## Publications

37 results found

Doohan P, Willis A, Hwang Y, 2019, Shear stress-driven flow: the state space of near-wall turbulence as Reτ →∞, *Journal of Fluid Mechanics*, Vol: 874, Pages: 606-638, ISSN: 0022-1120

An inner-scaled, shear stress-driven flow is considered as a model of independentnear-wall turbulence as Reτ → ∞. In this limit, the model is applicable to the nearwall region and the lower part of the logarithmic layer of various parallel shear flows,including turbulent Couette flow, Poiseuille flow and Hagen-Poiseuille flow. The modelis validated against damped Couette flow and there is excellent agreement between thevelocity statistics and spectra for y+ < 40. A near-wall flow domain of similar size tothe minimal unit is analysed from a dynamical systems perspective. The edge and fifteeninvariant solutions are computed, the first discovered for this flow configuration. Throughcontinuation in the spanwise width L+z, the bifurcation behaviour of the solutions overthe domain size is investigated. The physical properties of the solutions are exploredthrough phase portraits, including the energy input and dissipation plane, and streak,roll and wave energy space. Finally, a Reynolds number is defined in outer units and thehigh-Re asymptotic behaviour of the equilibria is studied. Three lower branch solutionsare found to scale consistently with vortex-wave interaction (VWI) theory, with waveforcing localising around the critical layer.

Lakshmi M, Fantuzzi G, Fernández-Caballero J, et al., 2019, Finding extremal periodic orbits with polynomial optimisation, with application to a nine-mode model of shear flow, Publisher: arXiv

Tobasco et al. [Physics Letters A, 382:382-386, 2018] recently suggested thattrajectories of ODE systems which optimise the infinite-time average of acertain observable can be localised using sublevel sets of a function thatarise when bounding such averages using so-called auxiliary functions. In thispaper we demonstrate that this idea is viable and allows for the computation ofextremal unstable periodic orbits (UPOs) for polynomial ODE systems. First, weprove that polynomial optimisation is guaranteed to produce auxiliary functionsthat yield near-sharp bounds on time averages, which is required in order tolocalise the extremal orbit accurately. Second, we show that points inside therelevant sublevel sets can be computed efficiently through direct nonlinearoptimisation. Such points provide good initial conditions for UPO computations.We then combine these methods with a single-shooting Newton-Raphson algorithmto study extremal UPOs for a nine-dimensional model of sinusoidally forcedshear flow. We discover three previously unknown families of UPOs, one of whichsimultaneously minimises the mean energy dissipation rate and maximises themean perturbation energy relative to the laminar state for Reynolds numbersapproximately between 81.24 and 125.

Smitha M, Keaveny E, Hwang Y, The instability of gyrotactically-trapped cell layers, *Journal of Fluid Mechanics*, ISSN: 0022-1120

Several meters below the coastal ocean surface there are areas of high ecological activitythat contain thin layers of concentrated motile phytoplankton. Gyrotactic trapping hasbeen proposed as a potential mechanism for layer formation of bottom-heavy swimmingalgae cells, especially in flows where the vorticity varies linearly with depth (Durham,Stocker & Kessler,Science, vol. 323, 2009, pp. 1067-1070). Using a continuum modelfor dilute microswimmer suspensions, we report that an instability of a gyrotacticallytrapped cell-layer can arise in a pressure-driven plane channel flow. The linear stabilityanalysis reveals that the equilibrium cell-layer solution is hydrodynamically unstabledue to negative microswimmer buoyancy (i.e. a gravitational instability) over a range ofbiologically relevant parameter values. The critical cell concentration for this instabilityis found to beNc'104cells/cm3, a value comparable to the typical maximum cellconcentration observed in thin layers. This result indicates that the instability may bea potential mechanism for limiting the layer’s maximum cell concentration, especiallyin regions where turbulence is weak, and motivates the study of its nonlinear evolution,perhaps, in the presence of turbulence.

Yang Q, Willis A, Hwang Y, 2019, Exact coherent states of attached eddies in channel flow, *Journal of Fluid Mechanics*, Vol: 862, Pages: 1029-1059, ISSN: 0022-1120

A new set of exact coherent states in the form of a travelling wave is reported in plane channel flow. They are continued over a range in Re from approximately 2600 up to 30 000, an order of magnitude higher than those discovered in the transitional regime. This particular type of exact coherent states is found to be gradually more localised in the near-wall region on increasing the Reynolds number. As larger spanwise sizes L + z are considered, these exact coherent states appear via a saddle-node bifurcation with a spanwise size of L + z ' 50 and their phase speed is found to be c + ' 11 at all the Reynolds numbers considered. Computation of the eigenspectra shows that the time scale of the exact coherent states is given by h/Ucl in channel flow at all Reynolds numbers, and it becomes equivalent to the viscous inner time scale for the exact coherent states in the limit of Re → ∞. The exact coherent states at several different spanwise sizes are further continued to a higher Reynolds number, Re = 55 000, using the eddy-viscosity approach (Hwang & Cossu, Phys. Rev. Lett., vol. 105, 2010, 044505). It is found that the continued exact coherent states at different sizes are self-similar at the given Reynolds number. These observations suggest that, on increasing Reynolds number, new sets of self-sustaining coherent structures are born in the near-wall region. Near this onset, these structures scale in inner units, forming the near-wall self-sustaining structures. With further increase of Reynolds number, the structures that emerged at lower Reynolds numbers subsequently evolve into the self-sustaining structures in the logarithmic region at different length scales, forming a hierarchy of self-similar coherent structures as hypothesised by Townsend (i.e. attached eddy hypothesis). Finally, the energetics of turbulent flow is discussed for a consistent extension of these dynamical systems notions to high Reynolds numbers.

Ibrahim J, Yang Q, Doohan P,
et al., 2019, Phase-space dynamics of opposition control in wall-bounded turbulent flows, *Journal of Fluid Mechanics*, Vol: 861, Pages: 29-54, ISSN: 0022-1120

We investigate the nonlinear phase-space dynamics of plane Couette flow and plane Poiseuille flow under the action of opposition control at low Reynolds numbers in domains close to the minimal unit. In Couette flow, the effect of the control is analysed by focussing on a pair of non-trivial equilibrium solutions. It is found that the control only slightly modifies the statistics, turbulent skin friction and phase-space projection of the lower-branch equilibrium solution, which, in this case, is in fact identical to the edge state. On the other hand, the upper-branch equilibrium solution and mean turbulent state are modified considerably when the control is applied. In phase space, they gradually approach the lower-branch equilibrium solution on increasing the control amplitude, and this results in an elevation of the critical Reynolds number at which the equilibrium solutions first occur via a saddle-node bifurcation. It is also found that the upper-branch equilibrium solution is stabilised by the control. In Poiseuille flow, we study an unstable periodic orbit on the edge state and find that it, too, is modified very little by opposition control. We again observe that the turbulent state gradually approaches the edge state in phase space as the control amplitude is increased. In both flows, we find that the control significantly reduces the fluctuating strength of the turbulent state in phase space. However, the reduced distance between the turbulent trajectory and the edge state yields a significant reduction in turbulence lifetimes for both Couette and Poiseuille flow. This demonstrates that opposition control greatly increases the probability of the trajectory escaping from the turbulent state, which takes the form of a chaotic saddle.

Maretvadakethope S, Keaveny EE, Hwang Y, 2019, The instability of gyrotactically trapped cell layers

© 2019 Cambridge University Press. Several metres below the coastal ocean surface there are areas of high ecological activity that contain thin layers of concentrated motile phytoplankton. Gyrotactic trapping has been proposed as a potential mechanism for layer formation of bottom-heavy swimming algae cells, especially in flows where the vorticity varies linearly with depth (Durham et al.Science, vol. 323(5917), 2009, pp. 1067-1070). Using a continuum model for dilute microswimmer suspensions, we report that an instability of a gyrotactically trapped cell layer can arise in a pressure-driven plane channel flow. The linear stability analysis reveals that the equilibrium cell-layer solution is hydrodynamically unstable due to negative microswimmer buoyancy (i.e. a gravitational instability) over a range of biologically relevant parameter values. The critical cell concentration for this instability is found to be, a value comparable to the typical maximum cell concentration observed in thin layers. This result indicates that the instability may be a potential mechanism for limiting the layer's maximum cell concentration, especially in regions where turbulence is weak, and motivates the study of its nonlinear evolution, perhaps, in the presence of turbulence.

Dunstan J, Lee K, Hwang Y,
et al., 2018, Evaporation-driven convective flows in suspensions of non-motile bacteria, *Physical Review Fluids*, Vol: 13, ISSN: 2469-990X

We report a novel form of convection in suspensions of the bioluminescent marine bacterium Photobacterium phosphoreum. Suspensions of these bacteria placed in a chamber open to the air create persistent luminescent plumes most easily visible when observed in the dark. These flows are strikingly similar to the classical bioconvection pattern of aerotactic swimming bacteria, which create an unstable stratification by swimming upwards to an air-water interface, but they are a puzzle since the strain of P. phosphoreum used does not express flagella and therefore cannot swim. When microspheres were used instead of bacteria, similar flow patterns were observed, suggesting that the convective motion was not driven by bacteria but instead by the accumulation of salt at the air-water interface due to evaporation of the culture medium. Even at room temperature and humidity, and physiologically relevant salt concentrations, the water evaporation was found to be sufficient to drive convection patterns. To prove this hypothesis, experiments were complemented with a mathematical model that aimed to understand the mechanism of plume formation and the role of salt in triggering the instability. The simplified system of evaporating salty water was first studied using linear stability analysis, and then with finite element simulations. A comparison between these three approaches is presented. While evaporation-driven convection has not been discussed extensively in the context of biological systems, these results suggest that the phenomenon may be broadly relevant, particularly in those systems involving microorganisms of limited motility.

Cho M, Hwang Y, Choi H, 2018, Scale interactions and spectral energy transfer in turbulent channel flow, *Journal of Fluid Mechanics*, Vol: 854, Pages: 474-504, ISSN: 0022-1120

Spectral energy transfer in a turbulent channel flow is investigated at Reynolds number Re ≃1700 , based on the wall shear velocity and channel half-height, with a particular emphasis on full visualization of triadic wave interactions involved in turbulent transport. As in previous studies, turbulent production is found to be almost uniform, especially over the logarithmic region, and the related spanwise integral length scale is approximately proportional to the distance from the wall. In the logarithmic and outer regions, the energy balance at the integral length scales is mainly formed between production and nonlinear turbulent transport, the latter of which plays the central role in the energy cascade down to the Kolmogorov microscale. While confirming the classical role of the turbulent transport, the triadic wave interaction analysis unveils two new types of scale interaction processes, highly active in the near-wall and the lower logarithmic regions. First, for relatively small energy-containing motions, part of the energy transfer mechanisms from the integral to the adjacent small length scale in the energy cascade is found to be provided by the interactions between larger energy-containing motions. It is subsequently shown that this is related to involvement of large energy-containing motions in skin-friction generation. Second, there exists a non-negligible amount of energy transfer from small to large integral scales in the process of downward energy transfer to the near-wall region. This type of scale interaction is predominant only for the streamwise and spanwise velocity components, and it plays a central role in the formation of the wall-reaching inactive part of large energy-containing motions. A further analysis reveals that this type of scale interaction leads the wall-reaching inactive part to scale in the inner units, consistent with the recent observation. Finally, it is proposed that turbulence production and pressure–strain spectra supp

Pausch M, Yang Q, Hwang Y,
et al., 2018, Quasilinear approximation for exact coherent states in parallel shearflows, *Fluid Dynamics Research*, ISSN: 0169-5983

n the quasilinear approximation to the Navier-Stokes equation a minimalset of nonlinearities that is able to maintain turbulent dynamics is kept.Fortransitional Reynolds numbers, exact coherent structures provide an opportunity fora detailed comparison between full direct numerical solutions of the Navier-Stokesequation with their quasilinear approximation. We here show for both plane Couetteflow and plane Poiseuille flow that the quasilinear approximation is able to reproducethe mean properties of exact coherent structures. For higher Reynolds numbersdifferences in the stability properties and the friction values for the upper branchappear that are connected with a reduction in the number of downstream wavenumbersin the quasilinear approximation. The results show the strengths and limitations ofthe quasilinear approximation and suggest modelling approaches for turbulent flows.

Yang Q, Willis AP, Hwang Y, 2017, Energy production and self-sustained turbulence at the Kolmogorov scale inCouette flow, *Journal of Fluid Mechanics*, Vol: 834, Pages: 531-554, ISSN: 0022-1120

Several recent studies have reported that there exists a self-similar form of invariant solutions down to the Kolmogorov microscale in the bulk region of turbulent Couette flow. While their role in a fully developed turbulent flow is yet to be identified, here we report that there exists a related mechanism of turbulence production at the Kolmogorov microscale in the bulk region of turbulent Couette flow by performing a set of minimal-span direct numerical simulations up to friction Reynolds number . This mechanism is found to essentially originate from the non-zero mean shear in the bulk region of the Couette flow, and involves eddy turn-over dynamics remarkably similar to the so-called self-sustaining process (SSP) and/or vortex–wave interaction (VWI). A numerical experiment that removes all other motions except in the core region is also performed, which demonstrates that the eddies at a given wall-normal location in the bulk region are sustained in the absence of other motions at different wall-normal locations. It is proposed that the self-sustaining eddies at the Kolmogorov microscale correspond to those in uniform shear turbulence at transitional Reynolds numbers, and a quantitative comparison between the eddies in uniform shear and near-wall turbulence is subsequently made. Finally, it is shown that turbulence production by the self-sustaining eddies at the Kolmogorov microscale is much smaller than that of full-scale simulations, and that the difference between the two increases with Reynolds number.

de Giovanetti M, Sung HJ, Hwang Y, 2017, Streak instability in turbulent channel flow: the seeding mechanism of large-scale motions, *Journal of Fluid Mechanics*, Vol: 832, Pages: 483-513, ISSN: 0022-1120

It has often been proposed that the formation of large-scale motion (or bulges) is aconsequence of successive mergers and/or growth of near-wall hairpin vortices. In thepresent study, we report our direct observation that large-scale motion is generated byan instability of an ‘amplified’ streaky motion in the outer region (i.e. very-large-scalemotion). We design a numerical experiment in turbulent channel flow up to Reτ '2000where a streamwise-uniform streaky motion is artificially driven by body forcing inthe outer region computed from the previous linear theory (Hwang & Cossu, J. FluidMech., vol. 664, 2015, pp. 51–73). As the forcing amplitude is increased, it is foundthat an energetic streamwise vortical structure emerges at a streamwise wavelength ofλx/h '1–5 (h is the half-height of the channel). The application of dynamic modedecomposition and the examination of turbulence statistics reveal that this structureis a consequence of the sinuous-mode instability of the streak, a subprocess of theself-sustaining mechanism of the large-scale outer structures. It is also found that thestatistical features of the vortical structure are remarkably similar to those of the largescalemotion in the outer region. Finally, it is proposed that the largest streamwiselength of the streak instability determines the streamwise length scale of very-largescalemotion.

Cassinelli A, de Giovanetti M, Hwang Y, Streak instability in near-wall turbulence revisited, *Journal of Turbulence*, ISSN: 1468-5248

The regeneration cycle of streaks and streamwise vortices plays a central role in the sustain-ment of near-wall turbulence. In particular, the streak breakdown phase in the regenerationcycle is the core process in the formation of the streamwise vortices, but its current under-standing is limited particularly in a real turbulent environment. This study is aimed at gainingfundamental insight into the underlying physical mechanism of the streak breakdown in thepresence of background turbulent uctuation. We perform a numerical experiment based ondirect numerical simulation, in which streaks are arti cially generated by a body forcingcomputed from previous linear theory. Upon increasing the forcing amplitude, the arti ciallydriven streaks are found to generate an intense uctuation of the wall-normal and spanwisevelocities in a fairly large range of amplitudes. This cross-streamwise velocity uctuationshows its maximum atλ+x≈20000 (λ+xis the inner-scaled streamwise wavelength), but itonly appears forλ+x≤3000 - 4000. Further examination with dynamic mode decompositionreveals that the related ow eld is composed of sinuous meandering motion of the drivenstreaks and alternating cross-streamwise velocity structures, clearly reminiscent of sinuous-mode streak instability found in previous studies. Finally, it is shown that these structuresare reasonably well aligned along the critical layer of the secondary instability, indicating thatthe surrounding turbulence does not signi cantly modify the inviscid in ectional mechanismof the streak breakdown via streak instability and/or streak transient growth.

de Giovanetti M, Hwang Y, Choi H, 2016, Skin-friction generation by attached eddies in turbulent channel flow, *Journal of Fluid Mechanics*, Vol: 808, Pages: 511-538, ISSN: 1469-7645

Despite a growing body of recent evidence on the hierarchical organization of the selfsimilarenergy-containing motions in the form of Townsend’s attached eddies in wallboundedturbulent flows, their role in turbulent skin-friction generation is currentlyknown very little. In this paper, the contribution of each of these self-similar energycontainingmotions to turbulent skin friction is explored up to Reτ ≃ 4000. Threedifferent approaches are employed to quantify the skin-friction generation by the motions,the spanwise length scale of which is smaller than a given cut-off wavelength: 1) FIKidentity in combination with the spanwise wavenumber spectra of the Reynolds shearstress; 2) confinement of the spanwise computational domain; 3) artificial damping ofthe motions to be examined. The near-wall motions are found to continuously lose theirrole in skin-friction generation on increasing the Reynolds number, consistent with theprevious finding at low Reynolds numbers. The largest structures given in the form ofvery-large-scale and large-scale motions are also found to be of limited importance: dueto a non-trivial scale-interaction process, their complete removal yields only 5 ∼ 8% ofskin-friction reduction at all the Reynolds numbers considered, although they are foundto be responsible for 20 ∼ 30% of total skin friction at Reτ ≃ 2000. Application of all thethree approaches consistently reveals that the largest amount of skin friction is generatedby the self-similar motions populating the logarithmic region. It is further shown thatthe contribution of these motions to turbulent skin friction gradually increases with theReynolds number, and that these coherent structures are eventually responsible for mostof turbulent skin-friction generation at sufficiently high Reynolds numbers.

Cossu C, Hwang Y, Self-sustaining processes at all scales in wall-boundedturbulent shear flows, *Royal Society of London. Philosophical Transactions A. Mathematical, Physical and Engineering Sciences*, ISSN: 1364-503X

We collect and discuss the results of our recentstudies which show evidence of the existence ofa whole family of self-sustaining motions in wallboundedturbulent shear flows with scales rangingfrom those of buffer-layer streaks to those of largescaleand very-large-scale motions in the outer layer.The statistical and dynamical features of this familyof self-sustaining motions, which are associated withstreaks and quasi-streamwise vortices, are consistentwith those of Townsend’s attached eddies. Motionsat each relevant scale are able to sustain themselvesin the absence of forcing from larger- or smaller-scalemotions by extracting energy from the mean flow viaa coherent lift-up effect. The coherent self-sustainingprocess is embedded in a set of invariant solutions ofthe filtered Navier-Stokes equations which take intofull account the Reynolds stresses associated with theresidual smaller-scale motions.

Hwang Y, 2016, Mesolayer of attached eddies in turbulent channel flow, *Physical Review Fluids*, ISSN: 2469-990X

Recent experimental measurements have reported that the outer peak of the streamwisewavenumber spectra of the streamwise velocity depends on the Reynolds number. Starting fromthis puzzling observation, here it is proposed that the wall-parallel velocity components of eachof the energy-containing motions in the form of Towsnend’s attached eddies exhibit inner-scalingnature in the region close to the wall. Some compelling evidence on this proposition has been presentedwith a careful inspection of scaling of velocity spectra from DNS, a linear analysis with aneddy viscosity, and the recently computed statistical structure of the self-similar energy-containingmotions in the logarithmic region. This observation suggests that the viscous wall effect wouldnot be negligible at least below the peak wall-normal location of each of the energy-containingmotions in the logarithmic and outer regions, reminiscent of the concept of the ‘mesolayer’ previouslyobserved in the mean momentum balance. It is shown that this behavior emerges due to aminimal form of scale interaction, modeled by the eddy viscosity in the linear theory, and enablesone to explain the Reynolds-number-dependent behavior of the outer peak as well as the near-wallpenetration of the large-scale outer structures in a consistent manner. Incorporation of this viscouswall effect to Townsend’s attached eddies, which were originally built with an inviscid approximationat the wall, also reveals that the self-similarity of the wall-parallel velocity components of theenergy-containing motions would be theoretically broken in the region close to the wall.

Hwang Y, Willis AP, Cossu C, 2016, Invariant solutions of minimal large-scale structures in turbulent channel flow for Reτ up to 1000, *Journal of Fluid Mechanics*, Vol: 802, ISSN: 1469-7645

Understanding the origin of large-scale structures in high Reynolds number wall turbulencehas been a central issue over a number of years. Recently, Rawat et al. (J.Fluid Mech., 2015, 782, p515) have computed invariant solutions for the large-scalestructures in turbulent Couette flow at Reτ ≃ 128 using an over-damped LES with theSmagorinsky model to account for the effect of the surrounding small-scale motions.Here, we extend this approach to an order of magnitude higher Reynolds numbers inturbulent channel flow, towards the regime where the large-scale structures in the formof very-large-scale motions (long streaky motions) and large-scale motions (short vorticalstructures) energetically emerge. We demonstrate that a set of invariant solutions canbe computed from simulations of the self-sustaining large-scale structures in the minimalunit (domain of size Lx = 3.0h streamwise and Lz = 1.5h spanwise) with midplanereflection symmetry at least up to Reτ ≃ 1000. By approximating the surrounding smallscales with an artificially elevated Smagorinsky constant, a set of equilibrium states arefound, labelled upper- and lower-branch according to their associated drag. It is shownthat the upper-branch equilibrium state is a reasonable proxy for the spatial structureand the turbulent statistics of the self-sustaining large-scale structures.

Hwang Y, Bengana Y, 2016, Self-sustaining process of minimal attached eddies in turbulent channel flow, *Journal of Fluid Mechanics*, Vol: 795, Pages: 708-738, ISSN: 1469-7645

It has been recently shown that the energy-containing motions (i.e. coherent structures)in turbulent channel flow exist in the form of Townsend’s attached eddies by a numericalexperiment which simulates the energy-containing motions only at a prescribed spanwiselength scale using their self-sustaining nature (Hwang, 2015, J. Fluid Mech., 767,p254). In the present study, a detailed investigation of the self-sustaining process of theenergy-containing motions at each spanwise length scale (i.e. the attached eddies) inthe logarithmic and outer regions is carried out with an emphasis on its relevance to‘bursting’, which refers to an energetic temporal oscillation of the motions (Flores &Jim´enez, 2010, Phys. Fluids, 22, 071704). It is shown that the attached eddies in thelogarithmic and outer regions, composed of streaks and quasi-streamwise vortical structures,bear the self-sustaining process remarkably similar to that in the near-wall region:i.e. the streaks are significantly amplified by the quasi-streamwise vortices via the liftupeffect; the amplified streaks subsequently undergo a ‘rapid streamwise meanderingmotion’, reminiscent of streak instability or transient growth, which eventually resultsin breakdown of the streaks and regeneration of new quasi-streamwise vortices. For theattached eddies at a given spanwise length scale λz between λ+z ≃ 100 and λz ≃ 1.5h,the single turn-over time period of the self-sustaining process is found to be T uτ /λz ≃ 2(uτ is the friction velocity), which corresponds well to the time scale of the bursting.Two additional numerical experiments, designed to artificially suppress the lift-up effectand the streak meandering motions, respectively, reveal that these processes are essentialingredients of the self-sustaining process of the attached eddies in the logarithmic andouter regions, consistent with several previous theoretical studies. It is also shown thatthe

Rawat S, Cossu C, Hwang Y,
et al., 2015, On the self-sustained nature of large-scale motions in turbulent Couette flow, *Journal of Fluid Mechanics*, Vol: 782, Pages: 515-540, ISSN: 1469-7645

Hogan B, Babataheri A, Hwang Y,
et al., 2015, Characterizing cell adhesion by using micropipette aspiration, *Biophysical Journal*, Vol: 109, Pages: 209-219, ISSN: 1542-0086

Gouget CLM, Hwang Y, Barakat AI, 2015, Model of cellular mechanotransduction via actin stress fibers, *Biomechanics and Modeling in Mechanobiology*, Vol: 15, Pages: 331-344, ISSN: 1617-7959

Hwang Y, 2015, Statistical structure of self-sustaining attached eddies in turbulent channel flow, *Journal of Fluid Mechanics*, Vol: 767, Pages: 254-289, ISSN: 1469-7645

Hwang Y, Kumar P, Barakat AI, 2014, Intracellular regulation of cell signaling cascades: how location makes a difference, *JOURNAL OF MATHEMATICAL BIOLOGY*, Vol: 69, Pages: 213-242, ISSN: 0303-6812

- Author Web Link
- Cite
- Citations: 5

Hwang Y, Pedley TJ, 2014, Stability of downflowing gyrotactic microorganism suspensions in a two-dimensional vertical channel, *Journal of Fluid Mechanics*, Vol: 749, Pages: 750-777, ISSN: 1469-7645

Hwang Y, 2014, Structural sensitivities of soft and steep nonlinear global modes in spatially developing media, *European Journal of Mechanics B - Fluids*, Vol: 49, Pages: 322-334, ISSN: 0997-7546

Hwang Y, Pedley TJ, 2013, Bioconvection under uniform shear: linear stability analysis, *Journal of Fluid Mechanics*, Vol: 738, Pages: 522-562, ISSN: 1469-7645

Hwang Y, Kim J, Choi H, 2013, Stabilization of absolute instability in spanwise wavy two-dimensional wakes, *JOURNAL OF FLUID MECHANICS*, Vol: 727, Pages: 346-378, ISSN: 0022-1120

- Author Web Link
- Open Access Link
- Cite
- Citations: 27

Hwang Y, 2013, Near-wall turbulent fluctuations in the absence of wide outer motions, *Journal of Fluid Mechanics*, Vol: 723, Pages: 264-288, ISSN: 0022-1120

Numerical experiments that remove turbulent motions wider than λz+ ∼ 100 are carried out up to Reφ = 660 in a turbulent channel. The artificial removal of the wide outer turbulence is conducted with spanwise minimal computational domains and an explicit filter that effectively removes spanwise uniform eddies. The mean velocity profile of the remaining motions shows very good agreement with that of the full simulation below y+ ∼ 40, and the near-wall peaks of the streamwise velocity fluctuation scale very well in the inner units and remain almost constant at all the Reynolds numbers considered. The self-sustaining motions narrower than λz+ ∼ 100 generate smaller turbulent skin friction than full turbulent motions, and their contribution to turbulent skin friction gradually decays with the Reynolds number. This finding suggests that the role of the removed outer structures becomes increasingly important with the Reynolds number; thus one should aim to control the large scales for turbulent drag reduction at high Reynolds numbers. In the near-wall region, the streamwise and spanwise velocity fluctuations of the motions of λ z+ ≤ 100 reveal significant lack of energy at long streamwise lengths compared to those of the full simulation. In contrast, the losses of the wall-normal velocity and the Reynolds stress are not as large as those of these two variables. This implies that the streamwise and spanwise velocities of the removed motions penetrate deep into the near-wall region, while the wall-normal velocity and the Reynolds stress do not. © 2013 Cambridge University Press.

Hwang Y, Gouget CLM, Barakat AI, 2012, Mechanisms of cytoskeleton-mediated mechanical signal transmission in cells, *Communicative and Integrative Biology*, Vol: 5, Pages: 538-542, ISSN: 1942-0889

Recent experiments have demonstrated very rapid long-distance transmission of mechanical forces within cells. Because the speed of this transmission greatly exceeds that of reaction-diffusion signaling, it has been conjectured that it occurs via the propagation of elastic waves through the actin stress fiber network. To explore the plausibility of this conjecture, we recently developed a model of small amplitude stress fiber deformations in prestressed viscoelastic stress fibers subjected to external forces. The model results demonstrated that rapid mechanical signal transmission is only possible when the external force is applied orthogonal to the stress fiber axis and that the dynamics of this transmission are governed by a balance between the prestress in the stress fiber and the stress fiber's material viscosity. The present study, which is a follow-up on our previous model, uses dimensional analysis to: (1) further evaluate the plausibility of the elastic wave conjecture and (2) obtain insight into mechanical signal transmission dynamics in simple stress fiber networks. We show that the elastic wave scenario is likely not the mechanism of rapid mechanical signal transmission in actin stress fibers due to the highly viscoelastic character of these fibers. Our analysis also demonstrates that the time constant characterizing mechanical stimulus transmission is strongly dependent on the topology of the stress fiber network, implying that network organization plays an important role in determining the dynamics of cellular responsiveness to mechanical stimulation. © 2012 Landes Bioscience.

Hwang Y, Barakat AI, 2012, Dynamics of mechanical signal transmission through prestressed stress fibers., *PLoS One*, Vol: 7

Transmission of mechanical stimuli through the actin cytoskeleton has been proposed as a mechanism for rapid long-distance mechanotransduction in cells; however, a quantitative understanding of the dynamics of this transmission and the physical factors governing it remains lacking. Two key features of the actin cytoskeleton are its viscoelastic nature and the presence of prestress due to actomyosin motor activity. We develop a model of mechanical signal transmission through prestressed viscoelastic actin stress fibers that directly connect the cell surface to the nucleus. The analysis considers both temporally stationary and oscillatory mechanical signals and accounts for cytosolic drag on the stress fibers. To elucidate the physical parameters that govern mechanical signal transmission, we initially focus on the highly simplified case of a single stress fiber. The results demonstrate that the dynamics of mechanical signal transmission depend on whether the applied force leads to transverse or axial motion of the stress fiber. For transverse motion, mechanical signal transmission is dominated by prestress while fiber elasticity has a negligible effect. Conversely, signal transmission for axial motion is mediated uniquely by elasticity due to the absence of a prestress restoring force. Mechanical signal transmission is significantly delayed by stress fiber material viscosity, while cytosolic damping becomes important only for longer stress fibers. Only transverse motion yields the rapid and long-distance mechanical signal transmission dynamics observed experimentally. For simple networks of stress fibers, mechanical signals are transmitted rapidly to the nucleus when the fibers are oriented largely orthogonal to the applied force, whereas the presence of fibers parallel to the applied force slows down mechanical signal transmission significantly. The present results suggest that cytoskeletal prestress mediates rapid mechanical signal transmission and allows temporall

Hwang Y, Cossu C, 2011, Self-sustained processes in the logarithmic layer of turbulent channel flows, *PHYSICS OF FLUIDS*, Vol: 23, ISSN: 1070-6631

- Author Web Link
- Cite
- Citations: 32

This data is extracted from the Web of Science and reproduced under a licence from Thomson Reuters. You may not copy or re-distribute this data in whole or in part without the written consent of the Science business of Thomson Reuters.