1983
DOI: 10.1007/bf02570527
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Profile and departure size of condensation drops on vertical surfaces

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1984
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Cited by 22 publications
(20 citation statements)
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“…In the prior work [1] it was demonstrated that in satisfying the transversality condition associated with the variable lower end point, Young's equation was automatically satisfied by the solution provided that the surface energies contained therein are taken to be for the advancing condition. The transversality condition can no longer be applied at the advancing end of the drop since the first derivative off2(x) at this location is not continuous.…”
Section: K1(0)r Q D~mentioning
confidence: 97%
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“…In the prior work [1] it was demonstrated that in satisfying the transversality condition associated with the variable lower end point, Young's equation was automatically satisfied by the solution provided that the surface energies contained therein are taken to be for the advancing condition. The transversality condition can no longer be applied at the advancing end of the drop since the first derivative off2(x) at this location is not continuous.…”
Section: K1(0)r Q D~mentioning
confidence: 97%
“…This is an extension of the work presented in [1], in Which the general profile of a two-dimensional drop on a vertical surface was computed, with the departure profile and size being obtained as a special limit. The two-dimensional profiles were taken to be approximations to the mid-plane profiles of drops, and good comparisons between computed departure sizes and measurements made at earth and high gravity fields simulated by centrifugal acceleration.…”
Section: Introductionmentioning
confidence: 99%
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“…Energy-minimization techniques have been widely used to model the static droplet shape on an incline [12,[21][22][23][24][25]. Two-dimensional droplets were initially modeled using energy-based methods by Frenkel [12] and later by Merte and co-workers [21,22].…”
mentioning
confidence: 99%
“…Two-dimensional droplets were initially modeled using energy-based methods by Frenkel [12] and later by Merte and co-workers [21,22]. Frenkel provided upper bounds on the critical inclination for droplet sliding, whereas Merte and co-workers obtained 2D droplet shapes and receding contact angles with the advancing angle and critical droplet size provided as inputs.…”
mentioning
confidence: 99%