Turbulent Bursts in Couette-Taylor Flow.
Turbulent Bursts in Couette-Taylor Flow.
复制标题
库埃特-泰勒流中的湍流爆发。
DOI:
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发表时间:
1996
影响因子:
8.6
通讯作者:
P. Marcus
中科院分区:
文献类型:
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作者:
K. Coughlin;P. Marcus
A new mathematical model for turbulent bursts in the three-dimensional flow between concentric, rotating cylinders (Couette-Taylor flow) is presented. Within a certain flow regime, if the parameters are held fixed, the flow oscillates in time between a spatially laminar phase (temporally chaotic Interpenetrating Spiral Vortex flow) and a turbulent phase. Our mathematical model is based on our previously published [1] fully-resolved, direct numerical simulation (i.e., using the Navier-Stokes equation with no turbulence modeling). Prom these simulations we developed a physical model [2] that breaks up the cycle into four physical processes: (1) the flow sets up a laminar equilibrium of vortices (Interpenetrating Spiral Vortex flow); (2) the equilibrium becomes unstable to a linear Floquet mode which grows exponentially from random, small initial conditions; (3) this mode acts as a finite–amplitude trigger for a shear-driven instability which results in large–amplitude, space–filling turbulence; and (4) after the turbulence exhausts the energy stored in the mean azimuthal component of the flow, dissipation causes it to collapse and the cycle repeats. Here, we derive a mathematical model from the Navier–Stokes equations using approximations based on the physical model. We show how well the model agrees with the numerically computed velocities, how it explains correlations and other properties of the numerically computed fields, and how it makes predictions that could be tested in future experiments.