AC Electrospraying & Electrospinning
AC Electrospraying & Electrospinning
Electrospraying or electrohydrodynamic atomisation using high frequency (>10 kHz) electric fields exhibit significantly distinct behaviour compared to DC or low frequency AC electrosprays. For moderately high conductivity fluids, the characteristic sharp conical meniscus, known as the Taylor cone, in DC electrosprays is not observed. Instead, the meniscus resonates vigorously at a frequency corresponding to the inverse of the capillary-inertia time scale, periodically ejecting droplets via a tip streaming mechanism or from the tip of a long slender microjet. Due to the high frequency of polarity reversal, there is insufficient time for charge separation and subsequently double layer tangential conduction to occur within the meniscus. As such, there is no charge accumulation at the meniscus tip to produce the focussing mechanism for the formation of a sharp conical shape. In addition, a consequence of this is that the 1-10 μm order ejected drops do not carry net charge. These electroneutral drops, which are of the correct size for maximum dosage, is therefore suitable for pulmonary drug delivery, wherein charge drops which lead to surface adsorption and compound ionisation effects are undesirable. The absence of charge also renders the current and hence power requirement for the device low, which then makes the device suitable for miniaturisation.
1.LY Yeo, D Lastochkin, S-C Wang, H-C Chang. A New AC Electrospray Mechanism by Maxwell-Wagner Polarization and Capillary Resonance. Phys Rev Lett 92, 133902 (2004) (PDF).
2.LY Yeo, Z Gagnon, H-C Chang. AC Electrospray Biomaterials Synthesis. Biomaterials 26, 6122 (2005) (PDF).
3.LY Yeo, JR Friend. Electrospinning Carbon Nanotube Polymer Composite Nanofibers. J Exp Nanosci 1, 177 (2006) (PDF).
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