Previous Page  10 / 13 Next Page
Information
Show Menu
Previous Page 10 / 13 Next Page
Page Background

Quantum Physics, Optics and

Laser Technologies

Page 35

conferenceseries

.com

Volume 5

Journal of Lasers, Optics & Photonics

Physicists Congress 2018

May 09-10, 2018

May 09-10, 2018 Tokyo, Japan

International Conference on

Hydrodynamical aspect of the physical vacuum

Valeriy I Sbitnev

National Research Center Kurchatov Institute, Russia

A

t present, we imagine the physical vacuum as a superfluid quantum medium containing enormous amount of particle-

antiparticle pairs arising and annihilating continuously. It is the Bose-Einstein condensate existing at super low

temperatures of the cosmic space. OK, let it be so. Then a motion of this cold superfluid quantum medium can be described

in the non-relativistic limit by pair of equations - the Navier-Stokes equation and the continuity equation. However, the first

equation describes motion of a classical viscous fluid. We need to modify this equation. The modifications concern to the

pressure gradient

P and to the term incorporating the viscosity of the fluid. The modification of the pressure gradient leads

to appearance of the quantum potential, Q, which turns out to be equal to the pressure divided by the density distribution, ρ.

Namely, Q=P/ρ. As a result, the above-mentioned pair of equations leads to emerging the Schrodinger equation when defining

the wave function in the polar form bearing information about the velocity, v, of the fluid and the density distribution. With

regard to the modification of the viscosity, it would seem that, in the first approximation, we could discard it. This is not a good

idea. Instead, we suppose

1

That is, the viscosity coefficient is a parameter fluctuating about zero. It means that there is an energy exchange within this

superfluidmedium. It is the zero-point energy fluctuations. By multiplying the modified Navier-Stokes equation by the operator

curl, we come to the vorticity equation

2

This equation in the cylindrical coordinate system permits to consider the vortex in its cross-section geometry. Solutions for

the vorticity ω and for the angular velocity v are as follows:

3

4

Here Γ is the integration constant and ν=μ/ρM is the kinematic viscosity; ρM is the mass density of the superfluid medium, and

σ is an arbitrary constant such that the denominators in equation (3) are always positive. The solution (3) is non-decreasing

in time and has a non-zero vortex core slightly fluctuating in time. It comes to the Gaussian coherent vortex cloud with time.\

olga.sbitneva@gmail.com

Valeriy I Sbitnev, J Laser Opt Photonics 2018, Volume 5

DOI: 10.4172/2469-410X-C1-020