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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Published in | Quarterly journal of mechanics and applied mathematics Vol. 51; no. 4; pp. 553 - 561 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Oxford
Oxford University Press
01.11.1998
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Subjects | |
Online Access | Get full text |
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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. |
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Bibliography: | ark:/67375/HXZ-TRGDSRL6-F istex:BA4E812216133CA197F67EFF438F6669C4068345 local:4 |
ISSN: | 0033-5614 1464-3855 |
DOI: | 10.1093/qjmam/51.4.553 |