Abstract
The onset of instability in a liquid annular jet enclosing another fluid, and surrounded
by a gas in a pipe is analysed by use of a spectra-collocation method. The dynamic
responses to the variation of different flow parameters are elucidated by use of
numerical results. Two linearly independent convectively unstable interfacial modes
of disturbances are found. In general, the para-sinuous mode has a larger amplification
rate than the para-varicose mode. It is shown that to initiate encapsulation of core
fluid with a uniform shell fluid, the growth of the para-sinuous mode must be
promoted and the para-varicose mode must be suppressed. Suppression of the
paravaricose mode in a finite range of wavenumbers is possible by varying the flow
parameters. The effects of ten relevant parameters on instability are discussed. In
certain parameter space, the annular jet becomes absolutely unstable with respect to
the sinuous mode. The transition Weber number below which the flow is absolutely
unstable and above which the flow is convectively unstable is found as a function
of the Reynolds number when the rest of flow parameters are given. A successful
encapsulation of core fluid with a uniform shell fluid is possible if the process is
carried out outside of the parameter space of absolute instability, and if an external
forcing is introduced at a frequency within a band in which the para-varicose mode
is stable but the para-sinuous mode is convectively unstable.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
25 articles.
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