Chiesa Andrea, Stefanelli Ulisse
University of Vienna, Faculty of Mathematics and Vienna School of Mathematics, Oskar-Morgenstern-Platz 1, A-1090 Vienna, Austria.
University of Vienna, Faculty of Mathematics, Oskar-Morgenstern-Platz 1, A-1090 Vienna, Austria.
Z Angew Math Phys. 2025;76(2):53. doi: 10.1007/s00033-025-02434-9. Epub 2025 Jan 30.
We investigate the evolution of a two-phase viscoelastic material at finite strains. The phase evolution is assumed to be irreversible: One phase accretes in time in its normal direction, at the expense of the other. Mechanical response depends on the phase. At the same time, growth is influenced by the mechanical state at the boundary of the accreting phase, making the model fully coupled. This setting is inspired by the early stage development of solid tumors, as well as by the swelling of polymer gels. We formulate the evolution problem by coupling the balance of momenta in weak form and the growth dynamics in the viscosity sense. Both a diffused- and a sharp-interface variant of the model are proved to admit solutions and the sharp-interface limit is investigated.
我们研究了有限应变下两相粘弹性材料的演化。假设相演化是不可逆的:一个相在其法线方向上随时间增长,以牺牲另一个相为代价。力学响应取决于相。同时,生长受到生长相边界处力学状态的影响,使得该模型完全耦合。这种设定的灵感来源于实体肿瘤的早期发展以及聚合物凝胶的溶胀。我们通过将弱形式的动量平衡和粘性意义下的生长动力学耦合来表述演化问题。证明了该模型的扩散界面和尖锐界面变体都存在解,并研究了尖锐界面极限。