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Phys. Fluids 24, 022104 (2012); http://dx.doi.org/10.1063/1.3680867 (39 pages)
The physics of aerobreakup. II. Viscous liquids
(Received 6 June 2011; accepted 14 December 2011; published online 14 February 2012; publisher error corrected 16 February 2012)
© 2012 American Institute of Physics
Article Outline
- INTRODUCTION
- EXPERIMENTAL METHODS
- NUMERICAL SIMULATION METHODS
- LONG-WAVE PHENOMENA
- SHORT-WAVE PHENOMENA
- Scaling laws of the second criticality
- Interfacial instabilities
- The key early morphologies
- The viscous K-H instability
- The sonic effects
- BREAKUP TIMES
- Timings of breakup processes in RTP
- Timings of breakup processes in SIE
- PARTICLE-CLOUD DYNAMICS
- CONCLUSIONS
RELATED DATABASES
KEYWORDS and PACS
ARTICLE DATA
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T. G. Theofanous and G. J. Li, “On the physics of aerobreakup,” Phys. Fluids 20, 052103 (2008)PHFLE6000020000005052103000001.
V. V. Mitkin,, A. N. Rozhkov, and T. G. Theofanous, “Pulse jets, rims and elastic-liquid sheets: Rheology at high strain rates and rupture criteria,” AIP Conf. Proc. 1027, 1126 (2008)APCPCS001027000001001126000001.
C.-L. Ng and T. G. Theofanous, “Modes of aero-breakup with visco-elastic liquids. Pulse jets, rims and elastic-liquid sheets: Rheology at high strain rates,” AIP Conf. Proc. 1027, 183 (2008)APCPCS001027000001000183000001.
K. O. Mikaelian, “Rayleigh–Taylor instability in finite-thickness fluids with viscosity and surface tension,” Phys. Rev. E 54, 3676–80 (1996).
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