Next, we assign the astronaut ¤ with the following problem:
4. The astronautós experiments
Astronaut ¤, in order o prove which of the two phases (Phase I or Phase II) his rocket is in, acts as follows:
a. The device for measuring velocity
To begin with, astronaut ¤ places near the floor CD of his chamber, a device ┼ that radiates e.g. two parallel laser beams L1 and L2. Those parallel laser beams are at a small distance d from one another, and are parallel to the floor CD of the chamber. Beams L1 and L2
are connected to e.g. an oscilloscope, which acts as a chronometer.
where t is the time recorded by the oscilloscope (chronometer), when mass m crossed the known distance d between the two parallel Laser beams L1 and L2.
b. Performing the experiments
Astronaut ¤, after installing the device ┼
for measuring velocity, as described above, now performs the following experiments:
Subsequently, conclusions ┴ and ┬, as detailed above, are astronaut Oós answer to the problem we set him.
5. Various other conclusions drawn by the astronaut
following the above correct answer he gave to the problem we set him, now proceeds to other conclusions regarding the Phase (Phase I or Phase II) his rocket S is in.
where F is the reading of dynamometer D and m is a known mass attached to the end of the dynamometerós spring.
Thus, from the first of relations (2.6) the velocity §1 of mass m1 , is:
and the velocity §2 of mass m2, is:
From relations (5) and (6), because m1<m2, it follows that §1 > §2.
Dividing now by member relations (5) and (6), we have:
And based on relation (4), relation (7) yields:
In relation (8), because m1, m2, k are known, astronaut ¤ also knows the mass ╠ of the celestial body, where his rocket S is docked.
Also, from the first of relations (2.6), we have
Now, by replacing the ╠ in relation (9) with that of relation (8), we have:
In relation (10) factors §1, h, m1, k are known.
Where G is the constant of universal attraction.
In relation (13) factors G, h, §1, m1, m2, k are known. Subsequently, on the basis of relation (13), astronaut ¤
also knows the radius R of mass ╠, where his rocket S is docked.
In other words:
ANOTHER MISTAKE BY EINSTEIN...
As is well known, in the źequivalence principle╗ (weak equivalence principle), Einstein claims that:
Now, if what Einstein claims above, fig. 4, on the źequivalence principle╗ were correct, then, during the elevatorós free fall in the gravitational field of mass ╠, mass m2 would remain at the centre ╩
of the elevator chamber (as would be the case if the elevator were an inertial reference system S, away from gravitational fields).
In other words:
Thus, in accordance wit the above, the źequivalence principle╗ of the General Theory of Relativity must be rejected as completely erroneous.
A QUESTION ON THE źEQUIVALENCE PRINCIPLE╗...
It is well known that, in the źstrong equivalence principle╗, Einstein accepts that: źAll bodies (regardless of their mass) fall with the same velocity in the gravitational field of a mass M╗, (See http://www.tsolkas.gr/forums/777.jpg), book:Clifford M. Will, “Was Einstein right?”.
Following all that we examined in our project, and on the basis on Conclusion I and Conclusion II, it is clearly and undoubtedly proven that the źequivalence principle╗ (weak and strong equivalence principle) is a completely
erroneous theory of Physics.
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