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Confined Rayleigh-Bénard, Rotating Rayleigh-Bénard, and Double Diffusive Convection: A Unifying View on Turbulent Transport Enhancement through Coherent Structure Manipulation.
Chong, Kai Leong; Yang, Yantao; Huang, Shi-Di; Zhong, Jin-Qiang; Stevens, Richard J A M; Verzicco, Roberto; Lohse, Detlef; Xia, Ke-Qing.
Afiliação
  • Chong KL; Department of Physics, The Chinese University of Hong Kong, Shatin, Hong Kong, China.
  • Yang Y; Physics of Fluids Group and Max Planck Center Twente, MESA+Institute, J. M. Burgers Centre for Fluid Dynamics, University of Twente, 7500 AE Enschede, Netherlands.
  • Huang SD; SKLTCS and Department of Mechanics and Engineering Science, College of Engineering, Peking University, Beijing 100871, China.
  • Zhong JQ; Department of Physics, The Chinese University of Hong Kong, Shatin, Hong Kong, China.
  • Stevens RJAM; Shanghai Key Laboratory of Special Artificial Microstructure Materials and Technology and School of Physics Science and Engineering, Tongji University, Shanghai 200092, China.
  • Verzicco R; Physics of Fluids Group and Max Planck Center Twente, MESA+Institute, J. M. Burgers Centre for Fluid Dynamics, University of Twente, 7500 AE Enschede, Netherlands.
  • Lohse D; Physics of Fluids Group and Max Planck Center Twente, MESA+Institute, J. M. Burgers Centre for Fluid Dynamics, University of Twente, 7500 AE Enschede, Netherlands.
  • Xia KQ; Dipartimento di Ingegneria Industriale, University of Rome Tor Vergata, Rome 00133, Italy.
Phys Rev Lett ; 119(6): 064501, 2017 Aug 11.
Article em En | MEDLINE | ID: mdl-28949632
Many natural and engineering systems are simultaneously subjected to a driving force and a stabilizing force. The interplay between the two forces, especially for highly nonlinear systems such as fluid flow, often results in surprising features. Here we reveal such features in three different types of Rayleigh-Bénard (RB) convection, i.e., buoyancy-driven flow with the fluid density being affected by a scalar field. In the three cases different stabilizing forces are considered, namely (i) horizontal confinement, (ii) rotation around a vertical axis, and (iii) a second stabilizing scalar field. Despite the very different nature of the stabilizing forces and the corresponding equations of motion, at moderate strength we counterintuitively but consistently observe an enhancement in the flux, even though the flow motion is weaker than the original RB flow. The flux enhancement occurs in an intermediate regime in which the stabilizing force is strong enough to alter the flow structures in the bulk to a more organized morphology, yet not too strong to severely suppress the flow motions. Near the optimal transport enhancements all three systems exhibit a transition from a state in which the thermal boundary layer (BL) is nested inside the momentum BL to the one with the thermal BL being thicker than the momentum BL. The observed optimal transport enhancement is explained through an optimal coupling between the suction of hot or fresh fluid and the corresponding scalar fluctuations.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article