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Both partial and full Dirichlet temperature boundaries were considered.
Furthermore, the predetermined temperature boundaries of human skin feeling for hot and cold condition are 20 25 °C.
The temperature boundaries of the feasibility region were determined by the κ-carrageenan gelation temperature and solution viscosity.
Furthermore, the optimal mass charge nearly keeps constant with the heat transfer rate and the temperature boundaries, and increases linearly with the rise of the total heat transfer area, which indicates the optimal average density keeps constant.
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So, it is difficult to draw a clear temperature boundary between β # (Br) components.
The combined effects of the physical model parameters with nonuniform temperature boundary conditions are also analyzed.
Boundary layer studies suggest that the velocity and temperature boundary layer thicknesses are lower for higher Reynolds numbers.
Increasing heat generation therefore only aids temperature and increases temperature boundary layer thickness further from the wedge.
The temperature boundary conditions on the left side and the bottom of the model region are adiabatic.
The finite element model of the plate in different temperature boundary conditions was updated simultaneously utilizing the presented method.
The equation is valid for laminar, mixed convection conditions in vertical, internal, aiding flows with constant wall temperature boundary condition.
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