Stability of viscous long liquid filaments
arXiv:1307.3139 · doi:10.1063/1.4811849
Abstract
We study the collapse of an axisymmetric liquid filament both analytically and by means of a numerical model. The liquid filament, also known as ligament, may either collapse stably into a single droplet or break up into multiple droplets. The dynamics of the filament are governed by the viscosity and the aspect ratio, and the initial perturbations of its surface. We find that the instability of long viscous filaments can be completely explained by the Rayleigh-Plateau instability, whereas a low viscous filament can also break up due to end pinching. We analytically derive the transition between stable collapse and breakup in the Ohnesorge number versus aspect ratio phase space. Our result is confirmed by numerical simulations based on the slender jet approximation and explains recent experimental findings by Castrejon-Pita et al., PRL 108, 074506 (2012).
7 pages
References in corpus (1)
Cited by in corpus (14)
- The retraction of jetted slender viscoelastic liquid filaments
- Hydrodynamic behavior of the Pseudo-Potential lattice Boltzmann method for interfacial flows
- Dynamical formation of multiple quantum droplets in a Bose-Bose mixture
- Drop size characteristics of sprays emanating from circular and non-circular orifices in the atomization regime
- Viscoelastic Worthington jets & droplets produced by bursting bubbles
- Some fluid mechanical aspects of artistic painting
- Shape of a recoiling liquid filament
- Role of surfactant-induced Marangoni stresses in retracting liquid sheets
- Synchrotron X-ray phase-contrast imaging of ultrasonic drop atomization
- Drop pattern resulting from the breakup of a bidimensional grid of liquid filaments
- Nanoscopic jets and filaments of superfluid He-4 at zero temperature: a DFT study
- One-dimensional reduction of viscous jets. II. Applications
- Statistics of drops generated from ensembles of randomly corrugated ligaments
- Breakup of finite-size liquid filaments: Transition from no-breakup to breakup including substrate effects