SELF

66

O.N. Karavashkina and S.B. Karavashkin

The considered process of charge separation has great consequences. In particular, formation of electron cocoon is the necessary condition of protostar and star balance. Should by some reason the electron envelope dissipate, the forces of electric repel of positively charged atomic cores would cause the star destroyed. But the more hot substance has the star in depths the more abundant electron envelope it has.

The spherical dipole is electrically neutral body only on the whole. Within it, the substance is polarised and controlled by the laws acting between the capacitor armatures. (We would notice for those who like analogies, this not the least justifies a very popular now analogy between the atom and capacitor - this outwardly attractive but incorrect idea has here no concern.) From without the star is surrounded by the aureole of electron cocoon which is not detected instrumentally because of its distribution in the thick layer and at large radius from the centre of star. In the view of co-existence of fields, from without each star is electrically negative, so they electrically repel. Consequently, within the limits established by their co-existence, the star is a closed system in which all processes obey the laws of its own fields. This is the decisive condition of formation, existence and co-existence of celestial bodies.

Second important consequence is the following. With electrically similar surface charge of all stars, their collision in space becomes improbable. Any forces able to cause the collision experience the repel of volume charges of the same sign, and these charges are proportional to the mass of star and temperature in its centre. Such collisions could be possible as exclusions if the gravity attraction predominated over the electric repel in case of immediate approach to the distance at which their negatively charged envelops overlap. But this is possible only in case if the temperature of protostar and star core is quite low and the electron emission is negligible. But then the thermonuclear reactions are impossible - and such body cannot be a star. At the same time the star collision with the cold bodies and of cold bodies with each others is quite possible and observable, as cold bodies do not have a negative envelope creating a counter-force to the gravity attraction. Moreover, if speaking of interaction between the star and comparatively cold body, this interaction will be even intensified, due to creation in the cold body a dipole moment in the field of electron envelope of the hot body.

It follows from the said that we have to approach very selectively to modelling the interaction between the bodies in the university. In particular, describing the between-stars interaction, we cannot rely on hypotheses that we described in chapter 1 based on the stars collision. This corollary makes these hypotheses impracticable. Though the calculations made on their basis are sometimes very handsome and mechanically grounded (of course, if we disregard that these models do not note the electric repel). One of such simulations has been made in Hawaii university and shown in Fig. 2.15 copied from their web site.

Fig. 2.15. << Unequal-Mass Collision. This simulation presents a slightly off-center parabolic collision of two stars with a mass ratio of 2:1. Initially, each star was modeled as an n = 1.5 polytrope. A total of 49152 equal-mass particles were used; the calculation was run with an adaptive SPH code.

a) Projected View. The system is viewed along the orbital axis. Colors indicate the value of the entropy function a(S); blue indicates low values, while red indicates high values.
b) Meridional Slice. Only the 4096 particles nearest the orbital plane at each instant are shown. Viewing angle and color scheme are as above. The same slice of 4096 particles is shown in the following animations as well.
c) Viscous Dissipation. Here color indicates viscous dissipation in shocks; dark blue regions are adiabatic, while bright red indicates the strongest shocks. A meridional slice is shown.
d) Density. Here color indicates gas density; dark blue regions have the lowest densities, bright red regions have the highest. A meridional slice is shown.
f) Internal Energy. Here color indicates internal energy or temperature; blue regions are cool, red regions are hot. A meridional slice is shown.>>
Copied from http://www.ifa.hawaii.edu/research

With all beauty of this simulation, it is pity that the authors did not note such important factor which would essentially correct their calculations.