2015
DOI: 10.1007/s00028-015-0287-1
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On convergence of solutions to equilibria for fully nonlinear parabolic systems with nonlinear boundary conditions

Abstract: Convergence to stationary solutions in fully nonlinear parabolic systems with general nonlinear boundary conditions is shown in situations where the set of stationary solutions creates a C 2 -manifold of finite dimension which is normally stable. We apply the parabolic Hölder setting which allows to deal with nonlocal terms including highest order point evaluation. In this direction some theorems concerning the linearized systems is also extended. As an application of our main result we prove that the lens-sha… Show more

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Cited by 5 publications
(9 citation statements)
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“…where B m k is the natural discrete analogue of B k (t m ) and ξ m+ 1 2 k is an appropriate approximation in order to guarantee the unconditional stability for the generalized scheme.…”
Section: Extension To Non-neutral External Boundariesmentioning
confidence: 99%
See 1 more Smart Citation
“…where B m k is the natural discrete analogue of B k (t m ) and ξ m+ 1 2 k is an appropriate approximation in order to guarantee the unconditional stability for the generalized scheme.…”
Section: Extension To Non-neutral External Boundariesmentioning
confidence: 99%
“…A model for surface diffusion of a network of curves has been introduced in [41] for d = 2 and generalized to arbitrary space dimensions in [17,32]. Well-posedness was shown in [1] for d = 2 and in [37] for higher space dimensions. We will present the precise mathematical formulation of this evolution law in Section 2 below.…”
Section: Introductionmentioning
confidence: 99%
“…We can then express the equations in the fixed reference configuration by means of the Hanzawa transform Θ h , cf. [3], [26], [25], [30], [23], [13], [2]. The transformed system reads as…”
Section: Curvilinear Coordinates and Hanzawa Transformmentioning
confidence: 99%
“…Let us precisely state the problem. We consider a fixed, smooth, and bounded domain in two space dimensions Ω ⊂ ℝ 2 . We assume that the domain can be decomposed as Ω = Ω + (𝑡) ∪ Γ(𝑡) ∪ Ω − (𝑡), where Γ(𝑡) denotes the interior of Γ(𝑡), a smooth one-dimensional curve with two boundary points on 𝜕Ω.…”
Section: Introductionmentioning
confidence: 99%