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On a classification of steady solutions to two-dimensional Euler equations

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arxiv 2405.15327 v1 pith:LVCAEI55 submitted 2024-05-24 math.AP

classification math.AP
keywords flowflowssteadyanglesequationstwo-dimensionalwholebounded
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In this paper, we provide a classification of steady solutions to two-dimensional incompressible Euler equations in terms of the set of flow angles. The first main result asserts that the set of flow angles of any bounded steady flow in the whole plane must be the whole circle unless the flow is a parallel shear flow. In an infinitely long horizontal strip or the upper half-plane supplemented with slip boundary conditions, besides the two types of flows appeared in the whole space case, there exists an additional class of steady flows for which the set of flow angles is either the upper or lower closed semicircles. This type of flows is proved to be the class of non-shear flows that have the least total curvature. As consequences, we obtain Liouville-type theorems for two-dimensional semilinear elliptic equations with only bounded and measurable nonlinearity, and the structural stability of shear flows whose all stagnation points are not inflection points, including Poiseuille flow as a special case. Our proof relies on the analysis of some quantities related to the curvature of the streamlines.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Least total curvature solutions to steady Euler system and monotone solutions to semilinear equations in a strip

    math.AP 2025-07 accept novelty 6.0 of 10

    The authors construct case (c) least-total-curvature steady Euler flows in a strip and stable monotone semilinear solutions with non-convex superlevel sets.

  2. Remarks on radial symmetry of stationary and uniformly-rotating solutions for the 2D Euler equation

    math.AP 2025-06 conditional novelty 6.0 of 10

    Uniformly rotating 2D Euler solutions with compactly supported vorticity are forced to be radially symmetric whenever the angular velocity lies outside half the range of the vorticity, including irregular vortex patches.

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