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Simulation of liquid micro-jet in free expanding high-speed co-flowing gas streams

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Abstract

We present the development of an experimentally validated computational fluid dynamics model for liquid micro jets. Such jets are produced by focusing hydrodynamic momentum from a co-flowing sheath of gas on a liquid stream in a nozzle. The numerical model based on laminar two-phase, Newtonian, compressible Navier–Stokes equations is solved with finite volume method, where the phase interface is treated by the volume of fluid approach. A mixture model of the two-phase system is solved in axisymmetry using ~ 300,000 finite volumes, while ensuring mesh independence with the finite volumes of the size 0.25 µm in the vicinity of the jet and drops. The numerical model is evaluated by comparing jet diameters and jet lengths obtained experimentally and from scaling analysis. They are not affected by the strong temperature and viscosity changes in the focusing gas while expanding at nozzle outlet. A range of gas and liquid-operating parameters is investigated numerically to understand their influence on the jet performance. The study is performed for gas and liquid Reynolds numbers in the range 17–1222 and 110–215, and Weber numbers in the range 3–320, respectively. A reasonably good agreement between experimental and scaling results is found for the range of operating parameters never tackled before. This study provides a basis for further computational designs as well as adjustments of the operating conditions for specific liquids and gases.

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Acknowledgements

The authors would like to thank Henry Chapman (CFEL-DESY, Univ. of Hamburg, Center for Ultrafast Imaging) and Kenneth Beyerlein (CFEL-DESY) for fruitful discussions, Fabian Wilde and Jörg U. Hammel (Helmholtz-Zentrum Geesthacht, Germany) for X-ray projection image and Luigi Adriano (DESY) for technical support.

Funding

Funding for this research is provided by Centre of Free Electron Laser (CFEL) under project: Innovative methods for imaging with the use of X-ray free electron laser (XFEL) and synchrotron sources: simulation of gas-focused microjets, by the Helmholtz Association through program-oriented funds, and Slovenian Grant Agency (ARRS) within Program Group P2-0162 and Project J2-7384. The computations were performed on resources at DESY, Hamburg, Faculty of Mechanical Engineering, University of Ljubljana, and Institute of Metals and Technology, Ljubljana.

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Correspondence to Božidar Šarler.

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Appendix

Appendix

The Mach number Ma2 at axial position \({z_4}\) along the nozzle axis is calculated from

$$\frac{{{\text{M}}{{\text{a}}_1}}}{{{\text{M}}{{\text{a}}_2}}}{\left( {\frac{{1+\frac{{\gamma - 1}}{2}{\text{Ma}}_{2}^{2}}}{{1+\frac{{\gamma - 1}}{2}{\text{Ma}}_{1}^{2}}}} \right)^{\frac{{\gamma +1}}{{2\left( {\gamma - 1} \right)}}}}=\frac{{{A_{g2}}}}{{{A_{g1}}}}$$
(28)

where \({A_{{\text{g1}}}}\) and \({A_{{\text{g}}2}}\) represent the cross-sectional area at the gas inlet axial position \({z_1}\) and at axial position \({z_4}\) along the nozzle axis. \(\gamma ={{{c_{\text{p}}}} \mathord{\left/ {\vphantom {{{c_{\text{p}}}} {{c_{\text{v}}}}}} \right. \kern-0pt} {{c_{\text{v}}}}}\) is the ratio of specific heats at constant pressure and constant volume. The pressure at any location \({p_{2,{\text{g}}}}\) can be calculated, with given inlet gas pressure \({p_{{\text{inlet}},{\text{g}}}}\) as

$$\frac{{{p_{{\text{inlet}},{\text{g}}}}}}{{{p_{2,{\text{g}}}}}}={\left( {\frac{{1+\frac{{\gamma - 1}}{2}{\text{Ma}}_{2}^{2}}}{{1+\frac{{\gamma - 1}}{2}{\text{Ma}}_{1}^{2}}}} \right)^{\frac{\gamma }{{\gamma - 1}}}}.$$
(29)

As from experimental data the pressure is known at a distance 1.5 m upstream, \({p_{{\text{inlet}},{\text{g}}}}\) is estimated by performing single-phase compressible simulations in such a way that pressure is adjusted at inlet until an experimentally reported gas flow rate is measured at the nozzle’s gas inlet.

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Zahoor, R., Belšak, G., Bajt, S. et al. Simulation of liquid micro-jet in free expanding high-speed co-flowing gas streams. Microfluid Nanofluid 22, 87 (2018). https://doi.org/10.1007/s10404-018-2110-0

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