Abstract

In this study, various mixing and evaporation modeling assumptions typically considered for large-eddy simulation (LES) of the well-established Engine Combustion Network (ECN) Spray A are explored. A coupling between LES and Lagrangian particle tracking (LPT) is employed to simulate liquid n-dodecane spray injection into hot inert gaseous environment, wherein Lagrangian droplets are introduced from a small cylindrical injection volume while larger length scales within the nozzle diameter are resolved. This LES/LPT approach involves various modeling assumptions concerning the unresolved near-nozzle region, droplet breakup, and LES subgrid scales (SGS) in which their impact on common spray metrics is usually left unexplored despite frequent utilization. Here, multi-parametric analysis is performed on the effects of (i) cylindrical injection volume dimensions, (ii) secondary breakup model, particularly Kelvin–Helmholtz Rayleigh–Taylor (KHRT) against a no-breakup model approach, and (iii) LES SGS models, particularly Smagorinsky and one-equation models against implicit LES. The analysis indicates the following findings: (i) global spray characteristics are sensitive to radial dimension of the cylindrical injection volume, (ii) the no-breakup model approach performs equally well, in terms of spray penetration and mixture formation, compared with KHRT, and (iii) the no-breakup model is generally insensitive to the chosen SGS model for the utilized grid resolution.

Highlights

  • Multiphase flow mixing and evaporation phenomena play pivotal roles in various industrial and energy-related applications, such as fuel spray in engines of stationary energy and transportation sectors

  • Fuel spray is described by the injection of a high pressure and momentum liquid fuel into ambient gas

  • These fundamental studies have described the details of multi-stage mixing, droplet transport, atomization, and evaporation of fuel sprays

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Summary

Introduction

Multiphase flow mixing and evaporation phenomena play pivotal roles in various industrial and energy-related applications, such as fuel spray in engines of stationary energy and transportation sectors. Mixing of the liquid fuel and ambient gas under engine-relevant conditions with the presence of turbulence is an intricate process, which requires specific considerations and simplifying assumptions in numerical simulations. In a typical fuel spray, the liquid core has similar properties to the potential core of a single-phase jet [5,6,7,8] and it is under a strong shear stress. This strong shear results in primary breakup or atomization, leading to the formation of Energies 2020, 13, 3360; doi:10.3390/en13133360 www.mdpi.com/journal/energies

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