2015
DOI: 10.1080/14685248.2015.1052464
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Large-eddy simulations of temporally accelerating turbulent channel flow

Abstract: The unsteady turbulent channel flow subject to the temporal acceleration is considered in this study. Large-eddy simulations were performed to study the response of the turbulent flow to the temporal acceleration. The simulations were started with the fully developed turbulent channel flow at an initial Reynolds number of Re 0 = 3500 (based on the channel half-height and the bulk-mean velocity), and then a constant temporal acceleration was applied. During the acceleration, the Reynolds number of the channel f… Show more

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Cited by 6 publications
(4 citation statements)
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“…Taking advantage of the periodic boundary conditions in the two wall-parallel directions, the Poisson equation is solved in the Fourier space with a tridiagonal matrix inversion in the wall-normal direction. The in-house code has been verified extensively in our previous studies (see Chung and Talha 2011;Hurst et al 2014;Talha and Chung 2015).…”
Section: Simulation Setupmentioning
confidence: 99%
“…Taking advantage of the periodic boundary conditions in the two wall-parallel directions, the Poisson equation is solved in the Fourier space with a tridiagonal matrix inversion in the wall-normal direction. The in-house code has been verified extensively in our previous studies (see Chung and Talha 2011;Hurst et al 2014;Talha and Chung 2015).…”
Section: Simulation Setupmentioning
confidence: 99%
“…Taking the advantage of the periodic boundary condition in both streamwise and spanwise directions, the Poisson equation is solved in the Fourier space with a tridiagonal matrix inversion in the wall-normal direction. The in-house code has been verified extensively in our previous studies (see Chung and Talha, 2011;Hurst et al, 2014;Talha and Chung, 2015).…”
Section: Simulation Setupmentioning
confidence: 99%
“…1990; Lozano-Durán et al. 2020), flows with streamwise acceleration or deceleration (He, Ariyaratne & Vardy 2008, 2011; He & Ariyaratne 2011; Jung & Chung 2012; He & Seddighi 2013, 2015; Talha & Chung 2015; Jung & Kim 2017; Sundstrom & Cervantes 2018 c ; de Wiart, Larsson & Murman 2018), and flows with a streamwise oscillating pressure gradient (Tardu, Binder & Blackwelder 1994; Scotti & Piomelli 2001; Weng, Boij & Hanifi 2016; Sundstrom & Cervantes 2018 b ; Cheng et al. 2020).…”
Section: Introductionmentioning
confidence: 99%
“…While in general non-equilibrium may refer to any flow where the time derivative and/or nonlinear advection terms in the ensemble-averaged momentum balance are non-negligible, in this work we consider only non-stationary flows. Examples considered previously in the direct numerical simulations (DNS), LES and experimental literature include flows with spanwise wall movements in time such as wall oscillations (Jung, Mangiavacchi & Akhavan 1992;Quadrio & Ricco 2003;Ricco et al 2012;Yao, Chen & Hussain 2019), flows where a spanwise pressure gradient is applied suddenly (Moin et al 1990;Lozano-Durán et al 2020), flows with streamwise acceleration or deceleration (He, Ariyaratne & Vardy 2008Jung & Chung 2012;He & Seddighi 2013Talha & Chung 2015;Jung & Kim 2017;Sundstrom & Cervantes 2018c;de Wiart, Larsson & Murman 2018), and flows with a streamwise oscillating pressure gradient (Tardu, Binder & Blackwelder 1994;Scotti & Piomelli 2001;Weng, Boij & Hanifi 2016;Sundstrom & Cervantes 2018b;Cheng et al 2020).…”
Section: Introductionmentioning
confidence: 99%