Remotely powered self-propelling particles and micropumps based on miniature diodes

Microsensors and micromachines that are capable of self-propulsion through fluids could revolutionize many aspects of technology. Few principles to propel such devices and supply them with energy are known. Here, we show that various types of miniature semiconductor diodes floating in water act as self-propelling particles when powered by an external alternating electric field. The millimetre-sized diodes rectify the voltage induced between their electrodes. The resulting particle-localized electro-osmotic flow propels them in the direction of either the cathode or the anode, depending on their surface charge. These rudimentary self-propelling devices can emit light or respond to light and could be controlled by internal logic. Diodes embedded in the walls of microfluidic channels provide locally distributed pumping or mixing functions powered by a global external field. The combined application of a.c. and d.c. fields in such devices allows decoupling of the velocity of the particles and the liquid and could be used for on-chip separations.     

Torque-actuated valves for microfluidics

This paper describes torque-actuated valves for controlling the flow of fluids in microfluidic channels. The valves consist of small machine screws (> or =500 microm) embedded in a layer of polyurethane cast above microfluidic channels fabricated in poly(dimethylsiloxane) (PDMS). The polyurethane is cured photochemically with the screws in place; on curing, it bonds to the surrounding layer of PDMS and forms a stiff layer that retains an impression of the threads of the screws. The valves were separated from the ceiling of microfluidic channels by a layer of PDMS and were integrated into channels using a simple procedure compatible with soft lithography and rapid prototyping. Turning the screws actuated the valves by collapsing the PDMS layer between the valve and channel, controlling the flow of fluids in the underlying channels. These valves have the useful characteristic that they do not require power to retain their setting (on/off). They also allow settings between "on" and "off" and can be integrated into portable, disposable microfluidic devices for carrying out sandwich immunoassays.     

Selective ion extraction: a separation method for microfluidic devices

A separation concept, selective ion extraction (SIE), is proposed on the basis of the combination of hydrodynamic and electrokinetic flow controls in microfluidic devices. Using a control system with multiple pressure and voltage sources, the hydrodynamic flow and electric field in any section of the microfluidic network can be set to desired values. Mixtures of compounds sent into a T-junction on a chip can be completely separated into different channels on the basis of their electrophoretic mobilities. A simple velocity balance model proved useful for predicting the voltage and pressure settings needed for separation. SIE provides a highly efficient separation with minimal additional dispersion. It is an ideal technique for high-throughput screening systems and demonstrates the power of lab-on-a-chip systems.     

Electroosmotically induced hydraulic pumping on microchips: differential ion transport

The theory behind and operation of an electroosmotically induced hydraulic pump for microfluidic devices is reported. This microchip functional element consists of a tee intersection with one inlet channel and two outlet channels. The inlet channel is maintained at high voltage while one outlet channel is kept at ground and the other channel has no electric potential applied. A pressure-induced flow of buffer is created in both outlet channels of the tee by reducing electroosmosis in the ground channel relative to that of the inlet channel. Spatially selective reduction of electroosmosis is accomplished by coating the walls of the ground channel with a viscous polymer. The pump is shown to differentially transport ions down the two outlet channels. This ion discrimination ability of the pump is examined as a function of an analyte's electrophoretic velocity. In addition, we demonstrate that an anion can be rejected from the ground channel and made to flow only into the field-free channel if the electrophoretic velocity of the anion is greater than the pressure-generated flow in the ground channel. The velocity threshold at which anion rejection occurs can be selectively tuned by changing the flow resistance in the field-free channel relative to the ground channel.     

Pressure-driven laminar flow in tangential microchannels: an elastomeric microfluidic switch

This paper describes laminar fluid flow through a three-dimensional elastomeric microstructure formed by two microfluidic channels, fabricated in layers that contact one another face-to-face (typically at a 90 degree angle), with the fluid flows in tangential contact. There are two ways to control fluid flow through these tangentially connected microchannels. First, the flow profiles through the crossings are sensitive to the aspect ratio of the channels; the flow can be controlled by applying external pressure and changing this aspect ratio. Second, the flow direction of an individual laminar stream in multiphase laminar flow depends on the lateral position of the stream within the channel; this position can be controlled by injecting additional streams of fluid into the channel. We describe two microfluidic switches based on these two ways for controlling fluid flow through tangential microchannels and present theoretical arguments that explain the observed dependence of the flow profiles on the aspect ratio of the channels.     

Solute transport under oscillating electro-osmotic flow in a closed-ended cylindrical pore

Mass transfer in a closed-ended, cylindrical tube, under an oscillatory electro-osmotic flow, is theoretically studied. Analytical solutions are found for the distribution of the electric potential, the velocity field and the concentration field. The time-averaged mass flux is then calculated in terms of an effective diffusion coefficient, or dispersion coefficient, akin to the classical Taylor–Aris dispersion. Calculations suggest that enhancement of mass transfer in dead-end pores, modelled as a closed-ended cylindrical tube, should be possible using an AC electric field under acceptable operating conditions, allowing, for example, up to a threefold enhancement in pores with a radius of 1 \(\upmu \)m.     

Electrothermal flow on electrodes arrays at physiological conductivities

AC electrothermal (ET) flow is inevitable for microfluidic systems dissipating electric energy in a conducting medium. Therefore, many practical applications of biomicrofluidics are prone to ET flow. Here, a series of observations are reported on ET flow in a microfluidic chamber that houses three electrode pairs. The observations indicate that the variations in liquid conductivity and channel height critically impact the structure and magnitude of the flow field. Observations indicate that after a critical conductivity a global ET flow is present in the chamber, while at lower conductivities a vortex is present at every electrode edge. In addition, no ET flow is observed when the chamber height is kept below a critical value at physiological conductivity (∼1.5 S/m). The experimental observations are compared with the numerical simulations of ET flow. The validity of the assumptions made in the current AC ET flow theory is also discussed in the light of the experimental data. The observations can be critical while designing microfluidic systems that involve power dissipation in conductive fluids.Inspec keywords: bioelectric phenomena, microfluidics, numerical analysis, bioMEMSOther keywords: electrode array, physiological conductivity, AC electrothermal flow, microfluidic system, electric energy, biomicrofluidics, microfluidic chamber, liquid conductivity, flow field structure, flow field magnitude, global ET flow, ET flow numerical simulation, AC ET flow theory, power dissipation, conductive fluid     

Microtubule alignment and manipulation using AC electrokinetics

The kinesin-microtubule system plays an important role in intracellular transport and is a model system for integrating biomotor-driven transport into microengineered devices. AC electrokinetics provides a novel tool for manipulating and organizing microtubules in solution, enabling new experimental geometries for investigating and controlling the interactions of microtubules and microtubule motors in vitro. By fabricating microelectrodes on glass substrates and generating AC electric fields across solutions of microtubules in low-ionic-strength buffers, bundles of microtubules are collected and aligned and the electrical properties of microtubules in solution are measured. The AC electric fields result in electro-osmotic flow, electrothermal flow, and dielectrophoresis of microtubules, which can be controlled by varying the solution conductivity, AC frequency, and electrode geometry. By mapping the solution conductivity and AC frequency over which positive dielectrophoresis occurs, the apparent conductivity of taxol-stabilized bovine-brain microtubules in PIPES buffer is measured to be 250 mS m(-1). By maximizing dielectrophoretic forces and minimizing electro-osmotic and electrothermal flow, microtubules are assembled into opposed asters. These experiments demonstrate that AC electrokinetics provides a powerful new tool for kinesin-driven transport applications and for investigating the role of microtubule motors in development and maintenance of the mitotic spindle.     

Electrokinetic injection techniques in microfluidic chips

The separation efficiency of a microfluidic chip is influenced to a significant degree by the flow field conditions within the injection microchannel. Therefore, an understanding of the physics of the flow within this channel is beneficial in the design and operation of such a system. The configuration of an injection system is determined by the volume of the sample plug that is to be delivered to the separation process. Accordingly, this paper addresses the design and testing of injection systems with a variety of configurations, including a simple cross, a double-T, and a triple-T configuration. This paper also presents the design of a unique multi-T injection configuration. Each injection system cycles through a predetermined series of steps, in which the electric field magnitude and distribution within the various channels is strictly manipulated, to effectuate a virtual valve. The uniquemulti-T configuration injection system presented within this paper has the ability to simulate the functions of the cross, double-T, and triple-T systems through appropriate manipulations of the electric field within its various channels. In other words, the proposed design successfully combines several conventional injection systems within a single microfluidic chip.     

Electrical control of individual droplet breaking and droplet contents extraction

The controllable extraction of the contents from an individual droplet is very important for the analysis and further processing of droplets. Most of the available methods lack the control and flexibility over the extraction of droplet contents. Here, we present a novel electrical-based method that can selectively break a droplet and extract its contents into aqueous buffer in a controllable manner on a microfluidic device. The device consisted of two layers, in which the top layer was modified to be hydrophobic for droplet generation and the bottom layer modified to be hydrophilic for maintaining aqueous buffer. A stable oil/water interface was formed at the intersection of the two layers where the oil and aqueous buffer met. When a droplet flew through the oil/water interface, a voltage was applied in the aqueous buffer. The generated electro-osmotic flow in the aqueous buffer and the electric field facilitated the breaking of the water/oil interface between the droplet and aqueous buffer, promoting the breaking of the droplet and a transient coalescence of the droplet with aqueous buffer. During the transient coalescence, droplet contents could be extracted into aqueous buffer. The amount of the droplet contents extracted into the aqueous buffer could be controlled by varying the strength of the electric field, and the droplet still existed and could be further processed after complete extraction of the droplet contents. This method could be used for droplet analysis and may provide a way to perform complex fluid handling in a droplet.     

Analyte distribution at channel intersections of electro-fluid-dynamic devices

Mass conservation is the guiding principle for analyte distribution at channel intersections of microfluidic devices, where analyte migration is mainly driven by an applied electric field, and in electro-fluid-dynamic (EFD) devices, where multiple fields and pressures can be applied simultaneously on the same channel network. This paper introduces another type of conservation, the conservation of effective volumetric flow rate, at channel intersections when the conductivity of the solution in the intersecting channels is maintained constant. This conservation principle provides an additional criterion needed to describe analyte migration in channels connecting to a common intersection and to predict how analyte is distributed into individual channels in the channel network of EFD devices, when multiple voltages and pressures are applied. The theoretical bases of effective volumetric flow rate balance are discussed, and the potential use of this principle in conjunction with the principle of mass conservation to predict the migration behavior of analytes is demonstrated. Junctions of different geometry in EFD devices are used to demonstrate the validity of these equations, and the measured velocities and numbers of microbeads in each channel agree with the predicted values.     

Integrated nanopore/microchannel devices for ac electrokinetic trapping of particles

We report integrated nanopore/microfluidic devices in which the unique combination of low pore density, conical nanopore membranes with microfluidic channels created addressable, localized high-field regions for electrophoretic and dielectrophoretic trapping of particles. A poly(ethylene terephthalate) track-etched membrane containing conical pores approximately 130 nm in diameter at the tip and approximately 1 microm in diameter at the base was used as an interconnect between two perpendicular poly(dimethylsiloxane) microfluidic channels. Integration of the nanopore membrane with microfluidic channels allowed for easy coupling of the electrical potentials and for directed transport of the analyte particles, 200 nm and 1 microm polystyrene microspheres and Caulobacter crescentus bacteria, to the trapping region. Square waves applied to the device generated electric field strengths up to 1.3 x 10(5) V/cm at the tips of the nanopores in the microchannel intersection. By varying the applied potentials from +/-10 to +/-100 V and exploring frequencies from dc to 100 kHz, we determined the contributions of electrophoretic and dielectrophoretic forces to the trapping and concentration process. These results suggest that tunable filter elements can be constructed in which the nanoporous elements provide a physical barrier and the applied ac field enhanced selectivity.     

Faceted design of channels for low-dispersion electrokinetic flows in microfluidic systems

A novel methodology for designing microfluidic channels for low-dispersion, electrokinetic flows is presented. The technique relies on trigonometric relations that apply for ideal electrokinetic flows, allowing faceted channels to be designed using common drafting software and a hand calculator. Flows are rotated and stretched along the abrupt interface between adjacent regions having differing specific permeability--a quantity with dimensions of length that we introduce to derive the governing equations. Two-interface systems are used to eliminate hydrodynamic rotation of bands injected into channels. Regions bounded by interfaces form faceted flow "prisms" with uniform velocity fields that can be combined with other prisms to obtain a wide range of turning angles and expansion ratios. Lengths of faceted prisms can be varied arbitrarily, simplifying chip layout and allowing the ability to reduce unwanted effects such as transverse diffusion and Joule heating for a given faceted prism. Designs are demonstrated using two-dimensional numerical solutions of the Laplace equation.     

Microvalves based on ionic polymer-metal composites for microfluidic application

Simple and highly efficient microvalve systems based on an ionic polymer-metal composite (IPMC) diaphragm actuator have been developed. The microvalve system that was fabricated in this work operates when open and close voltage is applied, due to the phenomena of lithium ion flux and the subsequent electro-osmotic drag of water to the cathode. IPMC was prepared by compositing with platinum nanoparticles on both sides of Nafion thin film. SEM images of the IPMC showed the high density and uniform size distribution of the Pt nanoparticles in the interpenetrating layer to ensure the proper performance of an IPMC actuator. The displacement of the IPMC for the microvalve was measured with a laser displacement meter. The application of open and close voltage made the operation of the valve faster. The fluorescence images of the flow in the fabricated IPMC-based microvalve system showed the successful operation of flow control in the microfluidic channel. The IPMC-based microvalve system shows a potential of IPMC for application as an actuator in microfluidic systems.     

Electro-osmotic transport in charged cylindrical micro- and nano-channels

Present paper deals with the electro-osmotic flow in a infinitely extended cylindrical micro- and nano-channel. The channel height is considered to be much less than the channel length. We consider a mixture of water or another neutral solvent and a salt compound such as sodium chloride for which the ionic species are entirely dissociated. We have developed a two-dimensional numerical model to analyze the flow characteristics and concentration distributions of a electro-osmotic flow without using the Debye-Hückel approximation. The governing system of equations consist of the mole fractions of ions, the potential and the fluid flow equations. Results are produced for the case, where the channel height is much greater than the width of the electric double layer (EDL) (micro-channel) and for the case where the channel height is of the order of the width of the EDL (nano-channel). For various values of mole fraction, we studied the electro-osmotic flow profiles and the potential distribution along the channel at different channel heights. In this case of steady flow the velocity field and the potential are identical. The electro-osmotic flow produces a uniform ‘plug profile’ at channel heights greater than 20 nm, which results in reduced sample species dispersion as compared to the velocity gradients associated with the pressure driven flows. Asymptotic solutions are obtained when the flow in a micro-channel is considered.     

Electrokinetic fluid control in two-dimensional planar microfluidic devices

We present microfluidic device designs with a two-dimensional planar format and methods to facilitate efficient sample transport along both dimensions. The basic device design consisted of a single channel for the first dimension which orthogonally intersected a high-aspect ratio second-dimension channel. To minimize dispersion of sample moving into and through the sample transfer region, control channels were placed on both sides of the first-dimension channel, and the electrokinetic flow from these control channels was used to confine the sample stream. We used SIMION and COMSOL simulations of the electric fields and fluid flow to guide device design. First, devices with one, two, and four control channels were fabricated and tested, and four control channels provided the most effective sample confinement. The designs were evaluated by measuring the sample stream widths and concentration to width ratios as a function of the electric field strength ratio in the control channels and first-dimension (1D) channel (EC/E1D). Next, both a single open channel and an array of parallel channels were tested for the second dimension, and improved performance was observed for the parallel channel design, with stream widths as narrow as 120 microm. The ease with which fluids could be introduced into both the first and second dimensions was also illustrated. Sample plugs injected into the planar region were confined as effectively as sample streams and were easily routed into the planar region by reconfiguring the applied potentials.     

Formation of stable stacking zones in a flow stream for sample immobilization in microfluidic systems

Electrocapture is a multifunctional microfluidic tool that can be used for concentration, sample cleanup, multistep reactions, and separation of biomolecules. Herein, we investigate the mechanisms underlying the electrocapture principle. A microfluidic electrocapture device was found to be capable of generating regions of different electric field, which are maintained in the flow by electric and hydrodynamic forces, with the zones of lower electric field strength upstream of those with higher strength. In addition to detection of the local electric fields by direct measurements, the existence of the zones was observed by the capture of a solution containing Coomassie and myoglobin. The two molecules were captured at different spots in a steady-state manner and were released (separated) at different electric fields. Considering these observations and the experimental values for the electric field strengths, flow velocities, and electrophoretic mobilities of DNA, proteins, and peptides, it is concluded that the macromolecules are captured between the field zones by a stacking mechanism.     

Electrokinetic focusing injection methods on microfluidic devices

This paper presents an experimental and numerical investigation into electrokinetic focusing injection on microfluidic chips. The valving characteristics on microfluidic devices are controlled through appropriate manipulations of the electric potential strengths during the sample loading and dispensing steps. The present study also addresses the design and testing of various injection systems used to deliver a sample plug. A novel double-cross injection microfluidic chip is fabricated, which employs electrokinetic focusing to deliver sample plugs of variable volume. The proposed design combines several functions of traditional sample plug injection systems on a single microfluidic chip. The injection technique uses an unique sequence of loading steps with different electric potential distributions and magnitudes within the various channels to effectuate a virtual valve.     

On-chip microfluidic transport and mixing using electrowetting and incorporation of sensing functions

An integrated system was developed that performs microfluidic transport, mixing, and sensing on a single chip. The operation principle for the microfluidic transport was based on electrowetting. A solution to be transported was confined in a space between a row of gold working electrodes and a protruding poly(dimethylsiloxane) (PDMS) structure. When a negative potential was applied to one of the gold working electrodes, it became hydrophilic, and the solution was transported through the flow channel. The solution could be transported in any desired direction in a network of flow channels by switching on necessary electrodes one by one. Furthermore, two solutions transported through two flow channels could be mixed using a mixing electrode based on the same principle. To demonstrate the applicability of a lab-on-a-chip, an air gap ammonia electrode was integrated by taking advantage of the open structure of the flow channel. Gaseous ammonia that was produced after pH adjustment and diffused through an air gap caused a pH change in the electrolyte layer, which was measured with an iridium oxide pH indicator electrode. The 90% response time was less than 1 min for the millimolar order of ammonia. The calibration curve was linear down to 10 microM. The ammonia-sensing system was also applied to construct biosensing systems for urea and creatinine. A linear relationship was observed between the potential and the logarithm of the concentration of the analytes down to 50 microM for both urea and creatinine. The developed microfluidic system can be a basic building block for future systems.     

High Throughput‐Per‐Footprint Inertial Focusing

Matching the scale of microfluidic flow systems with that of microelectronic chips for realizing monolithically integrated systems still needs to be accomplished. However, this is appealing only if such re‐scaling does not compromise the fluidic throughput. This is related to the fact that the cost of microelectronic circuits primarily depends on the layout footprint, while the performance of many microfluidic systems, like flow cytometers, is measured by the throughput. The simple operation of inertial particle focusing makes it a promising technique for use in such integrated flow cytometer applications, however, microfluidic footprints demonstrated so far preclude monolithic integration. Here, the scaling limits of throughput‐per‐footprint (TPFP) in using inertial focusing are explored by studying the interplay between theory, the effect of channel Reynolds numbers up to 1500 on focusing, the entry length for the laminar flow to develop, and pressure resistance of the microchannels. Inertial particle focusing is demonstrated with a TPFP up to 0.3 L/(min cm²) in high aspect‐ratio rectangular microfluidic channels that are readily fabricated with a post‐CMOS integratable process, suggesting at least a 100‐fold improvement compared to previously demonstrated techniques. Not only can this be an enabling technology for realizing cost‐effective monolithically integrated flow cytometry devices, but the methodology represented here can also open perspectives for miniaturization of many biomedical microfluidic applications requiring monolithic integration with microelectronics without compromising the throughput.