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The Origin of Gravity
The acceleration of a free falling particle is caused by the refraction of its
2 Bending of a Light Beam Passing a Massive Object
where c
is the speed of light in the gravitation-free space, cred is the reduced speed of light in the field, G is the
gravitational constant; M is the mass of the source, which is traditionally said to cause the gravitational potential; r is
the distance to the centre of the gravitational source. The power p is
1/2
or 1 depending on the direction of motion
in respect to the centre of gravity; that means it is 1 for the radial direction and
1/2
for the tangential one. |
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The deflection of a light beam passing the sun was correctly given for the first time by Albert Einstein. He predicted
the gravitational acceleration of the photon to be twice the value of the Newtonian acceleration (as it was for the first
time predicted by von Soldner in 1801). This was historically taken as an important proof of Einstein’s concept of
a 4-dimensional curved space-time. We will, however, see that Einstein’s concept is not necessary to achieve this
result. A calculation, which is based on the classical assumption of refraction, yields the same result. | |||||||||||||||||||
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(2.2) |
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Then taking into account the dependency of the reduction of c from x and y, which follows in a somewhat complex way from equations (2.1) and (2.2), we get |
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(2.3) |
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Here we suppose that the deflection is small (i.e. α < <1, so (x,y) describes an almost straight line).
We can then determine the differential deflection angle dα by applying the classical refraction mechanism: |
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If we now replace in eq. (2.4) r and x by ϑ, the angle between the direction of the vertex of the path (i.e. the closest position to the sun), and y by d, then we get |
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(2.6) |
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| The equation (2.6) integrated over dϑ from ϑ = -π/2 to ϑ = π/2 yields | |||||||||||||||||||
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(2.7) |
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- G
= 6.674 ·
10-11 m3 kg-1 s-2 |
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we get, after converting to angular units, the correct result of |
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1.75 arc-sec . |
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This corresponds to twice the normal gravitational acceleration (Newton) and conforms to the observation. This
numerical result as well as the analytical result (2.7) conform also to the prediction of general relativity – however
without any use of general relativity.
2.2 The Acceleration
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(2.8) |
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(2.9) |
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Now using (2.4): |
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(2.10) |
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(2.11) | ||||||||||||||||||
| which is the Newtonian acceleration. | |||||||||||||||||||
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From the dynamic parameters of an elementary particle, its spin and its magnetic moment, and also from its relativistic behaviour it follows that a particle is built by sub-particles, called here 'basic particles', which orbit each other at the speed or light c as shown in figure 3.1. |
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![]() Figure 3.1: Basic Particle Model |
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This structure was in
principle already detected in 1930 by Erwin Schrödinger, when he
analysed the Dirac function of the electron and found, that there must
be a permanent internal oscillation at the speed of light c, which he
called in German "Zitterbewegung" ("ZBW"). The Basic Particle Model assumes that this structure is valid for all leptons and also for all quarks
3.2 Conditions for the Refraction of an Elementary Particle 3.3 Gravity for an Object at Rest
3.3.1 Gravitational Acceleration in a Special Orientation |
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Figure 3.2 shows the accelerated motion downwards. Please note that here only the path of one of the two basic
particles is shown to keep the drawing simple. In this case the acceleration of the (composed) elementary particle is similar to the acceleration given in equation (2.11) |
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(3.1) | ||||||||||||||||||
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which is again the Newtonian acceleration.
3.3.2 Gravitational
Acceleration in Arbitrary Orientations |
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Figure
3.3: General orientation of a particle |
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In this case only the projection of the refraction into the vertical direction is effective for gravity. This means on the one hand, that the gravitational acceleration is reduced compared to the case above. But, on the other hand, the effect of reduction is compensated by the increase of refraction for the vertical component as it is visible in eq. (2.10), i.e. the term with a factor of 3. So, also in the case of an arbitrary orientation of the elementary particle we can get the result eq (3.1) |
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which is
the well known result for the classical case (Newton). 4 The Equivalence Principle
4.1 Equivalence Classically |
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4.2 Equivalence Based on the Particle Model If we look to the figure 3.2, it is obvious that the deflection of the path of the basic particles is independent of the radius of the particle and, because of the particle model used here, independent of the mass of the particle. So it has a very natural cause that the gravitational acceleration is independent of the mass. No assumptions about any equivalence are needed. Figure 3.2 shows, why an elementary particle at rest is subject to a gravitational acceleration. It is in fact gravitational lensing on a micro-scale. This is the physical cause that the gravitational acceleration is independent of the mass of an object. |
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(5.1) | ||||||||||||||||||
| Here t is the time in the system at rest, and τ describes the development of temporal processes in the system at motion. This equation is now derived with respect to dt and then squared and reordered: | |||||||||||||||||||
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(5.2) | ||||||||||||||||||
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In a gravitational field this time behaviour changes. The understanding of this change directly guides us to
the Schwarzschild solution.
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(5.3) | ||||||||||||||||||
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where vrad and vtan denote the radial und the tangential component of the speed respectively in relation to the centre of the gravitational source. Now we have to take into account that c changes in a gravitational field in the following way according to (2.1): |
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where p is
1/2
or 1 depending on the direction of motion in respect to the centre
of gravity. Further the size of the elementary particles changes in the gravitational field as a consequence of the change of the speed of light c in the field. By taking into account this fact when using eq.(5.3) we get – as deduced in detail in the appendix B: |
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(5.4) | ||||||||||||||||||
| It is usual to abbreviate the equations by using the common definition for the so-called Schwarzschild radius rs | |||||||||||||||||||
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(5.5) | ||||||||||||||||||
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(5.6) | ||||||||||||||||||
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which is a popular form of the Schwarzschild solution.
A detailed deduction is given in appendix B of the pdf-version.
6.1 Varying Speed of Light |
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According to the Basic Particle Model, the field of every basic particle is built by a similar collection of elementary charges (of the strong field), and it is so independent of the type of the elementary particle, to which the basic particle belongs. And so also the flow of exchange particles is independent of the type of the particle. Consequently also the reduction of c and so the gravitational effect is independent of the particle, which means that it is independent of the size and consequently independent of the mass of the elementary particle. Every elementary particle provides the same contribution to the gravitational field. This understanding is in contrast to the conventional physics, but it helps to overcome the principle problems of present gravitational physics.. Remark: There is an apparent conflict here to the fact that the forces within an elementary particle in the binding function have a limited range. This seems not to conform with the unlimited range of the effect of gravity. The solution is that the binding field is set up as a multi-pole field by a composition of monopole charges of the strong force. The exchange particles of those monopole charges, which cause the disturbance of the path of a light-like particle, have an unlimited range as we know it similarly about electric charges. 6.2 Speed Reduction in Detail |
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(6.1) | ||||||||||||||||||
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as this is a crossway disturbance of the path. In the radial direction it is |
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(6.2) | ||||||||||||||||||
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which is greater than in the former case as it is a longitudinal disturbance of the path. The effective amount of the influence onto the speed depends on two facts
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(6.3) | ||||||||||||||||||
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where again p=1 for radial motion and p=1/2
for tangential motion.
Further the binding field in an elementary particle and so the size of any objects in a gravitational field is given by the equation |
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We have used here
N to denote the number of elementary particles causing the gravitational field to reflect the fact that this influence is independent of the mass of a particle. And so we have to use a different gravitational constant denoted here as
g.
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7 Present Problems of Gravity
7.1 The "Dark Matter" Phenomenon Some decades ago it was detected that the rotational speed within and around big galaxies is in conflict with the equilibrium speed determined on the basis of standard gravity. Figure 7.1 shows the discrepancy for the galaxy NGC 3198. |
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Figure 7.1:
Equilibrium conflict at the galaxy NGC 3198
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The solid (green) curve labelled "disk" is the rotational speed dependent from the radius as a result of a normal gravitational calculation. The uppermost single values are measurements of the real speed; a curve (also solid, black) is fitted through these measurements. The medium solid (blue) line labelled "halo" describes the required distribution of the assumed "Dark Matter" in order to explain the measured values. The red dotted line, which is very close to the "halo" curve, follows from the assumption described above, that every elementary particle contributes equally to the gravitational field. It is the contribution of light particles (i.e. neutrinos and photons). In the drawing the height of this line was chosen to fit into the needs of this diagram, but it fits within a tolerance of a factor 2-3 to the assumed data; its curvature, however, is given by the natural distribution of the light particles and is not parameterised. Of the light particles mentioned, the photons are mainly generated by the hot, shining stars in the centre of the galaxy. The neutrinos are similarly generated by the nuclear processes within the stars, the sources of which are also mostly in or close to the centre of the galaxy. These particles build a continuous flow off the centre with the speed of light c (or almost this speed). This flow causes their spatial distribution to be |
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| where r is the distance to the centre of the galaxy. The number of particles N within a sphere up to a radius r0 is then | |||||||||||||||||||
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| The acceleration a in the gravitational field towards the centre is (r0 here renamed r) | |||||||||||||||||||
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| The centrifugal acceleration on the other hand is | |||||||||||||||||||
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In order to keep both accelerations in a balance, it follows for the orbital speed v that |
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This is
the reason for the curvature of the red dotted line in figure 7.1, and
so it provides the contribution to the gravitational field, which is
elsewhere assigned to the so called "Dark Matter".
8 Conclusion
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1. The weakness of this
effect (which is primarily not a force) The investigation of the cause of the related processes explains
1.The
phenomenon called Dark Matter
The
related understanding of relativity in general solves the apparent
problem of Dark Energy in a very easy - and physical - way.
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NOTE: The concept of the Basic Model of Matter was presented initially at the Spring Conference of the
German Physical Society (Deutsche Physikalische Gesellschaft) on 24
March 2000 in Dresden by Albrecht Giese. |
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Comments are welcome. 2010-07-01 |
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Appendices
Can be found in the
pdf-Version. |
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