Resolved energy budget of superstructures in Rayleigh-Benard convection

被引:25
作者
Green, Gerrit [1 ,2 ]
Vlaykov, Dimitar G. [1 ,3 ]
Pedro Mellado, Juan [4 ,5 ]
Wilczek, Michael [1 ,2 ]
机构
[1] Max Planck Inst Dynam & Self Org MPI DS, Fassberg 17, D-37077 Gottingen, Germany
[2] Univ Gottingen, Fac Phys, Friedrich Hund Pl 1, D-37077 Gottingen, Germany
[3] Univ Exeter, Coll Engn Math & Phys Sci, Astrophys Grp, Exeter EX4 4QL, Devon, England
[4] Max Planck Inst Meteorol, Bundesstr 53, D-20146 Hamburg, Germany
[5] Univ Politecn Cataluna, Dept Phys, Aerosp Engn Div, C Jordi Girona 1-3, ES-08034 Barcelona, Spain
关键词
turbulent convection; TURBULENCE; DYNAMICS; SIMULATIONS; TRANSPORT; PATTERNS; EQUATION; SCALES;
D O I
10.1017/jfm.2019.1008
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
Turbulent superstructures, i.e. large-scale flow structures in turbulent flows, play a crucial role in many geo- and astrophysical settings. In turbulent Rayleigh-Benard convection, for example, horizontally extended coherent large-scale convection rolls emerge. Currently, a detailed understanding of the interplay of small-scale turbulent fluctuations and large-scale coherent structures is missing. Here, we investigate the resolved kinetic energy and temperature variance budgets by applying a filtering approach to direct numerical simulations of Rayleigh-Benard convection at high aspect ratio. In particular, we focus on the energy transfer rate between large-scale flow structures and small-scale fluctuations. We show that the small scales primarily act as a dissipation for the superstructures. However, we find that the height-dependent energy transfer rate has a complex structure with distinct bulk and boundary layer features. Additionally, we observe that the heat transfer between scales mainly occurs close to the thermal boundary layer. Our results clarify the interplay of superstructures and turbulent fluctuations and may help to guide the development of an effective description of large-scale flow features in terms of reduced-order models.
引用
收藏
页数:28
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