scholarly journals Modeling of droplet and bubble detachment assisted by electrowetting-on-dielectric (EWOD)

2017 ◽  
Author(s):  
◽  
Haolun Xu

This work reports both theoretically and numerically a novel mechanism of electrowetting-induced jumping droplet and bubble detachment. Six different chapters were explored in this work. Chapter 1 gives the overview of the various works that have been done in the field and the applications of this work. Chapter 2 discusses the numerical method. Chapter 3 discusses the computational setup and experimental validation of the jumping droplet. Chapter 4 analyzes the jumping droplet and bubble detachment induced by EWOD. The flow field and various dynamics of droplet, bubble and interfacial wave have been discussed. Chapter 5 discusses the experimental setup and fabrication of electrowetting devices. The experiments proved that electrowetting driven interfacial wave can be achieved. Chapter 6 summarizes the EWOD principle and the future application. Electroweting-on-dielectric (EWOD) can be used to induce the detachment of micro-water droplet from hydrophobic surface. The level set method has been used to track the interface of water and air. The capillary wave on the droplet interface could be seen during the electrowetting effect. The sudden variation of the droplet base creates a disturbance that propagates along the surface in the form of a capillary wave. As the wetted area is reduced during this transformation, the excess surface energy is converted into kinetic energy which stretches the droplet vertically and eventually leads to the detachment from the substrate; the results have been validated with available experimental data. The physics of stretching, recoiling and detachment of the droplet have been investigated. Inspired by the potential demonstrated by electrowetting-controlled droplets, this work also investigates the potential advantages of electrowetting to disrupt bubble dynamics to improve phase change heat transfer. Electrowetting-on-dielectric is used to modulate the contact point movement at the water-air interface in a thin liquid film. Rapid oscillation of the contact line is achieved by a swift change of voltage under an AC signal. When disturbed with such contact angle changes, the interfacial wave between two immiscible fluids disrupts bubble dynamics. Numerical modeling reveals that an air bubble on a hydrophobic surface can be detached by the trough of such a wave. The frequency of interfacial wave is twice the voltage frequency. A higher voltage frequency leads to a smaller amplitude and higher celerity of the wave, while a lower voltage frequency leads to a larger wave amplitude and lower celerity. The bubble can easily detach when the voltage frequency from 2Hz-10Hz. However, the bubble fails to detach when the voltage frequency is 100Hz. This approach can be useful to improve two-phase cooling performance.

Author(s):  
Sheng Wang ◽  
Junxiang Shi ◽  
Hsiu-Hung Chen ◽  
Tiancheng Xu ◽  
Chung-Lung (C. L.) Chen

With the inspiration from electrowetting-controlled droplets, the potential advantages of electrowetting for bubble dynamics are investigated experimentally and numerically. In our experimental system, a 100 nanometer thin film gold metal was used as an electrode, and a 6.5 micrometer polydimethylsiloxane (PDMS) was spin-coated on the electrode acting both as an dielectric layer and hydrophobic surface. A two-phase model coupled with a electrostatics was used in our simulation work, where the body force due to the electric field acts as an external force. Our numerical results demonstrated that electrowetting can help the detachment of a small bubble by changing the apparent contact angle. Similar results were observed in our experiments that with electrowetting on dielectric, the contact angle of bubble on a hydrophobic surface will obviously decrease when a certain electrical field is applied either with a small size bubble (diameter around 1mm) or a relatively larger size bubble (diameter around 3 mm). When the applied voltage becomes high enough, both the experimental and numerical results demonstrate the characteristics of bubble detachment within a thin film liquid layer.


2017 ◽  
Vol 29 (10) ◽  
pp. 102105 ◽  
Author(s):  
Haolun Xu ◽  
Run Yan ◽  
Sheng Wang ◽  
Chung-Lung Chen

2016 ◽  
Vol 108 (18) ◽  
pp. 181601 ◽  
Author(s):  
S. Wang ◽  
H. H. Chen ◽  
C. L. Chen

Author(s):  
Nazmul Islam ◽  
Davood Askari

This paper describes the optimization of bidirectional micropump velocity by a deposition of hydrophobic nanoparticle (NP) monolayer. A nano-composite polymer coating contains a homogeneous mixture of Silicon NP in polydimithylsiloxane (PDMS) which will modify the micropump surface to a hydrophobic surface. For hydrophobic nature of PDMS, the monolayer coating will modify the hydrophilic surface of biased AC electroosmotic micropump to a hydrophobic surface. Based on the results obtained from our previous research work for the biased AC electroosmotic micropump, the pumping velocity was 300 micron/sec in 100μm channel thickness for applied voltage of 4.4V at 1 KHz frequency [1]. In that research, we had optimized the applied AC voltage, frequency, channel dimension, and electrode width. The main objective of this research is to investigate the micropump velocity through a surface modification process. Adding a thin monolayer will separate the electrode from the pumping liquid; thus eliminating the reaction on the electrode for applied voltage. In such case, we can apply high voltage to achieve high pumping rate.


Author(s):  
R. Panneer Selvam ◽  
Joseph Johnston ◽  
Suranjan Sarkar

In this paper, we present an extension of the level set method from 2D into 3D for solving multiphase flow problems using distributed parallel computing. The model solves the incompressible Navier-Stokes equations to study the behavior of a bubble immersed in a thin liquid film at microscale as found in a spray cooling environment. Since modeling all aspects of spray cooling, including nucleation, bubble dynamics, droplet impact, convection and thin film evaporation is very difficult at this time; these phenomena have been divided and studied separately in order to study the heat transfer behavior of each phenomenon individually. We studied the droplet impact effect as seen in spray cooling by our 3D multiphase model in earlier studies. Through the 3D multiphase model this study simulates the dynamics of a nucleating bubble in a thin liquid film that merges with the ambient atmosphere above the film. In this study we did not consider the droplet impact effect to concentrate on the vapor bubble dynamics in thin liquid film and its effect on heat transfer. The effect of convective flow is not considered to keep the 3-D model simple. However the 2D model was modified to simulate the effect that a horizontal flow of constant velocity has on the growth and detachment of a nucleating bubble and discussed in the second part of the paper. This study illustrates the importance of considering the convective flow effect in our 3-D multiphase flow model in future with droplet impact for spray cooling modeling studies.


Author(s):  
Youngsuk Nam ◽  
Gopinath Warrier ◽  
Jinfeng Wu ◽  
Y. Sungtaek Ju

The growth and departure of single bubbles on two surfaces with very different wettability is studied using high-speed video microscopy and numerical simulation. Isolated artificial cavities of approximately 10μm diameter are microfabricated on a bare and a Teflon-coated silicon substrate to serve as nucleation sites. The bubble departure diameter is observed to be almost three times larger and the growth period almost 60 times longer for the hydrophobic surface than for the hydrophilic surface. The waiting period is practically zero for the hydrophobic surface because a small residual bubble nucleus is left behind on the cavity from the previous ebullition cycle. The experimental results are consistent with our numerical simulations. Bubble nucleation occurs on nominally smooth hydrophobic regions with root mean square roughness (Rq) less than 1 nm even at superheat as small as 3 °C. Liquid subcooling significantly affects bubble growth on the hydrophobic surface due to increased bubble surface area. Fundamental understanding of bubble dynamics on heated hydrophobic surfaces will help to develop chemically patterned surfaces with enhanced boiling heat transfer and novel phase-change based micro-actuators and energy harvesters.


Author(s):  
Di Wu ◽  
Ying Piao ◽  
Yuan-yuan Duan ◽  
Zhen Yang

A series of experiments was conducted to observe nucleate boiling phenomena in horizontal tubes with inner diameters varying from 0.05 mm to 3.0 mm. Diverse behaviors of bubble growth were explored, identified by which tubes were classified into micro, mini and macro scales. In micro tubes (Di ≤ 200 μm), the liquid was emitted instantaneously with extremely fast liquid-vapor interfacial movement, referred as explosive emission boiling phenomenon. It is hard to record bubble growth process with high speed camera. In mini tubes (200 μm < Di < 2.5 mm), though liquid was also emitted outsides, the interface moves relative slow and the whole process of bubble growth can be observed. Two distinct stages, referred as spherical and oblate bubble growth stages, were divided. In macro tubes (Di ≥ 2.5 mm), only spherical bubble growth stage exists and the growth rate is much smaller than that in mini tubes. Furthermore, the mechanism of diverse bubble dynamics was analyzed. In mini/micro tubes, decreasing tube diameter can trigger a transition from spherical to oblate bubble growth and consequently establish a thin film between liquid-vapor interface and heated wall. The thin liquid film evaporates vigorously and accelerates the interfacial movement, which reversely enhances evaporation of thin film. A positive interaction between interfacial movement and thin film evaporation establishes, resulting in the interface moving faster and faster and consequently emitted liquid outsides instantaneously. In macro tubes, as tube diameter increasing, the transition and sequential positive interaction can not be raised. Hence, the bubble maintains growing spherically as that in pool boiling.


2005 ◽  
Author(s):  
Ding Li ◽  
Vijay K. Dhir

Complete numerical simulations of bubble dynamics including bubble growth, sliding motion, and bubble lift-off from a horizontal surface have been carried out for different gravity levels and flow velocities. In the model, the region of interest is divided into micro and macro regions. The micro region is the ultra thin liquid film that forms between the solid and evolving vapor-liquid interface. The region occupied by vapor and liquid—excluding the micro layer—is designated as the macro region. Complete conservation equations of mass, momentum, and energy for both phases are solved in this region. The interface shape is obtained by solving for the Level-Set function. The advancing and receding contact angles obtained from experiments are used as input to the model. The predictions are compared with data from experiments. The functional dependence of bubble diameter at departure and growth period on gravity is found to weaken with the increase in flow velocity.


Author(s):  
Wen Wu ◽  
Peipei Chen ◽  
Barclay G. Jones ◽  
Ty A. Newell

This research examines the influence of heating surface structure on bubble detachment, which includes bubble departure and bubble lift-off, under sub-cooled nucleate boiling condition, in order to obtain better understanding to the bubble dynamics on horizontal flat heat exchangers. Refrigerant R-134a is chosen as a simulant fluid due to its merits of having smaller surface tension, reduced latent heat, and lower boiling temperature than water. Experiments were run with varying experimental parameters e.g. pressure, inlet sub-cooled level, and flow rate, etc. High speed digital images at frame rates up to 4000 frames/s were obtained, showing characteristics of bubble movement. Bubble radius and center coordinates were calculated via Canny’s algorithm for edge detection and Fitzgibbon’s algorithm for ellipse fitting. Results were compared against the model proposed by Klausner et al. for prediction of bubble detachment sizes. Good overall agreement was shown, with several minor modifications and suggestions made to the assumptions of the model.


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