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Enhancing post-harvest sustainability in temperate crops through smart IoT-integrated indirect solar dryer. [PDF]
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2020
<p>The phenomenon of convective aggregation in idealised radiative convective equilibrium simulations has the ability to change the mean state of its domain. When compared to non-aggregation conditions, these simulations usually have warmer drier mean atmospheres, with stronger precipitation in the convective areas. Many of these
Beth Dingley, Guy Dagan, Philip Stier
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<p>The phenomenon of convective aggregation in idealised radiative convective equilibrium simulations has the ability to change the mean state of its domain. When compared to non-aggregation conditions, these simulations usually have warmer drier mean atmospheres, with stronger precipitation in the convective areas. Many of these
Beth Dingley, Guy Dagan, Philip Stier
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2007
At some boundary conditions the liquid at the bulk flow at heated surfaces may become saturated. So, we have flow boiling of saturated liquid in the two phase mixture. The heat transfer then consists of a predominant convective part and a nucleate boiling part. The total heat flux is then consumed for evaporation.
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At some boundary conditions the liquid at the bulk flow at heated surfaces may become saturated. So, we have flow boiling of saturated liquid in the two phase mixture. The heat transfer then consists of a predominant convective part and a nucleate boiling part. The total heat flux is then consumed for evaporation.
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1997
This chapter turns to forced convection. Instead of buoyancy forces, forced convection is a mechanism caused by pumps or fans. This concept is explained through a quick primer on fluid mechanics. Then, the chapter defines the heat transfer coefficient. Afterward, it explores the heat transfer correlations for external flow and for turbulent flow of non-
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This chapter turns to forced convection. Instead of buoyancy forces, forced convection is a mechanism caused by pumps or fans. This concept is explained through a quick primer on fluid mechanics. Then, the chapter defines the heat transfer coefficient. Afterward, it explores the heat transfer correlations for external flow and for turbulent flow of non-
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2015
Turbulence occurs nearly everywhere in nature. It is characterized by the efficient dispersion and mixing of vorticity, heat, and contaminants. In flows over solid bodies, such as airplane wings or turbine blades, or in confined flows through ducts and pipelines, and is responsible for increased drag and heat transfer. Turbulence is therefore a subject
Bahman Zohuri, Nima Fathi
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Turbulence occurs nearly everywhere in nature. It is characterized by the efficient dispersion and mixing of vorticity, heat, and contaminants. In flows over solid bodies, such as airplane wings or turbine blades, or in confined flows through ducts and pipelines, and is responsible for increased drag and heat transfer. Turbulence is therefore a subject
Bahman Zohuri, Nima Fathi
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Randomly forced Rayleigh-Bénard convection
Journal of Fluid Mechanics, 1980We consider the onset of Rayleigh–Bénard convection from random fluctuations arising within a fluid. In the specific case in which the fluctuations are thermodynamically determined, we reduce the problem to a random initial value problem for the Fourier modes. For the case of weak nonlinear convection, it is possible to truncate the number of modes and
Jhaveri, Bharat, Homsy, G. M.
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Influence of Lorentz forces on nanofluid forced convection considering Marangoni convection
Journal of Molecular Liquids, 2017Abstract Magnetohydrodynamic nanofluid forced convective heat transfer is investigated considering Marangoni convection. A two-phase model is selected for modeling of a nanofluid. The Runge-Kutta integration scheme is utilized to solve this problem.
M. Sheikholeslami, Ali J. Chamkha
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Battery thermal management system based on the forced-air convection: A review
ETransportation, 2021Xulai Yang, Qingsong Wang
exaly

