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Forced breakup of an elliptic jet (major axis view) under various stimulation frequencies

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Elliptic Liquid Jets

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In this work, the motion of liquid jets ejected from elliptical orifices was studied theoretically and experimentally. In the theoretical part of the study, the linear evolution of initially small disturbances on the jets was investigated using a three-dimensional instability analysis (for inviscid case) and a quasi-one-dimensional analysis (for viscous case). Temporal and spatial analyses are performed and the dispersion equations of waves on the jet column were derived to show the growth rate of disturbances for different modes under various conditions. An equation for the jet profile was suggested which described the axis-switching phenomenon and breakup for various conditions. The equations were approximated for small and large ellipticities, and well- known dispersion relations of circular and planar jets were retrieved.

Experiments were performed to validate the linear results and to investigate the jet velocity profile. Several nozzles with different ellipticities and length to diameter ratios were designed and their behaviors were examined under free (natural) and excited (forced) perturbations. The spatial evolution of the jet shape was captured using a high-speed camera. In the forced breakup case, the stimulations were performed by modulating the jet velocity with a piezoelectric actuator through given sinusoidal perturbations. The measured data are in good agreement with theoretical predictions except at high ellipticities where nonlinear effects are strong.

It was shown that in the capillary dominant regimes, the effect of ellipticity is increasing the growth rate and range of unstable wavenumbers. In this case only modes symmetric to both major and minor axes are unstable. At higher Weber numbers, as the aerodynamic forces become dominant, by increasing the ellipticity, growth rate is decreased. In these Weber numbers, as the ellipticity increases, the growth rates of the modes that are symmetric with respect to the major axis are larger than those of antisymmetric with respect to the major axis. Increasing the gas to liquid density ratio increases the disturbances growth rate, while increasing the liquid viscosity dampens the growth rate and shifts the maximum growth rate toward longer waves.

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Axis-switching of an elliptic jet: (a) major axis-view and (b) minor axis view

source: TSMF
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◄   FIGURE 2

The schematic of experimental setup

source: TSMF
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◄   FIGURE 3

Depiction of the most unstable waves for elliptic jets: (C, F) modes including, a) Ce0, b) Ce1, c) Ce2, and (S, G) modes including d) Se1, and e) Se2.

source: TSMF
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