Non-Newtonian flow in a thin film with boundary conditions of Coulomb's type

Author(s):  
F. Saidi
Physica ◽  
1963 ◽  
Vol 29 (11) ◽  
pp. 1219-1230 ◽  
Author(s):  
C.W. Searle ◽  
A.H. Morrish ◽  
R.J. Prosen

Author(s):  
Carlos J. Gomes ◽  
Marcela Madrid ◽  
Cristina H. Amon

The in-plane thermal conductivity of thin silicon films is predicted using equilibrium molecular dynamics, the Stillinger-Weber potential and the Green-Kubo relationship. Film thicknesses range from 2 to 200 nm. Periodic boundary conditions are used in the directions parallel to the thin film surfaces. Two different strategies are evaluated to treat the atoms on the surfaces perpendicular to the thin film direction: adding four layers of atoms kept frozen at their crystallographic positions, or restraining the atoms near the surfaces with a repulsive potential. We show that when the thin-film thickness is smaller than the phonon mean free path, the predictions of the in-plane thermal conductivity at 1000K differ significantly depending on the potential applied to the atoms near the surfaces. In this limit, the experimentally observed trend of decreasing thermal conductivity with decreasing film thickness is predicted when the surface atoms are subject to a repulsive potential in addition to the Stillinger-Weber potential, but not when they are limited by frozen atoms.


1984 ◽  
Vol 29 (2) ◽  
pp. 976-982 ◽  
Author(s):  
V. M. Agranovich ◽  
V. E. Kravtsov ◽  
T. A. Leskova ◽  
A. G. Mal'shukov ◽  
G. Hernández-Cocoletz ◽  
...  

1987 ◽  
Vol 183 ◽  
pp. 219-234 ◽  
Author(s):  
D. A. Reinelt

In displacing a viscous fluid from the gap between two closely spaced parallel plates, a thin film of the original fluid remains on the surface of each plate. Boundary conditions which connect the approximate equations in the region in front of the interface with the approximate solutions in the thin-film region are determined from local solutions of the equations in the vicinity of the interface edge. These interface conditions depend on both b/R (gap half-width/radius of curvature) and μUn/T, where μ is the viscosity of the original fluid, Un is the normal velocity of the interface edge, and T is the interfacial tension. These conditions are determined using perturbation method when μUn/T [Lt ] 1 and numerical methods when μUn/T is O(1). Though previous theories have shown qualitative agreement with experiments, it is hoped that these new boundary conditions improve the quantitative agreement.


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