Latest papers in fluid mechanics
Pore-scale study of counter-current imbibition in strongly water-wet fractured porous media using lattice Boltzmann method
Oil recovery from naturally fractured reservoirs with low permeability rock remains a challenge. To provide a better understanding of spontaneous imbibition, a key oil recovery mechanism in the fractured reservoir rocks, a pore-scale computational study of the water imbibition into an artificially generated dual-permeability porous matrix with a fracture attached on top is conducted using a recently improved lattice Boltzmann color-gradient model. Several factors affecting the dynamic countercurrent imbibition processes and the resulting oil recovery have been analyzed, including the water injection velocity, the geometry configuration of the dual permeability zones, interfacial tension, the viscosity ratio of water to oil phases, and fracture spacing if there are multiple fractures. Depending on the water injection velocity and interfacial tension, three different imbibition regimes have been identified: the squeezing regime, the jetting regime, and the dripping regime, each with a distinctively different expelled oil morphology in the fracture. The geometry configuration of the high and low permeability zones affects the amount of oil that can be recovered by the countercurrent imbibition in a fracture-matrix system through transition of the different regimes. In the squeezing regime, which occurs at low water injection velocity, the build-up squeezing pressure upstream in the fracture enables more water to imbibe into the permeability zone closer to the fracture inlet thus increasing the oil recovery factor. A larger interfacial tension or a lower water-to-oil viscosity ratio is favorable for enhancing oil recovery, and new insights into the effect of the viscosity ratio are provided. Introducing an extra parallel fracture can effectively increase the oil recovery factor, and there is an optimal fracture spacing between the two adjacent horizontal fractures to maximize the oil recovery. These findings can aid the optimal design of water-injecting oil extraction in fractured rocks in reservoirs such as oil shale.
Author(s): Jacob S. Bach and Henrik Bruus
Bulk-driven acoustic (Eckart) streaming is the steady flow resulting from the time-averaged acoustic energy flux density in the bulk of a viscous fluid. In simple cases, like the one-dimensional single standing-wave resonance, this energy flux is negligible, and therefore the bulk-driven streaming i...
[Phys. Rev. E 100, 023104] Published Wed Aug 07, 2019
Numerical investigation of vibration-induced droplet shedding on smooth surfaces with large contact angles
Author(s): Mostafa Moradi, Mohammad Hassan Rahimian, and Seyed Farshid Chini
In this work, numerical simulations are performed to study the droplet response to the vertical vibration of the substrate, under various frequencies and amplitudes using the multiphase lattice Boltzmann method. First, the numerical results are validated against published experimental data. The effe...
[Phys. Rev. E 100, 023105] Published Wed Aug 07, 2019
Author(s): C. M. Mackenzie Dover and K. Sefiane
Contact angle hysteresis is measured on micropillar surfaces with four different area fractions. To fit the data at higher area fractions, the Cassie law is modified to account for capillary bridges.
[Phys. Rev. Fluids 4, 081601(R)] Published Wed Aug 07, 2019
Author(s): Daniel J. Walls, Andrew S. Ylitalo, David S. L. Mui, John M. Frostad, and Gerald G. Fuller
The time-dependent spreading behaviors of a rinsing liquid across a horizontal, rotating substrate pre-coated with thin liquid films is investigated. Four distinct growth behaviors in time of the azimuthally averaged spreading radius are observed and explained with lubrication theory.
[Phys. Rev. Fluids 4, 084102] Published Wed Aug 07, 2019
We consider the stability problem for wide, uniform stationary open flows down a slope with constant inclination under gravity. Depth-averaged equations are used with arbitrary bottom friction as a function of the flow depth and depth-averaged velocity. The stability conditions for perturbations propagating along the flow are widely known. In this paper, we focus on the effect of oblique perturbations that propagate at an arbitrary angle to the velocity of the undisturbed flow. We show that under certain conditions, oblique perturbations can grow even when the perturbations propagating along the flow are damped. This means that if oblique perturbations exist, the stability conditions found in the investigation of the one-dimensional problem are insufficient for the stability of the flow. New stability criteria are formulated as explicit relations between the slope and the flow parameters. The ranges of the growing disturbances propagation angles are indicated for unstable flows.
This study is concerned with the nonlinear interactions between pairs of intersecting Alfvén waves in a magnetized plasma and used the modified Korteweg–de Vries equation to study nonlinear interactions. The modulation instability analysis shows the existence of periodic traveling wave solution in the system. Two different types of waves interaction solutions, namely, the periodic wave interaction solutions and the solitary wave interaction ones, are captured analytically. It is found that the wave resonance for the periodic waves interaction could happen as various wave numbers are nearly the same. In this case, the subsidiary waves could not be neglected. It is also found that the interaction for solitary waves, different solitons eventually regain their original states. The solitons with higher energy possess more speed as compared to the low energy solitons. The phenomenon of Alfvén wave interaction can be of importance for understanding the transport mechanism of magnetic waves in various processes of heating and transport of energy in space, solar wind, and astrophysical plasma.
The spreading of a liquid film across a rotating surface is inherently unstable due to the centrifugal force, which causes the formation of rivulets along the spreading front. This instability produces a rich diversity of spreading patterns and is important to control for the optimization of spin-coating and spin-rinsing of silicon wafers during the fabrication of microelectronics. The present work is an experimental investigation of the evolution of rivulets arising from this instability during the spreading of an impinging water jet across a rotating substrate that is precoated with a thin, aqueous film. To characterize these rivulets, we developed a high-speed imaging apparatus and image-processing software that traces the spreading front over time. We show how the morphology of the spreading front is qualitatively affected by varying the Reynolds number of the impinging jet, the ratio of centrifugal to Coriolis forces, and the type of liquid used to precoat the substrate. For quantitative analysis of rivulets, we measured the “compactness ratio” of the spreading front, which quantifies deviation from a circular spreading front. We used the compactness ratio to demonstrate that rivulets are suppressed most strongly at low rotation rates, at high flow rates, and on substrates precoated with water, although with notable exceptions.
Author(s): E. F. Strong, M. Pezzulla, F. Gallaire, P. Reis, and L. Siconolfi
The drag of perforated thin disks is studied at low Reynolds numbers via displacement controlled experiments and simulations. It is shown that the drag of the disks is affected by the size of the voids, but not by the disk thickness. Good agreement is observed with existing analytical solutions.
[Phys. Rev. Fluids 4, 084101] Published Tue Aug 06, 2019
Author(s): R. A. Antonia, S. L. Tang, L. Djenidi, and Y. Zhou
A relatively extensive survey of published data shows that the 4/5 law has not yet been observed in either experiments or simulations because the Reynolds number is not sufficiently large.
[Phys. Rev. Fluids 4, 084602] Published Tue Aug 06, 2019
To fulfill the increasing need for large power generation by wind turbines, the concept of multirotor wind turbines has recently received attention as a promising alternative to conventional massive single-rotor wind turbines. To shed light on the viability of this concept, large-eddy simulation is employed in this study to compare wake flow properties of a multirotor wind turbine with those of a single-rotor turbine. The wake of a multirotor turbine is found to recover faster at short downwind distances, where the whole wake is characterized as an array of localized high velocity-deficit regions associated with each rotor. However, as the wake moves downstream, rotor wakes start interacting with each other until they eventually form a single wake. This transition from a wake array to a single wake adversely affects the initial fast recovery of multirotor turbine wakes. A budget analysis of mean kinetic energy is performed to analyze the energy transport into the wake before and after this transition. In addition, the effect of different geometrical configurations on wake characteristics of a multirotor turbine was examined. We found that the recovery rate of multirotor turbine wakes is enhanced by the increase in rotor spacing, whereas the number and rotation direction of rotors do not play a significant role in the wake recovery. A simple analytical relationship is also developed to predict the streamwise distance at which the transition from a wake array to a single wake occurs for multirotor wind turbines.
Intermolecular interactions are responsible for the macroscopic properties of materials. Self-assembled micelles of ionic surfactants in the presence of salt are a result of the balance between hydrophobic-hydrophilic and ionic forces. For example, sodium salicylate (NaSal) undoubtedly offers a powerful means of increasing the viscoelasticity of hexadecyl trimethylammonium bromide (CTAB) solutions by orders of magnitude, which results from the formation of wormlike micelles (WLMs). The efficiency of this additive relies on its ability to integrate and alter the repulsive interactions governing CTAB micelles. Consequently, small modifications in the molecular structure of NaSal influences the nature of these interactions. Nevertheless, the full potential of formulation for tailoring the system’s viscoelasticity has yet to be unleashed. Herein, we investigate a series of structurally similar molecules varying in terms of geometry and size. The depth and molecular orientation of their insertion into the micellar core were monitored by proton nuclear magnetic resonance (1H-NMR) and correlated with the corresponding viscoelastic response. After detailed observation of the impact of molecular interactions on zero-shear viscosity η0, we discuss it in terms of the effective packing parameter (PPeff). All the investigated additives increased PPeff, triggering anisotropic micellar growth toward WLMs. The simplicity of our approach is attractive for predicting and controlling the viscoelastic properties of WLM solutions from an intermolecular level.
The forcing in round jets has large scale effects on the development and characteristics of the flow field such as the entrainment, spreading rate, and mixing of the flow. In the present work, an active control technique called the large scale flapping perturbation is studied for influencing the evolution of the circular jet. Direct numerical simulation of incompressible, spatially developing circular jets at a Reynolds number of 1000 is reported. The flow field has been explored by solving three-dimensional unsteady Navier-Stokes equations using second order spatial and temporal discretization. Among the considered variables (apart from the excitation amplitude), the perturbation frequency is the most important controlling parameter. For a circular jet at an excitation frequency of 0.1, there is evidence of a Y-shaped bifurcation on the bifurcating plane, while no bifurcation is observed on the other orthogonal plane. With an increase in the excitation frequency to 0.3, the circular jet issued from the orifice divides itself into three parts and a ψ-shaped bifurcation is obtained on the bifurcating plane. The development of the ψ-shaped bifurcation may be due to the interaction of the consecutive vortex ring and the formation of elongated vortices. However, with further increase in the excitation frequency, the spreading rate becomes weaker with the evidence of formation of the ψ-shaped bifurcation.
A generalized model for the chaotic disintegration of a liquid due to an arbitrarily shaped projectile is proposed. In particular, the model uses percolation theory to predict the fragmentation process of blood, resulting in forward spatter to determine the number of droplets, as well as their sizes and initial velocities resulting from the flow field generated by a 7.62 × 39 mm and a 0.45 auto bullet. Blood viscoelasticity, which slows down the initial velocities of the droplets, is accounted for. The main physical mechanisms responsible for the chaotic disintegration of blood in the case of forward spattering are (i) the Rayleigh-Taylor instability associated with denser blood accelerating toward lighter air and (ii) a cascade of instability phenomena triggered by the original Rayleigh-Taylor instability because the Reynolds number is of the order of 107. Blood is viscoelastic, therefore, its disintegration into individual droplets results in ligament formation with strong uniaxial elongation, which is characterized by the extremely high values of the Deborah number leading to an almost purely elastic behavior and brittlelike fracture. The blood droplet spray then propagates in air, and deposition on the floor is calculated accounting for gravity and air drag forces, with the latter being diminished by the collective effect related to the droplet-droplet interaction. Also, the experimental data acquired in this work are presented and compared with the theoretical predictions. The agreement between the predictions and the data is satisfactory. The present fluid mechanical model holds great promise for forensic applications.
Author(s): Koshun Ogawa, Haruki Oga, Hiroki Kusudo, Yasutaka Yamaguchi, Takeshi Omori, Samy Merabia, and Laurent Joly
Molecular dynamics simulations are a powerful tool to characterize liquid-solid friction. A slab configuration with periodic boundary conditions in the lateral dimensions is commonly used, where the measured friction coefficient could be affected by the finite lateral size of the simulation box. Her...
[Phys. Rev. E 100, 023101] Published Mon Aug 05, 2019
Author(s): J. Meibohm and B. Mehlig
We study a one-dimensional model for heavy particles in a compressible fluid. The fluid-velocity field is modeled by a persistent Gaussian random function, and the particles are assumed to be weakly inertial. Since one-dimensional fluid-velocity fields are always compressible, the model exhibits spa...
[Phys. Rev. E 100, 023102] Published Mon Aug 05, 2019
Author(s): T. Zagvozkin, A. Vorobev, and T. Lyubimova
The stability of a shear flow imposed along a diffusive interface that separates two miscible liquids (a heavier liquid lies underneath) is studied using direct numerical simulations. The phase-field approach is employed for description of a thermo- and hydrodynamic evolution of a heterogeneous bina...
[Phys. Rev. E 100, 023103] Published Mon Aug 05, 2019
Author(s): Xiaodong Cai, Ralf Deiterding, Jianhan Liang, Mingbo Sun, and Dezun Dong
Using adaptive numerical solutions of the reactive Navier-Stokes equations we clarify the mechanism of detonation stabilization in supersonic expanding channels, and further demonstrate that by dynamically controlling a moving boundary dynamically stationary detonation propagation is possible.
[Phys. Rev. Fluids 4, 083201] Published Mon Aug 05, 2019
Instability driven by shear thinning and elasticity in the flow of concentrated polymer solutions through microtubes
Author(s): Bidhan Chandra, Rahul Mangal, Debopam Das, and V. Shankar
Polymers make flow in a tube unstable at low Reynolds numbers. An investigation shows that laminar flows of polymer solutions in a tube become unstable, unlike Newtonian fluids, at a Reynolds number as low as 10. This occurs because of the elastic and shear-thinning nature of polymer solutions.
[Phys. Rev. Fluids 4, 083301] Published Mon Aug 05, 2019
Author(s): Ramkarn Patne and V. Shankar
Flow of Bingham fluids is unstable if channel walls are deformable. Laminar flows of Bingham fluids in rigid-walled channels are stable to tiny disturbances. A study finds that if the walls are made deformable, the flow becomes unstable at very low Reynolds number.
[Phys. Rev. Fluids 4, 083302] Published Mon Aug 05, 2019