scholarly journals Characterising Momentum Flux Events in High Reynolds Number Turbulent Boundary Layers

Fluids ◽  
2021 ◽  
Vol 6 (4) ◽  
pp. 168
Author(s):  
Rahul Deshpande ◽  
Ivan Marusic

The momentum flux in a canonical turbulent boundary layer is known to have a time-series signature that is characterised by a highly intermittent variation, which includes very short periods of intense flux activity. Here, we study the variation in these flux signal characteristics across almost a decade of flow Reynolds number (Reτ) by analysing datasets acquired using miniature cross-wire probes with matched spatial resolution. The analysis is facilitated by conditionally sampling the signal based on the quadrant (Qi; i = 1–4) and magnitude of the flux, revealing fractional cumulative contribution from Q4 to increase at a much faster rate than from Q2 with Reτ. An episodic description of the flux signal is subsequently undertaken, which associates this rapid increase in Q4 contributions with the emergence of extreme and rare flux events with Reτ. The same dataset is also used to test Townsend’s hypothesis on the active and inactive components of the momentum flux, which are obtained for the first time by implementing a spectral linear stochastic estimation-based decomposition methodology. While the active component is found to be the dominant contributor to the mean momentum flux consistent with Townsend’s hypothesis, the inactive component is found to be small but non-zero, owing to the non-linear interactions associated with the modulation phenomenon. Finally, an episodic description of the active and inactive momentum flux signal is undertaken to highlight the starkly different time series characteristics of the two flux components. The inactive flux signal is found to comprise individual statistically significant events associated with all four quadrants, leading to a small net contribution to the total flux.

An experimental investigation and a theoretical appraisal are presented which enlarge upon previous observations of multiple steady flows in a Taylor apparatus where the fluid-filled annulus is comparatively short. The aim of the experiments was a systematic exploration of all anomalous modes in this apparatus, namely those stable flows that exist only at sufficiently high Reynolds number R and are always distinct from the primary flow developed by gradually increasing R from small values. Having been established at high R , an anomalous mode will always collapse eventually if R is then gradually reduced. The theoretical material bearing on the interpretation of the experi­ments is reviewed in §2, where mathematical details are largely deferred but several new conclusions are demonstrated. In particular, some curious facts are revealed about the limits of stability for anomalous modes comprising even numbers of Taylor cells, and about the properties of flows comprising a single cell only. Following a description of the apparatus in § 3, which includes an account of several improvements that have been introduced since the earlier experiments, the new experimental results are reported in § 4. They include stability curves (critical R against aspect ratio of annulus) for anomalous modes consisting of from two to seven Taylor cells (§ 4.1), observations on collapse routes for all these modes (§ 4.3), and measurements of various phenomena exhibited by the single-cell mode (§ 4.5). These and other phenomena recorded here for the first time are seen to accord with the theoretical prospectus.


1981 ◽  
Vol 103 (1) ◽  
pp. 88-95 ◽  
Author(s):  
D. M. Rooney ◽  
R. D. Peltzer

Model tests were performed in a wind tunnel to determine vortex shedding patterns induced around a circular cylinder by spanwise shear in transitional Reynolds number flow. In addition, mean and fluctuating pressure measurements were obtained. The introduction of shear in the upstream flow generated two distinct cells of vortex frequencies behind the cylinder in the transcritical regime, thereby documenting for the first time that the re-established high Reynolds number shedding closely parallels patterns already observed in subcritical flow. The two cell pattern did not permit any correlation between shear level and cell length to be found.


2011 ◽  
Vol 133 (10) ◽  
Author(s):  
Amitesh Kumar ◽  
Manab Kumar Das

The study of a two-dimensional, steady, incompressible, turbulent flow of a dual jet consisting of a wall jet and an offset jet has been simulated numerically. The standard high Reynolds number two-equation k-ɛ model is used as the turbulence model. The Reynolds number is considered as 20000 for all the computations because the flow becomes fully turbulent. The merge point and the combined point have been obtained and compared with other results. The central streamline has been plotted and observed to follow an arc of a circle. The momentum flux has been computed along the axial length for the wall jet, offset jet and the dual jet and compared. A similarity profile has been obtained in the downstream direction. A detailed discussion has been provided on the pressure field, Reynolds stress, kinetic energy and its dissipation rate. The jet growth rate in terms of half-width, the decay of maximum velocity and the jet width are presented


1994 ◽  
Vol 9 (3) ◽  
pp. 279-285 ◽  
Author(s):  
Rahima K. Mohammed ◽  
Tim A. Osswald ◽  
Timothy J. Spiegelhoff ◽  
Esther M. Sun

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