JP2007298010A - Fluid transportation mechanism and fluid transportation method - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To transport any fluid by using a straight-pipe type or linear flow passage as a flow passage of transportation fluid and using drive force generated by a boiling propagation phenomenon as conveyance power while preventing heat to obtain the drive force from affecting the transportation fluid. <P>SOLUTION: This fluid transportation mechanism (1) has the flow passage (5) for the transportation fluid (4), a drive liquid storage region (3) and a diaphragm (6). A heating element (10) with a heating face (10a) for heating the drive liquid (2) is arranged in the drive liquid storage region (3). A trigger part (11) of which the temperature is increased to overheating temperature higher than that of the heating face (10a) generates trigger bubbles (P) in a heating element end part, and induces the boiling propagation phenomenon on the heating face (10a). The drive liquid storage region (3), the heating element (10) and the diaphragm (6) are extended along the flow passage (5), and bubbles (B) are generated along the storage region (3) due to the boiling propagation phenomenon. The diaphragm (6) forms a deformation part (6a) raised inside the flow passage (5) and traveled along the flow passage (5). <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

  The present invention relates to a fluid transport mechanism and a fluid transport method. More specifically, the present invention uses a driving force generated by a boiling propagation phenomenon as conveyance power, and heat generated during the propagation of boiling acts on a transport fluid. In particular, the present invention relates to a fluid transport mechanism and a fluid transport method that enable transport of an arbitrary fluid.

  In fluid transport mechanisms such as microactuators and micropumps used for fluid transport, piezoelectric elements, shape memory alloys, boiling bubbles, and the like are used as driving force generation sources. In a fluid transport mechanism using a piezoelectric element or a shape memory alloy, the structure and control of drive electric signals are complicated. On the other hand, the fluid transport mechanism using boiling bubbles can simplify the structure and driving signal, and is suitable for downsizing, and is excellent in responsiveness and reproducibility. It is used for applications such as liquid ejection heads. In recent years, it has been proposed to apply such a fluid transport mechanism to various uses such as circuit board preparation, film coating, or DNA synthesis.

  However, in the fluid transport mechanism using boiling bubbles, only the phenomenon of bubble generation and bubble disappearance in response to pulse heating occurs repeatedly, and in order to form a fluid flow in a specific direction in the microchannel,・ Asymmetric structure such as a diffuser (continuous change in cross-sectional area in one direction) is formed in the flow path, or multiple heaters arranged along the flow path are heated in time series to generate bubbles and bubbles A method of giving a phase difference to annihilation must be adopted (WJYang, Thermal Science and Engineering, 9-4 (2001), pp.3-8, and TKJun & CJKim, J. Applied Physics, 83- 11 (1998), pp. 5658-5664).

With respect to such a fluid transport mechanism, an ink jet printer configured to separate discharge liquid (ink) and foaming liquid by a movable separation membrane, and to transmit pressure generated by foaming of the foaming liquid to the discharge liquid by deformation of the movable separation film Japanese Patent Application Laid-Open No. 2000-85129 discloses a liquid discharge head. A recess is formed in the movable separation membrane located in the bubble generation region of the foaming liquid, and the recess is deformed by the foam generation pressure of the foaming liquid. The bubble generation region is connected to a supply / discharge channel for foaming liquid, and the supply / discharge channel allows the foaming solution to flow out of the bubble generation region so as to equalize the liquid pressure in the bubble generation region during foaming / defoaming. Let it flow into the bubble generation area. Therefore, the movable separation film moves up and down reliably and stably and deforms the concave portion of the movable separation film, so that the ejection stability of the liquid ejection head can be improved as described in JP-A-2000-85129. It may be.
JP 2000-85129 A WJYang, Thermal Science and Engineering, 9-4 (2001), pp. 3-8 TKJun & CJKim, J. Applied Physics, 83-11 (1998), pp. 5658-5664

  However, the conventional fluid transport mechanism using the movable separation membrane that separates the flow path of the transport fluid and the storage area of the driving fluid periodically causes the deformation of the movable separation membrane in the specific portion of the flow path, and the specific portion It is only configured to pressurize or depressurize the transport fluid by changing the volume of the transport fluid. That is, the transport power of the transport fluid is generated by the movable separation membrane in a direction perpendicular to the membrane surface or a direction perpendicular to the membrane surface (hereinafter referred to as “out-of-plane direction”) due to the generation and defoaming of bubbles in the driving liquid storage area. The specific part is displaced, and the flow path part of the transport fluid in contact with the specific part of the movable separation membrane is merely pressurized or depressurized, and the membrane direction of the movable separation membrane (the direction along the membrane surface or the direction parallel to the membrane surface ( Hereinafter, it is referred to as “in-plane direction”))). For example, in the liquid discharge head disclosed in Japanese Patent Laid-Open No. 2000-85129 (Patent Document 1), the bubbles grow only in the vertical direction of the heating element, and the movable separation film is displaced vertically above the bubbles. Just do it.

  Therefore, in order to transport a transport fluid in a specific direction using such a fluid transport mechanism, irregularities, undulations or flow obstructions in the flow path are possible so that the fluid can be transported in a specific direction only by the behavior in the out-of-plane direction of the membrane. Forming an object or the like, changing the flow path or changing the flow path section continuously, or designing the flow path before and after the drive part to be asymmetrical with respect to the drive part, The transport direction of the fluid is determined by the flow path form. For this reason, the flow path of the transport fluid cannot be designed as a straight flow path with a low flow resistance that does not include irregularities or flow obstacles, and the transport fluid is transported bidirectionally. It cannot be designed as a flow path.

  Further, in the conventional fluid transport mechanism, the transport amount of the transport fluid is determined by the behavior in the out-of-plane direction of the membrane and the flow path form, and thus the transport amount cannot be adjusted, and the membrane reciprocates. Since the transport timing is determined by the cycle of movement, a large amount of fluid cannot be transported continuously.

  On the other hand, the present inventors have proposed a micropump in which the transport fluid is heated directly and the transport fluid flows in the transport direction by the boiling propagation phenomenon of the transport fluid itself (Japan Society for Multiphase Flow Studies) Lecture Proceedings (2005), pp. 225-226), this mechanism may be used to design fluid transport mechanisms such as micropumps. However, in such a type of fluid transport mechanism, the transport fluid is directly exposed to a high temperature that causes bumping, and therefore the types of fluid that can be transported are limited. For example, it is not preferable to apply such a fluid transport mechanism to a micropump used in the field of chemistry or biotechnology from the viewpoint of loss of function due to transformation / decomposition of components in the liquid. Thus, there is a need for the development of a fluid transport mechanism that can transport any fluid while minimizing the influence of the heat supplied for the boiling propagation phenomenon.

  The present invention has been made in view of such a problem, and an object of the present invention is to use a straight pipe type or a straight flow path as a flow path for transport fluid and to obtain heat for obtaining a driving force. It is an object of the present invention to provide a fluid transport mechanism and a fluid transport method that prevent the fluid from affecting the transport fluid and enable the transport of an arbitrary fluid.

  Another object of the present invention is to provide a fluid transport mechanism and a fluid transport method capable of transporting fluid in both directions in such a fluid transport mechanism and fluid transport method.

  It is another object of the present invention to provide a fluid transport mechanism and a fluid transport method capable of adjusting the transport amount of the transport fluid in the fluid transport mechanism and the fluid transport method.

In order to achieve the above object, the present invention provides a flow path of a fluid to be transported, a driving liquid storage area that generates bubbles in the driving liquid by bumping of the driving liquid, and a diaphragm that separates the flow path and the storing area. In a fluid transport mechanism having
A heating element provided with a heating surface disposed in the storage area and configured to heat the driving liquid sealed in the storage area;
Raising the temperature to a superheat temperature higher than the superheat temperature of the heat generating surface, generating bubbles at the end of the heat generating body, and having a trigger portion for inducing a boiling propagation phenomenon on the heat generating surface;
The housing area, the heating element and the diaphragm extend along the flow path, the trigger portion is disposed at an end of the heating element, and the diaphragm moves on the heating surface due to the boiling propagation phenomenon. To provide a fluid transport mechanism characterized by forming a deformed portion that rises in the flow path and transitions along the flow path.

The present invention also encloses a driving liquid in a driving liquid storage area that is in contact with a flow path of a fluid to be transported via a diaphragm, generates bubbles in the driving liquid by bumping of the driving liquid, and deforms the diaphragm. In the fluid transport method for transporting the fluid in the flow path,
A heating element having a heating surface for raising the temperature to the first overheating temperature is disposed in the housing area, and a trigger portion for raising the temperature to a second overheating temperature higher than the first overheating temperature is provided at an end of the heating element. And generating a bumping bubble in the driving liquid by the trigger part to induce and advance a boiling propagation phenomenon on the heating surface,
The fluid is characterized in that the diaphragm is deformed by bubbles that move and grow on the heat generating surface, the deformed portion of the diaphragm is shifted in the transport direction of the fluid, and the fluid is transported by the deformed portion. Provide transportation methods.

  The present inventor can obtain a driving force for deforming the diaphragm in the out-of-plane direction and in the in-plane direction by a group of bubbles generated by the boiling propagation phenomenon of the liquid, and has the directivity, responsiveness and reproducibility of the boiling propagation phenomenon. It has been found experimentally that the transport of fluid can be controlled by utilizing this, and the present invention has been achieved based on such knowledge.

  According to the above configuration of the present invention, bubbles (trigger bubbles) generated at the end portion (trigger portion) of the heating element grow while moving on the heating surface of the heating element, and deform the diaphragm. The deformed portion of the diaphragm rises in the flow path of the fluid to be transported, transitions in the fluid transport direction, and pushes the fluid in the transport direction. The heat possessed by the bubbles is lost during the growth process, and the bubbles are condensed and defoamed sequentially from the rear, reach the other end (front end) of the heating element, and then disappear completely. It is possible to control the heat generation at the end of the heating element (trigger part) and the heat generation surface, and to control the progress of the boiling propagation phenomenon on the heat generation surface.

  Therefore, according to the present invention, the pressure that causes the fluid to flow in the transport direction and the deformation of the flow path contour are obtained by the deformation in the out-of-plane direction and the in-plane direction of the diaphragm. It can be designed to be a straight pipe-type flow path or a straight flow path that does not include an object or the like.

  Also, the end of the heating element (trigger part) only needs to generate heat for a short time so as to generate a trigger bubble that induces the boiling propagation phenomenon, and if the heating surface continues to generate heat to the extent that the boiling propagation phenomenon proceeds. Well, the heat generating surface is separated from the flow path of the transport fluid by the diaphragm and is also separated from the fluid in position. Moreover, the driving liquid around the bubbles actually has a temperature much lower than the boiling temperature of the driving liquid. Therefore, the heat for obtaining the driving force, that is, the heat generation at the end of the heating element and the heating surface does not act directly on the transport fluid, and the influence of the heat generation on the transport fluid is only limited, and thus, The fluid transport mechanism of the present invention can transport any fluid, such as a liquid used in the chemical or bio field.

  Preferably, the first superheat temperature is set to a temperature having a degree of superheat of 50K or more with respect to the boiling point temperature of the driving liquid. The boiling propagation phenomenon is a phenomenon that occurs regardless of the type of liquid under the condition that the heating surface is as smooth as a vapor deposition film and there are only slight scratches or depressions of 0.1 μm or less on the heating surface. It is believed that. Therefore, in this specification, the “heat generating surface” means a high-temperature heat transfer surface having properties and physical properties that cause the boiling propagation phenomenon to proceed and does not hinder this phenomenon. In the present specification, the secondary fluid (transport fluid) is understood as a concept including not only liquids such as aqueous solutions, organic liquids, and oils but also fluid substances such as powders.

  The present invention also provides a fluid transport mechanism having the above-described configuration, wherein the trigger portion is disposed in pairs at both ends of the heating element. The advancing direction of the boiling propagation phenomenon is determined by the position of the heated trigger part, and the fluid is transported in the advancing direction of the boiling propagation phenomenon, so the transport direction of the fluid is set by the arrangement of the trigger part or the trigger It can be controlled by selective heating of the part.

  Further, the present invention provides the fluid transport mechanism having the above-described configuration, wherein the heating element and the trigger portion are made of an electric heating element through which a pulse current is passed, and an electric circuit for controlling the pulse current is provided. Provide transport mechanism. According to such a configuration, by controlling the pulse width, pulse voltage, and phase of the pulse voltage signal, it is possible to control the boiling propagation phenomenon on the heating surface and adjust the transport amount of the transport fluid.

  According to the fluid transport mechanism and the fluid transport method of the present invention, the transport fluid is transported by the deformation in the out-of-plane direction and the in-plane direction of the diaphragm. It can be used as a flow path. In addition, since the heat generating surface of the driving liquid storage area is separated from the flow path of the transport fluid by the diaphragm, the influence of the heat of the heat generating surface on the transport fluid is suppressed. Therefore, according to the fluid transport mechanism and the fluid transport method of the present invention, any fluid can be transported using the boiling propagation phenomenon.

  In addition, according to the fluid transport mechanism and the fluid transport method of the present invention, the trigger portions are arranged at both ends of the heating element to set or control the fluid transport direction, thereby transporting the fluid bidirectionally. can do.

  Furthermore, according to the fluid transport mechanism and the fluid transport method of the present invention, by using an electric heating element to which a pulse current is passed as a heating element and a trigger unit, by controlling the pulse width, pulse voltage and phase of the pulse current, The boiling propagation phenomenon on the heat generating surface can be controlled and the transport amount of the transport fluid can be adjusted.

  According to a preferred embodiment of the present invention, the fluid transport mechanism constitutes a micropump or microactuator provided with a microchannel for transporting the transport fluid. Preferably, the driving fluid storage area is formed by a groove having an elongated recess shape whose both ends are terminated by end walls, or a circulation flow including a reflux path for returning the driving fluid in front of the heating element to the rear of the heating element. It has a road form.

  If desired, a plurality of driving liquid storage areas are arranged in parallel to the flow path, and a plurality of diaphragm deforming portions are formed. According to such a configuration, the behavior of the deforming portion can be synchronized, and the transport liquid can be transported by a powerful pump action using a plurality of deforming portions.

  Preferably, the electric heating element is formed of a metal thin film formed on a substrate, and the metal thin film is formed at an elongated effective heat generating portion, a pair of electrode portions disposed at both ends of the effective heat generating portion, and an end portion of the effective heat generating portion. And a reduced portion of the connected voltage tap. The voltage circuit includes a main circuit connected to the electrode and a trigger circuit connected to the voltage tap, and the reduction unit constitutes a trigger unit. The trigger circuit energizes the reduced voltage portion with the pulse voltage signal to cause the reduced portion to generate heat. Preferably, the voltage circuit supplies the pulse voltage signal to the heating element and the trigger unit, and controls the pulse width, pulse voltage, and phase of the pulse voltage signal, thereby controlling the boiling propagation phenomenon on the heating surface.

  In a preferred embodiment of the present invention, the trigger portions are disposed at both ends of the heating element, and the traveling direction of the boiling propagation phenomenon is set by selective heating of the trigger portion. According to such a structure, the transport direction of the fluid can be controlled by controlling the heating of the trigger portion.

  As the diaphragm, a flexible film material (for example, silicon rubber or resin film) having a thickness of about 10 μm and having stretchability, adhesion, impermeability, strength, chemical resistance and heat insulation is preferable. Can be used. Further, as the substrate, a composite structure substrate having a low thermal conductivity layer such as SiO2 directly under the heating element and a high thermal conductivity material such as silicon as a base material of the substrate can be preferably used. The low thermal conductivity layer prevents heat dissipation loss of the heating element during pulse heating, and the base material of the high thermal conductivity material prevents excessive temperature rise of the substrate.

  FIG. 1A is a longitudinal sectional view showing a structure of a fluid transport mechanism according to the present invention, and FIG. 1B is a sectional view taken along line II in FIG. 1A. FIG. 2 is a longitudinal sectional view showing the principle of a fluid transportation method using the fluid transportation mechanism shown in FIG.

  As shown in FIG. 1, the fluid transport mechanism 1 includes a drive liquid storage area 3 in which a drive liquid (primary liquid) 2 can be sealed, and a transport liquid flow path 5 for transporting the transport liquid (secondary liquid) 4. And a diaphragm 6 that separates the storage area 3 and the transport liquid flow path 5. The storage area 3 is formed by sealing the top opening channel of the storage area forming member 7 with a horizontal diaphragm 6, and the driving liquid 2 is enclosed in the storage area 3. A thin film heater 10 extending in the direction of the flow path is disposed on the bottom surface of the driving liquid storage area 3, and a trigger portion 11 that generates a trigger bubble P (FIG. 2) is disposed at the end of the thin film heater 10. The flow path 5 is formed by sealing the bottom opening type channel of the flow path forming member 8 with the diaphragm 6. The inner wall surface 8a of the flow path forming member 8 does not have irregularities, undulations, and the like, does not have an asymmetric portion, and forms a straight pipe type flow path having an equal cross section over the entire length in the fluid transport mechanism 1. Both ends of the channel 5 are opened or connected to channels of other systems, and the channel 5 transports the transport liquid 4 in the direction of arrow A from one end (upstream end) to the other end (downstream end). The diaphragm 6 is made of a horizontal flexible membrane material extending along the flow path 1, isolates the driving liquid 2 and the transport liquid 4, and elastically deforms locally in response to a sudden pressure change of the driving liquid 2. Has possible deformability.

  The heat generating surface 10a of the heater 10 in contact with the driving liquid 2 is heated to a predetermined temperature (liquid overheating temperature) by energization heating of the heater 10. The liquid superheat temperature of the heat generating surface 10a is set to a temperature having a degree of superheat of 50K or more with respect to the boiling point temperature of the driving liquid 2. When the heating surface 10a is heated to the liquid superheat temperature, the trigger portion 11 is energized, and when the surface temperature of the trigger portion 11 is raised to a temperature higher than the liquid superheat temperature, as shown in FIG. 11, trigger bubbles P are generated. The heat generating surface 10a extends downstream from the trigger portion 11, and the bubbles P have the property of moving to the side receiving heat supply and growing. Accordingly, the bubbles P move in the direction of arrow A along the heat generating surface 10a, are further heated by the heat generating surface 10a, and grow into bubbles B while rapidly expanding. The thermal energy received by the bubbles B is consumed by the growth of the bubbles B, and as a result, the bubbles B are quickly defoamed. The defoaming of the bubbles B acts to attract the rear liquid (driving liquid) in the direction of arrow A.

  A main circuit and a trigger circuit (not shown) for controlling heating of the heater 10 and the trigger unit 11 are connected to the heater 10 and the trigger unit 11, and the heater 10 and the trigger unit 11 are energized and heated by these circuits, and a heating sequence is performed. Can be repeated at a constant repetition frequency to cause the heater 10 and the trigger unit 11 to generate heat periodically. Thereby, the boiling propagation phenomenon occurs periodically on the heater 10, and the transport liquid 4 is transported continuously in the direction of arrow A.

  Boiling propagation is a kind of “sudden boiling phenomenon”, and in order to continuously generate bubbles B, not only the heating of the heater 10 and the trigger part 11 need to repeatedly generate boiling with a high superheat degree. It is necessary to quickly eliminate the bubbles B on the heat generating surface 10a. Therefore, the rapid disappearance of the bubbles B is an important factor in maintaining the boiling propagation phenomenon on the heat generating surface 10a. For example, in sufficiently degassed water or ethanol, since the non-condensable gas remains slightly after the bubbles B disappear, it is difficult to repeatedly cause the boiling propagation of the driving liquid 2 to occur. Therefore, as the driving liquid 2, a liquid in which the non-condensable gas does not remain after the bubbles B disappear is preferably used.

  As shown in FIG. 2, the bubbles B growing on the heat generating surface 10 a locally increase the volume of the driving liquid 2 due to the expansion thereof, and the diaphragm 6 is moved to the secondary side (of the flow path 5 by the vapor pressure of the bubbles B). To the side) and deform. The diaphragm 6 forms a deformed portion 6 a that protrudes toward the flow path 5, and the deformed portion 6 a changes or transitions in the direction of arrow A due to the boiling propagation of the driving liquid 2. The deforming part 6a locally reduces the volume of the flow path 5, and the front inclined surface of the deforming part 6a presses the transport liquid 4 in the flow path 5 forward and pushes the transport liquid 4 in the direction of arrow A. work.

  The bubbles P are generated in the trigger unit 11 in response to the pulse current supplied to the trigger unit 11, grow as a group of bubbles B moving on the heat generating surface 10a as shown in FIG. After reaching the front edge, it disappears. In the state where the heater 10 is pulse-heated by the main circuit and the heat generating surface 10a is preheated in advance, a pulse current (trigger signal) giving a predetermined phase difference (time difference) is supplied to the trigger unit 11 by the trigger circuit. Thus, the group of bubbles B periodically move on the heat generating surface 10a, and the deforming portion 6a sequentially moves in the direction of the arrow A. By repeating the heating sequence by the main circuit and the trigger circuit at a predetermined frequency and periodically causing the boiling propagation phenomenon on the heat generating surface 10a, the diaphragm 6 is waved so as to push the transport liquid 4 in the direction of arrow A or It pulsates.

  The growth process of the group of boiling bubbles B growing on the heat generating surface 10a can be controlled by the liquid superheating temperature of the heat generating surface 10a and the relative position of the trigger part 11 with respect to the heat generating surface 10a. The position of the deformed portion 6a formed by the bubbles B changes in the direction of arrow A along the heat generating surface 10a, and the deformed portion 6a sequentially decreases the cross-sectional area of the flow path 5 in the transport direction (arrow A direction). Therefore, the fluid transport mechanism 1 transports the transport liquid 4 in the direction of arrow A by the same mechanical action as that of the ironing pump. That is, according to the fluid transport mechanism 1 of the present invention, the driving force for deforming the diaphragm 6 is obtained mainly by the rapid acceleration of the liquid around the bubble (driving liquid 2) due to the high vapor pressure at the beginning of the bubble growth. Due to the deformation and displacement behavior, the transport power of the transport liquid 4 is obtained. Since the directionality and speed of the displacement behavior of the diaphragm 6 depend on the boiling peculiarity called the boiling propagation phenomenon, the boiling propagation direction of the driving liquid 2 (accordingly, the transport liquid 4) due to the positional relationship between the trigger portion 11 and the heat generating surface 10 a. The transport amount of the transport liquid 4 by one boiling propagation changes according to the length of the heat generating surface 10a and the like. Therefore, the transport direction of the transport liquid 4 does not depend on the shape (asymmetry or the like) of the fluid transport path 1 and is determined by the relative positions of the heat generating surface 10a and the trigger portion 11, and the transport amount of the transport liquid 4 is the heater 10 And the repetition period of the pulse current application sequence of the trigger unit 11, the liquid overheating temperature of the heat generating surface 10a, the length of the heat generating surface 10a, and the like.

  According to such a fluid transport mechanism 1, the heat generation of the trigger portion 11 is only a short-time pulse heat generation, and the heat generating surface 10 a is separated from the transport liquid 4 by the diaphragm 6 and transported also in terms of position. Separate from liquid 4. Accordingly, only the driving liquid 2 in the vicinity of the trigger unit 11 and the heater 10 is only heated to a high temperature. Moreover, the driving liquid 2 around the expanding bubble B actually has a temperature considerably lower than the boiling point temperature of the driving liquid 2. Further, the transport liquid 4 is separated from the driving liquid 2 by the diaphragm 6, and the heat held by the driving liquid 2 is merely conducted to the transport liquid 4 through the diaphragm 6. Therefore, according to the fluid transport mechanism 1 configured as described above, the influence of heat on the transport liquid 4 can be minimized.

  It is desirable to adjust the operating temperature range, vapor pressure, etc. of the driving liquid 2 in accordance with the temperature conditions and physical properties of the transport liquid 4, and therefore the components and composition of the driving liquid 2 are the operating temperatures of the driving liquid 2. It is appropriately selected according to the range and vapor pressure. As the driving liquid 2, for example, an aqueous solution, an organic liquid, an oil, an alternative chlorofluorocarbon, a cryogenic liquid, or the like can be used. It is desirable to set so that it does not remain in area 3.

  By using one long heater as the heater 10, a series of boiling propagation phenomena that last for a relatively long time occur in the driving liquid storage region 3. A large amount of the transport liquid 4 can be transported. On the other hand, by using a heater 10 having a relatively short overall length, a boiling propagation phenomenon that is completed in a relatively short time is repeatedly generated in the drive liquid storage area 3, thereby transporting the transport liquid. 4 can be transported in small increments. Such a difference in the transport mode is selectively adopted as appropriate according to the purpose of use of the fluid transport mechanism 1.

  FIG. 3 is a vertical cross-sectional view of the fluid transport mechanism 1 illustrating the structure of the driving liquid storage area 3.

  The driving liquid storage area 3 shown in FIG. 3A is composed of an elongated recess-shaped groove whose both ends are terminated by an end wall 3a. The storage area 3 is sealed by a diaphragm 6, and the driving liquid 2 is sealed in the storage area 3. The bubbles B generated in the storage area 3 due to the heat generated by the trigger unit 11 and the heater 10 rapidly expand as shown by the phantom line and urge the driving liquid 2 in the moving direction of the bubbles B. Is blocked by the front end wall 3 a, the vapor pressure of the bubble B mainly acts on the diaphragm 6 as a pressure for pushing up the diaphragm 6. Such a structure of the accommodating area 3 is, for example, when the repetition frequency of the pulse current to be applied to the heater 10 and the trigger unit 11 is set to be relatively small and the generation period of the trigger bubble P is set to be relatively long. Preferably it can be adopted. As described above, the heating propagation of the heater 10 and the trigger unit 11 is repeated at a constant repetition frequency to cause the heater 10 and the trigger unit 11 to generate heat periodically, whereby the boiling propagation phenomenon occurs periodically on the heater 10. The transport liquid 4 is transported continuously in the direction of arrow A.

  FIG. 3B shows a driving liquid storage area 3 in the form of a circulation channel. The storage area 3 has a reflux path 3d separated from the forward flow path 3b by the partition wall 9, and the forward flow path 3b and the reflux path 3d communicate with each other by a communication flow path 3c disposed in front and rear of the heater 10, respectively. . Bubbles B (indicated by phantom lines) generated in the storage area 3 urge the driving liquid 2 in the moving direction of the bubbles B, and at least a part of the driving liquid 2 flows out from the front communication path 3c to the reflux path 3d. Then, it returns to the forward flow path 3b from the rear communication path 3c. Such a structure of the accommodating area 3 is, for example, when the repetition frequency of the pulse current to be applied to the heater 10 and the trigger unit 11 is set to be relatively large and the generation period of the trigger bubble P is set to be relatively short. Preferably it can be adopted. As described above, the heating propagation of the heater 10 and the trigger unit 11 is repeated at a constant repetition frequency to cause the heater 10 and the trigger unit 11 to generate heat periodically, whereby the boiling propagation phenomenon occurs periodically on the heater 10. The transport liquid 4 is transported continuously in the direction of arrow A.

  FIG. 4 is a vertical cross-sectional view of the fluid transport mechanism 1 illustrating another structure of the driving liquid storage area 3.

  The fluid transport mechanism 1 shown in FIGS. 4 (A) and 4 (B) includes a plurality of driving liquid storage areas 3 arranged around the flow path 5. The fluid transport mechanism 1 shown in FIG. 4 (A) is provided with a storage area 3 having both ends closed by end walls 3a, similar to the fluid transport mechanism 1 shown in FIG. 3 (A). The fluid transport mechanism 1 shown has a storage area 3 in the form of a circulation channel, similar to the fluid transport mechanism 1 shown in FIG.

  As shown in FIGS. 4A and 4B, according to the fluid transport mechanism 1 having a configuration in which a plurality of storage areas 3 are formed in parallel around the flow path 5, a plurality of deformed portions 6a are connected to the transport liquid flow path. Can be formed simultaneously. By simultaneously raising the temperature of the heat generating surface 10a to a predetermined temperature (liquid overheating temperature) and synchronizing the pulse current of the trigger unit 11, a trigger bubble is generated as shown in phantom lines in FIGS. 4 (A) and 4 (B). P can be generated at the same time in each of the storage areas 3, and the transport liquid 4 can be transported by the plurality of deformation portions 6a. According to the fluid transport mechanism 1 having such a configuration, a high driving force (conveyance power) is obtained, so that the transport liquid 4 is transported by the powerful pump action of the fluid transport mechanism 1.

  FIG. 5A is a perspective view showing an embodiment of a micropump to which the fluid transport mechanism of the present invention is applied, and FIG. 5B is an exploded perspective view of the micropump shown in FIG. 5A. . FIGS. 6A and 6B are a plan view and a partially enlarged view showing the structure of the thin film heater formed on the substrate.

  A micropump 20 shown in FIG. 5A has a multilayer structure in which a substrate 21, a resin sheet 22, a diaphragm 6, a resin sheet 23, and a glass plate 24 are integrally laminated. End portions of the transport liquid channel 5 are opened at both end surfaces of the micropump 20.

  As shown in FIG. 5B, the heater 10 is formed on the substrate 21. The heater 10 is formed of a metal thin film pattern formed on the center of the upper surface of the substrate 21 by vapor deposition or sputtering. The metal thin film of this example consists of a platinum vapor deposition film, and has the effective heat generating part 12 about width (W) 0.2-1 mm and length (L) 2-10 mm. As shown in FIG. 6, a pair of voltage taps 13 are connected to both end portions of the effective heat generating portion 12 via a reduced portion having a width of about 0.1 mm. The reduction part of the voltage tap 13 constitutes the trigger part 11. The voltage tap 13 is used as a boiling start means for generating the trigger bubble P and also as a temperature measuring means.

  As shown in FIG. 5A, a resin sheet 22 in which a housing area forming slit 26 for forming the driving liquid housing area 3 is formed at the center is overlaid on the substrate 21. The resin sheet 26 has a thickness of about 0.2 to 0.5 mm. The slit 26 has a width of about 0.5 to 3 mm and a total length of about 1 to 1.2 times the length (L) of the effective heat generating portion 12. In this example, a silicon rubber sheet is used as the resin sheet 22, but another resin, rubber or elastomer sheet may be used as the sheet 22. The slit 26 penetrates the resin sheet 22 vertically. The slit 26 and the heater 10 are aligned in the laminated state of the resin sheet 22 and the substrate 21, and form a top opening-shaped groove that can accommodate the driving liquid 2.

  By overlapping the diaphragm 6 on the resin sheet 22 in a state where the slit 26 is filled with the driving liquid 2, the driving liquid containing area 3 in which the driving liquid 2 is enclosed is formed. The diaphragm 6 is made of a resin-made flexible film material having a thickness of about 10 μm, for example, a polyvinylidene chloride film material, and is a deformation that can be elastically deformed locally in response to a change in the pressure of the driving liquid 2. Have the ability.

  A resin sheet 23 including a flow path forming slit 27 for forming the transport liquid flow path 5 is further overlapped on the diaphragm 6. The resin sheet 23 has a thickness of about 0.2 to 0.5 mm. The slit 27 has substantially the same width (about 0.5 to 3 mm) as the slit 26 and penetrates the resin sheet 23 vertically. The slit 27 is disposed on the center line of the resin sheet 23 and extends over the entire length of the resin sheet 23. In this example, a silicon rubber sheet is used as the sheet 23, but other resin, rubber, or elastomer sheet-like material may be used as the sheet 23.

  A rectangular flat glass plate 24 is further stacked on the resin sheet 23 to form the micropump 20 having a laminated structure shown in FIG. The opening ends of the transport liquid channel 5 located on both end faces of the micropump 20 are connected to the channels 51 and 52 of the transport liquid 4, and the transport liquid 4 is injected into the channels 5, 51 and 52 by a micro syringe or the like. Is done.

  FIG. 7A is a circuit configuration diagram showing an electric circuit for driving the micropump 20.

  The electric circuit for driving the micropump 20 includes a waveform generator, a high-speed power amplifier, a digital oscilloscope, and a standard resistor (a resistor that maintains a constant electric resistance value without being affected by heat generated by current). Is incorporated. The waveform generator generates a rectangular pulse voltage signal, and the high-speed power amplifier amplifies the pulse voltage signal. The electric circuit includes a main circuit for energizing the heater 10 and a trigger circuit for energizing the voltage tap 13, and the high-speed power amplifier is incorporated in the main circuit and the trigger circuit, respectively.

  As shown in FIG. 6, the end portion of the metal thin film of the heater 10 is enlarged, and the electrode portions 15 to which the conductive wires 61 can be connected are formed at both ends of the heater 10. As shown in FIG. 5B, the energization wires 61 constituting the main circuit are connected to the respective electrode portions 15, and the energization wires 62 constituting the trigger circuit are respectively connected to the voltage tap 13 and the electrode portion 15. The Since the trigger unit 11 that generates electricity generates the trigger bubble P, the transport direction of the micropump 20 is set in the direction of arrow A shown in FIG. The measurement signal lines 63 and 64 of the digital oscilloscope are connected to the voltage tap 13 and the standard resistor, respectively, and the potential difference between the taps and the energization current of the heater 10 are measured by the oscilloscope. The heat flux value and the heat transfer surface temperature are obtained.

  FIG. 7B is a pulse waveform diagram showing waveforms of pulse voltage signals energized in the main circuit and the trigger circuit, respectively.

  A rectangular pulse voltage signal generated by the waveform generator is amplified by a high-speed power amplifier and is passed through the electrode portion 15 of the heater 10 as a heating current. The heater 10 generates Joule heat, and the heat generating surface 10a is heated. When the heat transfer surface temperature (average temperature) of the heater 10 determined by the potential difference between the voltage taps 13 and the energization current of the heater 10 reaches a temperature T (liquid superheat temperature) of a predetermined superheat degree, the pulse width (time A pulse voltage signal of (width) δ = about 0.1 ms is applied to the trigger circuit as a trigger signal. The trigger portion 11 of the upstream voltage tap 13 (13a) generates heat, and a boiling bubble (trigger bubble P) is generated in the trigger portion 11. By inducing a boiling propagation phenomenon on the heat generating surface 10a using this bubble as a trigger, the propagating bubble B moves on the heat generating surface 10a in the direction of arrow A and disappears sequentially. In this process, the diaphragm 6 is pushed up by the bubbles B, and a deformed portion 6 a (FIG. 2) protruding in the transport liquid channel 5 is formed. Since the deforming portion 6 transitions in the traveling direction of the propagation bubble B, the transport liquid 4 in the flow path 5 is transported in the propagation direction (arrow A direction).

  The transport liquid 4 is transported continuously in the direction of arrow A by repeating the heating sequence by the main circuit and the trigger circuit at a constant repetition frequency and periodically causing the boiling propagation phenomenon on the heater 10.

  The difference between the temperature T for determining the energization timing of the trigger signal and the boiling point temperature of the driving fluid 2, that is, the degree of superheat, is set to a temperature of 50K or higher. The degree of superheat is appropriately determined according to the type and physical properties of the driving liquid 2. However, in order to advance the boiling propagation phenomenon on the heater 10, overheating is performed on almost all driving liquids regardless of the type and physical properties of the transport liquid 4. It is desirable to set the degree to 50K or higher.

  By applying a pulse voltage signal (trigger signal) for generating a trigger bubble to the voltage tap 13 (13b) on the opposite side of the heater 10, the moving direction of the propagation bubble B is reversed and the transport direction of the transport liquid 4 is reversed. be able to. Such reversal of the transport direction can be achieved by reconnecting the trigger circuit to the electrode portion 15 (15b) and the voltage tap 13b on the opposite side of the heater 10, or connecting the trigger circuit to both electrode portions 15 in advance. It can be executed by switching operation.

  FIG. 8 is an electric circuit configuration diagram and a pulse waveform diagram showing a performance test method of the micropump 20. In FIG. 8, components that are substantially the same as or equivalent to the components shown in FIG.

  The inventor conducted a performance test of the micropump 20 using the experimental apparatus shown in FIG. The experimental apparatus shown in FIG. 8 includes a microchannel 70 for measuring the transport amount of the micropump 20 and a high-speed video camera 71 that captures the flow state of the transport liquid 4 and the boiling state of the driving liquid 2. .

  FIG. 9 shows the structure of the microchannel 70.

  The microchannel 70 includes a pair of capillary tubes 72 and a resin plate 74 in which a pair of through holes 73 are formed. The tube 72 is inserted into the through hole 73. A pair of circular ports 5 a into which tubes 72 can be inserted are formed at both ends of the transport liquid channel 5. The in-pipe region of the tube 72 communicates with the flow path 5 through the circular port 5a. The transport liquid 4 is injected into the flow path 5 and the tube 72 at the start of the experiment.

  The high-speed video camera 71 is connected to a controller via a signal line 76, and the controller is connected to a digital oscilloscope via a signal line 77. A light source 75 is disposed adjacent to the high-speed video camera 71 and irradiates the micropump 20 with imaging light. The high-speed video camera 7 images the flow of the fluid in the flow path 5 through the glass plate 24 and images the liquid level of the transport liquid 5 in the tube 72. The controller analyzes the imaging result and records the flow state of the transport liquid 5 and the liquid level in the tube.

  In the experimental apparatus shown in FIG. 8, the heater 10 is made of a platinum vapor deposition film formed on a quartz glass substrate 21 (FIG. 5), and has an effective heat generating portion having a width of 0.5 mm, a length of 5 mm, and a thickness of 0.25 μm. Twelve. The resin sheets 22 and 23 (FIG. 5) are made of a silicon rubber sheet having a thickness of 0.5 mm, and the diaphragm 6 is made of a polyvinylidene chloride film material (thickness 10 μm). The width of the slits 26 and 27 (FIG. 5) was set to 1.5 mm, and the total length of the slit 26 was set to about 12 mm. Further, as the driving liquid 2, a mixed liquid of 65% water, 20% ethylene glycol and 15% isopropanol was used, and water was used as the transport liquid 4.

  In the experiment using this experimental apparatus, the pulse voltage signal amplified by the high-speed power amplifier is energized to the heater 10 to cause the heater 10 to generate Joule heat, and the trigger signal is energized to the trigger circuit to generate the trigger bubble P and drive. A boiling propagation phenomenon was caused in the liquid storage area 3. By repeating the heating sequence by the main circuit and the trigger circuit at a constant repetition frequency (10 Hz) and periodically causing the boiling propagation phenomenon on the heater 10, the transport liquid (water) 4 is transported in the direction of arrow A. In the downstream tube 72, the liquid level increased, and in the upstream tube 72, the liquid level decreased. As a result of imaging the meniscus on the surface of the water column in the capillary tube 72 with the high-speed video camera 7, water moves (transports) in the propagation direction (arrow A direction) at a speed of about 10 mm per minute due to the behavior of the meniscus. It was confirmed experimentally.

  The preferred embodiments of the present invention have been described in detail above, but the present invention is not limited to the above-described embodiments, and various modifications or changes can be made within the scope of the present invention described in the claims. Is possible.

  For example, by increasing the width (W) of the effective heat generating portion 12 and the widths of the slits 26 and 27, the displacement amount of the diaphragm 6 can be increased, and the transport capability of the fluid transport mechanism 1 can be enhanced.

  Further, the degree of superheat of the heater 10, the pulse width of the pulse voltage signal, and the like can be appropriately set and changed according to the type of the driving liquid.

  The present invention is preferably applied to a micropump, a microactuator, and the like that perform liquid transport and supply / discharge control of a micro flow rate with excellent responsiveness and controllability using a fine flow path with a simple structure. The present invention has a wide range of applications to microchips in the fields of chemistry, medicine, biotechnology, information, machinery, environment, space (for example, biological devices such as μTAS, various measurement / diagnosis / chemical analysis of environment, information devices such as optical switches Micromachine drive actuators, microthrusters (miniature satellite attitude control jetting devices), electronic equipment cooling, etc.) are expected.

FIG. 1A is a longitudinal sectional view showing a structure of a fluid transport mechanism according to the present invention, and FIG. 1B is a sectional view taken along line II in FIG. 1A. It is a longitudinal cross-sectional view which shows the principle of the fluid transport method using the fluid transport mechanism shown in FIG. It is a longitudinal cross-sectional view of the fluid conveyance mechanism which illustrates the structure of a drive fluid storage area. It is a longitudinal cross-sectional view of the fluid conveyance mechanism which illustrates the other structure of a driving fluid storage area. FIG. 5A is a perspective view showing an embodiment of a micropump to which the fluid transport mechanism of the present invention is applied, and FIG. 5B is an exploded perspective view of the micropump shown in FIG. 5A. . It is the top view and partial enlarged view which show the structure of the thin film heater formed into a film on the board | substrate. FIG. 7A is a circuit configuration diagram showing an electric circuit for driving the micropump, and FIG. 7B is a pulse waveform showing a waveform of a pulse voltage signal energized in the main circuit and the trigger circuit, respectively. FIG. It is the electric circuit block diagram and pulse waveform diagram which show the performance test method of a micropump. It is the top view which shows the structure of a microchannel, a longitudinal cross-sectional view, and an exploded perspective view.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Fluid transport mechanism 2 Drive liquid 3 Drive liquid accommodation area 4 Transport liquid 5 Transport liquid flow path 6 Diaphragm 6a Deformation part 7 Containment area formation member 8 Flow path formation member 10 Heater 10a Heat generating surface 11 Trigger part P Trigger bubble B Bubble A direction (Transport direction)

Claims (11)

In a fluid transport mechanism having a flow path of a fluid to be transported, a driving liquid storage area that generates bubbles in the driving liquid by bumping of the driving liquid, and a diaphragm that separates the flow path and the storage area.
A heating element provided with a heating surface disposed in the storage area and configured to heat the driving liquid sealed in the storage area;
Raising the temperature to a superheat temperature higher than the superheat temperature of the heat generating surface, generating bubbles at the end of the heat generating body, and having a trigger portion for inducing a boiling propagation phenomenon on the heat generating surface;
The housing area, the heating element and the diaphragm extend along the flow path, the trigger portion is disposed at an end of the heating element, and the diaphragm moves on the heating surface due to the boiling propagation phenomenon. A fluid transport mechanism characterized by forming a deformed portion that rises in the flow path and transitions along the flow path.   The fluid transport mechanism according to claim 1, wherein the trigger portion is disposed in a pair at both ends of the heating element.   3. The fluid transport mechanism according to claim 1, wherein the heating element and the trigger portion are made of an electric heating element that generates heat and is provided with an electric circuit that supplies a pulse voltage signal to the electric heating element.   4. The fluid transport mechanism according to claim 1, wherein the housing area has a reflux path for allowing the driving liquid in front of the heating element to flow back to the rear of the heating element. 5.   5. The fluid transport mechanism according to claim 1, wherein the plurality of storage areas are arranged in parallel to the flow path.   The electric heating element is formed of a metal thin film formed on a substrate, and the metal thin film is formed on an elongated effective heat generating portion, a pair of electrode portions disposed at both ends of the effective heat generating portion, and an end portion of the effective heat generating portion. The voltage circuit includes a main circuit connected to the electrode and a trigger circuit connected to the voltage tap, and the reduction unit includes the trigger unit. 4. The fluid transport mechanism according to claim 3, wherein the trigger circuit supplies a pulse voltage signal to the reduction unit to generate heat. A driving liquid is enclosed in a driving liquid storage area in contact with a flow path of a fluid to be transported via a diaphragm, and bubbles are generated in the driving liquid by bumping of the driving liquid, and the fluid in the flow path is generated by deformation of the diaphragm. In the fluid transportation method of transporting
A heating element having a heating surface for raising the temperature to the first overheating temperature is disposed in the housing area, and a trigger portion for raising the temperature to a second overheating temperature higher than the first overheating temperature is provided at an end of the heating element. And generating a bumping bubble in the driving liquid by the trigger part to induce and advance a boiling propagation phenomenon on the heating surface,
The fluid is characterized in that the diaphragm is deformed by bubbles that move and grow on the heat generating surface, the deformed portion of the diaphragm is shifted in the transport direction of the fluid, and the fluid is transported by the deformed portion. Transport method.   The said trigger part is arrange | positioned at the both ends of the said heat generating body, the advancing direction of a boiling propagation phenomenon is set by the selective heating of this trigger part, and the transport direction of a fluid is controlled. Fluid transportation method.   A pulse voltage signal is applied to the heating element constituting the heating element and the trigger unit, and the pulse width, pulse voltage, and phase of the pulse voltage signal are controlled, and the boiling propagation phenomenon on the heating surface is controlled. The fluid transport method according to claim 7 or 8.   The plurality of deformation portions are formed by the plurality of storage areas arranged in parallel to the flow path, and the behavior of the deformation portions is synchronized. Fluid transport method.   The fluid transport method according to any one of claims 7 to 10, wherein the first superheat temperature is set to a temperature having a degree of superheat of 50K or more with respect to a boiling point temperature of the driving liquid.

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