Abstract:Whether an electrified jet breaks up whilst the jet maintains a straight line (varicose), or alternatively the jet trajectory becomes chaotic (whipping), depends on the competition of the interfacial forces. Starting from the competition of normal stresses on the jet surface, we derive scaling laws in different electro-hydrodynamic operating regimes as a function of fluid properties and the flow rate. The onset of whipping occurs when this scaling function reaches a threshold, which is independent of the elect… Show more
The rapid development of fascinating new optoelectronic materials and devices calls for innovative production of micro/nanostructures in a high-resolution, large-scale, low-cost fashion, preferably compatible with flexible/wearable applications. Powerful electrohydrodynamic (EHD)...
The rapid development of fascinating new optoelectronic materials and devices calls for innovative production of micro/nanostructures in a high-resolution, large-scale, low-cost fashion, preferably compatible with flexible/wearable applications. Powerful electrohydrodynamic (EHD)...
“…In the latter system, sequential images are taken with incremental trigger delay to observe the phenomena and take measurements with time interval of the order of 10 µs [75]. This provides an inexpensive visualizing system which has been used, for instance, to study the role of capillary waves in the break-up regimes of electrified jet [29] and to measure the jet break-up length [28].…”
Section: Techniques To Detect Wavesmentioning
confidence: 99%
“…The surface elasticity has been introduced only relatively recently to the dispersion condition of jet waves by Noskov [1], who derived an equation that corrects Bohr's formula [87] used for the determination of the surface tension from the wave characteristics. Another important field of investigation are waves on charged surfaces, jets and droplets, which have important role in electrojetting (see, e.g., [28,29]). To characterize capillary waves, we built our own apparatus and developed a code to process the wave images captured in the experiment.…”
Section: Flat Waves On a Surface Covered With A Surfactantmentioning
confidence: 99%
“…As a result, the fundamental understanding of the wave growth is essential for the control of the destabilization of multi-phase systems. The growth rate of waves at the surface of an electrified jet can be used to estimate the break-up length [28] and understand the transition from varicose to whipping instabilities in electrohydrodynamic jetting [29]. The ripples play a role in a number of surface phenomena, sometimes in a nonintuitive way.…”
The methods to study capillary waves have been reviewed, together with the emerging practical applications of theirs and new theoretical developments in the field. The focus is on monochromatic ripples of frequency in the range 0.1-10 kHz. A capillary wave apparatus has been constructed that combines several recent advances on the technique. It is based on profilometry of waves decaying with distance, with a highspeed video camera detecting light refracted by the surface. A code to process the images has been developed that executes a regression analysis to determine the characteristics of the wave. High precision and accuracy have been achieved: standard deviation from the mean of ±0.5% for the wavelength and ±7% for the decay length; mean deviations from the theoretical values ±0.2% for the wavelength and ±5% for the decay length. An analytic approximation for the dispersion relation has been used to determine the Gibbs elasticity of a surfactant monolayer from the data for decay length vs. frequency. The elasticity of an octanol monolayer has been determined with precision of ±1 mN/m, in excellent agreement with the theoretical value. Surface tension can be measured from the wavelength data with precision of ±0.3 mN/m. It has been demonstrated that the effect of the surface elasticity on the wavelength is significant and accurate wavelength data can actually be used to determine the elasticity if the surface tension is known.
“…52). Using the scaling laws (72), Xia et al (2019) have found experimentally that whipping arises in the cone-jet mode of electrospray when the dimensionless number G = Γ 2 e δ 1/3 µ takes values above the threshold G 155.…”
IV. Results of spatio-temporal and global stability analyses A. Convective-to-absolute instability transition B. Global stability V. Capillary instabilities A. End-pinching instability B. Rayleigh instability C. Rayleigh stability analysis D. Boundary layer and viscosity effects E. Confinement effects F. Compound jets G. Viscoelasticity effects H. Electrified jets
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