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 E27: Flow Instability: Transition to Turbulence II |
Hide Abstracts |
Chair: Bjoern Hof, Max Planck Institute Room: Georgia World Congress Center B315 |
Sunday, November 18, 2018 5:10PM - 5:23PM |
E27.00001: Stochastic switching in a nonequilibrium crystal: a simple model for intermittent dynamics Guram Gogia, Justin C Burton Flow intermittency in the transition to turbulence is an important and long-standing problem in fluid mechanics. Nonlinear dynamics and geometric heterogeneity are known to strongly affect the patterns and range over which intermittency is observed. We have developed an experimental and numerical system which also displays stochastic, intermittent dynamics, and is sensitive to nonlinearities and heterogeneities. The experiments utilize dusty (complex) plasma, which consists of colloidal particles (dust) immersed in rarified charged gas (plasma) environment. Inertia is important: unlike colloidal suspensions that are characterized by overdamped dynamics, microparticles in plasma obey virtually underdamped dynamics. At low gas pressures, particles in a quasi-2D crystalline layer experience self-induced vertical vibrations that result in switching between crystalline and gas-like phases. The initiation of the gas-phase is due to an energy cascade from high-frequency modes to low-frequency modes in the system, leading to intermittent dynamics over a broad range of time scales. The dynamics can also be cast as two coupled ODEs for the kinetic energy in horizontal and vertical directions which resemble similar equations used to model the transition to turbulence. |
Sunday, November 18, 2018 5:23PM - 5:36PM |
E27.00002: Energy exchange in the transitional flow over bluff bodies Daniel M Moore, Christopher Letchford, Michael Amitay Transition behavior of separating shear layers on sharp edged bodies has been shown to rely heavily on the freestream Reynolds number. In contrast, many parameters investigated in the wake demonstrate an approximate invariance with respect to Reynolds number (e.g., the Strouhal number for a 2D square prism). The apparent attenuation of Reynolds number influence on transitioning shear layers between leading and trailing edges is examined in the current study from a phenomenological perspective on a series of rectangular sections and angles of attack. PIV and hot wire techniques were used in pursuit of identifying and tracking the energetic scales in the flow and their spatio-temporal migration. Results reveal the severity of coupling between the two regions of instability and subsequent consequences for aerodynamic loading. |
Sunday, November 18, 2018 5:36PM - 5:49PM |
E27.00003: Turbulent Transition with LES with the Wall-Adapting Local Eddy-Viscosity Model Minwoo Kim, Jiseop Lim, Seungtae Kim, Solkeun Jee, Jaeyoung Park, Donghun Park Large-eddy simulation (LES) is investigated for turbulent transition in a wall-bounded boundary layer. Behaviors of subgrid-scale models in the transition have not been fully understood yet. The wall-adapting local eddy-viscosity (WALE) model is of the interest in this study. The WALE model formulation is investigated in connection with flow structures in laminar, transitional and turbulent boundary layers. The boundary layer stability theory is used for the LES inlet, providing dominant disturbances in the pre-transitional boundary layer. |
Sunday, November 18, 2018 5:49PM - 6:02PM |
E27.00004: On the final stages of transition to turbulence in wall bounded flows David Goldstein, Saikishan Suryanarayanan, Garry L. Brown Using immersed boundary DNS, we first examine all phases of the process of transition to turbulence caused by a discrete roughness element. We demonstrate that after the initial receptivity, spatial amplification of the steady distortion, and the subsequent modal instability of the lifted up structure, transition proceeds via a mutual, local, amplification of the fluctuating streamwise and spanwise vorticity. We observe that the near-wall spanwise vorticity is stretched by dw/dz induced by a streamwise vortex tube present above it. This results in a local flow acceleration, and the du/dx leads to the stretching of streamwise vorticity. Thus this process is responsible for the amplification of streamwise vorticity near the wall, leading to the formation of familiar hairpin vortices. The relation of this process to the subsequent breakdown to chaos and counter gradient transport of mean vorticity to the wall is discussed. We study whether these observations are applicable to other routes to transition, such as free stream driven Klebanoff-mode bypass transition. |
Sunday, November 18, 2018 6:02PM - 6:15PM |
E27.00005: Global receptivity analysis of the flow over a hypersonic cone Tim Flint, Parviz Moin, M. J. Philipp Hack In high-speed flight, increased viscous heating past the onset of transition to turbulence is a critical limiting factor in the design of hypersonic vehicles. Acoustic exponential instabilities, which are ineffective at low Mach numbers, become active and open up additional avenues for breakdown to turbulence in the compressible boundary layer. The seeding of the instabilities is generated during the receptivity stage which governs the initiation of a disturbance field inside the shear, for instance by external disturbances. The present study rigorously analyses the receptivity process of the high-speed flow over a cone geometry by leveraging the structural sensitivity information provided by the adjoint linearized governing equations. As such, the approach enables the direct identification of the free-stream conditions which are most effective at triggering perturbation growth in the boundary layer. The study is facilitated via a curvilinear formulation of the governing equations which allows the incorporation of the effects of the cone geometry as well as shock waves. |
Sunday, November 18, 2018 6:15PM - 6:28PM |
E27.00006: Influence of superhydrophobic surfaces on the laminar-to-turbulent transition in a channel flow. Francesco Picella, Stefania Cherubini, Jean-Christophe Robinet Tailoring bio-mimetic rough surfaces researchers are accessing new approaches reducing drag in wall bounded shear flows. Among them Underwater SuperHydrophobic Surfaces (U-SHS) have proven to be capable of dramatically reduce skin friction of an overlying liquid turbulent flow, providing a stable, lubricating layer of gas bubbles trapped within the surface's nano-sculptures. As long as a specific set of geometrical and thermodynamical conditions are ensured, wetting transition is avoided and the no-slip boundary condition at the wall is relaxed; this so called 'Lotus effect' is typically achieved when the length scale of U-SHS roughnesses is several order of magnitudes smaller than the overlying flow, bringing out both experimental and numerical challenges. In this framework we want to study, by means of numerical simulations, the influence of U-SHS in a closed channel, following the complete evolution from laminar, to transitional and fully developed turbulent flow. We report the results of transition over U-SHS taking into account the dynamics of each microscopic liquid-gas free-surface by means of a fully coupled fluid-structure solver and show that U-SHS can triple transition time to turbulence. |
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2024 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700