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Mean Droplet Size and Local Velocity in Horizontal Isothermal Free Jets of Air and Water, respectively, Viscous Liquid in Quiescent Ambient Air
Author(s) -
Al Rabadi S.,
Friedel L.,
Al Salaymeh A.
Publication year - 2007
Publication title -
chemical engineering and technology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.403
H-Index - 81
eISSN - 1521-4125
pISSN - 0930-7516
DOI - 10.1002/ceat.200600233
Subject(s) - breakup , sauter mean diameter , nozzle , mechanics , weber number , isothermal process , air entrainment , chemistry , entrainment (biomusicology) , break up , viscosity , materials science , thermodynamics , turbulence , physics , reynolds number , composite material , rhythm , acoustics
Measurements using two‐dimensional Phase Doppler Anemometry as well as high speed cinematography in free jets at several nozzle exit pressures and mass flow rates, show that the Sauter mean droplet diameter decreases with increasing air and liquid‐phase mass flow ratio due to the increase of the air stream impact on the liquid phase. This leads to substantial liquid fragmentation, respectively primary droplet breakup, and hence, satellite droplet formation with small sizes. This trend is also significant in the case of a liquid viscosity higher than that of water. The increased liquid viscosity stabilizes the droplet formation and breakup by reducing the rate of surface perturbations and consequently droplet distortions, ultimately also leading, in total, to the formation of smaller droplets. The droplet velocity decreases with the nozzle downstream distance, basically due to the continual air entrainment and due to the collisions between the droplets. The droplet collisions may induce further liquid fragmentation and, hence, formation of a number of relatively smaller droplets respectively secondary breakup, or may induce agglomeration to comparatively larger liquid fragments that may rain out of the free jet.