time axes of energy

[AntonioLao]

The time axes of 1st power of energy are outward radials from a spherically symmetric center. These outward vectors give descriptions for all radiation phenomena from the Big Bang and supernovae to all forms of electromagnetic radiations.

It is clear that the distinction between mass and energy can be demonstrated just by the orientations of these respective time axes. Pure mass would have all time axes pointed inward. Pure energy would have all time axes pointed outward. If there are equal numbers of inward and outward pointers then the resulting configuration is called continuous space. It is proportional to the 1st power of energy and the constant of proportionality is the speed of light. Furthermore, continuous space gave the appearance of a 2D manifold or surface. When it is closed, mass is inside and energy outside. If not closed then it is a Moebius strip. In the limit of contraction to 1D, two distinct nonequivalent topologies emerged. These are the squares of energy of quantized space.

[Guille]

Let me think If I understood the post completely.

First, you say that if E=m then the given product is CS (continious space). You say that CS*c& 1st power of energy (where & means proportional). What is the first power of energy? You say that CS is 2d and that if it's closed, then E>CS>m. You say that when CS is open, then it's moebius strip, yopu say that two distinct nonequivalent topologies emerge: E^2 and QS. But isn't E^2=QS? I remeber that you said that H=E^2 or something before.

[AntonioLao]

you say that if E=m

Only their time axes.

[math]E[/math] is the 1st power of energy
[math]E^2[/math] is the 2nd power of energy
[math]E^3[/math] is the 3rd power of energy

[Guille]

Only their time axes.

[math]E[/math] is the 1st power of energy
[math]E^2[/math] is the 2nd power of energy
[math]E^3[/math] is the 3rd power of energy

thanks.

Can you make me remember: What is the convertion of CS to QS?

[AntonioLao]

Can you make me remember: What is the convertion of CS to QS?

multiply both sides of Einstein's field equations of general relativity by a factor of light speed.
[math]c(R_{\mu\nu}-\frac{1}{2}g_{\mu\nu} R = -T_{\mu\nu})[/math]