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Nonlinear dual-mode instability of planar liquid sheets

Published online by Cambridge University Press:  06 August 2015

Chen Wang
Affiliation:
School of Astronautics, Beijing University of Aeronautics and Astronautics, Beijing 100191, PR China
Lijun Yang*
Affiliation:
School of Astronautics, Beijing University of Aeronautics and Astronautics, Beijing 100191, PR China
Hanyu Ye
Affiliation:
School of Astronautics, Beijing University of Aeronautics and Astronautics, Beijing 100191, PR China
*
Email address for correspondence: [email protected]

Abstract

The nonlinear temporal instability of gas-surrounded planar liquid sheets, whose linear instability contains both sinuous and varicose modes, is studied. Both the weakly nonlinear analysis using a second-order perturbation expansion and the numerical simulation using a boundary integral method have been applied. Their comparison shows that the weakly nonlinear analysis can precisely predict the shapes of sheets for most of the time of disturbance evolution and qualitatively explain the instability mechanism when sheets break up. Both the first harmonics of the linear sinuous mode and linear varicose mode are varicose; they contribute to the breakup of sheets, but the first harmonic generated by the coupling between the linear sinuous and varicose modes is sinuous; it plays an important role in modulating the wave profile. The instability with various initial phase differences between the upper and lower interfaces is examined. Except for the varicose initial disturbance, the linear sinuous mode dominates in the shapes of sheets when their amplitudes grow large. Within the second-order analysis, the major modes that can cause the breakup include the linear varicose mode, the first harmonic of the linear sinuous mode and the first harmonic of the linear varicose mode. The effects of various flow parameters have been investigated. At relatively large wavenumbers where approximate analytical and numerical results agree well when sheets break up, increasing the wavenumber reduces the wave amplitude. Reducing the initial disturbance amplitude makes the first harmonic of the linear sinuous mode the dominant mode in causing the breakup. Increasing the Weber number or gas-to-liquid density ratio significantly reduces breakup time and enhances instability.

Type
Papers
Copyright
© 2015 Cambridge University Press 

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References

Asare, H. R., Takahashi, R. K. & Hoffman, M. A. 1981 Liquid sheet jet experiments: comparison with linear theory. Trans. ASME J. Fluids Engng 103, 595603.Google Scholar
Baker, G. R. & Beale, J. T. 2004 Vortex blob methods applied to interfacial motion. J. Comput. Phys. 196, 233258.CrossRefGoogle Scholar
Beale, J. T., Hou, T. Y. & Lowengrub, J. S. 1996 Convergence of a boundary integral method for water waves. SIAM J. Numer. Anal. 33, 17971843.CrossRefGoogle Scholar
Clark, C. J. & Dombrowski, N. 1972 Aerodynamic instability and disintegration of inviscid liquid sheets. Proc. R. Soc. Lond. A 329, 467478.Google Scholar
Crapper, G. D., Dombrowski, N. & Pyott, G. A. D. 1975 Large amplitude Kelvin–Helmholtz waves on thin liquid sheets. Proc. R. Soc. Lond. A 342, 209224.Google Scholar
Hagerty, W. W. & Shea, J. F. 1955 A study of the stability of plane fluid sheets. Trans. ASME J. Appl. Mech. 22, 509514.Google Scholar
Hou, T. Y., Lowengrub, J. S. & Shelley, M. J. 1994 Removing the stiffness from interfacial flows with surface tension. J. Comput. Phys. 114, 312338.Google Scholar
Hou, T. Y., Lowengrub, J. S. & Shelley, M. J. 1997 The long-time motion of vortex sheets with surface tension. Phys. Fluids 9, 19331954.CrossRefGoogle Scholar
Jazayeri, S. A. & Li, X. 2000 Nonlinear instability of plane liquid sheets. J. Fluid Mech. 406, 281308.Google Scholar
Kan, K. & Yoshinaga, T. 2007 Instability of a planar liquid sheet with surrounding fluids between two parallel walls. Fluid Dyn. Res. 39, 389412.Google Scholar
Matsuuchi, K. 1974 Modulational instability of nonlinear capillary waves on thin liquid sheet. J. Phys. Soc. Japan 37, 16801687.Google Scholar
Matsuuchi, K. 1976 Instability of thin liquid sheet and its break-up. J. Phys. Soc. Japan 41, 14101416.CrossRefGoogle Scholar
Mehring, C. & Sirignano, W. A. 1999 Nonlinear capillary wave distortion and disintegration of thin planar liquid sheets. J. Fluid Mech. 388, 69113.Google Scholar
Mitra, S. K., Li, X. & Renksizbulut, M. 2001 On the breakup of viscous liquid sheets by dual-mode linear analysis. AIAA J. Propul. Power 17, 728735.Google Scholar
Pozrikidis, C. 1992 Boundary Integral and Singularity Methods for Linearized Viscous Flow. Cambridge University Press.Google Scholar
Rangel, R. H. & Sirignano, W. A. 1991 The linear and nonlinear shear instability of a fluid sheet. Phys. Fluids A 3, 23922400.Google Scholar
Squire, H. B. 1953 Investigation of the instability of a moving liquid film. Brit. J. Appl. Phys. 4, 167169.CrossRefGoogle Scholar
Tammisola, O., Sasaki, A., Lundell, F., Matsubara, M. & Söderberg, L. D. 2011 Stabilizing effect of surrounding gas flow on a plane liquid sheet. J. Fluid Mech. 672, 532.Google Scholar
Yang, L., Wang, C., Fu, Q., Du, M. & Tong, M. 2013 Weakly nonlinear instability of planar viscous sheets. J. Fluid Mech. 735, 249287.Google Scholar
Yuen, M.-C. 1968 Non-linear capillary instability of a liquid jet. J. Fluid Mech. 33, 151163.Google Scholar