<p>We use numerical simulations to study the interaction between a turbulent jet, discharged vertically from a circular nozzle at the bottom of a horizontal liquid layer of height <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_0=0.35\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>h</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.35</mn> </mrow> </math></EquationSource> </InlineEquation> m, and surface waves. All simulations are run at a fixed value of the jet Reynolds number (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( \textrm{Re}_{j}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>Re</mtext> <mi>j</mi> </msub> </math></EquationSource> </InlineEquation> = 20,000, based on the nozzle diameter) and for two different values of the surface waves elevation, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(H=0.02\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo>=</mo> <mn>0.02</mn> </mrow> </math></EquationSource> </InlineEquation> m (simulation <i>R</i>1) and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(H=0.03\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo>=</mo> <mn>0.03</mn> </mrow> </math></EquationSource> </InlineEquation> m (simulation <i>R</i>2). A reference simulation, assuming a free surface without waves, is also performed for comparison purposes (simulation <i>R</i>0). We focus on the influence of the surface waves on the jet flow field, considering in particular the behavior of the jet width and of the mean jet velocity—which we analyze applying a phase-averaged technique. Our results show that surface waves induce a reduction of the vertical component of the jet velocity, and a corresponding increase of the horizontal components of the jet velocity. In particular, we observe that the reduction of the centerline mean vertical velocity (along the vertical direction <i>z</i>) is linear in the region close to the jet nozzle, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="92" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_0/W_m\sim z\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mn>0</mn> </msub> <mo stretchy="false">/</mo> <msub> <mi>W</mi> <mi>m</mi> </msub> <mo>∼</mo> <mi>z</mi> </mrow> </math></EquationSource> </InlineEquation>, but can be faster than linear (superlinear) in the region close to the liquid surface, for the larger amplitude waves. Correspondingly, the jet width increases linearly with <i>z</i>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="707_2025_4321_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="92" /> </InlineMediaObject> <EquationSource Format="TEX">\(b \sim C \left( z/d_0 \right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>∼</mo> <mi>C</mi> <mfenced close=")" open="("> <mi>z</mi> <mo stretchy="false">/</mo> <msub> <mi>d</mi> <mn>0</mn> </msub> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, but at a slope <i>C</i> that does depend on the distance from the liquid surface. These findings suggest that surface waves enhance entrainment and dilution, offering insights for improving jet–wave interaction models and parameterizations.</p>

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Large eddy simulation of a turbulent submerged jet interacting with a wave environment

  • D. Maraglino,
  • D. De Padova,
  • M. Mossa,
  • F. Zonta,
  • A. Soldati

摘要

We use numerical simulations to study the interaction between a turbulent jet, discharged vertically from a circular nozzle at the bottom of a horizontal liquid layer of height \(h_0=0.35\) h 0 = 0.35 m, and surface waves. All simulations are run at a fixed value of the jet Reynolds number ( \( \textrm{Re}_{j}\) Re j = 20,000, based on the nozzle diameter) and for two different values of the surface waves elevation, \(H=0.02\) H = 0.02 m (simulation R1) and \(H=0.03\) H = 0.03 m (simulation R2). A reference simulation, assuming a free surface without waves, is also performed for comparison purposes (simulation R0). We focus on the influence of the surface waves on the jet flow field, considering in particular the behavior of the jet width and of the mean jet velocity—which we analyze applying a phase-averaged technique. Our results show that surface waves induce a reduction of the vertical component of the jet velocity, and a corresponding increase of the horizontal components of the jet velocity. In particular, we observe that the reduction of the centerline mean vertical velocity (along the vertical direction z) is linear in the region close to the jet nozzle, \(W_0/W_m\sim z\) W 0 / W m z , but can be faster than linear (superlinear) in the region close to the liquid surface, for the larger amplitude waves. Correspondingly, the jet width increases linearly with z, \(b \sim C \left( z/d_0 \right) \) b C z / d 0 , but at a slope C that does depend on the distance from the liquid surface. These findings suggest that surface waves enhance entrainment and dilution, offering insights for improving jet–wave interaction models and parameterizations.