Abstract
A rivulet is a narrow steam of liquid located on a solid surface and sharing a curved interface with the surrounding gas. Capillary instabilities are investigated by a linearized stability theory. The formulation is for small, static rivulets whose contact (common or three-phase) lines are fixed, move but have fixed contact angles or move but have contact angles smooth functions of contact-line speeds. The linearized stability equations are converted to a disturbance kinetic-energy balance showing that the disturbance response exactly satisfies a damper linear harmonic-oscillator equation. The 'damping coefficient' contains the bulk viscous dissipation, the effect of slip along the solid and all dynamic effects that arise in the third contact-line condition. For small disturbances changes in contact angle with contact-line speed constitute a purely dissipative process. Results are independent of slip model at the liquid-solid interface as long as a certain integral inequality holds. Sufficient conditions for stability are obtained in all cases. Refs.
Original language | English (US) |
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Pages (from-to) | 225-242 |
Number of pages | 18 |
Journal | Journal of fluid Mechanics |
Volume | 98 |
Issue number | pt 2 |
State | Published - 1980 |
ASJC Scopus subject areas
- Condensed Matter Physics
- Mechanics of Materials
- Mechanical Engineering