Global well-posedness is established for a nonlocal curve evolution of an immersed elastic filament, together with convergence to resistive force theory as the filament thickness approaches zero.
The slender body free boundary problem
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abstract
We consider the slender body free boundary problem describing the evolution of an inextensible, closed elastic filament immersed in a Stokes fluid in $\mathbb{R}^3$. The filament elasticity is governed by Euler-Bernoulli beam theory, and the coupling between this 1D elasticity law and the surrounding 3D fluid is governed by the slender body Neumann-to-Dirichlet (NtD) map, which treats the filament as a 3D object with constant cross-sectional radius $0<\epsilon\ll1$. This map serves as a mathematical justification for slender body theories wherein such 3D-1D couplings play a central role. We develop a solution theory for the filament evolution under this coupling. Our analysis relies on two main ingredients: (1) an extraction of the principal symbol of the slender body NtD map, from the author's previous work, and (2) a detailed treatment of the tension determination problem for enforcing the inextensibility constraint. Our work provides a mathematical foundation for various computational models in which a slender filament evolves according to a 1D elasticity law in a 3D fluid. This forms a key development in our broader program to place slender body theories on firm theoretical footing.
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math.AP 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
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A nonlocal curve evolution for an immersed elastic filament: global existence and convergence to resistive force theory
Global well-posedness is established for a nonlocal curve evolution of an immersed elastic filament, together with convergence to resistive force theory as the filament thickness approaches zero.