The polarization of light and the cólor velocities

The light polarization and cólor velocities

So far, we have always described the photon that moves over a plane xz. Nevertheless, each photon moves over a plane xz’ creating generic angles q when related to plane xz. Thus, among the various photons of a light ray, if we choose, through a filter, just the ones that have the same axle q ,we would be doing the light polarization in a laboratory.


Cólor´s velocity U on the same direction of the photon translation (x axle)

c = photon translation velocity viewed by an observer on the source as a reference, in the other words, at a rest state when related to the photon.

v = colores´s tangential velocity A and B in the orbit around their gravity center.

u = projection of the velocity v over axle, where u = v x cos a.

U = c + u, that represents the cólor´s translation velocity over axle x.

The cólor´s arrival at a shield.

One color on a surface xz arrives at a shield with a length P1P2 that is equal to the photon’s diameter, arriving at a generic position P with velocity U, where U varies from c – v to c + v, when it arrives at a shield on the positions P2e P1 ,respectively.

The science knows that the light works as both wave and particle, according to their practical results. However, it does not know the process to obtain this performance. Being very simple, to consider that photon is composed of two cólores, Logics Deductions can explain the reason why the light is waves and particles at the same time. To confirm the consistency of this simple argument, it explains the reason why the violet cólor, with maximum velocity c + v, due to it arrives at a metal plate with a higher velocity and, therefore with more energy, what does not happen with a red light (c – v), it can pull off one electron from this metallic plate, it explains clearly, as it was not done by the science yet, the photoelectric effect.

Electromagnetic wave

It exists two identical electromagnetic waves related to the type A and B cólores for each photon that have a phase’s difference between them of 180º.

- Wave length l = 5,02 x 10-7 m (constant), equal to l of the linear wave.

Velocity of the colores on the emission

Velocity of the cólores on the arrival

The length wave l is the distance between two cólores of the same type, which have the same polarization to both observer on the light source and observer on receiver.

The cólor´s velocity is U, on its emission U = c + u, where U varies from c – v to c + v.

On the arrival to the receiver:

U = c1 + u

Altering from c1 – v to c1 + v,

being

U = v cos a,
c1 = c – Va,

where a is the angle created between the tangential´s velocity direction v and the photon´s translation direction.

The emission´s frequency f

f = U/ l

The arrival’s frequency f’

f’ = U/l

We must remember that de length’s wave l of an electromagnetic wave is not as Science defines when we consider the distance between the valleys of the same wave.

Wave’s length measure’s made by physicist.

The physicists, to measure the wave’s length of a light ray that arrives at a galaxy, makes it pass through a split and then through a diffraction grating, conducting the photons of this light ray to different directions according to the various diffraction angles, that varies according to the wave’s length of each photon. Thus, they obtain many specters of this light ray, supplying the atoms characteristics of chemical elements that created this ray.

 

Iron’s spectroscopy to the arrival of the light ray

Iron’s spectroscopy at rest state in laboratory

If we know the values of l’ and l, we are able to calculate the redshift Z of this light ray, where

,

If we have the Z value, finally, we obtain the deviation’s velocity value Va of the galaxy that emitted the light ray, through the formula:

,

To physicists, the light way is composed of a great number of photons; each one of them has a frequency and wave length intrinsic, walking on the same velocity c.
Thus, through the formula =c/ lf, they calculate the frequency of each one of these photons, considering that the velocity of all photons is constant and equal to c.

Through the light emitted by galaxies, considering the constant velocity c, physicists modifies the length’s wave of this light and consequently its frequency f through the formula f= c/ l.

Through the wave’s length l e l’ obtained from a spectroscopy of an element to a light ray that arrives from some galaxy and the same element at a rest state in a laboratory, and through the formula

c= lf,

we obtain the frequencies f’ e f . Thus, using these values in the Doppler effect formula:

,

they obtain, in another way, the deviation’s velocity value Va of the light source emitter.

Actually, what happens on fact is that, on the linear wave of the photons, they always arrive with the same wave’s length l, but with velocity c1 = c – Va, where Va is given according to the deviation’s velocity of the source.

To the source on the earth as a reference point, which deviation’s velocities are insignificant when compared to the light velocity, we will have Va = 0 and therefore c1 = c. Thus, we can use the formula of the undulatory physics v = l f, so we will get v = c and then, we will acquire c = l f, it is valid for the light emitted from all sources that have Va » 0.
In case of the light emitted from galaxies whose deviation’s velocities are significant, with values altering to those very close to c, we will have c1 = l f’, and as l is always constant, so the frequency f’ of the light’s arrival varies according to the arrival velocity c1 of the photons.
In case of the colores´ wave, we will use the same spectrographic results, giving another interpretation, as it is shown:
What the physicists interpret as photon is actually a cólor of this photon. Each cólor arrives at a diffraction grating with a velocity U=c1+u, varying from c1 - v to c1 + v and having its direction changed in the diffraction grating according to the arrival’s velocity of the color and the refraction law. Each one of these angles will define a wave’s length and consequently a frequency, according to what physicists had already set up. Briefly, physicists think that a light ray is composed of photons that always have the same constant velocity c, varying their wave’s length with its frequency; but, actually, photon’s velocities vary with the deviation’s velocities of their sources, we know that physicists don not detect photons, but their cólores, which are represented by waves which translations velocities vary from c1 – v to c1 + v.
As the wave length is the spacing between two photons of the same polarization or between two waves of cólor, being always constant, so, for each cólor’s velocity that varies between c1 – v and c1 + v, we will have an arrival frequency f’ given by the formula f’ = c1/l.
We can conclude that, although the mathematics formality used by the physicist is correct, the interpretation needs to be revaluated as it follows:
Instead of considering that the light is composed of different photons, each one with different wave’s length and frequency, we must consider that light is composed of identical photons, each one composed of two equal cólores that arrives at a spectrograph as an electromagnetic wave with different velocities, creating different angles in the diffraction grating according to refraction law. As the wave’s cólores always have the same length wave l ,we will obtain all specter frequencies of the visible light, through the formula

,

 

Where

f’ = light arrival’s frequency;
l = wave length, that is always Constant;
U =velocity of the cólor arrival, being U = c1 + u;
c1 = velocity of photon arrival = c - Va, where
u = v cos a, where
v = orbital velocity of the cólor, and
a = the angle created between the velocity direction v and the direction x of the photon´s translation.

We can consider the value l of that one that physicists calculate for the solar light case, since that we can think the deviation’s velocity of the sun is around zero, it means that Va » 0

To Va = 0, according to Logic Deductions, we have:

c1 = c - Va,

thus,

c1 = c.

On the linear wave, we will have c1 = lf. In case of the solar light, where Va = 0, we will have

c = lf,

that is the same formula as undulatory physic, that provides the value of l and f, being

l = 5,02 x 10-7 m,
f = 5,976096 x 1014 Hz.

Thus, as we have the value of l stationaried, the velocity of c1 varies only according to the frequency variation.

Deduction logics consistence with classic physic data

In order to confirm the consistence of what it has been saying, we will analyze the example as it shown:

The galaxy CLASXS 509 has a redshift Z= 1,016 according to astronomic datas.

For this value of Z, the science calculates the deviation velocity by the formula:

 

.

 

Thus:

,

 

Va = 0,605075257.

 

We know that photons are always emitted with the same frequency f and the same length’s wave l, which values are:

f = 5,976096 x 10s14 Hz,
l = 5,02 x 10-7 m,

and that the translation’s velocity of the photon is always c =1 to the observer on his source so, we can calculate the arrival frequency f’ of the light ray of this galaxy, applying the Doppler effect’s formula, where:

.

Thus, we calculate

f’ = 5,976096 x 1014 x (1 – 0,6057075257)
f’ = 2,360108 x 1014 Hz

As we know the value of Va and f’ of the light ray of the galaxy CLASX 509, Logic Deductions can calculate the real c1 velocity that photons emitted from this galaxy arrive at us, in two ways, as it follows:

First: Considering the influence of Va velocity over these photons velocities,

c1 = c – Va,
c1 = 1 – 0,605075257,
c1 = 0,3949247436.

Second: Using the formula of undulatory physic v=lf’ we will have:

v = 5,02 x 10-7 x 2,360108 x 1014;
v = 0,39492477.

Through the results obtained above, we can observe that c1 = v, it show us the consistence of Deduction Logics´ assertion, it means c1 = c – Va, with the formula of undulatory physics v = lf’.
The internauta can verify that this consistence is given for any galaxy.