<p>This research investigates bioconvective nanofluid flow across a linearly stretching surface within a permeable medium in a two-dimensional boundary layer, driven by its relevance to advanced cooling systems and biomedical engineering applications. The model considers water-based <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(Ti{O}_{2}-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mi>i</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(Cu-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water nanofluids, incorporating thermal radiation via the Rosseland approximation and an applied magnetic field. The governing equations are altered into dimensionless form using non-similarity transformations and reduced to coupled ordinary differential equations (ODEs) through the local non-similarity (LNS) method, solved numerically using MATLAB’s bvp4c solver. Results, validated against existing benchmark studies with less than 0.25% deviation, reveal several key parametric effects. Increasing the magnetic parameter <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> enhances drag but reduces velocity, with the skin-friction coefficient rising by 3.24%, 4.34%, and 1.61% for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(Ti{O}_{2}-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mi>i</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water and 7.02%, 2.44%, and 1.32% for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(Cu-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water as <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(M\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>M</mi> </math></EquationSource> </InlineEquation> increases from 0.2 to 0.8. The local Nusselt number shows dual behavior: for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(Ti{O}_{2}-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mi>i</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water, heat transfer increases by 11.34% at <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(M=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.4 but decreases by 1.90% at <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(M=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.6, while <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(Cu-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water exhibits up to 29.59% enhancement at <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(M=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.4 before decreasing by 19.72% at <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(M=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.8. The Eckert number <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\((Ec)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>E</mi> <mi>c</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> weakens heat transfer due to viscous dissipation, reducing the Nusselt number by 28.6% <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(Ti{O}_{2}-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mi>i</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water) and 2.95% (<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(Cu-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water) as <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(Ec\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Ec</mi> </mrow> </math></EquationSource> </InlineEquation> rises from 0.1 to 1.9. Conversely, the radiation parameter <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(({R}_{\text{t}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mi>R</mi> <mtext>t</mtext> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> promotes heat transport, enhancing the Nusselt number by up to 3.7% for <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(Ti{O}_{2}-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mi>i</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water and 0.7% for <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(Cu-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>water. Increasing the stretching/porosity parameter (<i>λ</i>) reduces both skin-friction and heat transfer, while a higher Peclet number enhances microorganism density, reinforcing bioconvective stability.</p>

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Magneto-Radiative Effects on Bioconvective Nanofluid Flow in Porous Media: A Numerical Approach for Cooling Optimization

  • Umar Farooq,
  • Tao Liu,
  • M. Mahtab Alam,
  • Ali Alshamrani

摘要

This research investigates bioconvective nanofluid flow across a linearly stretching surface within a permeable medium in a two-dimensional boundary layer, driven by its relevance to advanced cooling systems and biomedical engineering applications. The model considers water-based \(Ti{O}_{2}-\) T i O 2 - water and \(Cu-\) C u - water nanofluids, incorporating thermal radiation via the Rosseland approximation and an applied magnetic field. The governing equations are altered into dimensionless form using non-similarity transformations and reduced to coupled ordinary differential equations (ODEs) through the local non-similarity (LNS) method, solved numerically using MATLAB’s bvp4c solver. Results, validated against existing benchmark studies with less than 0.25% deviation, reveal several key parametric effects. Increasing the magnetic parameter \((M)\) ( M ) enhances drag but reduces velocity, with the skin-friction coefficient rising by 3.24%, 4.34%, and 1.61% for \(Ti{O}_{2}-\) T i O 2 - water and 7.02%, 2.44%, and 1.32% for \(Cu-\) C u - water as \(M\) M increases from 0.2 to 0.8. The local Nusselt number shows dual behavior: for \(Ti{O}_{2}-\) T i O 2 - water, heat transfer increases by 11.34% at \(M=\) M = 0.4 but decreases by 1.90% at \(M=\) M = 0.6, while \(Cu-\) C u - water exhibits up to 29.59% enhancement at \(M=\) M = 0.4 before decreasing by 19.72% at \(M=\) M = 0.8. The Eckert number \((Ec)\) ( E c ) weakens heat transfer due to viscous dissipation, reducing the Nusselt number by 28.6% \(Ti{O}_{2}-\) T i O 2 - water) and 2.95% ( \(Cu-\) C u - water) as \(Ec\) Ec rises from 0.1 to 1.9. Conversely, the radiation parameter \(({R}_{\text{t}})\) ( R t ) promotes heat transport, enhancing the Nusselt number by up to 3.7% for \(Ti{O}_{2}-\) T i O 2 - water and 0.7% for \(Cu-\) C u - water. Increasing the stretching/porosity parameter (λ) reduces both skin-friction and heat transfer, while a higher Peclet number enhances microorganism density, reinforcing bioconvective stability.