This Blog Deals With Electrowetting

Electrowetting

Electrowetting is the modification of the wetting properties of a hydrophobic surface with an appliedelectric field.

The electrowetting behavior of mercury and other liquids on variably charged surfaces was probably first explained by Gabriel Lippmann in 1875 and was certainly observed much earlier. Froumkin used surface charge to change the shape of water drops in 1936. The term electrowetting was first introduced in 1981 to describe an effect proposed for designing a new type of display device ^[1]. The "fluid transistor" was first investigated by J. Brown in 1984-1988 under NSF Grants 8760730 & 8822197 ^[2], employing insulating dielectric and hydrophobic layers, immiscible fluids, DC or RF power; and mass arrays of miniature interleaved electrodes with large or matching Indium tin oxide (ITO) electrodes to digitally relocate nano droplets and control fluid flow electronically or optically.^[3] Electrowetting using an insulating layer on top of the bare electrodes was also studied by Bruno Berge in 1993 ^[4]. Electrowetting has since been commercialized for manipulation of droplets by Pollack et al at Duke University in 2000.^[5] By digitizing a large, insulator-coated working electrode into smaller electrodes and placing an ITO-coated, transparent glass plate as the counter electrode on top to sandwich the droplets. Because the liquid is discretized and programmably manipulated, this approach was called “Digital Microfluidics” History

Since then, a large number of applications based on electrowetting have been demonstrated. Currently five companies are at the forefront in commercializing electrowetting-based applications based on Cytonix ^[7]and Berge's later research: Clinical diagnostics by Advanced Liquid Logic^[8] which was spun out of Duke University, electronic paper by both Gamma Dynamics ^[9], which was spun out of the University of Cincinnati, and LiquaVista ^[10] which was spun out of Philips Research, liquid lenses by Varioptic^[11], andDigital PCR by Life Technologies and Sequenom. In some of these applications, electrowetting allows large numbers of droplets to be independently manipulated under direct electrical control without the use of external pumps, valves or even fixed channels. In e-paper and liquid lenses, droplets are manipulated in-place whereas in clinical diagnostics applications, droplets are moved around on the platform.

[edit]Electrowetting theory

The electrowetting effect has been defined as "the change in solid-electrolyte contact angle due to an applied potential difference between the solid and the electrolyte". The phenomenon of electrowetting can be understood in terms of the forces that result from the applied electric field.^[12][13] The fringing field at the corners of the electrolyte droplet tend to pull the droplet down onto the electrode, lowering the macroscopic contact angle and increasing the droplet contact area. Alternatively, electrowetting can be viewed from a thermodynamic perspective. Since the surface tension of an interface is defined as the Gibbs free energyrequired to create a certain area of that surface, it contains both chemical and electrical components, and charge becomes a significant term in that equation. The chemical component is just the natural surface tension of the solid/electrolyte interface with no electric field. The electrical component is the energy stored in the capacitor formed between the conductor and the electrolyte.

The simplest derivation of electrowetting behavior is given by considering its thermodynamic model. While it is possible to obtain a detailed numerical model of electrowetting by considering the precise shape of the electrical fringing field and how it affects the local droplet curvature, such solutions are mathematically and computationally complex. The thermodynamic derivation proceeds as follows. Defining the relevant surface tensions as:

 - The total, electrical and chemical, surface tension between the electrolyte and the conductor

 - The surface tension between the electrolyte and the conductor at zero electric field

 - The surface tension between the conductor and the external ambient

 - The surface tension between the electrolyte and the external ambient

θ - The macroscopic contact angle between the electrolyte and the dielectric

C - The capacitance of the interface, є_rє₀/t, for a uniform dielectric of thickness t and permittivity є_r

V - The effective applied voltage, integral of the electric field from the electrolyte to the conductor

Relating the total surface tension to its chemical and electrical components gives:

The contact angle is given by the Young-Dupre equation, with the only complication being that the total surface energy γ_ws is used:

Combining the two equations gives the dependence of θ on the effective applied voltage as:

An additional complication is that liquids also exhibit a saturation phenomena: after certain voltage, the saturation voltage, the further increase of voltage will not change the contact angle, and with extreme voltages the interface will only show instabilities.

However, surface charge is but one component of surface energy, and other components are certainly perturbed by induced charge. So, a complete explanation of electrowetting is unquantified, but it should not be surprising that these limits exist.

[edit]Materials

For reasons that are still under investigation, only a limited set of surfaces exhibit the theoretically predicted electrowetting behavior. Amorphous fluoropolymers are by far the best electrowetting materials discovered so far, and it has been found that their behaviour can be enhanced by the appropriate patterning. Three types of such polymers are commercially available: FluoroPel hydrophobic and superhydrophobic V-series polymers are sold by Cytonix, CYTOP is sold by Asahi Glass Co., and Teflon AF is sold by DuPont.

[edit]Applications

Electrowetting is now used in a wide range of applications from modulab to adjustable lenses, electronic displays (e-paper) and switches for optical fibers.