Spin and wave function as attributes of ideal fluid

@article{Rylov1999SpinAW,
  title={Spin and wave function as attributes of ideal fluid},
  author={Yuri A. Rylov},
  journal={Journal of Mathematical Physics},
  year={1999},
  volume={40},
  pages={256-278},
  url={https://api.semanticscholar.org/CorpusID:120576387}
}
  • Y. Rylov
  • Published 1999
  • Physics
  • Journal of Mathematical Physics
An ideal fluid whose internal energy depends on density, density gradient, and entropy is considered. Dynamic equations are integrated, and a description in terms of hydrodynamic (Clebsch) potentials occurs. All essential information on the fluid flow (including initial and boundary conditions) appears to be carried by the dynamic equations for hydrodynamic potentials. Information on initial values of the fluid flow is carried by arbitrary integration functions. Initial and boundary conditions… 

Hydrodynamic equations for incompressible inviscid fluid in terms of generalized stream function

An unexpected fact is discovered that the effective description of the rotational flow cannot be carried out without introduction of the Clebsch potentials.

Hidden Dynamical Variables in Rotational Flow of Barotropic Fluid

Inviscid barotropic fluid is investigated as a dynamical system by means of variational methods. Conventional description in terms of variables: (density ρ0, velocity v, and labelling of stream lines

Hidden Dynamical Variables in Rotational Flow of Barotropic Fluid

Inviscid barotropic fluid is investigated as a dynamical system by means of variational methods. Conventional description in terms of variables: (density ρ0, velocity v, and labelling of stream lines

Uniform formalism for description of dynamic and stochastic systems

The formalism of dynamics in the space-time, where motion of free particles is primordially stochastic, is considered. The conventional dynamic formalism, obtained for the space-time, where the

Applications of wave equations with logarithmic nonlinearity in fluid mechanics

We apply statistical mechanics and Madelung hydrodynamical presentation for an effective description of strongly-interacting many-body systems, such as Bose liquids or Korteweg-type fluids. The

On a model of a classical relativistic particle of constant and universal mass and spin

The deformation of the classical action for a point-like particle recently suggested by Staruszkiewicz gives rise to a spin structure which constrains the values of the invariant mass and the

Gas Dynamics as a Tool for Description of Nondeterministic Particles

Classical gas dynamic equations describe mean motion of stochastic gas molecules. The reason of this stochasticity is in teraction (collisions) between molecules. The wave function is the way to

Gas Dynamics as a Tool for Description of Nondeterministic Particles

Classical gas dynamic equations describe mean motion of stochastic gas molecules. The reason of this stochasticity is in teraction (collisions) between molecules. The wave function is the way to

Temperature-driven dynamics of quantum liquids: Logarithmic nonlinearity, phase structure and rising force

We study a large class of strongly interacting condensate-like materials, which can be characterized by a normalizable complex-valued function. A quantum wave equation with logarithmic nonlinearity
...

The equations for isentropic motion of inviscid fluid in terms of wave function

It is shown that by change of variables, the equations of motion of the inviscid fluid can transform into a differential equation for a wave function ψ, consisting of two complex components. A unit

Variation Principles of Hydrodynamics

It is shown that the Lagrangian equations for the motion of both incompressible and compressible fluids can be derived from variation principles. As has been pointed out by C. C. Lin, an important

HAMILTONIAN FLUID MECHANICS

This paper reviews the relatively recent application of the methods of Hamiltonian mechanics to problems in fluid dynamics. By Hamiltonian mechanics I mean all of what is often called classical

Variational principles in continuum mechanics

Variational principles for problems in fluid dynamics, plasma dynamics and elasticity are discussed in the context of the general problem of finding a variational principle for a given system of

Hamilton's principle and Ertel's theorem

Variation principles for the equations governing the motion of perfect fluids are of two types. In the first type, which corresponds to Hamilton’s principle in particle mechanics, the positions of

The derivation of the equations of motion of an ideal fluid by Hamilton's principle

    J. Herivel
    Physics
  • 1955
ABSTRACT A new formulation of Hamilton's principle for the case of an ideal fluid is proposed which is claimed to be the uniquely proper form for such a system. The resulting derivation of the

AN ACTION PRINCIPLE FOR MAGNETOHYDRODYNAMICS

The equations of motion of an inviscid, infinitely conducting fluid in an electromagnetic field are transformed into a form suitable for an action principle. An action principle from which these

A note on Hamilton's principle for perfect fluids

A derivation is given of the Eulerian equations of motion directly from the Lagrangian formulation of Hamilton's principle. The circulation round a circuit of material particles of uniform entropy

Langrangian Perturbation Theory of Nonrelativistic Fluids

In this paper the conventional description of adiabatic perturbations of stationary fluids in terms of a Lagrangian displacement is reexamined, to take account of certain difficulties that have been

The degree of knottedness of tangled vortex lines

Let u(x) be the velocity field in a fluid of infinite extent due to a vorticity distribution w(x) which is zero except in two closed vortex filaments of strengths K1, K2. It is first shown that the