4.7 Article

Oscillations of a ring-constrained charged drop

期刊

JOURNAL OF FLUID MECHANICS
卷 921, 期 -, 页码 -

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2021.512

关键词

drops; capillary flows; electrohydrodynamic effects

资金

  1. Purdue Process Safety and Assurance Center (P2SAC)
  2. Gedge Professorship
  3. Bilsland Dissertation Fellowship

向作者/读者索取更多资源

This study discusses the oscillation characteristics of free drops and charged drops constrained by solid rings under small-amplitude perturbations. It also investigates the effects of charge on oscillation modes. The research reveals that at the Rayleigh limit, oscillation frequencies of slightly charged constrained drops exhibit variation.
Free drops of uncharged and charged inviscid, conducting fluids subjected to small-amplitude perturbations undergo linear oscillations (Rayleigh, Proc. R. Soc. London, vol. 29, no. 196-199, 1879, pp. 71-97; Rayleigh, Philos. Mag., vol. 14, no. 87, 1882, pp. 184-186). There exist a countably infinite number of oscillation modes, n = 2, 3, ..., each of which has a characteristic frequency and mode shape. Presence of charge (Q) lowers modal frequencies and leads to instability when Q > Q(R) (Rayleigh limit). The n = 0 and n = 1 modes are disallowed because they violate volume conservation and cause centre of mass (COM) motion. Thus, the first mode to become unstable is the n = 2 prolate-oblate mode. For free drops, there is a one-to-one correspondence between mode number and shape (Legendre polynomial P-n). Recent research has shifted to studying oscillations of spherical drops constrained by solid rings. Pinning the drop introduces a new low-frequency mode of oscillation (n = 1), one associated primarily with COM translation of the constrained drop. We analyse theoretically the effect of charge on oscillations of constrained drops. Using normal modes and solving a linear operator eigenvalue problem, we determine the frequency of each oscillation mode. Results demonstrate that for ring-constrained charged drops (RCCDs), the association between mode number and shape is lost. For certain pinning locations, oscillations exhibit eigenvalue veering as Q increases. While slightly charged RCCDs pinned at zeros of P-2 have a first mode that involves COM motion and a second mode that entails prolate-oblate oscillations, the modes flip as Q increases. Thereafter, prolate-oblate oscillations of RCCDs adopt the role of being the first mode because they exhibit the lowest vibration frequency. At the Rayleigh limit, the first eigenmode - prolate-oblate oscillations - loses stability while the second - involving COM motion - remains stable.

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