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Euler Equations on 2D Singular Domains.

紀錄類型:	書目-語言資料,手稿 : Monograph/item
正題名/作者:	Euler Equations on 2D Singular Domains./
作者:	Han, Zonglin.
面頁冊數:	1 online resource (101 pages)
附註:	Source: Dissertations Abstracts International, Volume: 84-10, Section: B.
Contained By:	Dissertations Abstracts International84-10B.
標題:	Applied mathematics. -
電子資源:	click for full text (PQDT)
ISBN:	9798379413972

Euler Equations on 2D Singular Domains.
Han, Zonglin.

Euler Equations on 2D Singular Domains. - 1 online resource (101 pages)

Source: Dissertations Abstracts International, Volume: 84-10, Section: B.

Thesis (Ph.D.)--University of California, San Diego, 2023.

Includes bibliographical references

The Euler equations are a fundamental yet celebrated set of mathematical equations that describe the motions of inviscid, incompressible fluid on planar domains. They play a critical role in various fields of study including fluid dynamics, aerodynamics, hydrodynamics and so on. Though it was first written out in 1755, there are still many open questions regarding to this rich system, including some fundamental questions of Euler equations on singular domains. Unlike existence of weak solutions that were proven on considerably general domains, uniqueness of such solutions are still quite open on singular domains, even on convex domains. In this thesis, we will show uniqueness of weak solutions on singular domains given two different assumptions of initial vorticity ω0 ∈ L∞:1. ω0 is constant near the boundary.2. ω0 is constant near the boundary and has a sign (non-positive or non-negative).Under the first assumption, the previous best uniqueness results can only be applied to C1,1 domains except at finitely many corners with interior angles less than π. Here, we will extend the result to fairly general singular domains which are only slightly more restrictive than the exclusion of corners with angles larger than π, thus including all convex domains. We derive this by showing that the Euler particle trajectories cannot reach the boundary in finite time and hence the vorticity cannot be created by the boundary. We will also show that if the given geometric condition is not satisfied, then we can construct a domain and a bounded initial vorticity such that some particle could reach the boundary in finite time.Under the second assumption with the sign condition, the previous best uniqueness result can only be applied to C1,1 domains with finitely many corners with interior angels larger than π/2 . Here, we will extend the result to a class of general singular open bounded simply connected domains, which can be possibly nowhere C1 and there are no restrictions on the size of each angle.

Electronic reproduction.
Ann Arbor, Mich. :
ProQuest,
2024

Mode of access: World Wide Web

ISBN: 9798379413972Subjects--Topical Terms:

1069907
Applied mathematics.
Subjects--Index Terms:

Euler equationsIndex Terms--Genre/Form:

554714
Electronic books.

Euler Equations on 2D Singular Domains.
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245 1 0 $a Euler Equations on 2D Singular Domains.
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500 $a Source: Dissertations Abstracts International, Volume: 84-10, Section: B.
500 $a Advisor: Zlatos, Andrej.
502 $a Thesis (Ph.D.)--University of California, San Diego, 2023.
504 $a Includes bibliographical references
520 $a The Euler equations are a fundamental yet celebrated set of mathematical equations that describe the motions of inviscid, incompressible fluid on planar domains. They play a critical role in various fields of study including fluid dynamics, aerodynamics, hydrodynamics and so on. Though it was first written out in 1755, there are still many open questions regarding to this rich system, including some fundamental questions of Euler equations on singular domains. Unlike existence of weak solutions that were proven on considerably general domains, uniqueness of such solutions are still quite open on singular domains, even on convex domains. In this thesis, we will show uniqueness of weak solutions on singular domains given two different assumptions of initial vorticity ω0 ∈ L∞:1. ω0 is constant near the boundary.2. ω0 is constant near the boundary and has a sign (non-positive or non-negative).Under the first assumption, the previous best uniqueness results can only be applied to C1,1 domains except at finitely many corners with interior angles less than π. Here, we will extend the result to fairly general singular domains which are only slightly more restrictive than the exclusion of corners with angles larger than π, thus including all convex domains. We derive this by showing that the Euler particle trajectories cannot reach the boundary in finite time and hence the vorticity cannot be created by the boundary. We will also show that if the given geometric condition is not satisfied, then we can construct a domain and a bounded initial vorticity such that some particle could reach the boundary in finite time.Under the second assumption with the sign condition, the previous best uniqueness result can only be applied to C1,1 domains with finitely many corners with interior angels larger than π/2 . Here, we will extend the result to a class of general singular open bounded simply connected domains, which can be possibly nowhere C1 and there are no restrictions on the size of each angle.
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538 $a Mode of access: World Wide Web
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650 4 $a Mathematics. $3 527692
653 $a Euler equations
653 $a Lagrangian solutions
653 $a Singular domains
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690 $a 0364
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