Abstract

Gravity induced film flow over a rigid smoothly corrugated substrate heated uniformly from below, is explored. This is achieved by reducing the governing equations of motion and energy conservation to a manageable form within the mathematical framework of the well-known long-wave approximation; leading to an asymptotic model of reduced dimensionality. A key feature of the approach and to solving the problem of interest, is proof that the leading approximation of the temperature field inside the film must be nonlinear to accurately resolve the thermodynamics beyond the trivial case of ‘a flat film flowing down a planar uniformly heated incline.’ Superior predictions are obtained compared with earlier work and reinforced via a series of corresponding solutions to the full governing equations using a purpose written finite element analogue, enabling comparisons to be made between free-surface disturbance and temperature predictions, as well as the streamline pattern and temperature contours inside the film. In particular, the free-surface temperature is captured extremely well at moderate Prandtl numbers. The stability characteristics of the problem are examined using Floquet theory, with the interaction between the substrate topography and thermo-capillary instability modes investigated as a set of neutral stability curves. Although there are no relevant experimental data currently available for the heated film problem, recent existing predictions and experimental data concerning the behaviour of corresponding isothermal flow cases are taken as a reference point from which to explore the effect of both heating and cooling.

Highlights

  • Thin film flows are ubiquitous in the formation of functional surfaces/barriers, while playing a key role as part of numerous manufacturing/conversion process

  • An essential requirement of the proposed reduced asymptotic model (RAM)–θpara is that it returns the critical Reynolds number for the case of a ‘flat film flowing down a planar, uniformly heated incline.’

  • The RAM as presented, stems from the modelling approach of Ruyer-Quil & Manneville (2000). It embodies a parabolic temperature profile though the film obtained using a method of polynomial expansions, proving the temperature field must be nonlinear to ensure both a consistent transformation of the governing equation and for the heat flux boundary condition at the free surface to be satisfied universally

Read more

Summary

Introduction

Thin film flows are ubiquitous in the formation of functional surfaces/barriers, while playing a key role as part of numerous manufacturing/conversion process. Ruyer-Quil & Manneville (1998) addressed this problem by expanding Shkadov’s self-similar velocity profile to first order in the long-wave expansion, leading to a modified IBL model and recovery of the correct Recrit. Given the temperature distribution within ‘a flat film flowing down a planar, uniformly heated incline’ is linear, it has become commonplace to initiate a long-wave expansion with an assumed linear temperature dependence through the film, even though it is impossible for the latter to satisfy all of the required boundary conditions Proceeding in this way, the long-wave thermo-capillary mode was explored by Kalliadasis, Kiyashko & Demekhin (2003b) and Kalliadasis et al (2003a) using a mixed Shkadov-weighted-residual model; it fails to retrieve Recrit for uniformly heated substrate.

Problem formulation
Reduced asymptotic model
Linear stability analysis
Steady-state comparisons
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call