The rectification of ion transport pathways is an effective method to generate one-directional ion-dragged electrohydrodynamic flows. By setting an ion-exchange membrane in a flow channel, an electrically polarized condition is generated and causes a liquid flow to be driven when an electric field is externally applied.
To drive electrohydrodynamic (EHD) flows in aqueous solutions, the separation of cation and anion transport pathways is essential because a directed electric body force has to be induced by ionic motions in liquid. On the other hand, positive and negative charges attract each other, and electroneutrality is maintained everywhere in equilibrium conditions. Furthermore, an increase in an applied voltage has to be suppressed to avoid water electrolysis, which causes the solutions to become unstable. Usually, EHD flows can be induced in non-aqueous solutions by applying extremely high voltages, such as tens of kV, to inject electrical charges. In this study, two methods are introduced to generate EHD flows induced by electrical charge separations in aqueous solutions, where two liquid phases are separated by an ion-exchange membrane. Due to a difference in the ionic mobility in the membrane, ion concentration polarization is induced between both sides of the membrane. In this study, we demonstrate two methods. (i) The relaxation of ion concentration gradients occurs via a flow channel that penetrates an ion-exchange membrane, where the transport of the slower species in the membrane selectively becomes dominant in the flow channel. This is a driving force to generate an EHD flow in the liquid. (ii) A long waiting time for the diffusion of ions passing through the ion-exchange membrane enables the generation of an ion-dragged flow by externally applying an electric field. Ions concentrated in a flow channel of a 1 x 1 mm2 cross-section determine the direction of the liquid flow, corresponding to the electrophoretic transport pathways. In both methods, the electric voltage difference required for an EHD flow generation is drastically reduced to near 2 V by rectifying the ion transport pathways.
Recently, liquid flow control techniques have attracted much attention because of interest in the applications of micro- and nanofluidic devices1,2,3,4,5,6,7,8,9,10,11,12,13,14,15. In polar solutions, such as aqueous solutions and ionic liquids, ions and electrically charged particles usually bring about electrical charges in liquid flows. The transport of such polarized particles provides an expansion of various applications, such as single-molecule manipulation6,10,11,13,14,15,16,17, ion diode devices12,18, and liquid flow control19,20,21,22. EHD flow has been an applicable phenomenon for liquid flow control systems since Stuetzer1,2 invented the ion drag pump. Melcher and Taylor3 published an important article in which the theoretical framework of EHD flow was well reviewed and some outstanding experiments were also demonstrated. Saville4 and his coworkers23,24 contributed to the following expansion of EHD technologies in liquids. However, there were some limitations to inducing liquid flows driven by electric forces, because tens of kV have to be applied in liquids to inject electrical charges in non-polar solutions, such as oils, to polarize them1,2,3. This is a disadvantage for aqueous solutions because the water electrolysis that is induced by an electric potential higher than 1.23 V changes the characteristics of solutions and makes the solutions unstable.
In micro- and nanofluidic channels, surface charges of channel walls cause the concentration of counterions that effectively induce electroosmotic flows (EOFs) under externally applied electric fields25,26,27,28,29. Using EOFs, some liquid pumping techniques have been applied in aqueous solutions, reducing the electric voltages30,31,32. On the other hand, EOFs are limited to being generated in micro- and nanospaces in which surface areas become more dominant than liquid volumes. Furthermore, depending on the transport of highly concentrated ions very near the wall surfaces, such as in electric double layers, the slip boundary only causes the liquid flow, which may not be sufficient to make pressure gradients7,8,22,26,27. Fine tuning, such as to channel dimensions and salt concentrations, is required for the applications of EOF. In contrast, EHD flows driven by body forces seem to be available to transport masses and energies if the application voltages can be reduced to avoid degrading solvents. Recently, some researchers have suggested applications of EHD flows with low voltages33,34,35,36. Although these technologies have not yet been implemented, the frontiers are expected to expand.
In previous studies, we also conducted experimental and theoretical work on EHD flows in aqueous solutions37,38,39,40. It was supposed that the rectification of ion transport pathways was effective to generate electrically charged solutions that cause electric body forces under electric fields. By using an ion-exchange membrane and a flow channel crossing the membrane, we were able to rectify ionic currents. When applying an anion-exchange membrane, cations concentrated in the flow channel dragged the solvents and developed an EHD flow37,38,39. A difference in the mobility of ion species was an important factor when separating the cationic and anionic currents. Ion-exchange membranes effectively worked to modulate the mobility due to the ion selectivity. Ion transport phenomena were also investigated from the viewpoint of ionic current density influenced by applied electric fields41. These studies have been fruitful for developing manipulation techniques for single molecules, namely, micro- and nanoparticles, whose motions are strongly affected by thermal fluctuations11,16,17. EOFs and EHD flows are expected to expand the variety of precise flow control methods as well as pressure gradients.
In this study, we demonstrate two methods to drive EHD flows in aqueous solutions. First, an NaOH solution is used for a working fluid to drive an EHD flow37,38,39. An anion-exchange membrane separates the liquid into two parts. A polydimethylsiloxane (PDMS) flow channel with a cross-section of 1 x 1 mm and a length of 3 mm penetrates the membrane. By applying an electric potential of 2.2 V, the electrophoretic transport of Na+, H+, and OH− ions is induced along the electric fields. An anion-exchange membrane and a flow channel effectively work to separate the ion transport pathways, where anions dominantly pass through the membrane and cations concentrate in the flow channel, although both species usually move in opposite directions, maintaining the electroneutrality. Thus, such a condition does not cause a driving force for liquid flows. This structure is crucial to generating an EHD flow whose flow speed reaches on the order of 1 mm/s in the channel because highly concentrated cations accelerated by external electric fields drag solvent molecules. EHD flows are observed and recorded by using a microscope and a high-speed camera as shown in Figure 1. Second, a concentration difference between two liquid phases separated by an ion-exchange membrane causes an electrically polarized condition to be generated crossing an ion-exchange membrane40. In this study, we find the importance of a considerable waiting time to equilibrate ion distributions and a corresponding electric potential, which cause preferable conditions to apply to a body force in a liquid. Crossing the ion-exchange membrane, a weakly polarized condition is achieved. In such a condition, an externally applied electric field induces directional ion transport that generates a body force in a liquid, and as a result, the momentum transfer from the ions to the solvent develops an EHD flow.
As mentioned above, the present devices succeed in drastically decreasing the applied voltage difference to a few volts, and thus this method is can be used for aqueous solutions, although the conventional electrical charge injection methods required tens of kV and are limited to an application to non-aqueous solutions.
1. EHD Flow Induced by Rectified Ion Transport
2. Observation of Cation-induced EHD Flows
Figure 4 (video figure) presents a representative result of an EHD flow generation, resulting from the rectification of ion transport pathways and highly concentrated cations that induced a liquid flow in the channel, according to step 1 of the protocol. Figure 5 shows a result of the PIV analysis, where 20 data points near the center of the channel (y = z = 0 mm) were averaged. In the case of the 1 x 10−1 mol/L NaOH solution, when an electric potential of 2.2 V was applied at t = 5 s, the velocity of the tracer particles quickly increased to a peak value. After that, the velocity decreased and converged to 0. The peak velocity reached a near 2 mm/s. This is a typical result of an EHD flow generated by using an anion-exchange membrane and a 1 x 10−1 mol/L NaOH solution.
It was also confirmed that the electrophoretic transport velocity of tracer particles was much lower than the peak velocity of the liquid flow in the 1 x 10−1 mol/L NaOH solution38,39. As discussed in the literature39, this kind of EHD flow is considered to consist of reversed flows dragged by OH− passing through the membrane and Na+ and H+ concentrated in the flow channel to compensate for the anion transport in the membrane. As the concentration decreased, the transport behavior tended to become slower. This means that the duration-until the velocity reached a peak-and the decay time seemed to be longer, decreasing the peak value of the velocity. This result indicated that the number of ions whose motion was driven by electric forces decreased, and consequently, the electric body force in the liquid was also reduced.
One important observation is that continuous ionic currents rectified by the ion selective interfaces caused solvent molecules to be dragged in one direction and this caused a liquid flow to develop. In this case, there is a possibility that the liquid flow was enhanced by ion concentration polarization crossing the anion-exchange membrane that triggered the reverse flow in the channel. This point was already mentioned in a previous study39. It was supposed that AC fields were also effective to control liquid flows periodically changing directions. The present EHD flow was limited to transient responses because of the finite number of Na+ ions; this situation was not conducive to maintaining a steady cationic current, even though the applied voltage of 2.2 V was enough to induce the electrolysis of water. To generate constant EHD flows, we propose dragging solvent molecules with ion species that are the dominant carrier of the ionic current. Further details will be verified in our future work. Here, we introduced a representative result of an EHD flow that could be induced in NaOH solutions by rectifying ion transport pathways. Details about the concentration dependency and electric potential differences are also discussed by Yano, Doi, and Kawano37,38 and Yano, Shirai, Imoto, Doi, and Kawano39.
Figure 6 (video figure) shows a representative result of the EHD flow generated in an electrically polarized solution under ionic current conditions. The velocity response of the EHD flow was also analyzed by tracking the tracer particles, as shown in Figure 7, which was a typical result obtained by tracking a single particle near the center of the flow channel. When an electric potential of 2 V was applied from t = 2 to 8 s, polystyrene particles responded to the applied electric field. At t = 2 s, the particle quickly translocated in the backward direction, corresponding to the electrophoretic transport of negative charges. After a short-time response, the flow changed to the forward direction and the velocity became steady at 30 µm/s until the electric potential was turned off.
In this period, the negatively charged polystyrene particles moved in the direction of the transport of the positive charges. In general, the direction could not be reversed spontaneously under the one-directional electric field, even if the surface charge of the particles was fully shielded by the counter cations. Thus, this result indicated that cations dispersed in the solution were also electrophoretically transported along the electric fields, dragging solvent molecules that gradually developed a liquid flow. Negative charges highly concentrated on the particle surface caused an electric force stronger than that by cations distributed in the solution, and, thus, firstly drove the transport in the negative direction. After that, a liquid flow dragged by the cationic current increased a drag force on the particle. In this regime, velocity gradients were actually observed along the y-axis perpendicular to the flow direction, and, thus, a liquid flow generation was actually confirmed.
The behavior of polystyrene particles affected by EHD flows was also evaluated in a previous study, and it was found that the velocity of the EHD flow proportionally increased with an increasing ionic current. A waiting time of over 18 h before applying an external electric field is the most important factor for inducing a constant EHD flow, because it takes such a long time for the ion distributions to be equilibrated since they are almost uniform in the channel. As a result, Poiseuille-like flow patterns are steadily observed. On the other hand, we could not confirm a steady flow when the waiting time was not sufficient to achieve uniform ion distributions.
After observing a constant velocity, the electric potential was turned off at t = 8 s. Here, to quickly change the electric potential difference from 2 to 0 V, the shielded electrodes may require an excessive application of the electric potential to make both electrode surfaces equivalent. In that process, ions highly concentrated near the electrode surfaces receive repulsive electric forces, which result in reversed ionic currents. Especially, the cationic current that was dominant in the lower layer caused a liquid flow to be generated, and a transient response in the backward direction was actually observed in the experimental result, which immediately appeared when the electric potential was turned off and converged to 0 µm/s. Such processes in the EHD flow generation were typical in this experiment. Next to the steady EHD flow, the reverse flows observed when switching the electric potential on and off are also interesting. In the transient responses, electrochemical reactions at the electrode surfaces possibly cause drastic ion concentration gradients that induce the diffusion potential as well as externally applied electric potentials. Such complicated ion transport phenomena have not yet been clarified enough and, therefore, are subjects to be solved in future work.
The mechanisms of the EHD flow generation are schematically presented in Figure 8. An EHD flow induced in NaOH solutions is shown in Figure 8a, corresponding to the case of Figure 4. The EHD flow dragged by Na+ in the channel is triggered by the transport of OH− in an anion-exchange membrane. The unsteady flow is caused by the dissipation due to mass flux damping, momentum flux damping, surface mobility, and electrowetting of the electrode surfaces. Another mechanism of EHD flow induced under cationic current conditions, which are more dominant than anionic ones, is represented in Figure 8b. K+ ions first penetrate a cation-exchange membrane, causing cation-dominant conditions, and, as a result, EHD flow is induced along the cationic current.
As described above, maintaining electrically polarized conditions under ionic current conditions by reducing the application of the electric potentials is key to generating steady EHD flows. By using the present methods, a few volts may be sufficient to induce EHD flows in aqueous solutions, although water electrolysis is necessary to maintain constant ionic currents to enhance the momentum transfer from electrolyte ions to solvent molecules.
Figure 1: Photograph of experimental setup for EHD flow observation. Motions of tracer particles are traced by a microscope connected to a high-speed camera, recording the trajectories in the controller. Electric potentials are applied by using a potentiostat or a DC electric power source. Please click here to view a larger version of this figure.
Figure 2: Schematic illustration of an experimental device. A flow channel made of PDMS is fixed in an anion-exchange membrane and filled with an NaOH aqueous solution. Au electrodes are placed at both ends of the solution. The origin of the coordinate is set at the center of the square flow channel and an observation area is in an xy plane near x = 0.75 and z = 0 mm. Please click here to view a larger version of this figure.
Figure 3: Photograph of experimental setup and schematic diagram of a device to induce a cation-dragged EHD flow in an electrically polarized solution. A 1 mol/L KCl and 1 x 10−2 mol/L Tris-EDTA buffer solution and a 1 x 10−2 vol% polystyrene (PSt) particle dispersion in a 1 x 10−2 mol/L Tris-EDTA buffer solution are separated with a cation-exchange membrane, where the average diameter of the PSt particles is 1.01 µm. Please click here to view a larger version of this figure.
Figure 4 (video figure): A movie of EHD flow driven by the transport of Na+ ions concentrated in the flow channel. The tracer particles are transported along the direction of the electric field when an electric potential of 2.2 V is applied at t = 5 s. Negatively charged polystyrene particles are brought to the cathode side in an EHD flow driven by the cationic current in the channel. In the case of a 1 x 10−1 mol/L NaOH solution, a peak velocity near 2 mm/s is reached quickly after applying an electric potential, and the velocity successively decays to zero. Please click here to view this video. (Right-click to download.)
Figure 5: The response of EHD flow observed in the flow channel, resulting from the PIV analysis for the recorded movie of Figure 4. The velocity response (blue solid line) was obtained by the average of 20 points near the center of the channel (y = z = 0 mm). The velocity is quickly increased after applying an electric voltage of 2.2 V at 5 s and gradually converges to 0 mm/s. The sequence of the applied voltage is also shown with a red dashed line. Please click here to view a larger version of this figure.
Figure 6 (video figure): A movie of EHD flow observed in an electrically polarized solution, separating a 1 mol/L KCl solution and polystyrene dispersion by using a cation-exchange membrane. Applying an electric potential of 2 V from t = 2 to 8 s, the transport of tracer particles reflects an EHD flow driven by a cationic current. A constant flow velocity reaches 30 µm/s during the application of the potential. Additionally, the particles also briefly respond in the negative direction when the electric potential is turned on and off because the electrical charge of a particle firstly affects the motion. Please click here to view this video. (Right-click to download.)
Figure 7: The response of EHD flow observed in the channel, resulting from the PTV analysis for the recorded movie of Figure 6. The velocity response (blue solid line) was obtained by tracking a single particle near the center of the channel. The sequence of the applied voltage is also shown with a red dashed line. Please click here to view a larger version of this figure.
Figure 8: Schematics of EHD flow generation mechanisms corresponding to Figures 4 and 5 (panel a) and 6 and 7 (panel b). (a) Liquid flows are induced in an NaOH aqueous solution that is separated with an anion-exchange membrane, where EOF induced by an OH− transport in the membrane triggers a flow dragged by an Na+ transport in the channel and is partly dissipated with mass flux damping, momentum flux damping, surface mobility, and electrowetting of the electrode surfaces. (b) The cationic current is more dominant than the anionic current because K+ firstly penetrates a cation-exchange membrane, which contributes to a liquid flow dragged by cations under constant current conditions involving water electrolysis. Please click here to view a larger version of this figure.
The purpose of this study was to separate cations and anions in aqueous solutions in terms of spatial distributions and transport numbers. Using an anion-exchange membrane, the transport of anions and cations could be rectified in the membrane and in a flow channel that penetrates the membrane, respectively. Alternatively, a cation-exchange membrane that separated high and low concentration solutions worked to generate electrically polarized solutions after a considerable waiting time. As a result, rectified ionic currents succeeded in reducing the applied voltages to induce ion-dragged EHD flows.
The methods presented here are available for aqueous solutions with low application voltages in comparison to conventional methods that require extremely high voltages of tens of kV to inject electrical charges into non-polar solutions. It was clarified that EHD flows are effective in aqueous solutions as well as non-polar solutions.
However, the present methods depend on water electrolysis to maintain constant ionic currents in which the ideal potential of water electrolysis is known to be 1.23 V. Thus, there is a limitation on the applied voltage to avoid generating O2 and H2 bubbles that change the properties of a liquid. To overcome this limitation, materials of the electrodes and electrolyte solutions have to be appropriately determined to set electrochemical reactions at the electrode surfaces to generate ionic currents in the solutions. At every trial, the electrode surfaces should be polished and bared to make a strong electric field in the solution, enhancing the electrochemical reactions.
In this study, the use of ion-exchange membranes was proposed to rectify the transport pathways of ion species. On the other hand, the efficiency of EHD flow generation seemed to depend on the capability of the membranes. As discussed in the protocol, the diffusion of ions takes a considerable waiting time until it becomes stable. Therefore, the preprocess to increase the conductivity of the membranes is crucial to improving the efficiency of the EHD flow generation. When maintaining ionic current conditions in externally applied electric fields, transport properties of ions are improved, and electrically polarized conditions are effectively achieved.
In the future, EHD flows of aqueous solutions are expected to be applicable for liquid flow control systems in micro- and nanofluidic devices combined with EOFs and the like. Furthermore, applications for medical devices, in which ion transport has an important role to stimulate biological cells and signal transduction, are also challenging.
The authors have nothing to disclose.
The authors have no acknowledgments.
Sylgard 184 | Dow Corning Corp. | 3097366-0516, 3097358-1004 | PDMS |
Acetone | Wako Pure Chemical Industries, Ltd. | 012-00343 | |
Ethanol | Wako Pure Chemical Industries, Ltd. | 054-00461 | |
0.1 mol/L Sodium Hydroxide Solution | Wako Pure Chemical Industries, Ltd. | 196-02195 | |
Pottasium Chloride | Wako Pure Chemical Industries, Ltd. | 163-03545 | |
Tris-EDTA buffer 100x concentrate | Sigma-Aldrich Co. LLC. | T9285-10014L | |
2.93 μm polystyrene particle | Merck KGaA | L300 Rouge | Tracer particle |
1.01 μm polystyrene particle | Merck KGaA | K100(23716) | Tracer particle |
Anion exchange membrane | ASTOM Corp. | Neosepta AHA | |
Gold (Au) | Furuuchi Chemical Corp. | AUT-13301X | Sputtering target metal |
Titanium | Furuuchi Chemical Corp. | TIT-72301X | Sputtering target metal |
Chromium | Furuuchi Chemical Corp. | CRT-24301X | Sputtering target metal |
Hight-speed CMOS camera | Keyence Corp. | VW-600M | |
Microscope | Keyence Corp. | VW-9000 | |
Data logger | Keyence Corp. | NR-500, NR-HA08 | |
Laser displacement meter | Keyence Corp. | LK-G5000, LK-H008W | |
PIV and PTV software | DITECT Co. Ltd. | Flownizer 2D | |
Potentiostat | AMTEK Inc. | VersaSTAT4 | |
Inverted microscope | Olympus Corp. | IX73 | |
High-speed CMOS camera | Andor Technology Ltd. | Zyla 5.5 sCMOS | |
Function generator | NF Corp. | WF1945B | |
Function generator | NF Corp. | WF1973 | |
Ultrasonic cleaner | AS ONE Corp. | AS22GTU | |
Rotary pump | ULVAC, Inc. | G-100S | Degas liquid PDMS |
Rotary pump | ULVAC, Inc. | GLD-201A | Sputtering |
Molecular diffusion pump | ULVAC, Inc. | VPC-400 | Sputtering |