New Stationary $$N$$-Symmetric States of Three Point Vortices in a Two-Layer Rotating Fluid

Within the framework of the two-layer quasi-geostrophic model on a rotating plane, the motions for a special case of three point vortices with intensities $$\big{(}\kappa_{1}^{1},\kappa_{2}^{1},\kappa_{2}^{2}\big{)}=(4,1,-2)$$ are considered (here, the subscript denotes the layer number: 1 is the upper layer, 2 is the lower layer, and the superscript denotes the vortex number in the layer). Thus, it is assumed that one cyclonic vortex is located in the upper layer, and two vortices, cyclonic and anticyclonic, are located in the lower layer. It is shown that in the general case each vortex performs periodic motions in such a way that every half-period the vortex structure takes a collinear state. In this case, over time, the trajectory of each vortex completely fills a certain ring region around the vorticity center. However, among the continuum of these quasi-ordered trajectories, one can always find a family of closed periodic solutions, both purely circular (preserving the collinear structure) and more complex, so-called $$N$$ -modal ( $$N$$ -symmetric) stationary solutions. In this paper, these solutions are constructed and their main properties are described.

Authors

Institutions

Publication Details

Journal
Regular and Chaotic Dynamics
Published
2025-12-22
DOI
https://doi.org/10.1134/s1560354725550040
Primary Topic
Navier-Stokes equation solutions
Type
article
Field-Weighted Citation Impact
0.00
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

New Stationary $$N$$-Symmetric States of Three Point Vortices in a Two-Layer Rotating Fluid

Mikhail A. Sokolovskiy
Regular and Chaotic Dynamics
Navier-Stokes equation solutions
article

New Stationary $$N$$-Symmetric States of Three Point Vortices in a Two-Layer Rotating Fluid

Mikhail A. Sokolovskiy
article en

Abstract

Within the framework of the two-layer quasi-geostrophic model on a rotating plane, the motions for a special case of three point vortices with intensities $$\big{(}\kappa_{1}^{1},\kappa_{2}^{1},\kappa_{2}^{2}\big{)}=(4,1,-2)$$ are considered (here, the subscript denotes the layer number: 1 is the upper layer, 2 is the lower layer, and the superscript denotes the vortex number in the layer). Thus, it is assumed that one cyclonic vortex is located in the upper layer, and two vortices, cyclonic and anticyclonic, are located in the lower layer. It is shown that in the general case each vortex performs periodic motions in such a way that every half-period the vortex structure takes a collinear state. In this case, over time, the trajectory of each vortex completely fills a certain ring region around the vorticity center. However, among the continuum of these quasi-ordered trajectories, one can always find a family of closed periodic solutions, both purely circular (preserving the collinear structure) and more complex, so-called $$N$$ -modal ( $$N$$ -symmetric) stationary solutions. In this paper, these solutions are constructed and their main properties are described.

Regular and Chaotic DynamicsVol. 31(1)
Institute of Oceanology. PP Shirshov Russian Academy of Sciences (RU), Institute of Water Problems (RU)
Openalex Percentile: Top 25%
Navier-Stokes equation solutions
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.