Conveners
Thin Material Structures: MS-11-1
- Axel Voigt
Thin Material Structures: MS-11-2
- Weizhu Bao (National University of Singapore)
Description
Organisers: Weizhu Bao, Axel Voigt
-
Prof. Weizhu Bao (National University of Singapore)07/09/2026, 14:00Thin Material Structures
In this talk, I will present sharp interface models with anisotropic surface energy for simulating solid-state dewetting and the morphological evolution of patterned islands on a substrate. We will show how to derive the sharp interface model via thermovariation dynamics, i.e. variation of the interfacial energy via an open curve with two triple points moving along a fixed substrate. The sharp...
Go to contribution page -
Yifei Li (Tuebingen University)07/09/2026, 14:30Thin Material Structures
In this talk, we present a numerical analysis of the Eyles-King-Styles tumor growth model, a free boundary problem coupling a Poisson equation in the bulk \Omega with a forced mean curvature flow on its boundary \Gamma. Unlike existing evolving surface analyses based on integer-order Sobolev spaces, this bulk-surface coupling requires H^{1/2}-order regularity on \Gamma. We establish a...
Go to contribution page -
Marco Salvalaglio (TU Dresden)07/09/2026, 15:00Thin Material Structures
Solid-state dewetting is the process through which thin solid films break and retract on a substrate, leading to the formation of nanostructures. Dewetting in single-crystalline films is well understood as a surface-energy-driven phenomenon governed by surface diffusion. Polycrystalline films, by contrast, exhibit additional complexity due to the presence of extended defects (grain boundaries)...
Go to contribution page -
Prof. Buyang Li (The Hong Kong Polytechnic University)07/09/2026, 15:30Thin Material Structures
Finite element methods and kinematically coupled schemes that decouple the fluid velocity and structure displacement have been extensively studied for incompressible fluid-structure interaction (FSI) over the past decade. While these methods are known to be stable and easy to implement, optimal error analysis has remained challenging. Previous work has primarily relied on the classical...
Go to contribution page -
Maik Porrmann (Dresden University of Technology)08/09/2026, 10:30Thin Material Structures
We propose a numerical method for fluid deformable surfaces governed by surface Stokes flow and Helfrich bending energy under active growth, aiming to model shape evolution of the epithelium sheets in developmental processes. As a new extension of the model, we prevent self-intersections, which commonly arise under large deformations or low enclosed volume to area ratios, by incorporating the...
Go to contribution page -
Enno Igel (TU Dresden)08/09/2026, 11:00Thin Material Structures
We consider the surface Stokes-Helfrich problem using a stream function formulation. The formulation is considered for simply connected surfaces without boundary. It is based on a splitting of the velocity field in normal and tangential components and the Helmholtz decomposition of the tangential part. For its numerical solution the surface is approximated by higher order isoparametric...
Go to contribution page -
Albert Chern (University of California San Diego)08/09/2026, 11:30Thin Material Structures
Scalar vorticity formulation for fluid equations on surfaces is computationally attractive. However, the vorticity equation is incomplete on a non-simply-connected surface. We derive a new evolution equation for the finite dimensional harmonic (cohomology) components of the flow. We also show that the vorticity equation has a curvature-dependent, vorticity production term in addition to the...
Go to contribution page -
20. Surface Beris-Edwards-Helfrich models - how local orientational order can influence global shapeAxel Voigt08/09/2026, 12:00Thin Material Structures
We consider general models for hydrodynamic surface liquid crystals on (self-)evolving surfaces. We focus on nematic liquid crystals and model them using a Q-tensor approach. The model will be derived using the Lagrange-d´Alambert principle. Our Q-tensor is a 3D object defined on the surface. Here we address specific forms, essentially "surface conforming" Q-tensors, with eigenvectors in...
Go to contribution page