2019
DOI: 10.1007/s00205-019-01384-7
|View full text |Cite
|
Sign up to set email alerts
|

The Euler Equations in Planar Domains with Corners

Abstract: When the velocity field is not a priori known to be globally almost Lipschitz, global uniqueness of solutions to the two-dimensional Euler equations has been established only in some special cases, and the solutions to which these results apply share the property that the diffuse part of the vorticity is constant near the points where the velocity is insufficiently regular. Assuming that the latter holds initially, the challenge is then to propagate this property along the Euler dynamic via an appropriate cont… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
27
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
5
3

Relationship

1
7

Authors

Journals

citations
Cited by 14 publications
(28 citation statements)
references
References 29 publications
1
27
0
Order By: Relevance
“…Lacave first proved in [14] that if ∂Ω is C 1,1 except at finitely many corners that are all exact sectors with angles greater than π 2 , and ω 0 has a constant sign and is constant near ∂Ω, then ω will indeed remain constant near ∂Ω forever and weak solutions are unique. Then, together with Zlatoš, they showed the same result when ∂Ω is C 1,1 except at finitely many corners of arbitrary angles from (0, π) that do not need to be exact sectors, and without the sign restriction on ω 0 [17]. In both works, Euler particle trajectories for bounded solutions (general ones in [17] and with a constant sign in [14]) were shown to remain in Ω for all time (again approaching ∂Ω no faster than double-exponentially), and in [17] this was even proved to hold when ∂Ω is only C 1,γ (for some γ > 0) except at finitely many corners with angles from (0, π).…”
Section: Prior Existence and Uniqueness Resultsmentioning
confidence: 68%
See 1 more Smart Citation
“…Lacave first proved in [14] that if ∂Ω is C 1,1 except at finitely many corners that are all exact sectors with angles greater than π 2 , and ω 0 has a constant sign and is constant near ∂Ω, then ω will indeed remain constant near ∂Ω forever and weak solutions are unique. Then, together with Zlatoš, they showed the same result when ∂Ω is C 1,1 except at finitely many corners of arbitrary angles from (0, π) that do not need to be exact sectors, and without the sign restriction on ω 0 [17]. In both works, Euler particle trajectories for bounded solutions (general ones in [17] and with a constant sign in [14]) were shown to remain in Ω for all time (again approaching ∂Ω no faster than double-exponentially), and in [17] this was even proved to hold when ∂Ω is only C 1,γ (for some γ > 0) except at finitely many corners with angles from (0, π).…”
Section: Prior Existence and Uniqueness Resultsmentioning
confidence: 68%
“…Moreover, [17] also constructed examples of domains smooth everywhere except at a single corner with an arbitrary angle from (π, 2π) where Euler particle trajectories can reach ∂Ω in finite time, using an idea of Kiselev and Zlatoš [13].…”
Section: Prior Existence and Uniqueness Resultsmentioning
confidence: 99%
“…In addition, it is well-known that Yudovich [57] obtained the existence and uniqueness of global weak solutions if the initial vorticity ω 0 lies in L 1 ∩ L ∞ for the domain D = R 2 (see [47] for the bounded domain case). One can refer to [3,4,6,11,18,19,20,26,39,40,42,56,58] and the references therein for other related interesting and important aspects concerning with the two-dimensional incompressible Euler equations.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…For more details about renormalized solutions, we refer, for instance, to [16,Prop. 4.1] or [17,Sect. 3.2].…”
Section: Estimates With Precise Rate For Stronger Solutionsmentioning
confidence: 99%