Velocity and acceleration statistics in rapidly rotating Rayleigh-Benard convection

被引:10
|
作者
Rajaei, Hadi [1 ,2 ]
Alards, Kim M. J. [1 ,2 ]
Kunnen, Rudie P. J. [1 ,2 ]
Clercx, Herman J. H. [1 ,2 ]
机构
[1] Eindhoven Univ Technol, Dept Appl Phys, Fluid Dynam Lab, POB 513, NL-5600 MB Eindhoven, Netherlands
[2] Eindhoven Univ Technol, JM Burgers Ctr Fluid Dynam, POB 513, NL-5600 MB Eindhoven, Netherlands
基金
欧洲研究理事会;
关键词
rotating turbulence; turbulent convection; waves in rotating fluids; PARTICLE TRACKING VELOCIMETRY; FULLY-DEVELOPED TURBULENCE; HEAT-TRANSPORT; PRECESSING CYLINDER; 3-DIMENSIONAL FLOWS; LAGRANGIAN VELOCITY; GEOSTROPHIC REGIME; BOUNDARY-LAYER; PRANDTL NUMBER; ZONAL FLOWS;
D O I
10.1017/jfm.2018.751
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
Background rotation causes different flow structures and heat transfer efficiencies in Rayleigh-Benard convection. Three main regimes are known: rotation unaffected, rotation affected and rotation dominated. It has been shown that the transition between rotation-unaffected and rotation-affected regimes is driven by the boundary layers. However, the physics behind the transition between rotation-affected and rotation-dominated regimes are still unresolved. In this study, we employ the experimentally obtained Lagrangian velocity and acceleration statistics of neutrally buoyant immersed particles to study the rotation-affected and rotation-dominated regimes and the transition between them. We have found that the transition to the rotation-dominated regime coincides with three phenomena; suppressed vertical motions, strong penetration of vortical plumes deep into the bulk and reduced interaction of vortical plumes with their surroundings. The first two phenomena are used as confirmations for the available hypotheses on the transition to the rotation-dominated regime while the last phenomenon is a new argument to describe the regime transition. These findings allow us to better understand the rotation-dominated regime and the transition to this regime.
引用
收藏
页码:374 / 397
页数:24
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