Invariant p.d.f. property of velocity fluctuation in high-Reynolds-number turbulent boundary layer
Streamwise velocity fluctuations are measured in a zero-pressure gradient turbulent boundary layer at high Reynolds numbers. When normalised by the mean and standard deviation, u Subscript r <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:msub> <mml:mi>u</mml:mi> <mml:mi>r</mml:mi> </mml:msub> </mml:math> $u_r$ , the probability density function (p.d.f.) of the fluctuations exhibits invariance within distinct wall-normal regions. Two such regions were identified: one situated near the plateau of the turbulence intensity profile and the other associated with the logarithmic region ( left parenthesis u Subscript r Superscript plus Baseline right parenthesis squared equals upper A 1 ln left parenthesis y divided by delta right parenthesis plus upper B 1 <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:mo stretchy="false">(</mml:mo> <mml:msubsup> <mml:mi>u</mml:mi> <mml:mi>r</mml:mi> <mml:mo>+</mml:mo> </mml:msubsup> <mml:msup> <mml:mo stretchy="false">)</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:mo>=</mml:mo> <mml:msub> <mml:mi>A</mml:mi> <mml:mn>1</mml:mn> </mml:msub> <mml:mi>ln</mml:mi> <mml:mo></mml:mo> <mml:mo stretchy="false">(</mml:mo> <mml:mi>y</mml:mi> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mi>δ</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:mo>+</mml:mo> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:math> $(u_r^+)^2=A_1 \ln (y/\delta )+B_1$ ) consistent with Townsend’s attached-eddy hypothesis. The p.d.f. shapes in both regions are independent of Reynolds number, demonstrating their universality. The slope, upper A 1 <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:msub> <mml:mi>A</mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:math> $A_1$ , and additive constant, upper B 1 <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:math> $B_1$ , were evaluated to be upper A 1 asymptotically equals 1.42 <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:msub> <mml:mi>A</mml:mi> <mml:mn>1</mml:mn> </mml:msub> <mml:mo>≃</mml:mo> <mml:mn>1.42</mml:mn> </mml:math> $A_1 \simeq 1.42$ and upper B 1 asymptotically equals 1.75 <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>1</mml:mn> </mml:msub> <mml:mo>≃</mml:mo> <mml:mn>1.75</mml:mn> </mml:math> $B_1 \simeq 1.75$ , respectively, for upper O left parenthesis 10 Superscript 4 Baseline right parenthesis less than italic Re Subscript tau <mml:math xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mnf="http://cambridge.org/core/manifest" xmlns:cup="http://contentservices.cambridge.org" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:m="http://cambridge.org/core/metadata" xmlns:core="http://cambridge.org/core" xmlns:c="http://cambridge.org/core/content"> <mml:mi>O</mml:mi>
Authors
- Yoshiyuki Tsuji (ORCID: https://orcid.org/0000-0001-5109-0964)
- Atsushi IDO
Institutions
- Shanghai Tunnel Engineering (China) (CN)
- German Dutch Wind Tunnels (NL)
- Nagoya University (JP)
Publication Details
- Journal
- Journal of Fluid Mechanics
- Published
- 2026-06-18
- DOI
- https://doi.org/10.1017/jfm.2026.11568
- Primary Topic
- Fluid Dynamics and Turbulent Flows
- Type
- article
- Field-Weighted Citation Impact
- 0.00