@article{7397,
abstract = {Polymer additives can substantially reduce the drag of turbulent flows and the upperlimit, the so called “maximum drag reduction” (MDR) asymptote is universal, i.e. inde-pendent of the type of polymer and solvent used. Until recently, the consensus was that,in this limit, flows are in a marginal state where only a minimal level of turbulence activ-ity persists. Observations in direct numerical simulations using minimal sized channelsappeared to support this view and reported long “hibernation” periods where turbu-lence is marginalized. In simulations of pipe flow we find that, indeed, with increasingWeissenberg number (Wi), turbulence expresses long periods of hibernation if the domainsize is small. However, with increasing pipe length, the temporal hibernation continuouslyalters to spatio-temporal intermittency and here the flow consists of turbulent puffs sur-rounded by laminar flow. Moreover, upon an increase in Wi, the flow fully relaminarises,in agreement with recent experiments. At even larger Wi, a different instability is en-countered causing a drag increase towards MDR. Our findings hence link earlier minimalflow unit simulations with recent experiments and confirm that the addition of polymersinitially suppresses Newtonian turbulence and leads to a reverse transition. The MDRstate on the other hand results from a separate instability and the underlying dynamicscorresponds to the recently proposed state of elasto-inertial-turbulence (EIT).},
author = {Lopez Alonso, Jose M and Choueiri, George H and Hof, Björn},
issn = {0022-1120},
journal = {Journal of Fluid Mechanics},
pages = {699--719},
publisher = {CUP},
title = {{Dynamics of viscoelastic pipe flow at low Reynolds numbers in the maximum drag reduction limit}},
doi = {10.1017/jfm.2019.486},
volume = {874},
year = {2019},
}
@article{5878,
abstract = {We consider the motion of a droplet bouncing on a vibrating bath of the same fluid in the presence of a central potential. We formulate a rotation symmetry-reduced description of this system, which allows for the straightforward application of dynamical systems theory tools. As an illustration of the utility of the symmetry reduction, we apply it to a model of the pilot-wave system with a central harmonic force. We begin our analysis by identifying local bifurcations and the onset of chaos. We then describe the emergence of chaotic regions and their merging bifurcations, which lead to the formation of a global attractor. In this final regime, the droplet’s angular momentum spontaneously changes its sign as observed in the experiments of Perrard et al.},
author = {Budanur, Nazmi B and Fleury, Marc},
issn = {1089-7682},
journal = {Chaos: An Interdisciplinary Journal of Nonlinear Science},
number = {1},
publisher = {AIP Publishing},
title = {{State space geometry of the chaotic pilot-wave hydrodynamics}},
doi = {10.1063/1.5058279},
volume = {29},
year = {2019},
}
@article{5943,
abstract = {The hairpin instability of a jet in a crossflow (JICF) for a low jet-to-crossflow velocity ratio is investigated experimentally for a velocity ratio range of R ∈ (0.14, 0.75) and crossflow Reynolds numbers ReD ∈ (260, 640). From spectral analysis we characterize the Strouhal number and amplitude of the hairpin instability as a function of R and ReD. We demonstrate that the dynamics of the hairpins is well described by the Landau model, and, hence, that the instability occurs through Hopf bifurcation, similarly to other hydrodynamical oscillators such as wake behind different bluff bodies. Using the Landau model, we determine the precise threshold values of hairpin shedding. We also study the spatial dependence of this hydrodynamical instability, which shows a global behaviour.},
author = {Klotz, Lukasz and Gumowski, Konrad and Wesfreid, José Eduardo},
journal = {Journal of Fluid Mechanics},
pages = {386--406},
publisher = {Cambridge University Press},
title = {{Experiments on a jet in a crossflow in the low-velocity-ratio regime}},
doi = {10.1017/jfm.2018.974},
volume = {863},
year = {2019},
}
@article{6014,
abstract = {Speed of sound waves in gases and liquids are governed by the compressibility of the medium. There exists another type of non-dispersive wave where the wave speed depends on stress instead of elasticity of the medium. A well-known example is the Alfven wave, which propagates through plasma permeated by a magnetic field with the speed determined by magnetic tension. An elastic analogue of Alfven waves has been predicted in a flow of dilute polymer solution where the elastic stress of the stretching polymers determines the elastic wave speed. Here we present quantitative evidence of elastic Alfven waves in elastic turbulence of a viscoelastic creeping flow between two obstacles in channel flow. The key finding in the experimental proof is a nonlinear dependence of the elastic wave speed cel on the Weissenberg number Wi, which deviates from predictions based on a model of linear polymer elasticity.},
author = {Varshney, Atul and Steinberg, Victor},
issn = {2041-1723},
journal = {Nature Communications},
publisher = {Springer Nature},
title = {{Elastic alfven waves in elastic turbulence}},
doi = {10.1038/s41467-019-08551-0},
volume = {10},
year = {2019},
}
@article{6069,
abstract = {Electron transport in two-dimensional conducting materials such as graphene, with dominant electron–electron interaction, exhibits unusual vortex flow that leads to a nonlocal current-field relation (negative resistance), distinct from the classical Ohm’s law. The transport behavior of these materials is best described by low Reynolds number hydrodynamics, where the constitutive pressure–speed relation is Stoke’s law. Here we report evidence of such vortices observed in a viscous flow of Newtonian fluid in a microfluidic device consisting of a rectangular cavity—analogous to the electronic system. We extend our experimental observations to elliptic cavities of different eccentricities, and validate them by numerically solving bi-harmonic equation obtained for the viscous flow with no-slip boundary conditions. We verify the existence of a predicted threshold at which vortices appear. Strikingly, we find that a two-dimensional theoretical model captures the essential features of three-dimensional Stokes flow in experiments.},
author = {Mayzel, Jonathan and Steinberg, Victor and Varshney, Atul},
issn = {2041-1723},
journal = {Nature Communications},
publisher = {Springer Nature},
title = {{Stokes flow analogous to viscous electron current in graphene}},
doi = {10.1038/s41467-019-08916-5},
volume = {10},
year = {2019},
}
@article{6189,
abstract = {Suspended particles can alter the properties of fluids and in particular also affect the transition fromlaminar to turbulent flow. An earlier study [Mataset al.,Phys. Rev. Lett.90, 014501 (2003)] reported howthe subcritical (i.e., hysteretic) transition to turbulent puffs is affected by the addition of particles. Here weshow that in addition to this known transition, with increasing concentration a supercritical (i.e.,continuous) transition to a globally fluctuating state is found. At the same time the Newtonian-typetransition to puffs is delayed to larger Reynolds numbers. At even higher concentration only the globallyfluctuating state is found. The dynamics of particle laden flows are hence determined by two competinginstabilities that give rise to three flow regimes: Newtonian-type turbulence at low, a particle inducedglobally fluctuating state at high, and a coexistence state at intermediate concentrations.},
author = {Agrawal, Nishchal and Choueiri, George H and Hof, Björn},
issn = {10797114},
journal = {Physical Review Letters},
number = {11},
publisher = {APS},
title = {{Transition to turbulence in particle laden flows}},
doi = {10.1103/PhysRevLett.122.114502},
volume = {122},
year = {2019},
}
@article{6413,
abstract = {Phase-field methods have long been used to model the flow of immiscible fluids. Their ability to naturally capture interface topological changes is widely recognized, but their accuracy in simulating flows of real fluids in practical geometries is not established. We here quantitatively investigate the convergence of the phase-field method to the sharp-interface limit with simulations of two-phase pipe flow. We focus on core-annular flows, in which a highly viscous fluid is lubricated by a less viscous fluid, and validate our simulations with an analytic laminar solution, a formal linear stability analysis and also in the fully nonlinear regime. We demonstrate the ability of the phase-field method to accurately deal with non-rectangular geometry, strong advection, unsteady fluctuations and large viscosity contrast. We argue that phase-field methods are very promising for quantitatively studying moderately turbulent flows, especially at high concentrations of the disperse phase.},
author = {Song, Baofang and Plana, Carlos and Lopez Alonso, Jose M and Avila, Marc},
issn = {03019322},
journal = {International Journal of Multiphase Flow},
pages = {14--24},
publisher = {Elsevier},
title = {{Phase-field simulation of core-annular pipe flow}},
doi = {10.1016/j.ijmultiphaseflow.2019.04.027},
volume = {117},
year = {2019},
}
@article{6508,
abstract = {Segregation of maternal determinants within the oocyte constitutes the first step in embryo patterning. In zebrafish oocytes, extensive ooplasmic streaming leads to the segregation of ooplasm from yolk granules along the animal-vegetal axis of the oocyte. Here, we show that this process does not rely on cortical actin reorganization, as previously thought, but instead on a cell-cycle-dependent bulk actin polymerization wave traveling from the animal to the vegetal pole of the oocyte. This wave functions in segregation by both pulling ooplasm animally and pushing yolk granules vegetally. Using biophysical experimentation and theory, we show that ooplasm pulling is mediated by bulk actin network flows exerting friction forces on the ooplasm, while yolk granule pushing is achieved by a mechanism closely resembling actin comet formation on yolk granules. Our study defines a novel role of cell-cycle-controlled bulk actin polymerization waves in oocyte polarization via ooplasmic segregation.},
author = {Shamipour, Shayan and Kardos, Roland and Xue, Shi-lei and Hof, Björn and Hannezo, Edouard B and Heisenberg, Carl-Philipp J},
issn = {10974172},
journal = {Cell},
number = {6},
pages = {1463--1479.e18},
publisher = {Elsevier},
title = {{Bulk actin dynamics drive phase segregation in zebrafish oocytes}},
doi = {10.1016/j.cell.2019.04.030},
volume = {177},
year = {2019},
}
@article{6779,
abstract = {Recent studies suggest that unstable recurrent solutions of the Navier-Stokes equation provide new insights
into dynamics of turbulent flows. In this study, we compute an extensive network of dynamical connections
between such solutions in a weakly turbulent quasi-two-dimensional Kolmogorov flow that lies in the inversion symmetric subspace. In particular, we find numerous isolated heteroclinic connections between different
types of solutions—equilibria, periodic, and quasiperiodic orbits—as well as continua of connections forming
higher-dimensional connecting manifolds. We also compute a homoclinic connection of a periodic orbit and
provide strong evidence that the associated homoclinic tangle forms the chaotic repeller that underpins transient
turbulence in the symmetric subspace.},
author = {Suri, Balachandra and Pallantla, Ravi Kumar and Schatz, Michael F. and Grigoriev, Roman O.},
issn = {2470-0053},
journal = {Physical Review E},
number = {1},
publisher = {APS},
title = {{Heteroclinic and homoclinic connections in a Kolmogorov-like flow}},
doi = {10.1103/physreve.100.013112},
volume = {100},
year = {2019},
}
@phdthesis{6957,
abstract = {In many shear flows like pipe flow, plane Couette flow, plane Poiseuille flow, etc. turbulence emerges subcritically. Here, when subjected to strong enough perturbations, the flow becomes turbulent in spite of the laminar base flow being linearly stable. The nature of this instability has puzzled the scientific community for decades. At onset, turbulence appears in localized patches and flows are spatio-temporally intermittent. In pipe flow the localized turbulent structures are referred to as puffs and in planar flows like plane Couette and channel flow, patches arise in the form of localized oblique bands. In this thesis, we study the onset of turbulence in channel flow in direct numerical simulations from a dynamical system theory perspective, as well as by performing experiments in a large aspect ratio channel.
The aim of the experimental work is to determine the critical Reynolds number where turbulence first becomes sustained. Recently, the onset of turbulence has been described in analogy to absorbing state phase transition (i.e. directed percolation). In particular, it has been shown that the critical point can be estimated from the competition between spreading and decay processes. Here, by performing experiments, we identify the mechanisms underlying turbulence proliferation in channel flow and find the critical Reynolds number, above which turbulence becomes sustained. Above the critical point, the continuous growth at the tip of the stripes outweighs the stochastic shedding of turbulent patches at the tail and the stripes expand. For growing stripes, the probability to decay decreases while the probability of stripe splitting increases. Consequently, and unlike for the puffs in pipe flow, neither of these two processes is time-independent i.e. memoryless. Coupling between stripe expansion and creation of new stripes via splitting leads to a significantly lower critical point ($Re_c=670+/-10$) than most earlier studies suggest.
While the above approach sheds light on how turbulence first becomes sustained, it provides no insight into the origin of the stripes themselves. In the numerical part of the thesis we investigate how turbulent stripes form from invariant solutions of the Navier-Stokes equations. The origin of these turbulent stripes can be identified by applying concepts from the dynamical system theory. In doing so, we identify the exact coherent structures underlying stripes and their bifurcations and how they give rise to the turbulent attractor in phase space. We first report a family of localized nonlinear traveling wave solutions of the Navier-Stokes equations in channel flow. These solutions show structural similarities with turbulent stripes in experiments like obliqueness, quasi-streamwise streaks and vortices, etc. A parametric study of these traveling wave solution is performed, with parameters like Reynolds number, stripe tilt angle and domain size, including the stability of the solutions. These solutions emerge through saddle-node bifurcations and form a phase space skeleton for the turbulent stripes observed in the experiments. The lower branches of these TW solutions at different tilt angles undergo Hopf bifurcation and new solutions branches of relative periodic orbits emerge. These RPO solutions do not belong to the same family and therefore the routes to chaos for different angles are different.
In shear flows, turbulence at onset is transient in nature. Consequently,turbulence can not be tracked to lower Reynolds numbers, where the dynamics may simplify. Before this happens, turbulence becomes short-lived and laminarizes. In the last part of the thesis, we show that using numerical simulations we can continue turbulent stripes in channel flow past the 'relaminarization barrier' all the way to their origin. Here, turbulent stripe dynamics simplifies and the fluctuations are no longer stochastic and the stripe settles down to a relative periodic orbit. This relative periodic orbit originates from the aforementioned traveling wave solutions. Starting from the relative periodic orbit, a small increase in speed i.e. Reynolds number gives rise to chaos and the attractor dimension sharply increases in contrast to the classical transition scenario where the instabilities affect the flow globally and give rise to much more gradual route to turbulence.},
author = {Paranjape, Chaitanya S},
issn = {2663-337X},
keywords = {Instabilities, Turbulence, Nonlinear dynamics},
pages = {138},
publisher = {IST Austria},
title = {{Onset of turbulence in plane Poiseuille flow}},
doi = {10.15479/AT:ISTA:6957},
year = {2019},
}