TY - JOUR
T1 - On a slender dry patch in a liquid film draining under gravity down an inclined plane
AU - Wilson, S. K.
AU - Duffy, B. R.
AU - Davis, S. H.
PY - 2001
Y1 - 2001
N2 - In this paper two similarity solutions describing a steady, slender, symmetric dry patch in an infinitely wide liquid film draining under gravity down an inclined plane are obtained, The first solution, which predicts that the dry patch has a parabolic shape and that the transverse profile of the free surface always has a monotonieally increasing shape, is appropriate for weak surface-tension effects and far from the apex of the dry patch, The second solution, which predicts that the dry patch has a quartie shape and that the transverse profile of the free surface has a capillary ridge near the contact line and decays in an oseiliatory manner far from it, is appropriate for strong surface-tension effects (in particular, when the plane is nearly vertical) and near (but not too close) to the apex of the dry patch, With the average volume flux per unit width (or equivalently with the uniform height of the layer far from the dry patch) prescribed, both solutions contain a free parameter, For each value of this parameter there is a unique solution in the first case and either no solution or a one-parameter family of solutions in the second case, The solutions capture some of the qualitative features observed in experiments.
AB - In this paper two similarity solutions describing a steady, slender, symmetric dry patch in an infinitely wide liquid film draining under gravity down an inclined plane are obtained, The first solution, which predicts that the dry patch has a parabolic shape and that the transverse profile of the free surface always has a monotonieally increasing shape, is appropriate for weak surface-tension effects and far from the apex of the dry patch, The second solution, which predicts that the dry patch has a quartie shape and that the transverse profile of the free surface has a capillary ridge near the contact line and decays in an oseiliatory manner far from it, is appropriate for strong surface-tension effects (in particular, when the plane is nearly vertical) and near (but not too close) to the apex of the dry patch, With the average volume flux per unit width (or equivalently with the uniform height of the layer far from the dry patch) prescribed, both solutions contain a free parameter, For each value of this parameter there is a unique solution in the first case and either no solution or a one-parameter family of solutions in the second case, The solutions capture some of the qualitative features observed in experiments.
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U2 - 10.1017/S095679250100417X
DO - 10.1017/S095679250100417X
M3 - Article
AN - SCOPUS:0035626937
SN - 0956-7925
VL - 12
SP - 233
EP - 252
JO - European Journal of Applied Mathematics
JF - European Journal of Applied Mathematics
IS - 3
ER -