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Inhaltsverzeichnis - Mathematisches Institut der Universität zu Köln

Inhaltsverzeichnis - Mathematisches Institut der Universität zu Köln

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DMV Tagung 2011 - <strong>Köln</strong>, 19. - 22. September<br />

Bernd Kawohl<br />

<strong>Universität</strong> <strong>zu</strong> <strong>Köln</strong><br />

On an overdetermined boundary value problem<br />

Serrin proved in a well-known paper from 1971 that the overdetermined bvp −∆u = 1 in Ω, u = 0 AND<br />

∂u/∂ν = const. on ∂Ω has a solution u in a bounded connected domain Ω if and only if Ω is a ball. While<br />

Serrin’s Theorem is valid for fairly general and benign elliptic equations, Weinberger found a much simpler<br />

proof for the special case mentioned above. In my lecture I report on related questions for degenerate<br />

nonlinear equations, e.g. for −∆pu = 1 with p ∈ (1,∞]. Forp < ∞ Pohozaev-identities are one ingredient for<br />

the proof. For p = ∞ it is remarkable that there are other domains than balls, on which (viscosity)-solutions<br />

exist. These results were obtained in cooperation with the coauthors listed in the references.<br />

Literatur<br />

Kawohl, B. (2007) Overdetermined problems and the p-Laplacian, Acta Math. Univ. Comenianae 76, 77–<br />

83.<br />

Buttazzo, G. & Kawohl, B. (2011) Overdetermined boundary value problems for the ∞-Laplacian, Intern.Mathem.<br />

Res. Notices 2011 237–247.<br />

Kawohl, B. (2011) Fragalà, I., Gazzola, F. & Kawohl, B. Overdetermined problems for the ∞-Laplacian and<br />

web functions. submitted<br />

Hans Knüpfer<br />

<strong>Universität</strong> Bonn<br />

Propagation of three-phase contact lines - well-posedness and regularity<br />

The propagation of a liquid drop on a plate is characterized by the evolution of the three-phase contact<br />

line where air, liquid and solid meet. For thin viscous droplets, the evolution can be decribed by a class<br />

of scalar fourth or<strong>der</strong> degenerate parabolic equations, the so called thin-film equations. We consi<strong>der</strong><br />

well-posedness and regularity for these thin-film equations and other fluid models in the presence of a<br />

three-phase contact line. Since the consi<strong>der</strong>ed do not satisfy a maximum principle, the analysis has to<br />

be based on the un<strong>der</strong>lying dissipative structure. One important point in the analysis is to find suitable<br />

function spaces such that the model is well-posed.<br />

Stefan Krömer<br />

<strong>Universität</strong> <strong>zu</strong> <strong>Köln</strong><br />

Weak lower semicontinuity of multiple integrals revisited: the role of lower bounds<br />

For integral functionals on W 1,p , the standard result due to Acerbi and Fusco shows equivalence of<br />

quasiconvexity of the integrand and weak lower semincontinuity of the functional. This result relies on an<br />

additional assumption, a lower bound for the integrand, which is not purely technical (as a well-known<br />

example involving the determinant illustrates), but not optimal either. I will present a less restrictive<br />

condition that is also necessary. Interestingly, this optimal condition is weaker than boundary quasiconvexity<br />

as defined by Ball and Marsden, although for p-homogeneous integrands, it reduces to the latter.<br />

54

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