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Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
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Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
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Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating

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Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating
Journal Article

Shape effect on MHD flow of time fractional Ferro-Brinkman type nanofluid with ramped heating

2021
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Overview
The colloidal suspension of nanometer-sized particles of Fe 3 O 4 in traditional base fluids is referred to as Ferro-nanofluids. These fluids have many technological applications such as cell separation, drug delivery, magnetic resonance imaging, heat dissipation, damping, and dynamic sealing. Due to the massive applications of Ferro-nanofluids, the main objective of this study is to consider the MHD flow of water-based Ferro-nanofluid in the presence of thermal radiation, heat generation, and nanoparticle shape effect. The Caputo-Fabrizio time-fractional Brinkman type fluid model is utilized to demonstrate the proposed flow phenomenon with oscillating and ramped heating boundary conditions. The Laplace transform method is used to solve the model for both ramped and isothermal heating for exact solutions. The ramped and isothermal solutions are simultaneously plotted in the various figures to study the influence of pertinent flow parameters. The results revealed that the fractional parameter has a great impact on both temperature and velocity fields. In the case of ramped heating, both temperature and velocity fields decreasing with increasing fractional parameter. However, in the isothermal case, this trend reverses near the plate and gradually, ramped, and isothermal heating became alike away from the plate for the fractional parameter. Finally, the solutions for temperature and velocity fields are reduced to classical form and validated with already published results.