Surface tension effects in a wedge

The linearized Laplace-Young capillary equation has been solved for the depth of liquid contained in a region bounded by vertical walls at an arbitrary wedge angle 2α using the Kantorovich-Lebedev transform. These solutions accurately describe the surface displacement for surface contact angles γ cl...

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Bibliographic Details
Published inQuarterly journal of mechanics and applied mathematics Vol. 51; no. 4; pp. 553 - 561
Main Authors Fowkes, ND, Hood, MJ
Format Journal Article
LanguageEnglish
Published Oxford Oxford University Press 01.11.1998
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Summary:The linearized Laplace-Young capillary equation has been solved for the depth of liquid contained in a region bounded by vertical walls at an arbitrary wedge angle 2α using the Kantorovich-Lebedev transform. These solutions accurately describe the surface displacement for surface contact angles γ close enough to π/2, for both convex and concave (re-entrant) wedge angles. By matching solutions of the linearized Laplace-Young equation solutions on the exactly known one-dimensional nonlinear Laplace-Young wall solutions, far-field approximations are obtained for arbitrary contact angle γ situations for possibly a restricted range of wedge angles.
Bibliography:ark:/67375/HXZ-TRGDSRL6-F
istex:BA4E812216133CA197F67EFF438F6669C4068345
local:4
ISSN:0033-5614
1464-3855
DOI:10.1093/qjmam/51.4.553