Abstract

An exact 3-D solution for deterministic chaos of J wave groups with M internal waves governed by the Navier-Stokes equations is presented. Using the Helmholtz decomposition, the Dirichlet problem for the Navier-Stokes equations is decomposed into the Archimedean, Stokes, and Navier problems. The exact solution is derived by the method of decomposition in invariant structures (DIS). A cascade differential algebra is developed for four families of invariant structures: deterministic scalar kinematic (DSK) structures, deterministic vector kinematic (DVK) structures, deterministic scalar dynamic (DSD) structures, and deterministic vector dynamic (DVD) structures. The Helmholtz decomposition of anticommutators, commutators, and directional derivatives is computed in terms of the dot and cross products of the DVK structures. Computation is performed with the help of the experimental and theoretical programming in Maple. Scalar and vector variables of the Stokes problem are decomposed into the DSK and DVK structures, respectively. Scalar and vector variables of the Navier problem are expanded into the DSD and DVD structures, correspondingly. Potentialization of the Navier field is possible since internal vortex forces, which are described by the vector potentials of the Helmholtz decomposition, counterbalance each other. On the contrary, external potential forces, which are expressed via the scalar potentials of the Helmholtz decomposition, superpose together to form the gradient of a dynamic pressure. Various constituents of the kinetic energy and the total pressure are visualized by the conservative, multi-wave propagation and interaction of three-dimensional, nonlinear, internal waves with a two-fold topology, which are called oscillons and pulsons.

Highlights

  • Conservative interaction of N three-dimensional internal waves controlled by the Navier-Stokes equations has been studied in [1], where the existence theorem is proved for a partial solution of the correspondent boundary-value problem via the Stationary Kinematic Euler-Fourier (SKEF) functions

  • The experimental and theoretical Deterministic Scalar Kinematic (DSK) structures, which are used to solve the kinematic problem for scalar fluid-dynamic variables, generate experimental and theoretical Deterministic Vector Kinematic (DVK) structures, which are studied in Section 3 and are utilized to find vector variables of the kinematic problem

  • The most interesting properties of the scalar and vector kinematic structures that are studied in Section 2 and Section 3, respectively, are the scalar and vector structural oscillations, the scalar-vector duality, the quadrality of the theoretical DSK and DVK structures, and the equiprobability of the experimental DSK and DVK structures

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Summary

Introduction

Conservative interaction of N three-dimensional internal waves controlled by the Navier-Stokes equations has been studied in [1], where the existence theorem is proved for a partial solution of the correspondent boundary-value problem via the Stationary Kinematic Euler-Fourier (SKEF) functions. An extreme sophistication of the partial solution derived with the help of experimental and theoretical programming in Maple doesn’t permit development of a general solution for propagation and interaction of wave groups of internal waves. To overcome this challenge, a structural approach to this problem has been developed in [2], where the differential algebra of SKEF structures is studied and various applications of the SKEF structures for solving the Laplace equation and the Helmholtz equations are considered. Directions of further exploration of the deterministic chaos of internal waves are outlined there

Scalar Kinematic Structures
Vector Kinematic Structures
Scalar Dynamic Structures
Vector Dynamic Structures
The Stokes Field
The Navier Field
Discussion
Conclusions
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