Superphysics Superphysics
Chapter 13b

Solar Wind and Black Holes

by Rene Descartes Icon
4 minutes  • 725 words
Table of contents

Solar Wind: How Do They Radiate from the Sun?

The stellar air-aether [invisible spacetime particles] is continually pushed by 2 phenomena:

  1. By their fellow air-aether between them and the star at the center of their gravitational territory
  2. By the fire-aether [visible electromagnetic particles] of that star*.
Superphysics Note
This is solar wind since it has a pushing force or energy

They are not pushed at all by the others [beside them].

For example, those at E are not pushed by those at M, G, F, K, or H, but only by all those that are between the two lines AF and DG together with the fire-aether of the sun.

Solar Winds
Descartes explains why the solar wind goes outwards when the spacetime particles go inwards to cause stellar gravity

That is why they tend not only towards M, but also towards:

  • L,

  • N, and

  • generally all the air-aether that are in a straight line from the points on the sun.

To explain this outward motion, let us imagine the sun as a void.

Black Holes

Imagine the air-aether particles at E were all alone and that there was absolutely no light (fire-aether) anywhere, even where the sun is.

Solar Winds
Descartes explains why the solar wind goes outwards when the spacetime particles go inwards to cause stellar gravity
  1. If that air-aether at E disappeared, then the air-aether beyond circle FEG, say at M, will not fill its place since it tends to move away from it.

  2. The air-aether at F will also not fill it. This is because it is moving towards G with the same speed as it goes to R.

The void at E will move with them as long as others do not come from elsewhere to fill it.

  1. The air-aether within the circle FEG but beyond the lines AF and DG, such as those at H and K, will also not fill it.
  • This is even if their tendency to move away from S disposes them in some way. This is similar to how a rock’s weight disposes it to fall in a straight line and roll down a mountain sideways if it cannot fall straight down.

But such air-aether do not fill that void because of the continuous straight-line motions.

Nature always chooses the shortest way to arrive at the same effect.[57]

  • This is why the air-aether must travel in a straight line.
  • The continual straight-line motions impedes the air-aether from going into E.

If the air-aether at K advanced towards E and filled it, then the air-aether at the Sun S would take the place of K.

  • But this would create a new void at the circumference ABCD of the sun at the same time

But shortest way would be for the air-aether between the lines AF and DG advance straightaway towards E.

  • But by the time that air-aether reaches E, E has moved away.
  • It cannot curve to chase E in the same way that a falling rock falls straight down and not in a curve.

The air-aether between the lines AF and DG must advance together towards space E in order to fill it when it becomes void.

Only their inclination to move away from point S carries them toward E.

  • This inclination causes those between the lines BF and CG to tend to move more directly towards E than those that remain between the lines AF and BF, and DG and CG.
  • These latter parts are also disposed as the others to go there.

The effect is that:

  • space E is filled
  • a space of equal size in the circumference ABCD becomes void at the same time

The air-aethers are completely alike, but not all equal.

  • It does not matter which of them fill these places.
  • The motions that can cause them to be unequal are irrelevant.

The shortest way to fill E is for the air-aether at D to go to E via lines DG or DE.

If the air-aethers between the lines BF and CF advanced first towards E, then they would cause V to be void.

  • D would then have to fill this.
    • This would create a curved line DVE* just to fill E instead of a straight line DG, or DE.
  • This is contrary to my rules of motion.
Superphysics Note
This is why there are no swirls within an accretion disk of a black hole.

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