The flow is considered of a Newtonian fluid, of viscosity η and surface tension T , in the narrow gap between a pair of rollers of radii R 1 and R 2 , whose peripheral speeds are constant and equal to U 1 and U 2 respectively. The objective is to determine the coating thickness h 1 ∞ on the upper roller as a function of the non-dimensional parameters H 0 / R , η U / T and U 1 / U 2 , where H 0 is the minimum gap thickness, U = ½( U 1 + U 2 ), and 2 R −1 = R 1 −1 + R 2 −1 . Using lubrication theory to provide an adequate description of the fluid flow, two mathematical models are derived whose essential difference lies in the specification of the boundary conditions. In the separation model it is assumed that the pressure distribution will terminate at a position which is both a stagnation point and a point of separation, whereas the Reynolds model incorporates the classical Reynolds conditions. In each case, theoretical predictions for the non-dimensional coating thickness, h 1 ∞ / H 0 as a function of U 1 / U 2 are found to compare well with experiment. However, theory does suggest that the two models are applicable to different and complementary regions of parameter space, and hence together they may form a basis for further investigations into the various features of coating processes.
[1]
M R Hopkins,et al.
Viscous flow between rotating cylinders and a sheet moving between them
,
1957
.
[2]
Stanley Middleman,et al.
A theory of roll coating of viscous and viscoelastic fluids
,
1975
.
[3]
J. Pearson,et al.
The instability of uniform viscous flow under rollers and spreaders
,
1960,
Journal of Fluid Mechanics.
[4]
M. Savage.
Cavitation in lubrication. Part 1. On boundary conditions and cavity—fluid interfaces
,
1977,
Journal of Fluid Mechanics.
[5]
E. Pitts,et al.
The flow of thin liquid films between rollers
,
1961,
Journal of Fluid Mechanics.