Corner solutions of the Laplace–Young equation
The upper free surface $z=u(x,y)$ of a static fluid with gravity acting in the $z$ direction, occupying a volume $V$, satisfies the Laplace–Young equation. The fluid wets the vertical boundaries of $V$ so that the usual capillary contact conditions hold. This paper considers wedge shaped volumes $V$...
| Hlavní autoři: | , , |
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| Médium: | Journal article |
| Vydáno: |
2005
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