Using Nonlinear Transient Growth to Construct the Minimal Seed for Shear Flow Turbulence

2010 ◽  
Vol 105 (15) ◽  
Author(s):  
Chris C. T. Pringle ◽  
Rich R. Kerswell
1969 ◽  
Vol 1 (1) ◽  
pp. 245-264 ◽  
Author(s):  
O M Phillips
Keyword(s):  

2011 ◽  
Vol 682 ◽  
pp. 304-331 ◽  
Author(s):  
FAZLE HUSSAIN ◽  
DHOORJATY S. PRADEEP ◽  
ERIC STOUT

Growth of optimal transient perturbations to an Oseen vortex column into the nonlinear regime is studied via direct numerical simulation (DNS) for Reynolds number, Re (≡ circulation/viscosity), up to 10000. An optimal bending-wave transient mode is obtained from linear analysis and used as the initial condition. (DNS of a vortex column embedded in finer-scale turbulence reveals that optimal modes are preferentially excited during vortex–turbulence interaction.) Tilting of the optimal mode's radial vorticity perturbation into the azimuthal direction and its concomitant stretching by the column's strain field produces positive Reynolds stress, hence kinetic energy growth. Modes experiencing the largest growth are those with initial vorticity localized at a ‘critical radius’ outside the core, such that this perturbation vorticity resonantly induces core waves. Resonant forcing leads to growth of perturbation energy concentrated within the core. Moderate-amplitude (~5%) perturbations cause significant distortion of the core and generate secondary filament-like spiral structures (‘threads’) outside the core. As the mode evolves into the nonlinear regime, radially outward self-advection of thread dipoles accelerates growth arrest by removing the perturbation from the critical radius and disrupting resonant forcing. With increasing Re, the evolving vorticity patterns become more chaotic, more turbulent-like (finer scaled, contorted vorticity), and persist longer. This suggests that at typical Re (~106), nonlinear transient growth may indeed be able to break up, hence induce rapid decay of, column vortices – highly relevant for addressing the aircraft wake hazard crisis and the looming air traffic capacity crisis. In addition, we discover a regenerative transient growth scenario in which threads induce secondary perturbations closer to the vortex column. A parent–offspring regenerative mechanism is postulated and verified by DNS. There is a clear trend towards stronger regenerative growth with increasing Re. These results, showing an important role of transient growth in turbulent vortex decay, are highly relevant to the prediction and control of vortex-dominated flows.


1997 ◽  
Vol 343 ◽  
pp. 267-301 ◽  
Author(s):  
MEHEBOOB ALAM ◽  
PRABHU R. NOTT

Some recent studies have considered the stability of unbounded rapid granular shear flow, with the sole mechanism for stress generation being instantaneous inelastic collisions between grains. This paper extends these studies by presenting a linear stability analysis in which stress generation due to grain friction is also accounted for. This is accomplished by using the ‘frictional–kinetic’ model, which integrates in a simple manner the stress arising from the two mechanisms. Solution of the linearized equations of motion is obtained by allowing the wavenumber vector of the disturbances to rotate as a function of time. As in the case of a purely kinetic stress, it is found that the flow is stable to non-layering disturbances. Disturbances in the form of layering modes may lead to instability, depending on the solids fraction and material parameters. Instability is absent altogether if the balance of fluctuational energy is not considered or if the material is assumed to be incompressible. Friction may stabilize or destabilize the flow, depending on the inelasticity of grain collisions and the effective roughness of the medium. When a purely frictional stress is considered, it is found that the system is always neutrally stable. Even if the flow is asymptotically stable, there may be significant transient growth of disturbances due to the non-normality of the associated linear operator. The initial transient growth rate, as well as the temporal maximum of transient growth is enhanced by friction.


2018 ◽  
Vol 25 (12) ◽  
pp. 122303 ◽  
Author(s):  
A. E. Fraser ◽  
M. J. Pueschel ◽  
P. W. Terry ◽  
E. G. Zweibel
Keyword(s):  

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