Abstract

In this paper, the motion of the n-vortex system as it collapses to a point in finite time is studied. The motion of vortices is described by the set of ordinary differential equations that we are able to solve analytically. The explicit formula for the solution demands the initial location of collapsing vortices. To find the collapsing locations of vortices, the algebraic, nonlinear system of equations was built. The solution of that algebraic system was obtained using Newton’s procedure. A good initial iterate needs to be provided to succeed in the application of Newton’s procedure. An unconstrained Leverber–Marquart optimization procedure was used to find such a good initial iterate. The numerical studies were conducted, and numerical evidence was presented that if in a collapsing system n=50 point vortices include a few vortices with much greater intensities than the others in the set, the vortices with weaker intensities organize themselves onto the vortex sheet. The collapsing locations depend on the value of the Hamiltonian. By changing the Hamiltonian values in a specific interval, the collapsing curves can be obtained. All points on the collapse curves with the same Hamiltonian value represent one collapsing system of vortices. To show the properties of vortex sheets created by vortices, the passive tracers were used. Advection of tracers by the velocity induced by vortices was calculated by solving the proper differential equations. The vortex sheets are an impermeable barrier to inward and outward fluxes of tracers. Arising vortex structures are able to transport the passive tracers. In this paper, several examples showing the diversity of collapsing structures with the vortex sheet are presented. The collapsing phenomenon of many vortices, their ability to self organize and the transportation of the passive tracers are novelties in the context of point vortex dynamics.

Highlights

  • Studies of the discrete vortex systems began in 1858 with the publication of the Helmholtz paper [1], where the interaction of two linear vortices was investigated.Nowadays, the dynamics of the point vortex system still rouse interest among scientists

  • The most fascinating phenomenon related to the collapse of the system of vortices is the point in finite time

  • It was demonstrated numerically that the system of collapsing vortices in a self-similar motion can organize itself in vortex structures that are able to transport passive markers caught inside of that structures

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Summary

Introduction

Studies of the discrete vortex systems began in 1858 with the publication of the Helmholtz paper [1], where the interaction of two linear vortices was investigated. Numerical results related to some special feature of collapse system of vortices are presented. The boundary of the coherent vortex structure is impermeable for tracers from the inside out and vice versa It is evident from the numerical experiments that a collapse system of vortices that possess strong vortices organizes itself into a coherent vortex structure. It is shown numerically that a collapse system with one or a few strong vortices organizes itself into a vortex sheet. The self-organization of vortices generates interesting vortex structures that are able to transport the passive tracers. The description of the numerical algorithm is provided, followed by several examples of different shapes of collapsing structures of vortices with one, two and four strong vortices. Passive tracers were used to demonstrate the transporting features of collapsing vortex structures

Equations of Motion for n Vortices
Self Similar Motions of n-Vortices
Algebraic Equations for Collapse Locations of Vortices
Prelude Example
Dynamics of Passive Tracers
Remarks on the Determination of the Values of Strong Vortices
Numerical Results for the Collapse of 50 Vortices with One Strong Vortex
Collapse of 50 Vortices with Two Strong Vortices
The Case A1
The Case A3
The Case A4
The Case A5
Conclusions
Full Text
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