<p>In technical applications, pumping fluids through pipes often generates turbulent flows with high Reynolds numbers, where over 90% of the pumping energy is dissipated by near-wall turbulence. Relaminarization of such flows offers significant energy savings. Streamwise traveling waves of wall blowing and suction have been shown to relaminarize turbulent pipe flow at a low friction Reynolds number (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\textrm{Re}\tau =110\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Re</mtext> <mi>τ</mi> <mo>=</mo> <mn>110</mn> </mrow> </math></EquationSource> </InlineEquation>), reducing friction losses and energy consumption. This work extends the investigation to higher Reynolds numbers, demonstrating that traveling waves can trigger relaminarization up to <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\textrm{Re}\tau =720\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Re</mtext> <mi>τ</mi> <mo>=</mo> <mn>720</mn> </mrow> </math></EquationSource> </InlineEquation>. A parametric study is conducted at <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\textrm{Re}\tau =180\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Re</mtext> <mi>τ</mi> <mo>=</mo> <mn>180</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\textrm{Re}\tau =360\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Re</mtext> <mi>τ</mi> <mo>=</mo> <mn>360</mn> </mrow> </math></EquationSource> </InlineEquation>, examining upstream traveling waves (UTWs, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(c&lt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&lt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) and downstream traveling waves (DTWs, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(c&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) while varying amplitude <i>a</i>, celerity <i>c</i>, and wavelength <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>. Consistent with channel flow studies, UTWs destabilize the flow yet can generate sublaminar drag; only low-speed UTWs with large amplitudes effectively reduce energy consumption. For DTWs, a wide range of parameters reduces drag, but significant net energy savings occur only for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(0.067U_{c,lam}\lesssim a \lesssim 0.1U_\mathrm{{{c,lam}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0.067</mn> <msub> <mi>U</mi> <mrow> <mi>c</mi> <mo>,</mo> <mi>l</mi> <mi>a</mi> <mi>m</mi> </mrow> </msub> <mo>≲</mo> <mi>a</mi> <mo>≲</mo> <mn>0.1</mn> <msub> <mi>U</mi> <mrow> <mi mathvariant="normal">c</mi> <mo>,</mo> <mi mathvariant="normal">lam</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(c\approx U_\mathrm{{{c,lam}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>≈</mo> <msub> <mi>U</mi> <mrow> <mi mathvariant="normal">c</mi> <mo>,</mo> <mi mathvariant="normal">lam</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\lambda \approx 360\delta _\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>≈</mo> <mn>360</mn> <msub> <mi>δ</mi> <mi>ν</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, independent of Reynolds number. During relaminarization, the turbulent kinetic energy decays exponentially nearly to zero within <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(3D/u_\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mi>D</mi> <mo stretchy="false">/</mo> <msub> <mi>u</mi> <mi>τ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, while the flow accelerates to its terminal velocity over <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(65D/u_\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>65</mn> <mi>D</mi> <mo stretchy="false">/</mo> <msub> <mi>u</mi> <mi>τ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. The relaminarized flow exhibits half-vortical structures scaling in viscous units superimposed on a laminar profile, effectively reducing the pipe cross section. Within <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(180\le \textrm{Re}_\tau \le 540\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>180</mn> <mo>≤</mo> <msub> <mtext>Re</mtext> <mi>τ</mi> </msub> <mo>≤</mo> <mn>540</mn> </mrow> </math></EquationSource> </InlineEquation>, over 97% of the theoretically achievable drag reduction is realized. These scaling relations enable prediction of traveling wave-induced relaminarization at higher Reynolds numbers, offering a practical approach for energy-efficient turbulent pipe flow control.</p>

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Relaminarization of turbulent pipe flow induced by streamwise traveling wave wall transpiration and its scaling

  • Christian Bauer,
  • Claus Wagner

摘要

In technical applications, pumping fluids through pipes often generates turbulent flows with high Reynolds numbers, where over 90% of the pumping energy is dissipated by near-wall turbulence. Relaminarization of such flows offers significant energy savings. Streamwise traveling waves of wall blowing and suction have been shown to relaminarize turbulent pipe flow at a low friction Reynolds number ( \(\textrm{Re}\tau =110\) Re τ = 110 ), reducing friction losses and energy consumption. This work extends the investigation to higher Reynolds numbers, demonstrating that traveling waves can trigger relaminarization up to \(\textrm{Re}\tau =720\) Re τ = 720 . A parametric study is conducted at \(\textrm{Re}\tau =180\) Re τ = 180 and \(\textrm{Re}\tau =360\) Re τ = 360 , examining upstream traveling waves (UTWs, \(c<0\) c < 0 ) and downstream traveling waves (DTWs, \(c>0\) c > 0 ) while varying amplitude a, celerity c, and wavelength \(\lambda \) λ . Consistent with channel flow studies, UTWs destabilize the flow yet can generate sublaminar drag; only low-speed UTWs with large amplitudes effectively reduce energy consumption. For DTWs, a wide range of parameters reduces drag, but significant net energy savings occur only for \(0.067U_{c,lam}\lesssim a \lesssim 0.1U_\mathrm{{{c,lam}}}\) 0.067 U c , l a m a 0.1 U c , lam , \(c\approx U_\mathrm{{{c,lam}}}\) c U c , lam , and \(\lambda \approx 360\delta _\nu \) λ 360 δ ν , independent of Reynolds number. During relaminarization, the turbulent kinetic energy decays exponentially nearly to zero within \(3D/u_\tau \) 3 D / u τ , while the flow accelerates to its terminal velocity over \(65D/u_\tau \) 65 D / u τ . The relaminarized flow exhibits half-vortical structures scaling in viscous units superimposed on a laminar profile, effectively reducing the pipe cross section. Within \(180\le \textrm{Re}_\tau \le 540\) 180 Re τ 540 , over 97% of the theoretically achievable drag reduction is realized. These scaling relations enable prediction of traveling wave-induced relaminarization at higher Reynolds numbers, offering a practical approach for energy-efficient turbulent pipe flow control.