Theory of axisymmetric pendular rings

• A full spectrum of solutions of Young-Laplace equation for liquid menisci is found.
• The possible transitions between these menisci are described.
• The menisci do not exist if their geometric parameters do not fit a specific region.

We present the theory of liquid bridges between two solids, sphere and plane, with prescribed contact angles. We give explicit expressions for curvature, volume and surface area of pendular ring as functions of the filling angle ψψ for all available types of menisci: catenoid, sphere, cylinder, nodoid and unduloid (the meridional profile of the latter may have inflection points). There exists a rich set of solutions of the Young-Laplace equation for the shape of an axisymmetric meniscus of constant mean curvature. In case when the solids do not contact each other, these solutions extend Plateau’s sequence of meniscus evolution observed with increase of the liquid volume to include the unduloids at small filling angle, unduloids with multiple inflection points and multiple catenoids.The Young-Laplace equation with boundary conditions can be viewed as a nonlinear eigenvalue problem. Its unduloid solutions, menisci shapes and curvatures Hns(ψ), exhibit a discrete spectrum and are enumerated by two indices: the number n   of inflection points on the meniscus meridional profile MM and the convexity index s=±1s=±1 determined by the shape of a segment of MM contacting the solid sphere: the shape is either convex, s=1s=1, or concave, s=-1s=-1.For the fixed contact angles the set of the functions Hns(ψ) behaves in such a way that in the plane {ψ,H}{ψ,H} there exists a bounded domain where Hns(ψ) do not exist for any distance between solids. The curves Hns(ψ) may be tangent to the boundary of domain which is a smooth closed curve. This topological representation allows to classify possible curves and introduce a saddle point notion. We observe several types of saddle points, and give their classification.

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