Abstract

A new model for the behaviour of a thick, two-dimensional layer of fluid on the surface of a rotating cylinder is presented, incorporating the effects of inertia, rotation, viscosity, gravity and capillarity. Comparisons against direct numerical simulations (DNS) show good accuracy for fluid layers of thickness of the same order as the cylinder radius, even for Reynolds numbers up to . A rich and complex parameter space is revealed, and is elucidated via a variety of analytical and numerical techniques. At moderate rotation rates and fluid masses, the system exhibits either periodic behaviour or converges to a steady state, with the latter generally being favoured by greater masses and lower rotation rates. These behaviours, and the bifurcation structure of the transitions between them, are examined using a combination of both the low-order model and DNS. Specific attention is dedicated to newly accessible regions of parameter space, including the multiple steady state solutions observed for the same parameter values by Lopes et al. (J. Fluid Mech., vol. 835, 2018, pp. 540–574), where the corresponding triple limit point bifurcation structure is recovered by the new low-order model. We also inspect states in which the interface becomes multivalued – and thus outside the reach of the reduced-order model – via DNS. This leads to highly nonlinear multivalued periodic structures appearing at moderate thicknesses and relatively large rotation rates. Even much thicker films may eventually reach steady states (following complex early evolution), provided these are maintained by a combination of forces sufficiently large to counteract gravity.

Highlights

  • The flow of an annular film on the outside of a rotating circular cylinder is a fascinating and much-studied problem

  • Respectively a Reynolds number representing the relative significance of inertia compared to viscous effects, a Weber number encoding the balance of inertial effects to surface tension, the undisturbed radius of the interface, and the angular velocity of the disk

  • It is found that only the full long-wave model provides consistently good agreement with the exact solutions across the considered parameter ranges

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Summary

Introduction

The flow of an annular film on the outside of a rotating circular cylinder is a fascinating and much-studied problem. Experiments (Moffatt 1977; Preziosi & Joseph 1988; Melo & Douady 1993; Kelmanson 1995; de Bruyn 1997), thin-film models (Kelmanson 1995; Evans et al 2005) and linear stability analyses (Noakes, King & Riley 2005; Benilov & Lapin 2013) have shown that the fluid layer coating the rotating cylinder can be unstable to axial perturbations for sufficiently high rotation rates In his experiments involving syrup, Moffatt (1977) observed that this resulted in the formation of asymmetric ‘syrup rings’ spaced regularly in the axial direction.

Governing equations
Modelling
Long-wave boundary-layer equation
Weighted residual model
Thick-film gradient expansion model
Recovery of existing models
Results
Linear stability with no gravity
Nonlinear validation
Periodic behaviour
Modelling discussion
Conclusions
Transient numerical simulation of low-order models
Pseudo arc-length continuation codes
Direct numerical simulations
Full Text
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