Physical Review Fluids
Experimental study of a helical acoustic streaming flow
Author(s): Bjarne Vincent, Sophie Miralles, Daniel Henry, Valéry Botton, and Alban Pothérat
The acoustofluidic helix stirs fluid within a closed container efficiently with only one ultrasound source. The helical shape is obtained by reflecting the acoustic beam on the cavity walls. This acoustic forcing drives multiple descending jets, each impinging a vertical wall and wrapping around the central axis. Time-averaged and low-frequency unsteady flow structures have been obtained by three-dimensional particle tracking velocimetry and Eulerian field reconstructions. Both the velocity amplitudes of the overall time-averaged flow, and the vortex dynamics, depend on the dimensionless acoustic force magnitude called the acoustic Grashof number.
[Phys. Rev. Fluids 9, 024101] Published Thu Feb 29, 2024
High-fidelity reconstruction of large-area damaged turbulent fields with a physically constrained generative adversarial network
Author(s): Qinmin Zheng, Tianyi Li, Benteng Ma, Lin Fu, and Xiaomeng Li
In this work, we propose a novel framework for the high-fidelity reconstruction of large-area damaged turbulent fields with high resolution based on a physically constrained generative adversarial network. The network leverages complete/sparse fields of velocity components as physical constraints and adopts a PatchGAN discriminator network. The proposed reconstruction framework has been shown to achieve excellent reconstruction performance. The reconstructed flow fields are consistent with the raw flow fields in terms of magnitude, power spectrum, and two-point correlation function.
[Phys. Rev. Fluids 9, 024608] Published Thu Feb 29, 2024
Stable, entropy-consistent, and localized artificial-diffusivity method for capturing discontinuities
Author(s): Suhas S. Jain, Rahul Agrawal, and Parviz Moin
A localized artificial-diffusivity method is developed for capturing discontinuities, such as shocks and contacts, in compressible flows. A new sensor for contact discontinuity makes the method more localized, and a discretely consistent formulation eliminates the need for filtering the solution or filtering the sensors to obtain robust solutions. Improved predictions are observed in canonical shock-tube problems and large-eddy simulations of homogeneous isotropic turbulence.
[Phys. Rev. Fluids 9, 024609] Published Thu Feb 29, 2024
Capillary imbibition of shear-thinning fluids: From Lucas-Washburn to oscillatory regimes
Author(s): Camille Steinik, Davide Picchi, Gianluca Lavalle, and Pietro Poesio
We studied the filling dynamics of a shear-thinning fluid in a capillary tube. In regimes where inertial effects can be neglected, we generalize the Lucas-Washburn scaling relation to shear-thinning fluids, showing that the classical 1/2 scaling law holds only if an ad hoc time-dependent effective viscosity that applies to both Newtonian and shear-thinning fluids is introduced. In regimes where inertia competes with viscous and gravity effects, the system shows an oscillating behavior. The shear-thinning effect acts on the system, favoring such oscillating behavior.
[Phys. Rev. Fluids 9, 023305] Published Wed Feb 28, 2024
Hysteresis and ribbons in Taylor-Couette flow of a semidilute noncolloidal suspension
Author(s): Changwoo Kang, Michael F. Schatz, and Parisa Mirbod
Flow states in dispersed particle flow determine the performance in industrial applications such as chemical mixers and bioreactors. Hysteresis in flow transitions can modify the flow condition and thus can affect the efficiency. We numerically show hysteretic behaviors in the Taylor-Couette flow of a noncolloidal suspension with a rotating inner cylinder and a stationary outer one. We also examine a standing wave of weak counterrotating vortices, known as ribbons, that occurs as the primary instability.
[Phys. Rev. Fluids 9, 023901] Published Wed Feb 28, 2024
Spherical thermal counterflow of superfluid $^{4}\mathrm{He}$
Author(s): F. Novotný, Y. Huang, J. Kvorka, Š Midlik, D. Schmoranzer, Z. Xie, and L. Skrbek
Spherically symmetric thermal counterflow of superfluid 4He driven by a central heater is unaffected by shear thanks to the absence of walls. This quantum flow displays a two-fluid behavior and upon increasing drive undergoes a complex process of transition to quantum turbulence that involves formation of normal fluid turbulence above a certain critical threshold, drawing energy from a preexisting random tangle of quantized vortices. Spherically symmetric thermal counterflow can serve as a model flow for cosmological phenomena relating cosmic strings to quantized vortices, for processes occurring in neutron stars, or cosmological structure formation within superfluid models of dark matter.
[Phys. Rev. Fluids 9, L022601] Published Wed Feb 28, 2024
Viscoplastic rimming flow inside a rotating cylinder
Author(s): Thomasina V. Ball and Neil J. Balmforth
When a small fraction of viscoplastic fluid is placed into a rotating cylinder, steady states can be reached with pool at the bottom of the cylinder and a residual coating elsewhere. Lubrication theory used to model the film thickness builds on previous models by bridging between two asymptotic limits, incorporating both the gravitational force along the cylinder and the hydrostatic pressure gradients. The model predicts steady states are reached after a small number of rotations and allows exploration of drainage when the cylinder comes to a halt. Experiments using a Carbopol suspension provide a suitable comparison to test the thin film theory.
[Phys. Rev. Fluids 9, 023304] Published Tue Feb 27, 2024
Neighbor-induced unsteady force in the interaction of a cylindrical shock wave with an annular particle cloud
Author(s): Sam Briney, Andreas N. Osnes, Magnus Vartdal, Thomas L. Jackson, and S. Balachandar
A shock propagating through a cloud of particles results in highly unsteady forces on each particle in the cloud. In such a finite particle volume fraction scenario, reflected shocks from neighboring particles perturb the force on each particle from its value in the dilute limit. These forces have a delayed onset since the reflected shocks travel at finite speeds. This phenomenon is explored in detail using three-dimensional particle resolved simulations and a model is proposed to account for the unsteady nature of these forces.
[Phys. Rev. Fluids 9, 024308] Published Tue Feb 27, 2024
Grid-generated velocity fields at very small Reynolds numbers
Author(s): Dana Duong and Stavros Tavoularis
This article is the first to investigate velocity fields behind grids at very small Reynolds numbers that include flows with negligible fluctuations. Measurements were taken behind four square-mesh grids with varying designs, mesh sizes and solidities. We have documented and quantified the weakening of turbulent behavior as the Reynolds number diminishes and identified trends and patterns of the large- and small-scale anisotropies, the skewness and flatness factors of the velocity derivative and the dissipation parameter that have not been reported previously.
[Phys. Rev. Fluids 9, 024607] Published Tue Feb 27, 2024
Artificially thickened boundary layer turbulence due to trip wires of varying diameter
Author(s): Zhanqi Tang, Nan Jiang, Zhiming Lu, and Quan Zhou
Tripping effects are studied in artificially thickened turbulent boundary layers (AT-TBLs) within a finite-length test section. The emergence of the generated large-scale structures highlights the potential of the AT-TBLs to simulate high-Reτ boundary layer turbulence. We examine the noncanonical behaviors and external similarity under over-tripped conditions. The results emphasize the need for caution when pursuing excessive thickening of the boundary layer through leading-edge trips for generating high-Reτ canonical TBLs in a finite-length test section.
[Phys. Rev. Fluids 9, 024606] Published Mon Feb 26, 2024
Superflow passing over a rough surface: Vortex nucleation
Author(s): Thomas Frisch, Sergey Nazarenko, and Sergio Rica
The dynamics of a superfluid over a surface exhibits significant differences from compressible flow in ordinary fluids. In ordinary fluids, when the local speed exceeds the sound speed, intrinsic dissipation due to viscosity can enable a shock wave. However, in superfluids, lack of dissipation prevents shock waves. Instead, spatial modulation of a wave train of solitons, as in the figure, allows for a smooth transonic transition. This wave train has been observed to eventually become unstable, leading to quantized vortices and an effective drag on a rough surface. The wave train occurs beneath a lambda-shaped structure with a fore and back-front, reminiscent of ordinary compressible fluids.
[Phys. Rev. Fluids 9, 024701] Published Mon Feb 26, 2024
Measurement of an eddy diffusivity for chaotic electroconvection using combined computational and experimental techniques
Author(s): Arunraj Balaji-Wright, Felix Stockmeier, Richard Dunkel, Matthias Wessling, and Ali Mani
The Poisson-Nernst-Planck-Stokes equations capture the chaotic dynamics of electroconvection accurately, but direct numerical simulation of electroconvection is prohibitively expensive. Furthermore, prediction of the mean fields via application of Reynolds averaging leads to a closure problem. In this work, we combine the macroscopic forcing method, a numerical technique for measurement of closure operators in Reynolds-averaged equations, with high-fidelity experimental data in order to determine a leading order closure for chaotic electroconvection. Simulations of the Reynolds-averaged equations using the leading order closure accurately predict experimental polarization curves.
[Phys. Rev. Fluids 9, 023701] Published Fri Feb 23, 2024
Plume-surface interaction during lunar landing using a two-way coupled DSMC-DEM approach
Author(s): A. Bajpai, A. Bhateja, and R. Kumar
In this investigation, a novel two-way coupled gas-granular solver is developed, incorporating direct simulation Monte Carlo (DSMC) for gas particle collisions and discrete element method (DEM) for granular particle interactions. Gas-grain interaction model consists of momentum and energy exchange between the two phases. Using this framework, we have performed a comprehensive study of dust dispersion due to plume impingement on a lunar surface. We have predicted not only the velocity field of gas and grain phases, but also their temperature field, which can be meaningful information for spacecraft designers.
[Phys. Rev. Fluids 9, 024306] Published Fri Feb 23, 2024
Trapping of inertial particles in a two-dimensional unequal-strength counterrotating vortex pair flow
Author(s): Zilong Zhao, Zhiwei Guo, Zhigang Zuo, and Zhongdong Qian
This study indicates that small inertia particles can be trapped in a two-dimensional unequal-strength counter-rotating vortex pair (CVP) flow. Through analytical derivations of the particle motion in the potential CVP flow, this study first identifies a particle-attracting ring S0.
[Phys. Rev. Fluids 9, 024307] Published Fri Feb 23, 2024
Bounded flows of dense gases
Author(s): Sergiu Busuioc and Victor Sofonea
Numerical solutions of the Enskog equation obtained employing a Finite-Difference Lattice Boltzmann (FDLB) with half-range Gauss-Hermite quadratures and a Direct Simulation Monte Carlo (DSMC)-like particle method (PM), are systematically compared to determine the range of applicability of the simplified Enskog collision operator implemented in the Lattice Boltzmann framework. For low to moderate reduced density, the proposed FDLB model exhibits commendable accuracy for all bounded flows tested in this study, with substantially lower computational cost than the PM method.
[Phys. Rev. Fluids 9, 023401] Published Thu Feb 22, 2024
Numerical analysis of flow anisotropy in rotated-square deterministic lateral displacement devices at moderate Reynolds number
Author(s): Calum Mallorie, Rohan Vernekar, Benjamin Owen, David W. Inglis, and Timm Krüger
Deterministic lateral displacement (DLD) is a common method of separating suspensions of particles by their physical properties. DLD devices are typically limited to operation in the Stokes flow regime, which leads to high processing times, because their behavior becomes unpredictable at flow rates where fluid inertia is important. In this study, we show that the average flow direction in a typical DLD device can diverge from the direction of the applied pressure drop due to inertial effects, and present an explanation for why this happens. This new understanding may contribute to improved DLD designs for operation at high flow rates.
[Phys. Rev. Fluids 9, 024203] Published Wed Feb 21, 2024
Statistical state dynamics-based study of the stability of the mean statistical state of wall-bounded turbulence
Author(s): Brian F. Farrell and Petros J. Ioannou
In wall turbulence, the time-mean flow is returned to after almost any disturbance, which indicates that it is a stable statistical feature underlying the disorder of turbulence. However, the stability of this statistical feature can not be determined directly from the stability of the time-mean flow itself. What is required is a statistical stability analysis method. We determine the statistical stability of the time-mean state by averaging the dynamics of the return to the time-mean state over the turbulent attractor using the linear inverse model method.
[Phys. Rev. Fluids 9, 024605] Published Wed Feb 21, 2024
Flow mode and global transport of liquid metal thermal convection in a cavity with $\mathrm{Γ}=1/3$
Author(s): Xin-Yuan Chen (陈新元), Juan-Cheng Yang (阳倦成), and Ming-Jiu Ni (倪明玖)
In this experimental investigation we examine the dynamics of liquid metal thermal convection within an elongated cuboid cell with aspect ratio 1/3. We highlight the evolution of flow modes, transitioning from single- to double-roll mode, and transitional modes which are reconstructed by visualizing temperature data on the sidewall. As the Rayleigh number surpasses the critical value, the flow state transforms from a multiple-mode coexistence state to a single-roll mode-dominated configuration. Flow modes and global transport properties offer profound insights into the fundamental characteristics of thermal convection in liquid metals under strong lateral geometric confinement.
[Phys. Rev. Fluids 9, 023503] Published Tue Feb 20, 2024
Role of flow structures on the deposition of low-inertia particles in turbulent pipe flow
Author(s): Rasmus Korslund Schlander, Stelios Rigopoulos, and George Papadakis
We characterize the role of coherent structures on the transport and wall deposition of low-inertia particles in a turbulent pipe flow using extended proper orthogonal decomposition (EPOD) and spectral analysis. The equilibrium Eulerian approach is employed to model particle velocity and concentration. A new Fukagata-Iwamoto-Kasagi (FIK) identity is derived for the wall deposition rate coefficient (Sherwood number) and employed to quantify the contributions of the mean and fluctuating velocity and particle concentration fields for different Stokes, Froude and Reynolds numbers. New terms appear due to the inertia of the particles that encapsulate the turbophoresis effect.
[Phys. Rev. Fluids 9, 024303] Published Tue Feb 20, 2024
From discrete to continuum description of weakly inertial bedload transport
Author(s): Benjamin Fry, Laurent Lacaze, Thomas Bonometti, Pierre Elyakime, and François Charru
Granular bedload plays a crucial role in shaping streams and influencing their development over time. This process involves the movement of grains along the stream bed surface driven by the shear stress from the flowing water. For an accurate model on a practical scale, it is essential to grasp the key properties of the granular layer interacting with the water. Our focus lies in understanding the rheological characteristics of the water grain mixture when grain movement is localized within a thin layer near the bed surface and under a weakly inertial regime. This aims to expand our understanding of viscous-laminar properties mostly described for a thick shear layer in the literature.
[Phys. Rev. Fluids 9, 024304] Published Tue Feb 20, 2024