Abstract
The electrohydrodynamic instability of a thin film of initially static viscoelastic polymer under a mask is studied via a linear analysis. The conducting polymer film is separated from the mask by air. Under a normal electrical field, the initially flat polymer film self-assembles into well organized micro scale patterns. The driving force for the instability is an electrostatic force exerted on the free charges accumulated at the air-polymer interface. The electrical field is either applied externally or generated internally by the contact potentials at the interfaces of different materials. The system is unconditionally unstable. The elasticity of the polymer is found to destabilize the system. When the Deborah number is large enough, a resonant phenomenon appears as a result of the interaction between the two destabilizing mechanisms (the electrostatic force and the polymer elasticity). The resonance introduces two most unstable wave numbers, at which the growth rate of the disturbance is unbounded. The two most unstable wave numbers bifurcate at a minimum Deborah number, below which no resonance is found. The effects of the initial film thickness, the air gap thickness and the electrical properties of the conducting polymer on the instability are also investigated.
Original language | English (US) |
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Pages (from-to) | 91-99 |
Number of pages | 9 |
Journal | Journal of Non-Newtonian Fluid Mechanics |
Volume | 125 |
Issue number | 2-3 |
DOIs | |
State | Published - Jan 31 2005 |
All Science Journal Classification (ASJC) codes
- General Chemical Engineering
- General Materials Science
- Condensed Matter Physics
- Mechanical Engineering
- Applied Mathematics
Keywords
- Bifurcation
- Electrohydrodynamic instability
- Leaky dielectric model
- Non-Newtonian
- Resonance
- Thin film
- Viscoelastic instability