Bulletin of the American Physical Society
71st Annual Meeting of the APS Division of Fluid Dynamics
Volume 63, Number 13
Sunday–Tuesday, November 18–20, 2018; Atlanta, Georgia
Session G24: Microscale Flows: Particle Electrokinetics |
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Chair: Shaurya Parakash, Ohio State University Room: Georgia World Congress Center B312 |
Monday, November 19, 2018 10:35AM - 10:48AM |
G24.00001: Heterogeneous colloidal assembly: Band formation in a mixture of suspended particles Andrew J. Yee, Minami Yoda Evanescent-wave visualizations of the near-wall region in microchannels have shown that colloidal (radius a = O(100 nm)) polystyrene particles in a dilute (bulk volume fractions < 4×10-3) suspension assemble into “bands” that only exist within a few μm of the wall in Poiseuille and electroosmotic (EO) “counterflow.” The particles are concentrated in a liquid state into high aspect ratio structures with a cross-sectional dimension of a few μm and a length comparable to the channel length of O(1 cm). Recent results demonstrate that heterogeneous assembly is also possible with this approach. A dilute mixture of suspended a ≈ 250 nm particles with nearly a two-fold difference in ζ-potential (labeled with different fluorophores) form bands, and their composition—whether heterogeneous structures that contain both types of particles, or homogeneous structures consisting of only a single type of particle—can be controlled by the magnitude of the dc electric field that drives the EO flow at a given near-wall shear rate. The minimum electric field magnitude for heterogeneous assembly is less than that for either type of particle at its respective concentration in the mixture, suggesting that the different particles interact. |
Monday, November 19, 2018 10:48AM - 11:01AM |
G24.00002: Colloidal band assembly: Effect of streamwise position Minami Yoda, Andrew J. Yee Various studies have shown that colloidal particles in a flowing dilute suspension (volume fractions < 0.4%) are subject to wall-normal “lift” forces, which are usually repulsive. In combined Poiseuille and electroosmotic “counterflow,” however, the particles experience an attractive lift force instead. In this flow, the particles become concentrated near the wall and assemble into structures—“bands”—above a minimum electric field magnitude |Emin|. Recently, we have observed “partial banding,” where these structures only exist near the downstream end of the channel, suggesting that |Emin| depends on the streamwise location x in the channel. Revised “banding maps” that give |Emin| as a function of x for different near-wall (essentially constant) shear rates are presented. These observations also suggest that banding occurs once the near-wall particle concentration exceeds a minimum value—and the particle concentration increases with x because the particles are subject to the attractive lift force over a longer time. Evanescent-wave visualization is used to estimate the near-wall particle concentration as a function of time at different channel positions x at electric fields below |Emin| and above |Emin| before the bands form. |
Monday, November 19, 2018 11:01AM - 11:14AM |
G24.00003: Electrohydrodynamic printing of pre-assembled colloidal particle structures Shaurya Prakash, Varun Lochab Recent discoveries have shown that dilute suspensions of colloidal particles with diameters ranging from 200 nm – 1 µm can be assembled into distinct colloidal bands within microchannels (100 – 300 µm wide x 34 µm deep x 4 cm long). The band formation has been shown to require opposed Poiseuille and electrokinetic flows. Moreover, band formation occurs above a minimum applied potential (and consequently electric field) threshold at a given shear rate. Band formation is known to be a function of particle size, particle volume fraction, particle zeta potential, and the minimum electric field thresholds change in a non-linear fashion for particle mixtures. The colloidal bands present a unique, high throughput flow through system for assembling structures from pre-assembled high aspect ratio bands (~ O(104)), vs. current state-of-the-art particle-by-particle assembly methods. In this work, we discuss the design, fabrication, and development of a microchannel nozzle that acts as a printer for pre-formed particle bands at a representative diameter of 490 nm on a soft substrate. The impact of various Poiseuille and electrokinetic flow conditions on the printing of particles to substrates outside the channels will also be discussed. |
Monday, November 19, 2018 11:14AM - 11:27AM |
G24.00004: Electrokinetic motion of particles in xanthan gum solutions Amirreza Malekanfard, Logan Bulloch, Alicia Baldwin, Di Li, Xiangchun Xuan The interest in the ability to control and predict the motion of particles in microfluidic devices has been increasing. It is a known fact that particles move parallel to the applied electric field in straight uniform microchannels. Numerous studies have been conducted to investigate electrokinetic motion of particles in Newtonian fluids. However, the behavior in non-Newtonian fluids needs further study since many biological and chemical fluids exhibit non-Newtonian characteristics. In this work, we present an experimental study of electrokinetic motion of particles in xanthan gum solutions through straight rectangular microchannels. The effects of multiple parameters including electric field magnitude, particle size, microchannel depth and xanthan gum concentration are investigated. This study will provide useful experimental data for validating theoretical and numerical models on electrokinetic particle motion in shear-thinning fluids. |
Monday, November 19, 2018 11:27AM - 11:40AM |
G24.00005: Electrokinetics in concentrated suspensions of ideally polarizable spheres Siamak Mirfendereski, Jae Sung Park Electrokinetics plays an important role in many fields ranging processing techniques for fine particle systems to controlled drug release devices. In many situations, semi-dilute or dense suspensions are used, where hydrodynamic interactions become significant. However, the analysis of the electrokinetics in these suspensions has been poorly understood. In this study, we numerically investigate concentrated suspensions undergoing dielectrophoresis and induced-charge electrophoresis. Large-scale simulations are performed for suspensions at various volume fractions with periodic boundary conditions. Results show an intriguing suspension dynamics at different volume fraction regimes. In a dilute regime, the hydrodynamic diffusivity increases with a volume fraction before reaching a global maximum and then decreases in a semi-dilute regime until it approaches the local minimum at a volume fraction of 30%. Interestingly, the hydrodynamic diffusivity increases again in a concentrated regime until it reaches a local maximum at a volume fraction of 50% and then drastically decreases as it approaches the packing fraction. Further investigations are discussed to better understand this unique behavior in a concentrated regime. |
Monday, November 19, 2018 11:40AM - 11:53AM |
G24.00006: Liquid dielectrophoresis controlled detachment and re-attachment of bubbles Carl V. Brown, Andrew M.J. Edwards, Abi Roberts, Michael I. Newton, Ian C. Sage, Rodrigo Ledesma Aguilar, Glen McHale Air bubbles attached to surfaces in liquids can block flow in channels, amplify shear wall stress, and form dry patches in heat exchangers. Here we present a new method of controlling the wetting, detachment, and re-attachment of an air bubble in a dielectric liquid through an interface-localized form of liquid dielectrophoresis. We show the contact of the bubble with the surface obeys a dielectrowetting equation, analogous to electrowetting. Moreover, the bubble can be completely detached on demand from the surface with the application of a voltage to a patterned electrode on the surface. Once detached, bubbles are free to float beneath the surface and can be prevented from re-attaching to the surface by a thin liquid layer maintained by an applied voltage. The thickness of this liquid has a logarithmic dependence on the magnitude of the voltage, which we accurately describe by a theory that considers the energy balance due to liquid-dielectrophoresis and buoyancy of the liquid-bubble system. The critical re-attachment voltage is shown to depend on the material parameters of the liquid, and on the geometrical parameters of the electrode pattern. |
Monday, November 19, 2018 11:53AM - 12:06PM |
G24.00007: Opto-electrohydrodynamic control of rapid microvortex flow Choongbae Park Rapid and tunable opto-electrohydrodynamic (OEHD) microvortex flow generation and manipulation have been recently developed. The combination of AC electric fields and optical illumination allows for the easy and rapid creation of microvortex flows inside a microchannel for applications such as micropumping and micromixing. An opto-electrohydrodynamically generated microflow called a twin opposing microvortex (TOMV) flow has been simply manipulated and tuned by varying AC voltage and frequency as well as laser power and moving laser beam inside a TOMV device. Micron-resolution particle image velocimetry (μPIV) is used to measure velocity fields of three-dimensional (3D) microvortex flow generated under non-uniform electric fields and a highly focused laser beam. The magnitude of the in-plane velocity linearly depends on AC voltage while it shows a bell-shaped curve when the magnitude of the in-plane velocity is expressed as a function of AC frequency. When the AC frequency is increased to a few MHz, different microvortex flows are generated. The results presented are useful to understand underlying fluid mechanics in the TOMV flow and will be a foundation to develop effective and controllable microvortex flow in the rapidly growing field of micro/nano scale transport. |
Monday, November 19, 2018 12:06PM - 12:19PM |
G24.00008: Direct Numerical Simulation of Particles in Spatially Varying Electric Fields Edison Amah, Pushpendra Singh, Muhammad Janjua A numerical scheme is developed to simulate and study the motion of dielectric particles in the uniform and nonuniform electric fields of microfluidic devices. The motion of particles is simulated using a distributed Lagrange multiplier method (DLM) and the electric force acting on the particles is calculated by integrating the Maxwell stress tensor (MST) over the particle surfaces. The MST is obtained from the electric potential, which, in turn, is obtained by solving the electrostatic problem. In our numerical scheme, the domain is discretized using a finite element scheme and the Marchuk-Yanenko operator-splitting technique is used to decouple the difficulties associated with the incompressibility constraint, the nonlinear convection term, the rigid-body motion constraint and the electric force term. The MST results show that the ratio of the particle-particle interaction and dielectrophoretic forces decreases with increasing particle size. Consequently, when the spacing between the electrodes is comparable to the particle size, instead of collecting on the same electrode by forming chains, they collect at different electrodes. |
Monday, November 19, 2018 12:19PM - 12:32PM |
G24.00009: Inertial migration of an electrophoretic rigid sphere in an electroosmotic-Poiseuille flow Akash Choudhary, T Renganathan, S Pushpavanam Inertial focusing is the phenomenon of cross-stream migration of particles in the presence of finite inertia. This physics is employed to sort cells and droplets in microfluidic devices. To gain an enhanced control over this migration, recently a few experimental studies have applied an external electric field to sort particles based on their intrinsic properties such as charge density. We have analytically studied the migration of a rigid spherical particle in a two-dimensional Poiseuille flow, subjected to an externally imposed electric field. The particle and wall both have a uniform zeta potential and are assumed to have a thin electrical double layer. The electrostatic potential and velocity disturbances are evaluated by using the method of reflections. A semi-analytical expression for the lift force as a function of particle size (κ), zeta potential (ζp) and an electric Reynolds number (ReE) is obtained. To obtain an insight on this migration, we find the magnitude of the constituents of the lift force and draw a comparison with the buoyancy induced Saffman-lift. It is found that the leading-order modification (~O(κ ReE ζp) higher) in this lift is due to interaction of the additional ‘force-free phoretic’ disturbance with the background parabolic flow profile.
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Monday, November 19, 2018 12:32PM - 12:45PM |
G24.00010: Separating two attractive elongated particles by hydrodynamic interactions under alternating external field Micheline Abbas, Georges Bossis, Pavel Kuzhir In applications where magnetic particles are used to detect and dose targeted molecules, it is important to prevent particle clustering and aggregation. Elongated ferromagnetic particles can be more interesting than spherical ones due to their large magnetic moment, which facilitates their separation by magnets or the detection of their orientation relaxation time. Under alternating magnetic field, the rotational dynamics of elongated ferromagnetic particles results from the balance between magnetic torque that tends to align the particle axis with the field direction and viscous torque. As for their translational motion, it results from a competition between direct magnetic particle-particle interactions and solvent-flow-mediated hydrodynamic interactions. Due to particle anisotropy, this may lead to intricate translation-rotation couplings. Using numerical simulations and theoretical modeling of the system, we show that two ellipsoidal magnetic particles, initially in a head-to-tail attractive configuration resulting from their remnant magnetization, can repel each other due to hydrodynamic interactions when alternating field is operated. The separation takes place in a finite range of low frequencies, depending on the field and magnetization intensities. |
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