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Ether and
Magnetic field

Galileo and
Einstein
are wrong

Equivalence
Principle

Ether and
Equivalence
Principle

Proof  for
the advance
of Mercury's
perihelion


Open
Letter

 

The
Electro
gravitational
Theory I

The
Electro
gravitational
Theory II

The
Electro
gravitational
Theory III

The
Electro
gravitational
Theory IV

The
Electro
gravitational
Theory V

Generalised
Geometry

Mathematics
of degree

Video 01

Video 02


Ether
and
Light

 

THE “PARALLEL MIRRORS” EXPERIMENT

Lets assume, Fig. 1, that we have two identical rectangular mirrors 1 and 2, which are parallel to each other.
In their four corners, the mirrors are supported by four metal rods of a height d, which are vertical to the two mirrors 1 and 2.
In the middle BC of mirror 2 is a plane light source L, which emits a narrow laser beam L0.
The laser beam L0 is vertical to the two mirrors 1 and 2 .
In this case, the beam will be continuously reflected between the two mirrors 1 and 2, and always remain vertical to the two mirrors M1 and 2.
Therefore, the mirror 1 will be dark (not lit) on the right and left of the straight line B΄C΄ and the mirror 2 will be dark (not lit) on the right and left of the straight line BC.
Consequently, in the experimental device, only the two straight lines B΄C΄ and BC will be bright.
At this stage, the experimental device of Fig. 1, described above, is motionless in relation to the Earth.

Fig. 1

Next (and while the light source continues to emit the light beam L0) we place the experimental device on a vehicle moving towards the Earth at high velocity (e.g. satellite, spaceship, space shuttle, etc).
After what we discussed above, we now need to ponder the following:
a. If ether doesnt exist in Nature, (as claimed in the Theory of Relativity), then the beam L0 will be continuously reflected vertically between the two mirrors 1 and 2, leaving the mirror 1 dark (not lit)(to the right and left) of the straight line B΄C΄, and mirror 2 dark (not lit)(to the right and left) of the straight line BC, as described above Fig.1.
Conversely, if ether does exist in Nature and creates an etherosphere around the Earth (as claimed in the Electrogravitational Theory), then the light beam L0 will initially shift by a small angle 0, Fig.2, i.e.:

where c = the speed of light.
Following that, it will be continuously reflected between the mirrors 1 and 2, at points 1, 2, 3,…-1, and exit the area between the mirrors 1 and 2.


Experiment 21
Experimental
Verification

 


Experiment 22
Experimental
Verification

 


The mistakes
of Einstein

 


Spherical
Shell
Problem
 

Recapitu-
lation


TECHNOLOGY
Fusion:
The “ZEUS”
machine

 


CERN/OPERA
IKARUS
TSOLKAS

 

Fig. 2

Because, however, the angles of incidence and reflection of the light beam L0 on the two mirrors 1 and 2 are very small, it follows that the number of points 1, 2, 3,…-1, is very large.

As a consequence of the above, the mirror 1 will be lit on the left of the straight line B΄C΄ and the mirror 2 will also be lit on the left of straight line BC, Fig.1.
Obviously, the part of mirror 1 to the right of the straight line B΄C΄ will remain dark, as will the part of mirror 2 on the right of the straight line BC .
In Fig. 2, D are the parts that are lit.
Therefore, using a photographic camera F or a variety of photometers, we can ascertain whether the mirrors 1 and 2 have been lit, as described above.
 

Note: If we now reversed the direction of velocity of the experimental device, then the lit areas of mirrors 1 and 2 would also be reversed. Meaning, the bright parts would be dark, and the dark parts would be bright.

CONCLUSION

By performing the “parallel mirrors” experiment (as described above) we can ascertain whether or not ether does exist in Nature, and from the result we will know, once and for all, which of the two theories is correct: the Theory of Relativity, or the Electrogravitational Theory.
In addition, the “parallel mirrors” experiment, Fig. 1, can be performed when the whole rectangular parallelepiped A = (12345678) is made of a transparent solid or liquid material (e.g. glass, water, etc), with a high index of refraction n (n > 1), where the light beam L0 is reflected on the two parallel surfaces (1234) and (5678).

The purpose of the above is to give us a greater initial angle , i.e.:

where n > 1
so that relations (1) and (2) yield:

Apart from that, the experiments philosophy remains the same, as described above in Fig.1.

Finally, the “parallel mirrors” experiment is simple to construct, costs very little, and yields reliable results.

Photo. 1 depicts a space shuttle, which could easily be used to perform the “parallel mirrors” experiment, described above.

photo. 1

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