TY - JOUR
T1 - Regularity results in 2D fluid–structure interaction
AU - Breit, Dominic
N1 - Publisher Copyright:
© 2022, The Author(s).
PY - 2022/12/31
Y1 - 2022/12/31
N2 - We study the interaction of an incompressible fluid in two dimensions with an elastic structure yielding the moving boundary of the physical domain. The displacement of the structure is described by a linear viscoelastic beam equation. Our main result is the existence of a unique global strong solution. Previously, only the ideal case of a flat reference geometry was considered such that the structure can only move in vertical direction. We allow for a general geometric set-up, where the structure can even occupy the complete boundary. Our main tool—being of independent interest—is a maximal regularity estimate for the steady Stokes system in domains with minimal boundary regularity. In particular, we can control the velocity field in W2 , 2 in terms of a forcing in L2 provided the boundary belongs roughly to W3 / 2 , 2. This is applied to the momentum equation in the moving domain (for a fixed time) with the material derivative as right-hand side. Since the moving boundary belongs a priori only to the class W2 , 2, known results do not apply here as they require a C2-boundary.
AB - We study the interaction of an incompressible fluid in two dimensions with an elastic structure yielding the moving boundary of the physical domain. The displacement of the structure is described by a linear viscoelastic beam equation. Our main result is the existence of a unique global strong solution. Previously, only the ideal case of a flat reference geometry was considered such that the structure can only move in vertical direction. We allow for a general geometric set-up, where the structure can even occupy the complete boundary. Our main tool—being of independent interest—is a maximal regularity estimate for the steady Stokes system in domains with minimal boundary regularity. In particular, we can control the velocity field in W2 , 2 in terms of a forcing in L2 provided the boundary belongs roughly to W3 / 2 , 2. This is applied to the momentum equation in the moving domain (for a fixed time) with the material derivative as right-hand side. Since the moving boundary belongs a priori only to the class W2 , 2, known results do not apply here as they require a C2-boundary.
UR - http://www.scopus.com/inward/record.url?scp=85145181420&partnerID=8YFLogxK
U2 - 10.1007/s00208-022-02548-9
DO - 10.1007/s00208-022-02548-9
M3 - Article
AN - SCOPUS:85145181420
JO - Mathematische Annalen
JF - Mathematische Annalen
SN - 0025-5831
ER -