<p>The natural convection in a compact system with a heat source is a key focus in various engineering applications from electronic cooling to building ventilation, where the optimum position of the heat source and advanced coolants can enhance thermal performance. This study investigates the natural convection heat transfer of a cold square enclosure filled with <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({\text{Al}}_{2} {\text{O}}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Al</mtext> <mn>2</mn> </msub> <msub> <mtext>O</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>/water-based nanofluid and an internal square heat source. Here, an in-house developed lattice Boltzmann method (LBM)-based solver written in the C programming language is employed to conduct two-dimensional numerical simulations. Novelty of this study lies in the combined assessment of nanoparticle concentration (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\varphi\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> = 0%, 2%, and 4%), eccentricities of the heat source in both horizontal (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\chi_{{\text{h}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mtext>h</mtext> </msub> </math></EquationSource> </InlineEquation> = −&#xa0;0.2 to + 0.2) and vertical (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\chi_{{\text{v}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mtext>v</mtext> </msub> </math></EquationSource> </InlineEquation> = −&#xa0;0.2 to + 0.2) direction, and Rayleigh number (<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({\text{Ra}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>Ra</mtext> </math></EquationSource> </InlineEquation> = 10<sup>3</sup> to 10<sup>6</sup>) on natural convection within the enclosure using the LBM-based solver. These governing parameters significantly influence the streamlines, isotherm distribution, and both local and surface-averaged Nusselt numbers (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\overline{{{\text{Nu}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mtext>Nu</mtext> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation>) on the enclosure’s surface. The eccentric position of the heat source significantly alters the flow dynamics, mixing, and heat transfer rate. At <i>Ra</i> = 10<sup>3</sup> and 10<sup>4</sup>, the maximum heat transfer occurs at higher eccentricities owing to the dominance of conduction. For <i>Ra</i> = 10<sup>5</sup> and 10<sup>6</sup>, where both convection and conduction exist, the maximum heat transfer depends on the eccentricity. Additionally, the concentration of nanoparticles strongly affects the thermal performance of the enclosure. The maximum value of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\overline{{{\text{Nu}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mtext>Nu</mtext> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> is 6.19 found at <i>φ</i> = 4% with <i>Ra</i> = 10<sup>6</sup>, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\chi_{{\text{h}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mtext>h</mtext> </msub> </math></EquationSource> </InlineEquation> = 0.0, and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\chi_{\nu}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mi>ν</mi> </msub> </math></EquationSource> </InlineEquation> = −&#xa0;0.2. Notably, the enhancement of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\overline{{{\text{Nu}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mtext>Nu</mtext> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> (<i>En</i>) varies with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\chi_{{\text{h}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mtext>h</mtext> </msub> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\chi_{\nu}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mi>ν</mi> </msub> </math></EquationSource> </InlineEquation>, <i>Ra</i>, and <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\varphi\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation>. The maximum value of En is 8.83%, noticed at <i>φ</i> = 4%, <i>Ra</i> = 10<sup>6</sup>, <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\chi_{{\text{h}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <mtext>h</mtext> </msub> </math></EquationSource> </InlineEquation> = 0.2, and <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\chi\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>χ</mi> </math></EquationSource> </InlineEquation><sub>ν</sub>= 0. This demonstrates that the effectiveness of nanoparticles is significant at higher <i>Ra</i>. Furthermore, a regression analysis-based correlation equation is proposed to predict <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\overline{{{\text{v}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mtext>v</mtext> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> as a function of governing parameters, enabling the estimation of <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\overline{{{\text{Nu}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mtext>Nu</mtext> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> without performing expensive numerical simulations.</p>

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Numerical investigation on heat transfer in a cold enclosure containing Al2O3/water-based nanofluid with an eccentric heat source

  • Bibhas Chand,
  • Prabir Sikdar,
  • Puneet Kalra,
  • Sunil Manohar Dash

摘要

The natural convection in a compact system with a heat source is a key focus in various engineering applications from electronic cooling to building ventilation, where the optimum position of the heat source and advanced coolants can enhance thermal performance. This study investigates the natural convection heat transfer of a cold square enclosure filled with \({\text{Al}}_{2} {\text{O}}_{3}\) Al 2 O 3 /water-based nanofluid and an internal square heat source. Here, an in-house developed lattice Boltzmann method (LBM)-based solver written in the C programming language is employed to conduct two-dimensional numerical simulations. Novelty of this study lies in the combined assessment of nanoparticle concentration ( \(\varphi\) φ  = 0%, 2%, and 4%), eccentricities of the heat source in both horizontal ( \(\chi_{{\text{h}}}\) χ h  = − 0.2 to + 0.2) and vertical ( \(\chi_{{\text{v}}}\) χ v  = − 0.2 to + 0.2) direction, and Rayleigh number ( \({\text{Ra}}\) Ra  = 103 to 106) on natural convection within the enclosure using the LBM-based solver. These governing parameters significantly influence the streamlines, isotherm distribution, and both local and surface-averaged Nusselt numbers ( \(\overline{{{\text{Nu}}}}\) Nu ¯ ) on the enclosure’s surface. The eccentric position of the heat source significantly alters the flow dynamics, mixing, and heat transfer rate. At Ra = 103 and 104, the maximum heat transfer occurs at higher eccentricities owing to the dominance of conduction. For Ra = 105 and 106, where both convection and conduction exist, the maximum heat transfer depends on the eccentricity. Additionally, the concentration of nanoparticles strongly affects the thermal performance of the enclosure. The maximum value of \(\overline{{{\text{Nu}}}}\) Nu ¯ is 6.19 found at φ = 4% with Ra = 106, \(\chi_{{\text{h}}}\) χ h  = 0.0, and \(\chi_{\nu}\) χ ν  = − 0.2. Notably, the enhancement of \(\overline{{{\text{Nu}}}}\) Nu ¯ (En) varies with \(\chi_{{\text{h}}}\) χ h , \(\chi_{\nu}\) χ ν , Ra, and \(\varphi\) φ . The maximum value of En is 8.83%, noticed at φ = 4%, Ra = 106, \(\chi_{{\text{h}}}\) χ h  = 0.2, and \(\chi\) χ ν= 0. This demonstrates that the effectiveness of nanoparticles is significant at higher Ra. Furthermore, a regression analysis-based correlation equation is proposed to predict \(\overline{{{\text{v}}}}\) v ¯ as a function of governing parameters, enabling the estimation of \(\overline{{{\text{Nu}}}}\) Nu ¯ without performing expensive numerical simulations.