Hostname: page-component-76fb5796d-25wd4 Total loading time: 0 Render date: 2024-04-26T19:01:28.988Z Has data issue: false hasContentIssue false

Large Eddy Simulation of Two-Phase Flow Pattern and Transformation Characteristics of Flow Mixing Nozzle

Published online by Cambridge University Press:  29 July 2019

Jin Zhao
Affiliation:
School of Mechanical, Electronic and Control Engineering, Beijing Jiaotong University, Beijing 100044, China
Zhi Ning*
Affiliation:
School of Mechanical, Electronic and Control Engineering, Beijing Jiaotong University, Beijing 100044, China
Ming Lü
Affiliation:
School of Mechanical, Electronic and Control Engineering, Beijing Jiaotong University, Beijing 100044, China National Engineering Laboratory for Mobile Source Emission Control Technology, China Automotive Technology & Research Center, Tianjin 300300, China
*
*Corresponding author (zhining@bjtu.edu.cn)
Get access

Abstract

The two-phase flow pattern of a flow mixing nozzle plays an important role in jet breakup and atomization. However, the flow pattern of this nozzle and its transformation characteristics are still unclear. A diesel-air injection simulation model of a flow mixing nozzle is established. Then the two-phase flow pattern and transformation characteristics of the flow mixing nozzle is studied using a numerical simulation method. The effect of the air-diesel velocity ratio, ratio of the distance between the tube orifice and nozzle hole and the tube diameter (H/D), and the diesel inlet velocity was studied in terms of the jet breakup diameter (jet diameter at the breakup position) and jet breakup length (length of the diesel jet from the breakup position to the nozzle outlet). The results show that the jet breakup diameter decreases with the decrease in H/D or the increase in the air-diesel velocity ratio and diesel inlet velocity. The jet breakup length increases first and then decreases with the increase in H/D and air-diesel velocity ratio; the trend of the diesel inlet velocity is complicated. In addition, a change in the working conditions also causes some morphological changes that cannot be quantitatively analyzed in the diesel-air flow pattern. The transition characteristics of the flow pattern are analyzed, and it is found that the main reason for the change in the flow pattern is the change in the inertial force of the air, surface tension force, and viscous force of diesel (non-dimensional Reynolds number and Weber number describe the transition characteristics in this paper). The surface tension force of diesel decreases and the viscous force of diesel and inertial force of air increase when the air-diesel velocity ratio increases or H/D decreases. However, the effects of the diesel surface tension force and viscous force effect are much smaller than that of the air inertial force, which changes the diesel-air flow pattern from a drop pattern to a vibration jet pattern, broken jet pattern, and then a chaotic jet pattern.

Type
Research Article
Copyright
© The Society of Theoretical and Applied Mechanics 2019 

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Ganan-Calvo, A. M., “Generation of Steady Liquid Microthreads and Micron-Sized Monodisperse Sprays in Gas Streams,” Physical Review Letters, 80(2), pp. 285-288(1998).CrossRefGoogle Scholar
Ganan-Calvo, A. M., “Enhanced liquid atomization: From flow-focusing to flow-blurring.” Applied Physics Letters, 86(21), pp.4601(2005).CrossRefGoogle Scholar
Ganan-Calvo, A. M., et al., “Focusing Capillary Jets Close to the Continuum Limit,” Nature Physics, 3(10), pp.737-742(2007).CrossRefGoogle Scholar
Vega, E. J., et al., “Global and local instability of flow focusing: The influence of the geometry,” Physics of Fluids, 22(64105), pp.16(2010).CrossRefGoogle Scholar
Montanero, J. M., et al., “Global stability of the focusing effect of fluid jet flows.” Physical Review E Statistical Nonlinear & Soft Matter Physics, 83(3 Pt 2), pp.036309(2011).CrossRefGoogle ScholarPubMed
Montanero, J. M., Ganan-Calvo, A. M., “Stability of coflowing capillary jets under nonaxisymmetric perturbations.” Physical Review E Statistical Nonlinear & Soft Matter Physics, 77(4 Pt 2), pp.046301(2008).CrossRefGoogle ScholarPubMed
Herrada, M. A., et al., “Liquid flow focused by a gas: jetting, dripping, and recirculation.” Phys Rev E Stat Nonlin Soft Matter Phys, 78(2), pp.036323(2008).CrossRefGoogle ScholarPubMed
Acero, A. J., et al., “A new flow focusing technique to produce very thin jets.” Journal of Micromechanics & Microengineering, 23(6), pp.1063-1076(2013).CrossRefGoogle Scholar
Acero, A. J., et al., “Enhancement of the stability of the flow focusing technique for low-viscosity liquids.” Journal of Micromechanics & Microengineering, 22(115039), pp.1-6(2012).CrossRefGoogle Scholar
Vega, E. J., et al., “A novel technique for producing metallic microjets and microdrops.” Microfluidics & Nanofluidics, 14(1-2), pp.101-111(2013).CrossRefGoogle Scholar
Montanero, J. M., et al., “Micrometer glass nozzles for flow focusing.” Journal of Micromechanics & Microengineering, 20(7), pp.075035(2010).CrossRefGoogle Scholar
Ting, S., “Experimental and theoretical investigation on flow focusing.” Doctoral dissertation (2009).Google Scholar
Yang, L., et al., “Formation mechanism of the micro droplet based on the flow focusing structure.” Micronanoelectronic Technology, 52(9), pp.576-580(2015).Google Scholar
Liu, Z.M., Yang, Y., “Influence of geometry configurations on the microdroplets in flow focusing microfluidics.” Chinese Journal of Theoretical and Applied Mechanics, 48(4), pp.867-876(2016).Google Scholar
Azevedo, C. G. De., Costa, F. D. S., and Andrade, J. C. D., “Effects of nozzle exit geometry on spray characteristics of a blurry injector.” Atomization & Sprays, 23(3), pp.193-209(2013).CrossRefGoogle Scholar
Azevedo, C. G. De., Andrade, J. C. D., and Costa, F. D. S., “Effects of injector tip design on the spray characteristics of soy methyl ester biodiesel in a blurry injector.” Renewable Energy, 85, pp.287-294(2016).CrossRefGoogle Scholar
Simmons, B. M., Agrawal, A. K., “Flow Blurring Atomization for Low-Emission Combustion of Liquid Biofuels.” Combustion Science & Technology, 184(5), pp.660-675(2012).CrossRefGoogle Scholar
Jiang, L. L., Agrawal, A. K., “Investigation of Glycerol Atomization in the Near-Field of a Flow-Blurring Injector using Time-Resolved PIV and High-Speed Visualization.” IEEE International Conference on Neural Networks, pp.323-338(2014).CrossRefGoogle Scholar
Azevedo, C. G. De., Andrade, J. C. D., and Costa, F. D. S., “Flameless compact combustion system for burning hydrous ethanol.” Energy, 89, pp.158-167(2015).CrossRefGoogle Scholar
Jiang, L.L., “Investigation of atomization mechanisms and flame structure of a twin-fluid injector for different liquid fuels.” Dissertations & Theses - Gradworks (2014).Google Scholar
Azevedo, C. G. De., Andrade, J. C. D., and Costa, F. D. S., “Characterization of a blurry injector for burning biofuels in a compact flameless combustion chamber.” 14th Brazilian Congress of Thermal Sciences and Engineering, Rio de Janeiro, Brazil (2012).Google Scholar
Rosellllompart, J., Ganan-Calvo, A. M., “Turbulence in pneumatic flow focusing and flow blurring regimes.” Physical Review E Statistical Nonlinear & Soft Matter Physics, 77(3 Pt 2), pp.036321(2008).CrossRefGoogle Scholar