<p>In this study, large eddy simulations of natural convection in a cubical cavity with differently heated walls were conducted to investigate the anisotropic characteristics of turbulent flows with respect to spanwise boundary conditions at Rayleigh (<i>Ra</i>) number range of 10<sup>5</sup> to 10<sup>8</sup>. The adiabatic and cyclic conditions were imposed on the spanwise boundaries, respectively. The flow in the cubical cavity was steady at a very low <i>Ra</i> number of 10<sup>5</sup> regardless of spanwise boundary conditions. Whereas one- and two-component turbulences were dominant at <i>Ra</i> = 10<sup>6</sup>, and the distribution of the turbulence state differed significantly depending on the spanwise boundary conditions. As <i>Ra</i> increased to 10<sup>7</sup> and further to 10<sup>8</sup>, the adiabatic boundary condition made the turbulent flows adjacent to the spanwise boundaries resemble the two-component state while the flow state was close to the three-component state when using the cyclic boundary condition.</p>

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Characterization of anisotropic turbulence on natural convection flow in cubical cavity

  • Gi Su Mun,
  • Jongtae Kim,
  • Sang Bong Lee,
  • Woochan Seok

摘要

In this study, large eddy simulations of natural convection in a cubical cavity with differently heated walls were conducted to investigate the anisotropic characteristics of turbulent flows with respect to spanwise boundary conditions at Rayleigh (Ra) number range of 105 to 108. The adiabatic and cyclic conditions were imposed on the spanwise boundaries, respectively. The flow in the cubical cavity was steady at a very low Ra number of 105 regardless of spanwise boundary conditions. Whereas one- and two-component turbulences were dominant at Ra = 106, and the distribution of the turbulence state differed significantly depending on the spanwise boundary conditions. As Ra increased to 107 and further to 108, the adiabatic boundary condition made the turbulent flows adjacent to the spanwise boundaries resemble the two-component state while the flow state was close to the three-component state when using the cyclic boundary condition.