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Examining the inertial subrange with nanoscale cross-wire measurements of turbulent pipe flow at high Reynolds number near the centreline

Published online by Cambridge University Press:  26 May 2021

Clayton P. Byers Open the ORCID record for Clayton P. Byers [Opens in a new window] ,
Marcus Hultmark ,
Ivan Marusic Open the ORCID record for Ivan Marusic [Opens in a new window]  and
Matt K. Fu Open the ORCID record for Matt K. Fu [Opens in a new window]
Clayton P. Byers
Affiliation:
Department of Engineering, Trinity College, Hartford, CT06106, USA
Marcus Hultmark
Affiliation:
Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, NJ08544, USA
Ivan Marusic
Affiliation:
Department of Mechanical Engineering, University of Melbourne, Victoria3010, Australia
Matt K. Fu*
Affiliation:
GALCIT, Caltech, Pasadena, CA91125, USA
*
†Email address for correspondence: [email protected]
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Abstract

Highly resolved, two-component velocity measurements were made near the centreline of turbulent pipe flow for Reynolds numbers in the range $102 \le Re_\lambda \leq 411$ ($1800 \le Re_\tau \leq 24\,700$). These unique data were obtained with a nanoscale cross-wire probe and used to examine the inertial subrange scaling of the longitudinal and transverse velocity components. Classical dissipation rate estimates were made using both the integration of one-dimensional dissipation spectra for each velocity component and the third-order moment of the longitudinal structure function. Although the second-order moments and one-dimensional spectra for each component showed behaviour consistent with local isotropy, clear inertial range similarity and behaviour were not exhibited in the third-order structure functions at these Reynolds numbers. When corrected for the effects of radial inhomogeneities at the centreline following the generalized expression of Danaila et al. (J. Fluid Mech., vol. 430, 2001, pp. 87–109), re-derived for the pipe flow domain, the third-order moments of the longitudinal structure function exhibited a clearer plateau per the classical Kolmogorov ‘four-fifths law’. Similar corrections described by Danaila et al. (J. Fluid Mech., vol. 430, 2001, pp. 87–109) applied to the analogous equation for the mixed structure functions (i.e. the ‘four-thirds law’) also yielded improvement over all ranges of scale, improving with increasing Reynolds number. The rate at which the ‘four-fifths’ law and ‘four-thirds’ law were approached by the third-order structure functions was found to be more gradual than decaying isotropic turbulence for the same Reynolds numbers.

JFM classification

Turbulent Flows: Pipe flow Turbulent Flows: Turbulence theory
Type
JFM Papers
Information
Journal of Fluid Mechanics , Volume 919 , 25 July 2021 , A21
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Copyright
© The Author(s), 2021. Published by Cambridge University Press

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