Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid

The influences of superellipse shapes on natural convection in a horizontally subdivided non-Darcy porous cavity populated by Cu-water nanofluid are inspected in this paper. The impacts of the inner geometries <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" displa...

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Autor principal: Noura Alsedais
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Publicado: MDPI AG 2021
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spelling oai:doaj.org-article:c6e1ae26ac7b4c0db3441b788e53e9c42021-11-11T15:46:36ZNatural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid10.3390/en142169521996-1073https://doaj.org/article/c6e1ae26ac7b4c0db3441b788e53e9c42021-10-01T00:00:00Zhttps://www.mdpi.com/1996-1073/14/21/6952https://doaj.org/toc/1996-1073The influences of superellipse shapes on natural convection in a horizontally subdivided non-Darcy porous cavity populated by Cu-water nanofluid are inspected in this paper. The impacts of the inner geometries <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mi>n</mi><mo>=</mo><mn>0.5</mn><mo>,</mo><mn>1</mn><mo>,</mo><mn>1.5</mn><mo>,</mo><mn>4</mn></mrow><mo>)</mo></mrow><mo>,</mo></mrow></semantics></math></inline-formula> Rayleigh number <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo stretchy="false">(</mo><msup><mrow><mn>10</mn></mrow><mn>3</mn></msup><mo>≤</mo><mi>R</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mn>6</mn></msup><mo stretchy="false">)</mo></mrow></semantics></math></inline-formula>, Darcy number <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo stretchy="false">(</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>5</mn></mrow></msup><mo>≤</mo><mi>D</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>2</mn></mrow></msup><mo stretchy="false">)</mo></mrow></semantics></math></inline-formula>, porosity <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mn>0.2</mn><mo>≤</mo><mi>ϵ</mi><mo>≤</mo><mn>0.8</mn></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula>, and solid volume fraction <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mn>0.01</mn><mo>≤</mo><mo>∅</mo><mo>≤</mo><mn>0.05</mn></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula> on nanofluid heat transport and streamlines were examined. The hot superellipse shapes were placed in the cavity’s bottom and top, while the adiabatic boundaries on the flat walls of the cavity were considered. The governing equations were numerically solved using the finite volume method (FVM). It was found that the movement of the nanofluid upsurged as Ra boosted. The temperature distributions in the cavity’s core had an inverse relationship with increasing Rayleigh number. An extra porous resistance at lower Darcy numbers limited the nanofluid’s movement within the porous layers. The mean Nusselt number decreased as the porous resistance increased <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mi>D</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>4</mn></mrow></msup></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula>. The flow and temperature were strongly affected as the shape of the inner superellipse grew larger.Noura AlsedaisMDPI AGarticlenatural convectionsuperellipse shape cavitynanofluidporous mediathermal conductivitynon-Darcy porous cavityTechnologyTENEnergies, Vol 14, Iss 6952, p 6952 (2021)
institution DOAJ
collection DOAJ
language EN
topic natural convection
superellipse shape cavity
nanofluid
porous media
thermal conductivity
non-Darcy porous cavity
Technology
T
spellingShingle natural convection
superellipse shape cavity
nanofluid
porous media
thermal conductivity
non-Darcy porous cavity
Technology
T
Noura Alsedais
Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
description The influences of superellipse shapes on natural convection in a horizontally subdivided non-Darcy porous cavity populated by Cu-water nanofluid are inspected in this paper. The impacts of the inner geometries <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mi>n</mi><mo>=</mo><mn>0.5</mn><mo>,</mo><mn>1</mn><mo>,</mo><mn>1.5</mn><mo>,</mo><mn>4</mn></mrow><mo>)</mo></mrow><mo>,</mo></mrow></semantics></math></inline-formula> Rayleigh number <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo stretchy="false">(</mo><msup><mrow><mn>10</mn></mrow><mn>3</mn></msup><mo>≤</mo><mi>R</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mn>6</mn></msup><mo stretchy="false">)</mo></mrow></semantics></math></inline-formula>, Darcy number <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo stretchy="false">(</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>5</mn></mrow></msup><mo>≤</mo><mi>D</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>2</mn></mrow></msup><mo stretchy="false">)</mo></mrow></semantics></math></inline-formula>, porosity <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mn>0.2</mn><mo>≤</mo><mi>ϵ</mi><mo>≤</mo><mn>0.8</mn></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula>, and solid volume fraction <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mn>0.01</mn><mo>≤</mo><mo>∅</mo><mo>≤</mo><mn>0.05</mn></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula> on nanofluid heat transport and streamlines were examined. The hot superellipse shapes were placed in the cavity’s bottom and top, while the adiabatic boundaries on the flat walls of the cavity were considered. The governing equations were numerically solved using the finite volume method (FVM). It was found that the movement of the nanofluid upsurged as Ra boosted. The temperature distributions in the cavity’s core had an inverse relationship with increasing Rayleigh number. An extra porous resistance at lower Darcy numbers limited the nanofluid’s movement within the porous layers. The mean Nusselt number decreased as the porous resistance increased <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>(</mo><mrow><mi>D</mi><mi>a</mi><mo>≤</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>4</mn></mrow></msup></mrow><mo>)</mo></mrow></mrow></semantics></math></inline-formula>. The flow and temperature were strongly affected as the shape of the inner superellipse grew larger.
format article
author Noura Alsedais
author_facet Noura Alsedais
author_sort Noura Alsedais
title Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
title_short Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
title_full Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
title_fullStr Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
title_full_unstemmed Natural Convection over Two Superellipse Shapes with a Porous Cavity Populated by Nanofluid
title_sort natural convection over two superellipse shapes with a porous cavity populated by nanofluid
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/c6e1ae26ac7b4c0db3441b788e53e9c4
work_keys_str_mv AT nouraalsedais naturalconvectionovertwosuperellipseshapeswithaporouscavitypopulatedbynanofluid
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