scholarly journals Do extreme events trigger turbulence decay? – a numerical study of turbulence decay time in pipe flows

2021 ◽  
Vol 912 ◽  
Author(s):  
Takahiro Nemoto ◽  
Alexandros Alexakis

Abstract

2012 ◽  
Vol 62 (2) ◽  
pp. 97
Author(s):  
A Kartushinsky ◽  
Y Rudi ◽  
S Tisler ◽  
I Shcheglov ◽  
A Shablinsky

1996 ◽  
Vol 306 ◽  
pp. 293-323 ◽  
Author(s):  
Vadim Borue ◽  
Steven A. Orszag

High-resolution numerical simulations (with up to 2563 modes) are performed for three-dimensional flow driven by the large-scale constant force fy = F cos(x) in a periodic box of size L = 2π (Kolmogorov flow). High Reynolds number is attained by solving the Navier-Stokes equations with hyperviscosity (-1)h+1Δh (h = 8). It is shown that the mean velocity profile of Kolmogorov flow is nearly independent of Reynolds number and has the ‘laminar’ form vy = V cos(x) with a nearly constant eddy viscosity. Nevertheless, the flow is highly turbulent and intermittent even at large scales. The turbulent intensities, energy dissipation rate and various terms in the energy balance equation have the simple coordinate dependence a + b cos(2x) (with a, b constants). This makes Kolmogorov flow a good model to explore the applicability of turbulence transport approximations in open time-dependent flows. It turns out that the standard expression for effective (eddy) viscosity used in K-[Escr ] transport models overpredicts the effective viscosity in regions of high shear rate and should be modified to account for the non-equilibrium character of the flow. Also at large scales the flow is anisotropic but for large Reynolds number the flow is isotropic at small scales. The important problem of local isotropy is systematically studied by measuring longitudinal and transverse components of the energy spectra and crosscorrelation spectra of velocities and velocity-pressure-gradient spectra. Cross-spectra which should vanish in the case of isotropic turbulence decay only algebraically but somewhat faster than corresponding isotropic correlations. It is verified that the pressure plays a crucial role in making the flow locally isotropic. It is demonstrated that anisotropic large-scale flow may be considered locally isotropic at scales which are approximately ten times smaller than the scale of the flow.


2018 ◽  
Vol 56 (2) ◽  
pp. 245-255 ◽  
Author(s):  
Ming Zhao ◽  
Mohamed S. Ghidaoui ◽  
Moez Louati ◽  
Huan-Feng Duan

2015 ◽  
Vol 91 (4) ◽  
Author(s):  
Émeric Mercier ◽  
Armelle Even ◽  
Elodie Mirisola ◽  
Delphine Wolfersberger ◽  
Marc Sciamanna

2011 ◽  
Vol 130-134 ◽  
pp. 3603-3606
Author(s):  
Fu Sheng Yan ◽  
Wei Jun Zhang ◽  
Ru Quan Liang

This investigation deals with the study on the processes involved in the phenomenon about turbulence modification in dilute gas-particle turbulent flows. The proposed model, along with other selected turbulence modification models from the literature, is used to simulate a particle-laden vertical pipe flow. The simulation results show that the new model provides improved predictions of the experimental data.


2019 ◽  
Vol 27 (26) ◽  
pp. 37196 ◽  
Author(s):  
J. P. Lauterio-Cruz ◽  
H. E. Ibarra-Villalon ◽  
O. Pottiez ◽  
Y. E. Bracamontes-Rodriguez ◽  
O. S. Torres-Muñoz ◽  
...  

1998 ◽  
Vol 120 (1) ◽  
pp. 54-61 ◽  
Author(s):  
R. R. Parchen ◽  
W. Steenbergen

Both experimental and numerical studies have been performed aimed at the description of the decay of swirl in turbulent pipe flows. Emphasis is put on the effect of the initial velocity distribution on the rate of decay. The experiments show that, even far downstream of the swirl generator, the decay of the integral amount of angular momentum depends on the initial velocity distribution. This suggests that the description of the decay in terms of the widely suggested single exponential, function, is not sufficient. The calculations are based on (i) a standard k – ε model and (ii) models based on an algebraic transport model for the turbulent stresses. It appears that in a weakly swirling pipe flow, second-order models reduce to simple modifications of the standard k – ε model. While the standard k – ε model predicts a decay largely insensitive to the initial velocity distribution, the modified versions of the k – ε model, the ASM and the RSM, predict a strong sensitivity to the initial velocity distribution. Nevertheless, the standard k – ε model seems to predict the rate of decay of the swirl better than the second-order models. It is concluded that the corrections for the streamline curvature introduced by the second-order closures, largely overestimate the effect of rotation on the radial exchange of angular momentum.


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