Abstract
The coalescence of a cylinder with half-space by creeping viscous flow driven solely by surface tension is analysed using methods developed previously. The evolution of the shape with time is described, exactly, in terms of a time-dependent mapping function z = ,t) of the upper half-plane, conformal on Im 1 as t [rightward arrow] [infty infinity], which is consistent with Kuiken's analysis of an isolated disturbance. (Previously, the author reported an erroneous solution which behaved otherwise.) The results are compared with the coalescence of equal cylinders obtained previously. For a modest degree of coalescence, the shapes are rather alike. In the limit as t [rightward arrow] 0. the time dependence of the minimum widths (necks) are the same. At the times when the minimum widths disappear, the heights of the two shapes are equal.
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