Computational Design of Experiments for Compound Fuel Injector Nozzles

Michalek, Donna J.; Peschke, B. D.; Evers, Lawrence W.

doi:10.4271/971617

Cited by 5 publications

(2 citation statements)

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“…The documented effectiveness of the conversion, < 0.7% for the studied range of operation regimes, is in accordance with (Bayvel & Orzechowski, 1993;Loffler-Mang & Leuckel, 1991). Its decrease with p also agrees with previous literature Michalek, Peschke, & Evers, 1997;Petela, 1984;Rivette, 1996). Such a low a can be explained by the subthreshold interaction of the droplets with air, which does not reach the value required for the secondary breakup.…”

Section: Mean and Turbulent Kinetic Energies In The Spraysupporting

confidence: 91%

Air–liquid interactions in a pressure-swirl spray

Jedelský

Malý

Corral

et al. 2018

International Journal of Heat and Mass Transfer

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The energy transfer between a liquid hollow cone spray and the surrounding air has been studied using both imaging and phase-Doppler techniques. The spray was produced by a pressure-swirl atomizer discharging Jet A-1 fuel at inlet over pressures of p = 0.5, 1.0 and 1.5 MPa into quiescent ambient air. The liquid exits the nozzle as a conical film which thins as it spreads and develops long-and shortwave sinusoidal instabilities with breakup occurring, at the length smaller than that predicted by the inviscid model, to form film fragments and ultimately droplets downstream the spray. The single shot imaging characterised the spray regions of near-nozzle flow, the breakup processes and the developed spray. The phase-Doppler system resolved the three components of velocity and size for the droplet flow as measured on radial profiles for four axial distances from the nozzle exit. A Stokes number, Stk, analysis of the droplets' response times to the airflow timescales showed that droplets < 5 µm followed the airflow faithfully and so were used to estimate the local airflow velocity. This allowed a comparison of both the droplet and airflow fields in terms of their mean and fluctuating velocity components to be made. The formation of the hollow cone spray and the interaction of the fragments and droplets with the air, through viscous drag, induce complex entrained airflows. The airflow was found to be highly anisotropic, fluctuating preferentially in the downstream direction, and spatially varying within three distinct spray regions. The air drag establishes a positive size-velocity correlation of droplets; their Stk reduces with axial distance and increases with droplet size and p; so that Stk ≈ 1 for 20-40 µm droplets and the largest droplets (80-160 µm, Stk > 10) move ballistically. The spatially resolved mean and turbulent kinetic energies of the air and spectra of the droplet velocity fluctuations are detailed in the paper. These findings are relevant to scientists and engineers modelling the complex two-phase flows.

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