The initial misunderstanding

Maxwell, discovering that emptiness has permeability and permittivity, deduced that these were characteristics of space , that it would not be empty but full of a substance that fills it, which he called ether. It certainly could not control and measure in the nineteenth century whether this substance represents space or is contained in it and moves in it … Michelson followed Maxwell’s thought by seeking the relative wind of the Earth with respect to the motionless ether in absolute space. On this misunderstanding Einstein derived the Principle of Relativity .

All the measurements made so far, always and only with light, seem to have confirmed this principle which has so far never been violated. But … the light is an electromagnetic wave, the only one that Maxwell knew, but which, due to its very short wavelength, is difficult to measure. Today there is a whole range of sophisticated radiotechnical equipment; extremely precise and measurable frequency waves can be generated in its phase . And it is possible to build electromagnetic interferometers, despite the interdiction of the Principle of relativity established by Einstein . And that’s what I did as a simple radio technician and not a graduate in Relativity!

The Relativity Principle establishes that the laws of physics must be valid in every homogeneous reference system. If the principle of relativity were invalidated, the corpus of fundamental physical theories would be compromised.

Phase comparison in a wave … progressive!

A second violation interdiction, due this time to Maxwell himself, is that on Earth it is not possible to measure an electromagnetic Doppler effect of the 1st order, that is a v / c, since it is not possible to synchronize two different moments of a wave that propagates in the space. According to him, it is only possible to measure a second order Doppler, that is, to compare the wave with itself reflected. Instead, unlike light, microwaves of a few centimeters of wavelength can be taken along the way simply by comparing the phase with probes arranged along the way. Just take the plane wave with probes, reveal it with diodes placed in opposition along its path after ½ wavelength or odd multiples so that the phase is always in opposition. (Fig.1)

Fig. 1

In fig. 1 a sine wave electromagnetic plane (in blue) travels in a loaded guide at the speed of light (or almost in the guides). Under these conditions it is as if it were propagating in space. The sine wave moves at speed and all phases with it (the opposite phases are represented with black and red arrows), because it is progressive. The wave will always be in phase opposition after half wavelength or its odd multiples. Even if it moves at the speed of light, being progressive. At a distance of λ / 2, or odd multiples, of the opposing diodes, welded on top of interrupted turns – see photo fig. 2 – reveal, one the positive half-wave and the other the negative. In the path, if there is no movement of the ether, the wave captured by the second probe remains the same as the first. The detector diodes will give an equal and opposite voltage, which, added and integrated by through capacitors,

But if the medium moves ( youtu.be ), the second diode will intercept a wave modified by the Doppler, so the phase will no longer be opposite, and the second half-wave will be either shorter or longer than the first. (fig.1-top right, second and third cases). By adding the two half-waves – the positive and the negative – and integrating the signal with two through capacitors – which bypass the radio frequency and release the two diodes from the distance – we will have a voltage proportional to the ratio between the two durations. That is, their different duration due to the wind speed. This is a phase comparison based on the different duration of the two intercepted half-waves, the starting one, and, at a distance, the second half-wave modified by the phase Doppler effect *.

(it is a Doppler of the wave fronts, being that it is the medium that moves between two fixed antennas hit by the wave that propagates at constant speed c which is composed with the wind of speed v).

 

Fig. 2

In fig. 2 the basic diagram of a device in which the wave injected by the antenna on the right (RF in) travels the guide, ending in a microwave absorbent which transforms it into heat. The wave in the guide is flat and progressive – because it does not come back – and behaves as in open space. This device measures 1st order Doppler! 

Fig. 3 

In fig. 3: Above – the wave that propagates in the middle in quiet – therefore in the absence of Doppler: – the positive half-wave is equal to the negative (on the right). The sum of the two half-waves, integrated by through-capacitors, will always be zero. And this is what occurs in the horizontal plane . Below the same wave that propagates in the moving medium – therefore deformed by the Doppler effect – for which (on the right) the positive half-wave will be different from the negative. And that’s what occurs when you rotate the device in the vertical plane . integrated sum of the two half-waves will give a PROPORTIONAL voltage to the speed .

Mechanical realization

Fig. 4

In fig. 4 the plate containing the two interceptor loops, in this case 3 λ / 2., Inserted along one side of the guide. Experiments with this device are visible at the following addresses:

1.youtu.be 2.youtu.be 3.youtu.be 4.youtu.be 5.youtu.be  6.youtu.be

 

Measurement with standing waves

Premise – Stationary wave is a wave that goes left and right, or up and down, infinitely. The two half-waves that make up a standing wave contained in a cavity or line travel in the opposite direction. The one is positive the other negative. And they are easily separable with two diodes placed at the ends. Let S be the length of the cavity, c the propagation speed, v the wind speed, T the period, f the frequency = 1 / T, λ the wavelength, i.e. cT. A half-wave is obviously λ / 2 and lasting half a period, or T / 2.

If the medium is at rest, they remain equal, so their sum will be zero. Experimentally I measure that, by tilting the device, there is a positive voltage upwards and a negative voltage downwards (or vice versa according to the arrangement of the diodes).

However, when it goes up it becomes λ / 2 (1-c / v), because it goes against the wind v
and when it goes down it becomes λ / 2 (1 + c / v), because with favorable wind.

By definition λ = cT, so substituting,
when it goes up will be λ ‘/ 2 = cT / 2 (1-c / v),
and when it goes down λ “/ 2 = cT / 2 (1 + c / v)

But if λ varies, the times will also vary. The period T is always constant and composed of the sum of the half-periods:
the half-period of the rising half-wave λ ‘/ 2 will be t’ = T / 2 (1-c / v), therefore shorter and that of the falling half-wave λ ” / 2 will be t ”= T / 2 (1 + c / v), therefore longer.

Distributed constant phase discriminators are interferometers

In the sense that in the space traveled the wave suffers the effect of the wind, that is, the wave fronts compress or expand. (which does not happen in concentrated constant discriminators). So the half-waves traveling in the opposite direction are equal without the wind, but with the wind no.

Fig. 5

In Fig. 5 A resonant cavity device operating on these principles.

 

Fig. 6

 

In fig. 6 inside a cavity made in a box. The wave is introduced in the center with a loop and taken at the ends with two turns connected to two diodes placed in opposition; these are connected to pass-through capacitors, which bring out from the box the continuous revealed proportional to the diversity of the two half-periods, that is to the wind of the ether. Discrimination occurs, as in the previous case, on the basis of the different duration of the two half-periods .

The experiment is visible on: youtu.be . In it a light box is fixed to the generator only with the union, therefore slightly subject to the deformation of gravity. This distorts the reading of the phase variation. In order to avoid it, I then cemented it externally and fixed it on the side of the generator. I measured the speed which is about 1 Km / s (against the 2 Km / s of the hanging box): youtu.be

Phase bridge with distributed constants

The concept is the same as that with concentrated constants (fig. 7)

Fig. 7

And in the constant version distributed in a cavity, using a coaxial cable to phase out 90 ° (fig. 8)

Fig. 8

The wave is input from the central loop and arrives at the two opposite loops simultaneously. The 90 ° phase shift is made by the length of the coaxial cable that carries the wave of the left loop to the center of the right loop, which has at its ends the two discriminating diodes in opposition. In order to be 90 ° out of phase, the cable must be λ / 4 or odd multiples. Obviously, being the cavity λ / 2, or multiples, the cable will be of different λ / 4, also taking into account the phase velocity. The wave of the left loop travels the length of the cable, which modifies the λ causing the Heaviside eolotropy): thus the discriminator will give a + or – signal according to whether the device is directed upwards or downwards. In the absence of wind the phase discriminator will give a zero. This discriminator proved by far the most sensitive. In any sense, alas, starting with gravitational deformations, so you have to stiffen it in a concrete range.

Interferences:
Introduction

I had already experimentally noticed a relationship between propagation speed and static magnetic and electric fields. Putting a magnet close to a guide, or to a line, unbalances the phase bridge. It is also unbalanced by introducing an electrical voltage into a cavity. This is because the wavelength varies and this because the speed varies. A Doppler provoked by both fields !! This also reveals that the two fields move the ether. There is therefore a direct relationship between static electric and magnetic fields with the velocity of the ether .

This is the premise to understand the phenomenon that I describe.

Indirect demonstration of the existence and vertical movement of the ether!

Well: telegraphs transmitted in kilometric waves MODULATE the phase of the centimeter waves which, generated locally, both in cavities and in coaxial cables! Not believing possible, I tried to modify the λ in the device in the laboratory by superimposing a powerful electromagnet powered by the 50 Hz mains: nothing! the phenomenon does not occur! An extraordinary “Luxembourg effect” , not as an amplitude intermodulation, but as a phase intermodulation between very long waves and microwaves.

This phenomenon is only detectable with constant discriminators distributed in a microwave. No other instrument can be seen. So far nobody has noticed.

If the ether were immobile this would not happen. It must move from above in order to bring the information inside the devices, although well shielded.

And the discriminators reveal these telegraphs along with Heaviside’s eolotropy *! Evidently the interference occurs in the outer space. The ether must move with long waves, arriving already modulated before penetrating the devices. Therefore the ether arrives modulated in speed inside the cavities and on the cables, and alters – due to the Doppler effect – the wavelength of the microwave; for which the telegraphic signal is discriminated. I therefore came to the conclusion that kilometric waves act on the velocity of the ether falling.

This is due to the enormous transmitted powers (even megaWatt!); then if stationary waves are created between the Earth and the reflective layer, the fields in the womb multiply in intensity. For the long wave to become stationary vertically between Earth and Layer E, the frequency must be such that in the 60 km of height of the layer the wave is λ / 2 or multiple;
– 2500 Hertz, which would have a belly at 30 km, and multiples
– on the 2nd harmonic at 5 KHz, with fans at 15 and 30Km,
– on the 3rd harmonic 7.5 KHz at 7.5 Km, 15 Km, 22, 5 Km, 30 Km, 45 Km.

(a very powerful station transmits at only 50 Hz! One at about 1 KHz, another at 8.3 KHz, another at 33 KHz … yet another at 330 KHz … all transmitted telegraphs enter my devices!)

This is the demonstration that it is the ether in space that is modulated in speed

* Eolotropy “, (not in dictionaries) is anisotropy in matter, due to the wind of the ether. It is thanks to this brilliant intuition of Heaviside that my interferometers work.
** Heaviside layer, (the name given to this layer is the only acknowledgment by the thankless scientific community for its enormous contribution to telecommunications) is the ionized layer responsible for the propagation of long radio waves beyond the horizon, worldwide.

Impact on gravity

If the ether is the reference of the fields, as claimed by Maxwell, then the electric and magnetic fields move with it; therefore the atoms of the bodies, immersed in electromagnetic fields, would be pushed down. As a moving magnet drags magnetic materials and a moving electret drags the dielectrics, the two moving fields would drag all the bodies. So gravity would be nothing more than the pressure exerted on the bodies by the moving ether. This is what Robert J. Distinti predicted in his ng.pdf

I hypothesize that it is the swirling movement of the ether that rotates the Earth, the planets, the galaxies and the whole Universe

That is, it is not the ether that is “attracted” to gravity, but it is itself the cause of gravity. Its motion is swirling, and the shape of spiral galaxies may depend on this motion.

ARTICLE SOURCE: http://www.altrogiornale.org/fabio-mosca-letere-verticale-rivelato/

copyright Moscow Fabio
Fabio Mosca is on Energeticambiente.it : Fabio Moscow
Energeticambiente.it Discussion on: “Measurement of the ether via radio waves”
Email to contact Fabio Moscow: fa.mosca@yahoo.it

The ether and Discovery Explanation Of Gravity (c) Property Fabio Moscow by D.Domenico