<p>In this study, the heat transfer and fluid flow behavior of an arrow-ribbed absorber plate under turbulent conditions Reynolds number (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(Re\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Re</mi> </mrow> </math></EquationSource> </InlineEquation>) (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(3800 \le Re \le 18,000\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3800</mn> <mo>≤</mo> <mi>R</mi> <mi>e</mi> <mo>≤</mo> <mn>18</mn> <mo>,</mo> <mn>000</mn> </mrow> </math></EquationSource> </InlineEquation>) is examined using computational techniques. The influence of the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(Re\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Re</mi> </mrow> </math></EquationSource> </InlineEquation> and relative roughness pitch (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(P/e\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mo stretchy="false">/</mo> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation>) (<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(7.50 \le P/e \le 18.75)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>7.50</mn> <mo>≤</mo> <mi>P</mi> <mo stretchy="false">/</mo> <mi>e</mi> <mo>≤</mo> <mn>18.75</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> on the thermal energy extraction from the absorber plate is systemically investigated. Throughout the investigation, the non-dimensional height remained constant in the present study. The average Nusselt number <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\left( {\overline{{Nu_{{\text{r}}} }} } \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <mover> <mrow> <mi>N</mi> <msub> <mi>u</mi> <mtext>r</mtext> </msub> </mrow> <mo>¯</mo> </mover> </mfenced> </math></EquationSource> </InlineEquation> is increased with Reynolds number across all relative roughness pitches, whereas the average friction factor <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\left( {\overline{{f_{{\text{r}}} }} } \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <mover> <msub> <mi>f</mi> <mtext>r</mtext> </msub> <mo>¯</mo> </mover> </mfenced> </math></EquationSource> </InlineEquation> is decreased accordingly. Results from the numerical evaluation show that the highest <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\overline{{Nu_{{\text{r}}} }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mrow> <mi>N</mi> <msub> <mi>u</mi> <mtext>r</mtext> </msub> </mrow> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation>, approximately 5.33 times the smooth duct value, is achieved at <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(P/e\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mo stretchy="false">/</mo> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation> = 7.50 for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(Re\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Re</mi> </mrow> </math></EquationSource> </InlineEquation> = 3800. Meanwhile, the maximum growth in <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\overline{{f_{{\text{r}}} }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <msub> <mi>f</mi> <mtext>r</mtext> </msub> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation>, about 2.53 times the smooth case, is obtained for the same configuration. Additionally, the optimal thermal–hydraulic performance parameter (THPP) is determined to be 3.91 at <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(P/e\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mo stretchy="false">/</mo> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation> = 7.50 for <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(Re\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Re</mi> </mrow> </math></EquationSource> </InlineEquation> = 8000. Additionally, empirical correlations for the <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\overline{{Nu_{{\text{r}}} }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mrow> <mi>N</mi> <msub> <mi>u</mi> <mtext>r</mtext> </msub> </mrow> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\overline{{f_{{\text{r}}} }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <msub> <mi>f</mi> <mtext>r</mtext> </msub> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> have been proposed, achieving an accuracy of ± 6% and ± 8%, respectively, with a coefficient of determination (<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(R\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>R</mi> </math></EquationSource> </InlineEquation> <sup>2</sup> = 0.98). These empirical correlations provide valuable guidance for both academic research and industrial applications in optimal design of the solar air heater duct (SAHD). The findings establish a reliable foundation for enhancing the solar air heater system.</p>

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Computational investigation of the thermal and fluid dynamic behavior of a solar air heater with inverted arrow-shaped ribs

  • Akhilesh Kumar,
  • Subhash V. Lahane,
  • Shrikisan J. Parihar,
  • Sachin C. Borse

摘要

In this study, the heat transfer and fluid flow behavior of an arrow-ribbed absorber plate under turbulent conditions Reynolds number ( \(Re\) Re ) ( \(3800 \le Re \le 18,000\) 3800 R e 18 , 000 ) is examined using computational techniques. The influence of the \(Re\) Re and relative roughness pitch ( \(P/e\) P / e ) ( \(7.50 \le P/e \le 18.75)\) 7.50 P / e 18.75 ) on the thermal energy extraction from the absorber plate is systemically investigated. Throughout the investigation, the non-dimensional height remained constant in the present study. The average Nusselt number \(\left( {\overline{{Nu_{{\text{r}}} }} } \right)\) N u r ¯ is increased with Reynolds number across all relative roughness pitches, whereas the average friction factor \(\left( {\overline{{f_{{\text{r}}} }} } \right)\) f r ¯ is decreased accordingly. Results from the numerical evaluation show that the highest \(\overline{{Nu_{{\text{r}}} }}\) N u r ¯ , approximately 5.33 times the smooth duct value, is achieved at \(P/e\) P / e  = 7.50 for \(Re\) Re  = 3800. Meanwhile, the maximum growth in \(\overline{{f_{{\text{r}}} }}\) f r ¯ , about 2.53 times the smooth case, is obtained for the same configuration. Additionally, the optimal thermal–hydraulic performance parameter (THPP) is determined to be 3.91 at \(P/e\) P / e  = 7.50 for \(Re\) Re  = 8000. Additionally, empirical correlations for the \(\overline{{Nu_{{\text{r}}} }}\) N u r ¯ and \(\overline{{f_{{\text{r}}} }}\) f r ¯ have been proposed, achieving an accuracy of ± 6% and ± 8%, respectively, with a coefficient of determination ( \(R\) R 2 = 0.98). These empirical correlations provide valuable guidance for both academic research and industrial applications in optimal design of the solar air heater duct (SAHD). The findings establish a reliable foundation for enhancing the solar air heater system.