<p>This research presents a new analytical prediction model to calculate Manning’s roughness coefficient (n) through utilizing relative submergence (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(h/{D}_{50}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo stretchy="false">/</mo> <msub> <mi>D</mi> <mn>50</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>), Shields parameter (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\theta\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>θ</mi> </math></EquationSource> </InlineEquation>), Froude number (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(Fr\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Fr</mi> </mrow> </math></EquationSource> </InlineEquation>), and volumetric sediment concentration <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left({S}_{v}\right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <msub> <mi>S</mi> <mi>v</mi> </msub> </mfenced> </math></EquationSource> </InlineEquation> parameters. The proposed analytical equation took the form <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq5.gif" Format="GIF" Height="36" Rendition="HTML" Resolution="72" Type="Linedraw" Width="267" /> </InlineMediaObject> <EquationSource Format="TEX">\(n=0.041{\left(\frac{h}{{D}_{50}}\right)}^{-0.18}{\theta }^{0.15}F{r}^{-0.28}{S}_{v}^{-0.10}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>0.041</mn> <msup> <mrow> <mfenced close=")" open="("> <mfrac> <mi>h</mi> <msub> <mi>D</mi> <mn>50</mn> </msub> </mfrac> </mfenced> </mrow> <mrow> <mo>-</mo> <mn>0.18</mn> </mrow> </msup> <msup> <mrow> <mi>θ</mi> </mrow> <mrow> <mn>0.15</mn> </mrow> </msup> <mi>F</mi> <msup> <mrow> <mi>r</mi> </mrow> <mrow> <mo>-</mo> <mn>0.28</mn> </mrow> </msup> <msubsup> <mi>S</mi> <mrow> <mi>v</mi> </mrow> <mrow> <mo>-</mo> <mn>0.10</mn> </mrow> </msubsup> </mrow> </math></EquationSource> </InlineEquation> to achieve performance achievements of 16.3% absolute relative error coupled with NA of 0.85 and R<sup>2</sup> = 0.88 compared to five benchmarked models including Wu and Wang (J Hydraul Eng 125(12):1309–1312, 1999: ARE = 23.5%) and Deng et al. (J Sediment Res 5:24–29, 2007: R<sup>2</sup> = 0.15). The analysis demonstrated that flow Froude number (Fr) maintained (−0.28) the strongest effect which decreased n by 32% when Fr at 1.2 reached supercritical conditions. Sediment concentration <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({S}_{v}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mi>v</mi> </msub> </math></EquationSource> </InlineEquation> at 2000 ppm displayed (−0.10) dominant influence by dropping n by 25%. The model simulation applied with 10,000 iterations showed hydraulic radius (R) was the most responsive variable (total-order Sobol index = 0.50) based on uncertainty analysis through Monte Carlo simulations while Bayesian inference validated a 95% confidence interval spanning from 0.025 to 0.045 for n. When applied to changing bedforms with the <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41062_2025_2182_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\theta }^{0.15}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi>θ</mi> </mrow> <mrow> <mn>0.15</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> parameter the prediction accuracy increased by 15% under conditions of mobile bed movement (θ &gt; 0.06). The calculated models find practical use in adaptive flood prediction and sediment-charged channel constructions which lead to risk cuts of 15–25% in flood scenarios. The presented work combines empirical methods with data-based strategies to improve predictive capabilities for situations involving non-uniform unsteady fluid motions.</p>

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Derivation of a novel analytical formula for estimating Manning’s roughness coefficient in sand-bed channels

  • Jafar Chabokpour

摘要

This research presents a new analytical prediction model to calculate Manning’s roughness coefficient (n) through utilizing relative submergence ( \(h/{D}_{50}\) h / D 50 ), Shields parameter ( \(\theta\) θ ), Froude number ( \(Fr\) Fr ), and volumetric sediment concentration \(\left({S}_{v}\right)\) S v parameters. The proposed analytical equation took the form \(n=0.041{\left(\frac{h}{{D}_{50}}\right)}^{-0.18}{\theta }^{0.15}F{r}^{-0.28}{S}_{v}^{-0.10}\) n = 0.041 h D 50 - 0.18 θ 0.15 F r - 0.28 S v - 0.10 to achieve performance achievements of 16.3% absolute relative error coupled with NA of 0.85 and R2 = 0.88 compared to five benchmarked models including Wu and Wang (J Hydraul Eng 125(12):1309–1312, 1999: ARE = 23.5%) and Deng et al. (J Sediment Res 5:24–29, 2007: R2 = 0.15). The analysis demonstrated that flow Froude number (Fr) maintained (−0.28) the strongest effect which decreased n by 32% when Fr at 1.2 reached supercritical conditions. Sediment concentration \({S}_{v}\) S v at 2000 ppm displayed (−0.10) dominant influence by dropping n by 25%. The model simulation applied with 10,000 iterations showed hydraulic radius (R) was the most responsive variable (total-order Sobol index = 0.50) based on uncertainty analysis through Monte Carlo simulations while Bayesian inference validated a 95% confidence interval spanning from 0.025 to 0.045 for n. When applied to changing bedforms with the \({\theta }^{0.15}\) θ 0.15 parameter the prediction accuracy increased by 15% under conditions of mobile bed movement (θ > 0.06). The calculated models find practical use in adaptive flood prediction and sediment-charged channel constructions which lead to risk cuts of 15–25% in flood scenarios. The presented work combines empirical methods with data-based strategies to improve predictive capabilities for situations involving non-uniform unsteady fluid motions.