2. The Fall of Bodies

All bodies falls to earth always with the same velocity, independently from its mass, supposing that there is no resistance of the air. Since the field lines of the gravitational field are directed vertically towards the center of the earth (see also chapter 3 in Results), every fermion in a body moves during a free fall along these field lines. Each field line consists of numerous VG that are linked together by strings. For this reason, any fermion must interact with a certain amount of VG on each field line in order to fall to earth. It does not matter how many fermions a body has, since any fermion must realize these interactions independently from the other particles of the body since any particle is located on an individual field line (or group of field lines). As a result, each fermion falls at the same time to earth, independent of which body it is momentarily located. This furthermore means that each body falls at the same time to earth, independent of how many fermions it is made of.

We can demonstrate that fermions fall independently each other in a body and with the same speed, because any piece of matter falls with the same velocity to earth without rotating. If some particles of a certain body would fall faster to earth than others, certain pieces of matter would rotate while falling down, since one side of the corresponding body would tend to fall faster than the other side. Since this is not the case, we must suppose that any particle falls with the same speed. Since smaller bodies fall with the same speed as larger bodies which are made of more fermions, we can conclude that the number of fermions does not affect the free fall, e.g. fermions fall each other independently to earth.

 

3. Antigravitation

In addition to an electric field, charges also have a gravitational field due to their mass. Positive charges interact with VG of the BF. Therefore VG are used to build up the gravitational and electric fields of positive charges. In consequence, there is a competition between both fields for VG, so that the stronger field (electric field) weakens the weaker field (gravitational field). The gravitational field does no longer dispose of 100 % of the VG of the BF to be built up, with the result that it becomes weaker.

Since any VP in an EM field signifies a VG less in the corresponding gravitational field, the decrease of gravity for a body is proportional to the amount of positive charges of the body that determine how many VG are converted into VP of the corresponding electric fields:

[11]                  (-)FG ~ n q(+)

Where (-)FG: Decrease of gravity of a body

  n: Number of positive charges in the body

  q(+): Load of a positive charge in the body

This type of antigravitation (EM reduction of gravity) happens only through positive charges and can theoretically reach a value from 0 - 100 % according to how many VG of the BF positive charges interact with.

Negative charges, on the contrary, emit VG so that in this case there would be no deficit of VG that could produce antigravitation. In any way, VG produced by negative particles are very volatile and cannot always interact with nearby positive particles (i.e. in an atom), so that they escape partially to the BF without interacting. This always produces a slight deficit of VG close to negative particles and thus there is always a slight local reduction of gravity. In this sense, also negative particles would participate in antigravity, although not directly.

Antigravitation was found accidentally in an experiment with a turning superconductor that was suspended by solenoids.² In agreement with the experiment, antigravitation cannot be suddenly be switched on and off. It reaches a theoretical value up to a certain percentage. In the experiment, it was up to 2.1 %. This could be interpreted as if approximately 2.1 % of the VG of the BF had been converted into VP of the EM field, whereby the gravity had decreased in exactly this proportion.

The supposition that VP in EM fields must not necessarily be very abundant with respect to VG in a gravitational field, is supported by the considerations in chapter 4 of Results. If we approach two unequal poles, the field lines of both magnets combine to one unique field. This is an indication that these field lines are not so abundant as in the BF. Otherwise such type of an addition would probably not be possible because of the lack of space between two adjacent field lines (in the BF, this space is probably close to Planck's elementary length). Therefore, the supposition that its about 2.1 % of the total virtual bosons, is probably a realistic idea.