Scaling Laws for the Heterogeneously Heated Free Convective Boundary Layer

被引:50
|
作者
van Heerwaarden, Chiel C. [1 ]
Mellado, Juan Pedro [1 ]
De Lozar, Alberto [1 ]
机构
[1] Max Planck Inst Meteorol, D-20146 Hamburg, Germany
关键词
LARGE-EDDY SIMULATIONS; DIRECT NUMERICAL-SIMULATION; FINITE-DIFFERENCE SCHEMES; SURFACE HETEROGENEITY; LAND SURFACES; LENGTH SCALES; TEMPERATURE; TURBULENCE; DYNAMICS; OSCILLATIONS;
D O I
10.1175/JAS-D-13-0383.1
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
The heterogeneously heated free convective boundary layer (CBL) is investigated by means of dimensional analysis and results from large-eddy simulations (LES) and direct numerical simulations (DNS). The investigated physical model is a CBL that forms in a linearly stratified atmosphere heated from the surface by square patches with a high surface buoyancy flux. Each simulation has been run long enough to show the formation of a peak in kinetic energy, corresponding to the "optimal" heterogeneity size with strong secondary circulations, and the subsequent transition into a horizontally homogeneous CBL. Scaling laws for the time of the optimal state and transition and for the vertically integrated kinetic energy (KE) have been developed. The laws show that the optimal state and transition do not occur at a fixed ratio of the heterogeneity size to the CBL height. Instead, these occur at a higher ratio for simulations with increasing heterogeneity sizes because of the development of structures in the downward-moving air that grow faster than the CBL thickness. The moment of occurrence of the optimal state and transition are strongly related to the heterogeneity amplitude: stronger amplitudes result in an earlier optimal state and a later transition. Furthermore, a decrease in patch size combined with a compensating increase in patch surface buoyancy flux to maintain the energy input results in decreasing KE and a later transition. The simulations suggest that a CBL with a heterogeneity size smaller than the initial CBL height has less entrainment than a horizontally homogeneous CBL, whereas one with a larger heterogeneity size has more.
引用
收藏
页码:3975 / 4000
页数:26
相关论文
共 50 条
  • [31] INVESTIGATION OF TURBULENT FLOW BEHAVIOR IN A HEATED BOUNDARY LAYER
    Dennis, Kadeem
    Siddiqui, Kamran
    PROCEEDINGE OF THE ASME/JSME/KSME JOINT FLUIDS ENGINEERING CONFERENCE, 2019, VOL 1, 2019,
  • [32] Convective boundary-layer structure in the presence of wind-following swell
    Nilsson, Erik Olof
    Rutgersson, Anna
    Smedman, Ann-Sofi
    Sullivan, Peter P.
    QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2012, 138 (667) : 1476 - 1489
  • [33] The convective boundary layer on Mars: Some 1-D simulation results
    Savijarvi, Hannu
    ICARUS, 2012, 221 (02) : 617 - 623
  • [34] Turbulent mixing of reactive gases in the convective boundary layer
    G. H. L. Verver
    H. Van Dop
    A. A. M. Holtslag
    Boundary-Layer Meteorology, 1997, 85 : 197 - 222
  • [35] Electrodynamic properties and height of atmospheric convective boundary layer
    Anisimov, S. V.
    Galichenko, S. V.
    Mareev, E. A.
    ATMOSPHERIC RESEARCH, 2017, 194 : 119 - 129
  • [36] A numerical study of daily transitions in the convective boundary layer
    Sorbjan, Zbigniew
    BOUNDARY-LAYER METEOROLOGY, 2007, 123 (03) : 365 - 383
  • [37] The TKE budget in the convective Martian planetary boundary layer
    Martinez, G. M.
    Valero, F.
    Vazquez, L.
    QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2011, 137 (661) : 2194 - 2208
  • [38] On the impact of surface heterogeneity on a realistic convective boundary layer
    Huang, Hsin-Yuan
    Margulis, Steven A.
    WATER RESOURCES RESEARCH, 2009, 45
  • [39] A Lagrangian Decorrelation Time Scale in the Convective Boundary Layer
    Gervasio Degrazia
    Domenico Anfossi
    Haroldo Fraga De Campos Velho
    Enrico Ferrero
    Boundary-Layer Meteorology, 1998, 86 : 525 - 534
  • [40] A numerical study of daily transitions in the convective boundary layer
    Zbigniew Sorbjan
    Boundary-Layer Meteorology, 2007, 123 : 365 - 383