Abstract:Active, tunable,
and reversible opening and closing of particle
shells on droplets may facilitate chemical reactions in droplets and
enable various small-scale laboratory operations, including online
detection, measurement, and adjustment of droplet liquid. Manipulating
various types of particle shells in a controlled manner requires new
routes. This work provides a new strategy for controlling the spatial
arrangement of particle-covered oil droplets using electric fields
that expands the application of respon… Show more
“…Manipulating particles anchored on the droplet interface is one of the promised techniques for designing functional droplet. Using active structuring of a particle-covered droplet under the electric field, Rozynek et al demonstrated a millimeter-sized optical diaphragm [ 162 ] ( Figure 10 E). Li et al redistributed aluminum nanoparticles on an o/w emulsion droplet via an electric field for generating a Janus droplet [ 163 ] ( Figure 10 F).…”
Section: Applicationsmentioning
confidence: 99%
“…( D ) Stabilizing the shape of deformed colloidal particles by the interfacial jamming of nanoparticles [ 121 ]. ( E ) Optical diaphragm based on the particle self-assembly [ 162 ]. ( F ) Generation of an aluminum Janus particle using an electric field [ 163 ].…”
The field of droplet electrohydrodynamics (EHD) emerged with a seminal work of G.I. Taylor in 1966, who presented the so-called leaky dielectric model (LDM) to predict the droplet shapes undergoing distortions under an electric field. Since then, the droplet EHD has evolved in many ways over the next 55 years with numerous intriguing phenomena reported, such as tip and equatorial streaming, Quincke rotation, double droplet breakup modes, particle assemblies at the emulsion interface, and many more. These phenomena have a potential of vast applications in different areas of science and technology. This paper presents a review of prominent droplet EHD studies pertaining to the essential physical insight of various EHD phenomena. Here, we discuss the dynamics of a single-phase emulsion droplet under weak and strong electric fields. Moreover, the effect of the presence of particles and surfactants at the emulsion interface is covered in detail. Furthermore, the EHD of multi-phase double emulsion droplet is included. We focus on features such as deformation, instabilities, and breakups under varying electrical and physical properties. At the end of the review, we also discuss the potential applications of droplet EHD and various challenges with their future perspectives.
“…Manipulating particles anchored on the droplet interface is one of the promised techniques for designing functional droplet. Using active structuring of a particle-covered droplet under the electric field, Rozynek et al demonstrated a millimeter-sized optical diaphragm [ 162 ] ( Figure 10 E). Li et al redistributed aluminum nanoparticles on an o/w emulsion droplet via an electric field for generating a Janus droplet [ 163 ] ( Figure 10 F).…”
Section: Applicationsmentioning
confidence: 99%
“…( D ) Stabilizing the shape of deformed colloidal particles by the interfacial jamming of nanoparticles [ 121 ]. ( E ) Optical diaphragm based on the particle self-assembly [ 162 ]. ( F ) Generation of an aluminum Janus particle using an electric field [ 163 ].…”
The field of droplet electrohydrodynamics (EHD) emerged with a seminal work of G.I. Taylor in 1966, who presented the so-called leaky dielectric model (LDM) to predict the droplet shapes undergoing distortions under an electric field. Since then, the droplet EHD has evolved in many ways over the next 55 years with numerous intriguing phenomena reported, such as tip and equatorial streaming, Quincke rotation, double droplet breakup modes, particle assemblies at the emulsion interface, and many more. These phenomena have a potential of vast applications in different areas of science and technology. This paper presents a review of prominent droplet EHD studies pertaining to the essential physical insight of various EHD phenomena. Here, we discuss the dynamics of a single-phase emulsion droplet under weak and strong electric fields. Moreover, the effect of the presence of particles and surfactants at the emulsion interface is covered in detail. Furthermore, the EHD of multi-phase double emulsion droplet is included. We focus on features such as deformation, instabilities, and breakups under varying electrical and physical properties. At the end of the review, we also discuss the potential applications of droplet EHD and various challenges with their future perspectives.
“…14,15 Moreover, particle-covered droplets facilitate the fabrication of new materials [16][17][18] and can be designed to form novel adaptive structures. 19,20 Pickering droplets can also be used in basic research, e.g., as model systems for mimicking the physical properties of red blood cells 21 or for studying particle crystal growth and ordering or particle layer buckling on curved interfaces. [22][23][24][25][26] In many research areas, knowledge of the stability and mechanics of an individual Pickering droplet is essential, e.g., for the efficient fabrication of Pickering emulsions, 27 for designing emulsions with controlled stability, 28,29 and, in general, for the further development of the abovementioned research fields.…”
We studied the behavior of a nonspherical Pickering droplet subjected to an electric stress. We explained the effect of droplet geometry, particle size, and electric field strength, on the deformation and collapsing of particle-covered droplets.
“…Along with other "smart" materials, ERFs are widely used in technology in various devices such as shock absorbers, control valves, dampers and in microfluidics, robotics, sensors, etc [2]. The modern applications of the ER effect include sensors for rapid plague diagnostics and nanodiaphragms with adjustable aperture [3,4]. The several qualities are essential to the wide practical application of ERFs, namely significant change of rheological properties under electric field, low conductivity, chemical, aggregate and thermal stability.…”
Исследовано электрореологическое поведение суспензий галлуазита в полидиметилсилоксане с кинематической вязкостью 50, 100 и 400 сСт, концентрация наполнителя составляла 4 и 8 масс.%. Исследуемые суспензии являются электрореологическими жидкостями: под действием электрического поля все образцы проявляют вязкоупругие свойства, и значения предела текучести существенно возрастают. Изменение реологического поведения суспензий связано с образованием протяженных колончатых структур из частиц наполнителя вдоль силовых линий электрического поля. В работе изучена зависимость интенсивности электрореологического эффекта от напряженности электрического поля, концентрации наполнителя и вязкости дисперсионной среды. Показано, что значения предела текучести увеличиваются с возрастанием напряженности электрического поля и концентрации наполнителя. Выявлено, что в рамках точности эксперимента значения предела текучести не зависят от вязкости дисперсионной среды при фиксированной концентрации и напряженности электрического поля. Также была оценена седиментационная устойчивость суспензий. Скорость осаждения частиц галлуазита ниже в суспензиях на основе более вязких масел, что в первом приближении согласуется с формулой Стокса. Величина равновесного седиментационного отношения -высоты коллоидной фазы к общей высоте столба жидкости, зависит от концентрации наполнителя и оказывается выше для суспензий с большим содержанием частиц. Выявлен не монотонный характер зависимости относительной эффективности суспензий от вязкости дисперсионной среды для 8 масс.% суспензий. Показано, что комбинация трех параметров: вязкости дисперсионной среды, концентрации наполнителя и напряженности электрического поля позволяет получать электрореологические жидкости с заданными, прогнозируемыми свойствами.
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