Effect of nozzle upscaling on coaxial, gas-assisted atomization

Mass flow scaling of gas-assisted coaxial atomizers from laboratory to industrial scale is of major interest for a wide field of applications. However, there is only scarce knowledge and research concerning the effect of atomizer scale-up on liquid breakup and spray characteristics. The main objective of this study is therefore to derive basic principles for liquid jet breakup using upscaled nozzles to increase the liquid mass flow rate [Formula: see text]. For that purpose, atomizers with the same geometrical setup but increased sizes have been designed and experimentally investigated for [Formula: see text], 50, 100, and 500 kg/h, while the aerodynamic Weber number Weaero and gas-to-liquid ratio GLR have been kept constant. The primary jet breakup was recorded via high-speed imaging, and the liquid core length LC and the frequency of the Kelvin–Helmholtz instability fK were extracted. Applying these results as reference data, highly resolved numerical simulations have been performed to gain a deeper understanding of the effect of mass flow scaling. In the case of keeping Weaero and GLR constant, it has been shown by both experiments and simulations that the breakup morphology, given by a pulsating liquid jet with the disintegration of fiber-type liquid fragments, remains almost unchanged with the degree of upscaling n. However, the normalized breakup length [Formula: see text] has been found to be considerably increased with increasing n. The reason has been shown to be the decreased gas flow velocity vgas at the nozzle exit with n, which leads to a decreased gas-to-liquid momentum flux ratio j and an attenuated momentum exchange between the phases. Accordingly, the calculated turbulence kinetic energy of the gas flow and the specific kinetic energy in the liquid phase decrease with n. This corresponds to a decreased fKHI with n or [Formula: see text], respectively, which has been confirmed by both experiments and simulations. The same behavior has been shown for two liquids with different viscosities and at different Weaero. The obtained results allow a first-order estimate of the liquid breakup characteristics, where the influence of nozzle upscaling can be incorporated into j and Reliq in terms of n.

[1]  H. Bockhorn,et al.  Numerical simulations of air-assisted primary atomization at different air-to-liquid injection angles , 2022, International Journal of Multiphase Flow.

[2]  T. Kolb,et al.  Mass Flow Scaling of Gas-Assisted Coaxial Atomizers , 2022, Applied Sciences.

[3]  T. Kolb,et al.  Comparison of Central Jet and Annular Sheet Atomizers at Identical Gas Momentum Flows , 2021, Industrial & Engineering Chemistry Research.

[4]  T. Kolb,et al.  Towards system pressure scaling of gas assisted coaxial burner nozzles – An empirical model , 2021, Applications in Energy and Combustion Science.

[5]  T. Kolb,et al.  Effect of elevated pressure on air-assisted primary atomization of coaxial liquid jets: Basic research for entrained flow gasification , 2020, Renewable and Sustainable Energy Reviews.

[6]  T. Kolb,et al.  Effect of Solid Particles on Droplet Size Applying the Time-Shift Method for Spray Investigation , 2020, Applied Sciences.

[7]  S. Sahu,et al.  Influence of nozzle geometry on primary and large-scale instabilities in coaxial injectors , 2020 .

[8]  A. Aliseda,et al.  Influence of steady and oscillating swirl on the near-field spray characteristics in a two-fluid coaxial atomizer , 2020, International Journal of Multiphase Flow.

[9]  A. Kastengren,et al.  Comparison of X-ray and optical measurements in the near-field of an optically dense coaxial air-assisted atomizer , 2020 .

[10]  T. Kolb,et al.  Experimental investigation on the influence of system pressure on resulting spray quality and jet breakup applying pressure adapted twin-fluid nozzles , 2020, International Journal of Multiphase Flow.

[11]  S. Sahu,et al.  Liquid jet breakup unsteadiness in a coaxial air-blast atomizer , 2018 .

[12]  W. Sirignano,et al.  Planar liquid jet: Early deformation and atomization cascades , 2017 .

[13]  Johannes Janicka,et al.  Experimental and numerical investigation of the primary breakup of an airblasted liquid sheet , 2017 .

[14]  T. Kolb,et al.  Simulation of the primary breakup of a high-viscosity liquid jet by a coaxial annular gas flow , 2016 .

[15]  Laszlo Fuchs,et al.  Sensitivity of VOF simulations of the liquid jet breakup to physical and numerical parameters , 2016 .

[16]  S. Pirker,et al.  An Eulerian–Lagrangian hybrid model for the coarse-grid simulation of turbulent liquid jet breakup , 2016 .

[17]  F. Xiao,et al.  LES of turbulent liquid jet primary breakup in turbulent coaxial air flow , 2014 .

[18]  Hui Zhao,et al.  Effect of central tube thickness on wave frequency of coaxial liquid jet , 2014 .

[19]  B. Duret,et al.  Improving primary atomization modeling through DNS of two-phase flows , 2013 .

[20]  Anthony J. Robinson,et al.  Influence of surface tension implementation in Volume of Fluid and coupled Volume of Fluid with Level Set methods for bubble growth and detachment , 2013 .

[21]  Michel Versluis,et al.  High-speed imaging in fluids , 2013 .

[22]  Hui Zhao,et al.  Breakup and atomization of a round coal water slurry jet by an annular air jet , 2012 .

[23]  Djamel Lakehal,et al.  Subgrid-scale modelling of surface tension within interface tracking-based Large Eddy and Interface Simulation of 3D interfacial flows , 2012 .

[24]  A. J. Salazar,et al.  Modeling the disintegration of modulated liquid jets using volume-of-fluid (VOF) methodology , 2011 .

[25]  A. Umemura,et al.  Simulation of liquid jet primary breakup: Dynamics of ligament and droplet formation , 2010 .

[26]  Christophe Dumouchel,et al.  On the experimental investigation on primary atomization of liquid streams , 2008 .

[27]  Mikhael Gorokhovski,et al.  Modeling Primary Atomization , 2008 .

[28]  P. Dimotakis Two-dimensional shear-layer entrainment , 1986 .

[29]  J. Lasheras,et al.  Liquid Jet Instability and Atomization in a Coaxial Gas Stream , 2000 .

[30]  S. Ziada,et al.  PDA measurements of droplet size and mass flux in the three-dimensional atomisation region of water jet in air cross-flow , 2000 .