Abstract

The present paper describes a method to extrapolate the mean wall shear stress, $$\tau _{wall}$$ , and the accurate relative position of a velocity probe with respect to the wall, $$\Delta y$$ , from an experimentally measured mean velocity profile in a turbulent boundary layer. Validation is made between experimental and direct numerical simulation data of turbulent boundary layer flows with independent measurement of the shear stress. The set of parameters which minimize the residual error with respect to the canonical description of the boundary layer profile is taken as the solution. Several methods are compared, testing different descriptions of the canonical mean velocity profile (with and without overshoot over the logarithmic law) and different definitions of the residual function of the optimization. The von Karman constant is used as a parameter of the fitting process in order to avoid any hypothesis regarding its value that may be affected by different initial or boundary conditions of the flow. Results show that the best method provides an accuracy of $$\Delta u_\tau \le 0.6\,\%$$ for the estimation of the friction velocity and $$\Delta y^+\le 0.3$$ for the position of the wall. The robustness of the method is tested including unconverged near-wall measurements, pressure gradient, and reduced number of points; the importance of the location of the first point is also tested, and it is shown that the method presents a high robustness even in highly distorted flows, keeping the aforementioned accuracies if one acquires at least one data point in $$y^+<10$$ . The wake component and the thickness of the boundary layer are also simultaneously extrapolated from the mean velocity profile. This results in the first study, to the knowledge of the authors, where a five-parameter fitting is carried out without any assumption on the von Karman constant and the limits of the logarithmic layer further from its existence.

Highlights

  • Dimensional analysis applied to wall-bounded flows shows that the mean velocity profile, or equivalently the velocity gradient, can be described by just two non-dimensional parameters

  • It may explain why the value suggested by Nagib and Chauhan (2008) is κ = 0.384, since the authors of this paper considered the bump to account for the overshoot present over the log layer in order to estimate the von Kármán constant

  • The proposed method allows the post-processing of the mean velocity profile in turbulent boundary layers

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Summary

Introduction

Dimensional analysis applied to wall-bounded flows shows that the mean velocity profile, or equivalently the velocity gradient, can be described by just two non-dimensional parameters. As Prandtl first postulated, at sufficiently high Reynolds number, there is an inner layer in which the velocity profile is described by the viscous scales independently of δ and ue, the freestream velocity; du+ dy+. For the outer layer, the velocity profile is independent of ν implying that du+ dy+ outer (y/δ). One can argue that for δν ≪ y ≪ δ: inner(y+) = outer(y/δ). This condition can only be satisfied by both functions being a constant (Millikan 1938), resulting in κy1+, where κ is the von Kármán constant. It can be integrated to obtain the logarithmic law for the velocity u+

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