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Two-phase simulation of entropy optimized mixed convection flow of two different shear-thinning nanomaterials in thermal and mass diffusion systems with Lorentz forces. | LitMetric

AI Article Synopsis

  • This research examines the behavior of two shear thinning nanofluids that flow in a micro-channel under various conditions, focusing specifically on aspects like momentum, thermal energy, mass diffusion, and entropy generation.
  • The study finds that the hyperbolic tangent nanoliquid experiences better flow velocity compared to the Williamson nanofluid, although the latter exhibits higher thermal energy and concentration levels.
  • Key parameters such as Grashof number and Schmitt number significantly impact fluid flow rates and the concentration of the nanoliquids, while the temperature jump condition and variable thermal conductivity influence energy distribution and irreversibility within the system.

Article Abstract

This research compares the momentum, thermal energy, mass diffusion and entropy generation of two shear thinning nanofluids in an angled micro-channel with mixed convection, nonlinear thermal radiation, temperature jump boundary condition and variable thermal conductivity effects. The [Formula: see text] approach was used to solve the Buongiorno nonlinear governing model. The effect of different parameters on the flow, energy, concentration, and entropy generating fields have been graphically illustrated and explained. The hyperbolic tangent nanoliquid has a better velocity than the Williamson nanofluid. The Williamson nanofluid has higher thermal energy and concentration than the hyperbolic tangent nanoliquid in the microchannel. The Grashof number, both thermal and solutal, increases the fluid flow rate throughout the flow system. The energy of the nanoliquid is reduced by the temperature jump condition, while the energy field of the nanoliquid is enhanced by the improving thermal conductivity value. The nanoliquids concentration rises as the Schmitt number rises. The irreversibility rate of the channel system is maximized by the variable thermal conductivity parameter.

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Source
http://www.ncbi.nlm.nih.gov/pmc/articles/PMC10766953PMC
http://dx.doi.org/10.1038/s41598-023-50725-wDOI Listing

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