Initial breakup of a small-diameter liquid jet by a high-speed gas stream

Abstract

The situation of a small-diameter liquid jet exposed to a large-diameter high-speed gas jet (gas-to-liquid nozzle area ratio of order 100 to 1000) is investigated experimentally. Flow visualization and particle-sizing techniques are employed to examine the initial jet breakup process and primary liquid atomization. Observations of the initial breakup of the liquid jet in the near-nozzle region, combined with droplet-size measurements, are used in an effort to elucidate the dominant mechanism of primary breakup of the liquid. It is shown that for large aerodynamic Weber numbers, the bulk of the liquid atomization is completed within a few gas-jet diameters of the nozzle exit, inside of the potential cone of the gas flow. Breakup is therefore completed within the zone of constant ambient gas velocity. It is argued that the mechanism of initial jet breakup is similar to that of a liquid drop suddenly exposed to a high-speed gas stream. A phenomenological breakup model is proposed for the initial droplet size, based upon the accelerative, secondary destabilization (via Rayleigh-Taylor instability) of the liquid wave crests resulting from the primary Kelvin-Helmholtz instability of the liquid jet surface. Primary mean droplet sizes are shown to scale well on the most unstable Rayleigh-Taylor wavelength, and the dependence of the droplet diameter on both the atomizing gas velocity and the liquid surface tension are successfully captured by the proposed breakup model.

Structure of the Continuous Liquid Jet Core during Coaxial Air-Blast Atomisation

“…The successful atomization of the liquid jet into small droplets is essential for combustion, as it promotes evaporation and thorough mixing of the liquid fuel vapour with the surrounding gas. For this reason, the process of disintegration of the liquid jet by the high speed air co-flow is of great interest to combustion research and has been studied by a large number of researchers, including [1][2][3][4][5][6][7]. The main visualisation method of the liquid jet in these investigations is shadowgraphy.…”

Investigation of Fuel Atomization with Density Functions

“…Weber number of liquid (We L = 0.153), and gas-to-liquid surface of atomizer orifice (A gl = 15) were independent of the atomizing pressure [20,8]. Based on the dimensionless numbers, it is clear that the air jet dominates the flow.…”

“…In addition to the usual parameters, Mach number was also determined by Eq. (8). The results are summarized in Table 4.…”

Size distributions of sprays produced by violent wave impacts on vertical sea walls

“…One approach to modelling the spray is to use a PDF to represent the probable number of droplets with certain diameters and velocities in a given region [13][14][15][16][17]. The RosinRammler distribution was suggested [18] and has been found to be appropriate for many types of atomization spray [19].…”