Micropolar nanofluid flow in a stagnation region of a shrinking sheet with Fe3O4 nanoparticles
Conventional liquids have poor thermal conductivity, thus limiting their use in engineering. Therefore, scientists and researchers have created nanofluids, which consist of nanoparticles dispersed in a base fluid, to improve heat transfer properties in various fields, such as electronics, medicine,...
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| Main Authors: | , , , |
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| Format: | Article |
| Language: | English |
| Published: |
MDPI
2022
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| Online Access: | http://eprints.utem.edu.my/id/eprint/26288/2/WAINI2022%20MATHEMATICS-10-03184.PDF http://eprints.utem.edu.my/id/eprint/26288/ https://www.mdpi.com/2227-7390/10/17/3184 |
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| Summary: | Conventional liquids have poor thermal conductivity, thus limiting their use in engineering. Therefore, scientists and researchers have created nanofluids, which consist of nanoparticles dispersed in a base fluid, to improve heat transfer properties in various fields, such as electronics, medicine, and molten metals. In this study, we examine the micropolar nanofluid flow in a stagnation region of a stretching/shrinking sheet by employing the modified Buongiorno nanofluid model. The nanofluid consists of magnetite (Fe3O4) nanoparticles. The similarity equations are solved numerically using MATLAB software. The solution is unique for the shrinking strength (Formula presented.). Two solutions are found for the limited range of (Formula presented.) when (Formula presented.). The solutions terminate at (Formula presented.) in the shrinking region. The rise in micropolar parameter (Formula presented.) contributes to the increment in the skin friction coefficient (Formula presented.) and the couple stress (Formula presented.), but the Nusselt number (Formula presented.) and the Sherwood number (Formula presented.) decrease. These physical quantities intensify with the rise in the magnetic parameter (Formula presented.). Finally, we investigated the stability of the solutions over time. This work contributes to the dual solution and time stability analysis of the current problem. In addition, critical values of the main physical parameters are also presented. These critical values are usually known as the separation values from laminar to turbulent boundary layer flows. In this case, once the critical value is achieved, the process for the specific product can be planned according to the desired output to optimize the productivity. |
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