. In addition, by selecting a combination of particles and membranes with a high degree of adsorption, the pumping effect can be improved. Next, the colloidal solution in which the particles were placed was changed in various conditions to confirm its versatility. The results are shown below. Fig. 8 shows the flow characteristics when the colloidal solution using polyethylene particles is used as the driving fluid when the combination of electrodes is changed. Experiments were performed on stainless steel (anode) -stainless steel (cathode), silver (anode) -stainless steel (cathode), and silver (anode) -zinc (cathode). The flow characteristics were almost the same. Fig. 19 is the result of using a colloidal solution using polyethylene particles as the driving fluid and changing the filling rate of polyethylene particles in the range of 0.1% to 0.011%. At 0 · 0 0 0 1%, some flows are reduced, but above the charge rate, approximately the same flow can be obtained. Fig. 20 shows the results of the case where the particles were changed into silicon particles and the same experiment as in Fig. 19 was performed. Similar to FIG. 19, at 0.01%, some flow rates are reduced, but above the charge rate, approximately the same flow rate can be obtained. FIG. 2 is a structural diagram of another embodiment of a pumped second pipe 10, where an intermediate medium 2 1 is placed in the middle of a tube (such as a glass tube), and the ejection liquid 2 3 (in FIG. 2 3 ) Press from left to right to make them move. Here, a thin tube 2 6 need not be considered based on the impact of the drop. In this way, if the flow caused by the application of voltage is used as a power source, each of the -22-200523706 (20) types of pumps can be achieved. Figures 2 and 2 are structural diagrams of other embodiments of the pump of the present invention. In this example, in the minute flow generating device shown in Fig. 2, the anode and cathode to which a DC voltage is applied are switched to make the fluid reciprocate. In this case, 'the colloidal solution is used as the solution used in the driving part, and the fluid can be reciprocated. In Fig. 22, a colloidal flow is generated from the direction of the arrow, that is, the anode toward the cathode side, the intermediate medium 21 is pushed to the right, and the ejection liquid 23 is ejected from the tube 28. At this time, the ejection liquid 23 is prevented from flowing toward the supply tank 33 by the valve 34. On the other hand, in FIG. 23, a flow is generated in a direction completely opposite to that of FIG. 23, the intermediate medium 21 is pulled, and the ejection liquid 2 3 from the supply tank 3 3 is supplied into the connection pipe 3 丨. At this time, the ejection liquid 23 on the ejection side is prevented from being sucked in by the tube 28 by the valve 35. Thereby, it is possible to inhale and discharge, and it can be used continuously for a long time. Next, an application example of the small flow pump according to the present invention shown in Figs. 1A, 1B, or 2 will be described. First, Fig. 24 is a plan view of an embodiment of a pump system to which the present invention is applied, and Fig. 25 is a cross-sectional view taken along the line A-A thereof. The pump system 2000 is equipped with a pump 100 on the platform 201. The pump 100 has a flat structure. This is because when the flat pedestal 201 is mounted on a flat surface of a table, the pump is easy to assemble if the flat structure is used. Pump! 〇 〇 is composed of an upper frame i 〇 丨 and a lower frame 1 〇 2, and a housing 10 03 is mounted on the upper portion of the upper frame 101. Inside the casing] 03, there is a small flow generating device shown in Figure 1A,] B or Figure 2] 0 6 ° Here I know: the important point is the small flow generating device-23- 200523706 (21) The plane of the porous film 2 in the same direction as the plane of the upper frame 1 ο 1 is arranged in the same direction. This makes it easy to manufacture the device, and it is possible to reduce the occurrence of a bent portion in the flow path of the solution. In addition, on the inner surface of the upper frame 101, a passage 1 10 is provided so as to be connected to the communication port I 09 and the communication passage 1 1 1. When a DC voltage is applied to a pair of electrodes of the minute flow generation device 106, the solution passes through the input tube 104 and the enlarged path 107, and passes through the minute flow generation device 106 to the enlarged path 108 and the contact port. 1 0 9, passage 1 10, and contact passage Π 1 are discharged to the destination by the outlet pipe 105. The passage 1 10 is provided on the upper frame 101, but it may also be provided on the lower frame 102. The structure in which the upper frame 101 and the lower frame 102 are cut away is to facilitate the processing of the passage 110. Of course, the upper frame 101 and the lower frame 102 may be integrated. The pump 100 configured in this way is mounted on a flat-shaped pedestal 20], and a battery 1 1 is arranged on the pedestal 201, a voltage regulator (variable impedance)] 6, and an on / off switch 1 1 5 and battery storage section cover I 1 8. The voltage regulator 1 1 6 is connected to a controller (not shown). In the controller, as described above, according to the preset condition data and the relationship shown in equations (4) and (5), calculate the applied voltage to the required flow rate to form this voltage and adjust the voltage regulator. Instead, control is performed at a predetermined flow rate. Furthermore, the user can directly operate the voltage regulator 1 16 by referring to the characteristics of FIG. 11. This small flow generating device 106 is characterized by being capable of delivering a solution by a low-voltage power source such as a battery, so it can be driven by a dry battery ′ without the need for a large power supply. Therefore, the battery]] 7, -24- 200523706 (22) Impedance Π 6, switches 1 1 5 are all built into the pedestal 20], and can be easily transported. The voltage generated by the battery 1 1 7 can be applied to the electrodes (anode, cathode) of the small flow generating device using wires Π 2, 1 1 3, 1 1 4 and this voltage can be interposed on the wire 1 The impedance Π 6 of 1 4 can be adjusted, and it can be cut off by the power supply through the switch 1 1 5. Fig. 26 is a structural diagram of another embodiment of the pump system of the present invention. In this example, a method is shown in which the contact of the solution 20 as the driving liquid and the ejection liquid 23 is combined. A groove 202 is provided at an outlet portion of the outlet pipe 105 of the pump 100, and a partition wall 220 is provided inside the groove. With the partition wall 220 as the realm, the outlet end of the outlet pipe 105 is connected to the left space, and the right space of the partition wall 2 20 is connected to the telescopic via pipe 2 1 3, the valve 2 1 1, and the pipe 2 1 2 Tube 2 1 4 of the slot 2 0 3. The ejection liquid 2 3 enters this tank 230, and the telescopic tube 2 1 4 is pressed. The ejection liquid 2 3 is supplied to the tank 202 through the tube 2] 3, the valve 211, and the tube 2] 2 and then is passed through the tube 202. The valve 211 is closed to stop the supply operation. A pipe 207 is connected to the left side of the tank 202, and the ejection liquid 2 3 in the tank 202 is discharged through a valve 208 and a pipe 2 06 into a tank 205 provided separately. When a voltage is applied to a pair of electrodes of the minute flow generating device 106 provided in the casing 103 of the pump 100, the driving fluid 20 in the tank 204 is sucked through the tube 2 17 and passed The passage in the frame 101 is further passed through the pipe 105 and enters the left chamber in the groove 202. This solution (driving fluid) enters the small chamber on the right through the small hole in the partition wall 220, and pushes the ejection liquid 23 on the upper part. Thereby, the ejection liquid 2 3 is ejected into the tank 205 through the tube 206. When the specific gravity of the ejection liquid is smaller than the specific gravity of the solution -25- 200523706 (23), as shown in the figure, these may be brought into contact with the chamber on the right side of the tank 202. When the specific gravity of the solution 20 is smaller than that of the ejection liquid 23, contact these in the chamber on the left side of the tank 202, and when the solution 20 and the ejection solution 23 are mixed with each other, the medium (for example, Silicon oil) 2 1 can be installed at these interfaces. FIG. 7 is a structural diagram of another embodiment of the pump 100 of the present invention, which is in the path 1 1 0 of the embodiment of FIG. 25 and is placed in the intermediate medium 21, which is a realm. The driving liquid 20 is placed on the side, and the ejection liquid 23 is placed on the opposite side. As a method of inserting this ejection liquid, a thick Π9 with a valve 2 0 is provided on the upper part of the upper frame 1 0 1. After the ejection liquid 23 is introduced into the tube 119, the valve 12 is closed in real time. FIG. 28 is a structural diagram of another embodiment of the pump of the present invention. This is a groove 204 provided above the tube 104 connected to the housing 103. This groove 204 is filled with a driving fluid. At 20, the driving fluid is introduced into the passageway via the 104, minute flow generation device 丨 〇6 by gravity. Then, the ejection liquid 23 is discharged from the intermediate medium 21 through the outlet pipe 105 to the destination. This flow rate is changed according to the locality of the slot 20 04 provided above the minute flow generation device. However, as a method of adjusting the flow rate at this time, the application of electricity to the electrodes of the minute flow generation device 1 is adjusted. the way. When the flow rate is further increased, apply a positive direction of electricity and increase the amount. On the one hand, when the flow rate is to be reduced, a reverse pressure is applied so that it acts in the direction of stopping the flow rate. If the pressure is increased, the flow can be stopped safely. Among them, 23 is the pressure of the pipe in the management field. -26-(24) (24) 200523706 Fig. 29 is a structural diagram of another embodiment of the pump of the present invention. This is to install a blocking part 1 0 1 -a in the middle of the passage 1 1 0. Taking this as the realm, the tubes 1 2 2 and 1 2 3 are placed in the lower frame 10 02, and a long tube 1 2 1 is placed between these. To form a closed ring structure. A part of the long tube 1 2 1 which is the closed ring is connected to the tube 1 2 4 in a branch manner, and the ejection liquid 2 3 is filled into the inside via a valve 1 2 5. An intermediate medium 2 1 is inserted in advance on the way of the tube 1 22. In this way, even if a long period of time elapses, there is no fear that the flow will stop and a desired flow rate can be obtained. In this embodiment, the same effect can be obtained even if the groove 202 with the partition wall 220 shown in Fig. 26 is provided instead of the long pipe 121. FIG. 30 is a structural diagram of another embodiment of the pump 100 of the present invention. As in FIG. 29, a blocking portion 101a is provided in the middle of the passage 110, and as a realm, the tubes 122 and 123 are installed in the lower frame 102 and connected in a U shape, and the intermediate medium 2 is filled in the inside] . A valve 1 2 6 is installed in a part of the tube 22, and a solution (driving liquid) 2 0 is inserted through the valve. A valve 1 2 7 is installed in a part of the tube 1 2 3, and the ejection liquid 2 is inserted through the valve. 3. In this figure, its structure is a valve] 2 2, 1 2 3 The upper ends are connected to the upper part of the upper frame 101, and the upper ends of these are connected to the float 1 2 6, 2 7 but can also be connected at the A branch pipe is provided at a part of the U-shaped valves [22,] 23 in the lower frame 102, and the valves 126, 127 are connected. As described above, the pump or pump system of the present invention is suitable for analysis of biological substances, pharmaceuticals, foods, and the like. Fig. 31 shows an example in which the pump system of the present invention is installed in an analysis system such as blood. The analysis system shown in FIG. 3 is in addition to the chestnut system of the present invention -27-200523706 (25). The analysis system includes a computer-equipped analysis device 300, a display device 300, and a microscope 300. The microchannel provided on the ejection side of the minute flow pump 100 and the visualization function section 3 10 are combined, and a solution containing blood, DNA, or cells to be analyzed is flowed into the microchannel. Such operations make the object visible. The observation was then enlarged by a microscope 3 0 4. In this case, 'when the pump flow rate fluctuates or pulsates', the image of the enlarged object is vibrated, and accurate observation cannot be performed. When the pump of the present invention is used, since the pump flow rate does not fluctuate or pulsate, the image of the enlarged object does not vibrate, and observation with high accuracy can be performed. Furthermore, in the conventional pump, it is not possible to simply change the flow direction. However, in the pump of the present invention, it is possible to simply reverse the flow by changing the polarity of the electrode. The present invention has the following features, in addition to the fact that there is no fluctuation or pulsation, or that the flow can be simply reversed, as described above. (1) Flow rate control can be performed easily and freely by changing the voltage. (2) Since it can operate at low voltage, it has high safety. (3) Cheap. (4) Small. (5) There will be no blockage, which can ensure stable flow. With this, the pump system of the present invention can be further extended to the scope of experiments and researches on biological relationships. It can be installed and used in various medical equipment. -28-200523706 (26) [Brief description of the drawings] ‘FIG. 1A is a schematic view showing the principle of the minute flow generating device of the present invention; FIG. 1B is a perspective view showing a part of the minute flow generating device of the present invention. Fig. 2 is a configuration diagram of an embodiment of the minute flow generating device of the present invention. Fig. 3 is a diagram showing an example of a combination of a solution, a porous film, and the like used in an embodiment of the present invention. ^ FIG. 4 is a diagram showing an example of another combination of a solution, a porous film, and the like used in an embodiment of the present invention. FIG. 5 is a diagram showing an example of a flow rate characteristic of the present invention. FIG. 6 is a diagram showing another example of the flow rate characteristics of the present invention. FIG. 7 is a diagram showing another example of the flow rate characteristics of the present invention. FIG. 8 is a diagram showing another example of the flow rate characteristics of the present invention. Fig. 9 is a graph showing a pump output p q obtained by using the pump of the present invention as a pressure P; FIG. 10 is a graph showing a comparison between the formula (2) and the experiment 値. Fig. 11 is a diagram showing an example of the results of measuring the ejection stars for a voltage applied using the pump of the present invention. Fig. 12 is a schematic diagram of an electroosmotic flow in the case where an electrolyte aqueous solution (sodium chloride, potassium chloride) is used in the pump of the present invention. Figure] .3 shows the colloidal particles with positive ions absorbed. Fig. 4 is a diagram showing a flow state in the case where a colloidal solution is used in the pump of the present invention. -29- 200523706 (27) Fig. 5 shows the flow characteristics of the pump of the present invention using colloidal particles with a diameter of 0.1 μm to change the pore diameter of the fine pores of the porous film. Other conditions are the same. Illustration. FIG. 16 is a diagram illustrating the relationship between the diameter R of the colloidal particles, the pore diameter E and the film thickness D of the micropores. Fig. 17 is an explanatory diagram of a state in which A-type colloidal particles pass through fine pores opened in a porous film; Fig. 1 7 is an explanatory diagram of a state in which colloidal particles pass through fine pores opened in a porous film; An explanatory view of a state in which colloidal particles pass through fine pores opened in a porous film. Fig. 18 is a diagram showing another example of the flow rate characteristic of the pump of the present invention. Fig. 19 is a diagram showing another example of the flow rate characteristic of the pump of the present invention. Fig. 20 is a diagram showing the flow rate of the pump of the present invention. Figures of other examples of characteristics. Figure 21 is a view showing a modified example of the pump of the present invention. Fig. 22 is a structural diagram showing another embodiment of the pump of the present invention. FIG. 23 is a diagram showing the operation of one of the pumps shown in FIG. 22. Fig. 24 is a plan view showing an embodiment of the pumping system of the present invention. Fig. 25 is a cross-sectional view taken along the line A-A of Fig. 24. Fig. 26 shows the structure of another embodiment of the pumping system of the present invention. Fig. 27 shows the structure of another embodiment of the pumping section in the pumping system of the present invention. Fig. 28 is a block diagram showing another embodiment of a pumping section in the pumping system of the present invention. Fig. 29 is a block diagram showing another embodiment of a pump section in the pump system of the present invention. Fig. 30 is a block diagram showing another embodiment of the pumping section in the pumping system of the present invention. FIG. 3 is a diagram showing an application example of the pump system of the present invention. [Description of symbols of main components] 1 ... first pipeline 2 ... porous film 3 ... support 4 ... electrode (anode) 5 ... electrode (cathode) 6 ... DC power supply 7 ... switch 8 ... second Inflow pipe section 9 of the pipeline ... Outflow pipe section of the second pipeline] 〇 ... Second pipeline 20 ... Solution (driving liquid) 21 ... Intermediate medium 22 ... Slim tube 2 3 ... Ejection liquid 200523706 (29) 26 ·· · Outflow side pipe of the first pipeline 2 7… Inflow side pipe of the first pipeline] 00 ... Pump 1 0] ... Upper frame 1 0 1-a ... Clogging portion 1 0 2 ... Lower frame 103 ... Enclosure 1 0 4… input tube 1 05… outlet tube 1 06 ··· small flow generating device 1 07… enlarged path 1 08… enlarged path 1 09… contact port] 1 2… conductor 1 1 5… switch 1 1 6 ··· impedance 1 1 7… Battery 2 0 0 ··· Pump system

Claims (1)

200523706 (1) 十、申請專利範圍 1 · 一種微少流量產生裝置,其特徵爲: 具備有:配置於流通路之多孔質薄膜;設置於該多 孔質薄膜的兩側之一對電極;將溶液供給至前述流通路 之手段;及在前述一對電極間施加直流電壓之直流電源 前述溶液爲處理成不會產生電氣分解之溶液, 藉由在前述一對電極間施加直流電壓,使過前述多 孔質薄膜的前述溶液之流動產生。 2 .如申請專利範圍第1項之微少流量產生裝置,其 中在前述溶液中添加氧化劑。 3 .如申請專利範圍第2項之微少流量產生裝置,其 中前述電極爲可逆電極。 4 .如申請專利範圍第1項之微少流量產生裝置,其 中前述溶液爲使粒徑0 . (Π 〜〇 . 5 μηι之微粒子浮游於媒 體之液體。 5 .如申請專利範圍第4項之微少流量產生裝置,其 中前述溶液爲使微粒子分離於液體中之膠體狀溶液。 6 · —種微少流量產生裝置,其特徵爲: 具備有:配置於流通路之多孔質薄膜;設置於該多 孔質薄膜的兩側之一對電極;將溶液供給至前述流通路 之手段;及在前述一對電極間施加直流電壓之直流電源 則述多孔質薄膜的厚度爲5 μ m至2 0 0 μ m, -33- 200523706 (2) 前述多孔質薄膜與各電極之間隙爲1 m m至]0 m m。 7 .如申請專利範圍第6項之微少流量產生裝置,其 中前述溶液爲膠體狀溶液,而將前述多孔質薄膜的細微 孔的徑設爲E、膠體粒子的直徑設爲R時,前述E= ( 1 0 〜200 ) R,而當膜厚設爲D時,則D= ( 1/5〜2 ) E之範 圍。 8 . —種微少流量產生裝置,其特徵爲:配置於流通 路之多孔質薄膜;設置於該多孔質薄膜的兩側之一對電 極;將溶液供給至前述流通路之手段;在前述一對電極 間施加直流電壓之直流電源;及調整前述直流電源的電 壓之電壓調整手段, 前述溶液爲處理成不會產生電氣分解之溶液, 藉由前述電壓調整手段,可調整:以在前述一對電 極間施加直流電壓,使得經由前述多孔質薄膜之前述溶 液的流量。 9. 一種泵浦,其特徵爲:在申請專利範圍第]至8 項中任一項之微少流量產生裝置的後游側,介裝中間媒 體,在該後游側塡充成爲目的之噴出液而可輸送噴出液 〇 1 〇.如申請專利範圍第9項之泵浦,其中藉由前述電 壓的施加與停止、或使陽極與陰極之極性逆轉,使得成 爲目的之噴出液係從相連於出口管之供給槽經由出口管 噴出。 1 1.如申請專利範園第9項之泵浦,其中前述泵浦之 -34 - 200523706 (3) 構造係具有在平板狀的框內設置通路的構件者,在其輸 入側設置外殼,在其內部’將多孔質薄膜的水平面與平 板狀的框之水平面設置於相同方向,在此外殼設置溶液 的輸入管,而在對於通路的外殼呈相反之側’設置噴出 液用出口管。 1 2 .如申請專利範圍第1 1項之栗浦,其中使中間媒 體介裝於前述通路之一部分° 1 3 .如申請專利範圍第1 1項之泵浦’其中在前述通 路的一部分也就是較中間媒體更後游側的通路之一部分 設置噴出液之塡充口。 1 4 .如申請專利範圍第1】項之栗浦’其中在設置於 前述多孔質薄膜的兩側之電極’經由導線結合有使電壓 產生之直流電源。 1 5 .如申請專利範圍第1 1項之栗浦’其中在則述電 極與前述直流電源之間距被可調節電壓之控制機構。 16. ·—種栗浦系統,係在微少流量產生部的輸入側設 置落差槽,經由泵浦之通路,以利用重力將噴出液經由 出口管排出者,其特徵爲:具備有:在微少流量產生部 之電極施加逆電壓,控制該電壓,能控制流量之申請專 利範圍第9項之泵浦者。 1 7 ·如申請專利範圍第9項之泵浦’其中將前述泵浦 搭載於台座上,在該台座或台座之中設置可控制前述直 流電源及該電源的電壓之控制機構。 ]8 . —種分析裝置,係具備有申請專利範圍第9項之 -35- 200523706 (4) 泵浦、與顯微鏡之分析裝置,其特徵爲:組合設在使前 述微少流量的泵浦之噴出側之微管道與能見化功能部, 在前述微管道內使分析對象之溶液流動,而將該對象物 加以能見化,而以前述顯微鏡進行觀察。200523706 (1) 10. Scope of patent application1. A small flow generating device, which is characterized by: having a porous film disposed on a flow path; one pair of electrodes provided on both sides of the porous film; and supplying a solution Means for reaching the aforementioned flow path; and a DC power source for applying a DC voltage between the pair of electrodes, the solution is a solution which is not to be electrically decomposed, and a DC voltage is applied between the pair of electrodes to pass through the porous material. The flow of the aforementioned solution of the film is generated. 2. The micro flow generating device according to item 1 of the patent application scope, wherein an oxidant is added to the aforementioned solution. 3. The micro flow generating device according to item 2 of the patent application, wherein the aforementioned electrode is a reversible electrode. 4. The micro-flow generating device according to item 1 of the scope of patent application, wherein the aforementioned solution is a liquid that causes particles with a particle size of 0. (Π ~ 0.5 μηι to float in the media. 5. Such as the tiny amount of item 4 of the scope of patent application A flow generating device, wherein the aforementioned solution is a colloidal solution that separates fine particles from a liquid. 6 · A small flow generating device, comprising: a porous film disposed in a flow path; and a porous film provided in the porous film A pair of electrodes on both sides of the electrode; a means for supplying the solution to the flow path; and a DC power source for applying a DC voltage between the pair of electrodes, the thickness of the porous film is 5 μm to 200 μm,- 33- 200523706 (2) The gap between the porous film and each electrode is 1 mm to 0 mm. 7. The device for generating a small flow rate according to item 6 of the patent application, wherein the solution is a colloidal solution, and the porous When the diameter of the pores of the thin film is set to E and the diameter of the colloidal particles is set to R, the aforementioned E = (1 0 to 200) R, and when the film thickness is set to D, D = (1/5 ~ 2 ) The range of E. 8.-A kind of micro The flow generating device is characterized by: a porous film disposed on a flow path; a pair of electrodes provided on both sides of the porous film; a means for supplying a solution to the flow path; and applying a DC voltage between the pair of electrodes A direct current power source; and a voltage adjusting means for adjusting the voltage of the direct current power source, the solution is a solution that is not processed to cause electrical decomposition, and can be adjusted by the aforementioned voltage adjusting means to apply a direct current voltage between the pair of electrodes, The flow rate of the solution passing through the porous film. 9. A pump, characterized in that an intermediate medium is interposed on the rear side of the minute flow rate generating device according to any one of the scope of the patent application] to 8. On this rear side, the discharge liquid is filled as the intended discharge liquid, and the discharge liquid can be transported. 0. The pump of item 9 of the patent application scope, wherein the polarity of the anode and the cathode is reversed by applying and stopping the aforementioned voltage. The purpose is to make the ejection liquid be ejected from the supply tank connected to the outlet pipe through the outlet pipe. Among them, the aforementioned Pump No. -34-200523706 (3) Structure is a member provided with a passage in a flat frame, and a casing is provided on the input side, and the horizontal plane of the porous film and the flat frame are provided inside. The horizontal plane is set in the same direction, the input pipe for the solution is set in this case, and the outlet pipe for the ejection liquid is set on the side opposite to the shell of the passage. The intermediate medium is installed in a part of the aforementioned channel ° 1 3. For example, the pump of item 11 of the scope of the patent application 'where a part of the aforementioned channel is also a part of the channel on the downstream side than the intermediate medium. Fill your mouth. 14. As described in item 1 of the scope of patent application, Kuriura 'wherein the electrodes provided on both sides of the porous film are connected with a DC power source for generating a voltage via a wire. 15. A control mechanism capable of adjusting the distance between the electrode and the aforementioned DC power source as described in "Kuriura's" in the scope of patent application No. 11. 16. · —Kuripu system is equipped with a drop groove on the input side of the small flow generation unit, and the person who discharges the ejection liquid through the outlet pipe through the passage of the pump is characterized by having: The electrode of the generating part applies a reverse voltage to control the voltage, which can control the flow of the pump applied for the item 9 of the patent scope. 1 7 · If the pump of item 9 of the scope of patent application is used, the aforementioned pump is mounted on a pedestal, and a control mechanism capable of controlling the aforementioned DC power supply and the voltage of the power supply is provided in the pedestal or pedestal. ] 8. An analysis device equipped with -35- 200523706 of the ninth scope of the patent application (4) An analysis device with a pump and a microscope, characterized in that: a combination of a pump provided for the aforementioned small flow rate of the pump The microchannel and the visualization function part on the side flow the solution of the analysis target in the microchannel, visualize the target, and observe with the microscope.
TW093136330A 2003-11-27 2004-11-25 Micro flow rate generator, pump and pump system TW200523706A (en)

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PCT/JP2004/011559 WO2005052379A1 (en) 2003-11-27 2004-08-11 Micro flow rate generator, pump and pump system

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