Optoelectrowetting

Last updated

Optoelectrowetting (OEW) is a method of liquid droplet manipulation used in microfluidics applications. This technique builds on the principle of electrowetting, which has proven useful in liquid actuation due to fast switching response times and low power consumption. Where traditional electrowetting runs into challenges, however, such as in the simultaneous manipulation of multiple droplets, OEW presents a lucrative alternative that is both simpler and cheaper to produce. OEW surfaces are easy to fabricate, since they require no lithography, and have real-time, reconfigurable, large-scale manipulation control, due to its reaction to light intensity.

Contents

Theory

The traditional electrowetting mechanism has been receiving increasing interest due to its ability to control tension forces on a liquid droplet. As surface tension acts as the dominant liquid actuation force in nano-scale applications, electrowetting has been used to modify this tension at the solid-liquid interface through the application of an external voltage. The applied electric field causes a change in the contact angle of the liquid droplet, and in turn changes the surface tensions across the droplet. Precise manipulation of the electric field allows control of the droplets. The droplet is placed on an insulating substrate located in between an electrode.

Optoelectrowetting against traditional electrowetting diagram OEW diagram.png
Optoelectrowetting against traditional electrowetting diagram

The optoelectrowetting mechanism adds a photoconductor underneath the conventional electrowetting circuit, with an AC power source attached. Under normal (dark) conditions, the majority of the system's impedance lies in the photoconducting region, and therefore the majority of the voltage drop occurs here. However, when light is shined on the system, carrier generation and recombination causes the conductivity of the photoconductor spikes and results in a voltage drop across the insulating layer, changing the contact angle as a function of the voltage. The contact angle between a liquid and electrode can be described as: [1]


where VA, d, ε, and γLV are applied voltage, thickness of the insulation layer, dielectric constant of the insulation layer, and the interfacial tension constant between liquid and gas. In AC situations, such as OEW, VA is replaced with the RMS voltage. The frequency of the AC power source is adjusted so that the impedance of the photoconductor dominates in the dark state. The shift in the voltage drop across the insulating layer therefore reduces the contact angle of the droplet as a function of the light intensity. By shining an optical beam on one edge of a liquid droplet, the reduced contact angle creates a pressure difference throughout the droplet, and pushes the droplet's center of mass towards the illuminated side. Control of the optical beam results in control of the droplet's movement.

Using 4 mW laser beams, OEW has proven to move droplets of deionized water at speeds of 7mm/s.

Traditional electrowetting runs into problems because it requires a two-dimensional array of electrodes for droplet actuation. The large number of electrodes leads to complexity for both control and packaging of these chips, especially for droplet sizes of smaller scales. While this problem can be solved through integration of electronic decoders, the cost of the chip would significantly increase. [2] [3]

Single-sided continuous optoelectrowetting (SCOEW)

Droplet manipulation in electrowetting-based devices are usually accomplished using two parallel plates which sandwiches the droplet and is actuated by digital electrodes. The minimum droplet size that can be manipulated is determined by the size of pixilated electrodes. This mechanism provides a solution to the size limitation of physical pixilated electrodes by utilizing dynamic and reconfigurable optical patterns and enables operations such as continuous transport, splitting, merging, and mixing of droplets. SCOEW is conducted on open, featureless, and photoconductive surfaces. This configuration creates a flexible interface that allows simple integration with other microfluidic components, such as sample reservoirs through simple tubing. [4]

It is also known as open optoelectrowetting (O-OEW). [5]

Optoelectrowetting using a photocapacitance

Optoelectrowetting can also be achieved using the photocapacitance in a liquid-insulator-semiconductor junction. [6] The photo-sensitive electrowetting is achieved via optical modulation of carriers in the space charge region at the insulator-semiconductor junction which acts as a photodiode – similar to a charge-coupled device based on a metal-oxide-semiconductor.

Types of applications

Clinical diagnostics

Electrowetting presents a solution to one of the most challenging tasks in lab-on-a-chip systems in its ability to handle and manipulate complete physiological compounds. [7] Conventional microfluidic systems aren't easily adaptable to handle different compounds, requiring reconfiguration that often results in the device being impractical as a whole. Through OEW, a chip with one power source can be readily used with a variety of substances, with potential for multiplexed detection.

Optical actuation

Photoactuation in microelectromechanical systems (MEMS) has been demonstrated in proof-of-concept experiments. [8] [9] Instead of a typical substrate, a specialized cantilever is placed on top of the liquid-insulator-photoconductor stack. As light is shined on the photoconductor, the capillary force from the drop on the cantilever changes with the contact angle, and deflects the beam. This wireless actuation can be used as a substitute for complex circuit-based systems currently used for optical addressing and control of autonomous wireless sensors [10]

See also

Related Research Articles

Hydrophobe molecule or surface that has no attraction to water

In chemistry, hydrophobicity is the physical property of a molecule that is seemingly repelled from a mass of water. In contrast, hydrophiles are attracted to water.

Microfluidics refers to the behaviour, precise control, and manipulation of fluids that are geometrically constrained to a small scale at which surface forces dominate volumetric forces. It is a multidisciplinary field that involves engineering, physics, chemistry, biochemistry, nanotechnology, and biotechnology. It has practical applications in the design of systems that process low volumes of fluids to achieve multiplexing, automation, and high-throughput screening. Microfluidics emerged in the beginning of the 1980s and is used in the development of inkjet printheads, DNA chips, lab-on-a-chip technology, micro-propulsion, and micro-thermal technologies.

MOSFET Transistor used for amplifying or switching electronic signals.

The metal–oxide–semiconductor field-effect transistor, also known as the metal–oxide–silicon transistor, is a type of insulated-gate field-effect transistor that is fabricated by the controlled oxidation of a semiconductor, typically silicon. The voltage of the covered gate determines the electrical conductivity of the device; this ability to change conductivity with the amount of applied voltage can be used for amplifying or switching electronic signals.

Digital microfluidics

Digital microfluidics (DMF) is another platform for lab-on-a-chip systems that is based upon the manipulation of microdroplets. Droplets are dispensed, moved, stored, mixed, reacted, or analyzed on a platform with a set of insulated electrodes. Digital microfluidics can be used together with analytical analysis procedures such as mass spectrometry, colorimetry, electrochemical, and electrochemiluminescense.

Surface acoustic wave

A surface acoustic wave (SAW) is an acoustic wave traveling along the surface of a material exhibiting elasticity, with an amplitude that typically decays exponentially with depth into the material.

Electrowetting is the modification of the wetting properties of a surface with an applied electric field.

Deep-level transient spectroscopy (DLTS) is an experimental tool for studying electrically active defects in semiconductors. DLTS establishes fundamental defect parameters and measures their concentration in the material. Some of the parameters are considered as defect "finger prints" used for their identifications and analysis.

Contact angle

The contact angle is the angle, conventionally measured through the liquid, where a liquid–vapor interface meets a solid surface. It quantifies the wettability of a solid surface by a liquid via the Young equation. A given system of solid, liquid, and vapor at a given temperature and pressure has a unique equilibrium contact angle. However, in practice a dynamic phenomenon of contact angle hysteresis is often observed, ranging from the advancing (maximal) contact angle to the receding (minimal) contact angle. The equilibrium contact is within those values, and can be calculated from them. The equilibrium contact angle reflects the relative strength of the liquid, solid, and vapour molecular interaction.

ISFET

An ion-sensitive field-effect transistor (ISFET) is a field-effect transistor used for measuring ion concentrations in solution; when the ion concentration (such as H+, see pH scale) changes, the current through the transistor will change accordingly. Here, the solution is used as the gate electrode. A voltage between substrate and oxide surfaces arises due to an ion sheath. It is a special type of MOSFET (metal-oxide-semiconductor field-effect transistor), and shares the same basic structure, but with the metal gate replaced by an ion-sensitive membrane, electrolyte solution and reference electrode. Invented in 1970, the ISFET was the first biosensor FET (BioFET).

The name electrospray is used for an apparatus that employs electricity to disperse a liquid or for the fine aerosol resulting from this process. High voltage is applied to a liquid supplied through an emitter. Ideally the liquid reaching the emitter tip forms a Taylor cone, which emits a liquid jet through its apex. Varicose waves on the surface of the jet lead to the formation of small and highly charged liquid droplets, which are radially dispersed due to Coulomb repulsion.

Ultrahydrophobicity Material property

Ultrahydrophobic surfaces are highly hydrophobic, i.e., extremely difficult to wet. The contact angles of a water droplet on an ultrahydrophobic material exceed 150°. This is also referred to as the lotus effect, after the superhydrophobic leaves of the lotus plant. A droplet striking these kinds of surfaces can fully rebound like an elastic ball. Interactions of bouncing drops can be further reduced using special superhydrophobic surfaces that promote symmetry breaking, pancake bouncing or waterbowl bouncing.

Bio-MEMS

Bio-MEMS is an abbreviation for biomedical microelectromechanical systems. Bio-MEMS have considerable overlap, and is sometimes considered synonymous, with lab-on-a-chip (LOC) and micro total analysis systems (μTAS). Bio-MEMS is typically more focused on mechanical parts and microfabrication technologies made suitable for biological applications. On the other hand, lab-on-a-chip is concerned with miniaturization and integration of laboratory processes and experiments into single chips. In this definition, lab-on-a-chip devices do not strictly have biological applications, although most do or are amenable to be adapted for biological purposes. Similarly, micro total analysis systems may not have biological applications in mind, and are usually dedicated to chemical analysis. A broad definition for bio-MEMS can be used to refer to the science and technology of operating at the microscale for biological and biomedical applications, which may or may not include any electronic or mechanical functions. The interdisciplinary nature of bio-MEMS combines material sciences, clinical sciences, medicine, surgery, electrical engineering, mechanical engineering, optical engineering, chemical engineering, and biomedical engineering. Some of its major applications include genomics, proteomics, molecular diagnostics, point-of-care diagnostics, tissue engineering, single cell analysis and implantable microdevices.

The UBC Okanagan Digital Microfluidics Research Group is an interdisciplinary research group at University of British Columbia Okanagan that develops integrated devices for biochip applications. Lab-on-a-chip digital microfluidic devices are fabricated in digital architectures that merge micrometre-scale electrical circuitry with applications requiring dynamic fluid control, as voltage actuation signals from patterned electrodes are used to direct and actuate fluid flow within the chips. The structures are not application-specific. Fluid actuation signals for droplet mixing, splitting, and routing are set by the control software and can be reconfigured as needed and in real-time.

Centrifugal micro-fluidic biochip

The centrifugal micro-fluidic biochip or centrifugal micro-fluidic biodisk is a type of lab-on-a-chip technology, also known as lab-on-a-disc, that can be used to integrate processes such as separating, mixing, reaction and detecting molecules of nano-size in a single piece of platform, including a compact disk or DVD. This type of micro-fluidic biochip is based upon the principle of microfluidics; to take advantage of noninertial pumping for lab-on-a-chip devices using noninertial valves and switches under centrifugal force and Coriolis effect to distribute fluids about the disks in a highly parallel order.

Photoelectrowetting

Photoelectrowetting is a modification of the wetting properties of a surface using incident light.

Bio-FET

A field-effect transistor-based biosensor, also known as a biosensor field-effect transistor, field-effect biosensor (FEB), or biosensor MOSFET, is a field-effect transistor that is gated by changes in the surface potential induced by the binding of molecules. When charged molecules, such as biomolecules, bind to the FET gate, which is usually a dielectric material, they can change the charge distribution of the underlying semiconductor material resulting in a change in conductance of the FET channel. A Bio-FET consists of two main compartments: one is the biological recognition element and the other is the field-effect transistor. The BioFET structure is largely based on the ion-sensitive field-effect transistor (ISFET), a type of metal-oxide-semiconductor field-effect transistor (MOSFET) where the metal gate is replaced by an ion-sensitive membrane, electrolyte solution and reference electrode.

Droplet-based microfluidics manipulate discrete volumes of fluids in immiscible phases with low Reynolds number and laminar flow regimes. Interest in droplet-based microfluidics systems has been growing substantially in past decades. Microdroplets offer the feasibility of handling miniature volumes of fluids conveniently, provide better mixing, encapsulation, sorting, sensing and are suitable for high throughput experiments. Two immiscible phases used for the droplet based systems are referred to as the continuous phase and dispersed phase.

Paper-based microfluidics are microfluidic devices that consist of a series of hydrophilic cellulose or nitrocellulose fibers that guide liquid from an inlet to a desired outlet by imbibition. The technology builds on the conventional lateral flow test which is capable of detecting many infections agents and chemical contaminants. The main advantage of this is that it is largely a passively controlled device unlike more complex microfluidic devices. Development of paper-based microfluidic devices began in the early 21st century to meet a need for inexpensive and portable medical diagnostic systems.

Microfluidics refers to the flow of fluid in channels or networks with at least one dimension on the micron scale. In open microfluidics, also referred to as open surface microfluidics or open-space microfluidics, at least one boundary confining the fluid flow of a system is removed, exposing the fluid to air or another interface such as a second fluid.

Robin L. Garrell American chemist

Robin L. Garrell is an American chemist, academic and current President of The Graduate Center, CUNY. Until 2020, Garrell served as Vice Provost for Graduate Education and Dean of Graduate Division at University of California, Los Angeles (UCLA). Prior to this role, Garrell was assistant professor at the University of Pittsburgh from 1984 to 1991, then joined the faculty in the Department of Chemistry and Biochemistry at UCLA, where she became full professor and held a joint appointment in Bioengineering. Garrell assumed her current position at The Graduate Center on August 1, 2020.

References

  1. Need citation
  2. Pollack, Michael G.; Fair, Richard B.; Shenderov, Alexander D. (2000-09-11). "Electrowetting-based actuation of liquid droplets for microfluidic applications". Applied Physics Letters. AIP Publishing. 77 (11): 1725–1726. Bibcode:2000ApPhL..77.1725P. doi:10.1063/1.1308534. ISSN   0003-6951.
  3. Chiou, Pei Yu; Moon, Hyejin; Toshiyoshi, Hiroshi; Kim, Chang-Jin; Wu, Ming C. (2003). "Light actuation of liquid by optoelectrowetting". Sensors and Actuators A: Physical. Elsevier BV. 104 (3): 222–228. doi:10.1016/s0924-4247(03)00024-4. ISSN   0924-4247.
  4. Park, Sung-Yong; Teitell, Michael A.; Chiou, Eric P. Y. (2010). "Single-sided continuous optoelectrowetting (SCOEW) for droplet manipulation with light patterns". Lab on a Chip. Royal Society of Chemistry (RSC). 10 (13): 1655–61. doi:10.1039/c001324b. ISSN   1473-0197. PMID   20448870.
  5. Chuang, Han-Sheng; Kumar, Aloke; Wereley, Steven T. (2008-08-11). "Open optoelectrowetting droplet actuation". Applied Physics Letters. AIP Publishing. 93 (6): 064104. Bibcode:2008ApPhL..93f4104C. doi:10.1063/1.2970047. ISSN   0003-6951.
  6. Arscott, Steve (2011). "Moving liquids with light: Photoelectrowetting on semiconductors". Scientific Reports. 1 (1): 184. arXiv: 1108.4935 . Bibcode:2011NatSR...1E.184A. doi: 10.1038/srep00184 . ISSN   2045-2322. PMC   3240946 . PMID   22355699.
  7. Srinivasan, Vijay; Pamula, Vamsee K.; Fair, Richard B. (2004). "An integrated digital microfluidic lab-on-a-chip for clinical diagnostics on human physiological fluids". Lab on a Chip. Royal Society of Chemistry (RSC). 4 (4): 310–5. doi:10.1039/b403341h. ISSN   1473-0197. PMID   15269796.
  8. Gaudet, Matthieu; Arscott, Steve (2012-05-28). "Optical actuation of microelectromechanical systems using photoelectrowetting". Applied Physics Letters. 100 (22): 224103. arXiv: 1201.2873 . Bibcode:2012ApPhL.100v4103G. doi:10.1063/1.4723569. ISSN   0003-6951. S2CID   119208424.
  9. Bob Yirka (2012-01-02). "Research team creates photoelectrowetting circuit". Phys.org. Retrieved 2020-02-27.
  10. Yick, Jennifer; Mukherjee, Biswanath; Ghosal, Dipak (2008). "Wireless sensor network survey". Computer Networks. Elsevier BV. 52 (12): 2292–2330. doi:10.1016/j.comnet.2008.04.002. ISSN   1389-1286.