2008
DOI: 10.1080/14685240801964912
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Sensitivity analysis of initial condition parameters on the transitional temporal turbulent mixing layer

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Cited by 6 publications
(5 citation statements)
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“…In contrast, the flow field is dominated by more regular and smooth streamwise elongated vortices at M c = 1.8 and τ = 250. This phenomenon is consistent with previous studies of small-scale vortical structures in compressible mixing layer, where it is generally believed that the vortical structures are more aligned in the streamwise direction at higher M c , particularly in the transition region (Balaras et al 2001;Fathali et al 2008;Arun et al 2019;Li et al 2021).…”
Section: φ =supporting
confidence: 92%
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“…In contrast, the flow field is dominated by more regular and smooth streamwise elongated vortices at M c = 1.8 and τ = 250. This phenomenon is consistent with previous studies of small-scale vortical structures in compressible mixing layer, where it is generally believed that the vortical structures are more aligned in the streamwise direction at higher M c , particularly in the transition region (Balaras et al 2001;Fathali et al 2008;Arun et al 2019;Li et al 2021).…”
Section: φ =supporting
confidence: 92%
“…2001; Rossmann, Mungal & Hanson 2002; Fathali et al. 2008; Hickey, Hussain & Wu 2016; Arun et al. 2019; Li et al.…”
Section: Introductionmentioning
confidence: 99%
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“…This is appropriate because the velocity field drives the instability and turbulence, as observed in the single-density case; this approach also allows the disturbance to be consistent between Atwood numbers. Different velocity disturbances can produce significantly different growth rates at early times in mixing layers (Fathali et al 2008), but the present goal is to quickly establish self-similar growth and minimize long-lived large-scale structures that are uniquely associated with initial disturbances. To roughly resemble physical experiments, the velocity perturbation is confined to a thin (in y) region centred at the mean velocity profile interface.…”
Section: Initial Disturbancementioning
confidence: 99%
“…The first method utilizes a stochastic approach whereby the "turbulent" perturbations are comprised from random realizations having statistical equivalency to that of the actual turbulent flow field. 34,[41][42][43] The second method uses the output from DNS and Large Eddy Simulations ͑LES͒ that have been performed separately on an extended computational domain encompassing the splitter plate. [44][45][46] The third least expensive and simplest method of initiating the turbulence follows from linear stability theory.…”
Section: Problem Definitionmentioning
confidence: 99%