## 438(1): Orbit Around a Pseudoinfinite Mass in m Theory

438(1): Orbit Around a Pseudoinfinite Mass in m Theory

Many thanks, this is exactly what is required, graphing the effect of an increasing central mass. The complete m theory orbit equations were used in UFT419 with the S2 star. They were also used in UFT416 and UFT417 to produce very interesting results. So we just have to increase the central mass M in that code to as large a value as the computer can take. The Newtonian limit is fully analytical and will show the characteristics of the dark star, named by Michell in 1783. The complete equations (7) and (8) can be developed in several ways, for example by using a static m(r) to begin with, then repeating the method you suggest in the Newtonian limit. Finally the complete equations can be used with a finite dm(r) /dr and m(r) with various models. These are all well read papers so it is well known that all claims about dark holes completely ignore modern scholarship. It is well known that they ignore scholarship, so their claims are immediately rejected. The astronomical data probably indicate the existence of a Newtonian dark star modified by m theory. The complete equations (7) and (8) can be analyzed in many ways, some of this work has already been done in UFT416 ff.

438(1): Orbit Around a Pseudoinfinite Mass in m Theory

In which paper exactly did we use eqs.(7-8)? I will reactivate the calculation.

I think besides the mass m the intital conditions should be kept the same so that we see the impact of changing M. We will have to rescale the orbits because they shrink to zero.

Horst

Am 22.04.2019 um 10:50 schrieb Myron Evans:

438(1): Orbit Around a Pseudoinfinite Mass in m Theory

This is a development of UFT419, the orbit equations of m theory being the richly structured Eqs. (7) and (8) which can produce any observable orbit. Note carefully that they are not based on the Einstein field equation. In the Newtonian limit they reduce to the well known equations (9) and (10), which give conic section orbits (11). It is shown that if the central mass becomes infinite in the Newtonian limit, the orbit shrinks to a point of infinite mass density, the half right latitude approaches zero, the eccentricity approach 1, and the orbital velocity approaches infinity. A photon of mass m is captured by the pseudoinfinite M, and can never escape, because its escape velocity (26) must be infinite. All the characteristics of this type of orbit can be graphed in various ways. The area around the infinite mass will look completely dark, because all the photons have been captured. These graphics will probably reproduce the object claimed by standard model propaganda to be a "dark hole". The use of the complete m theory will produce a large amount of other information. However Newtonian dynamics can explain the so called "dark hole" photograph. The use of Newtonian graphics will show that "black hole" theory can be explained almost completely without using event horizons. In fact this was Hawking’s last thoughts on the subject. So the computer graphics could illustrate what happens to a Newtonian orbit as the central mass approaches infinity. Animations would be even better. There are no "black holes" because they are inferred from an incorrect geometry, the 1902 second Bianchi identity. The correct second Bianchi identity is the JCE identity of UFT88 to UFT313. Crothers, Robitaille and many others including Einstein and Hawking have argued against black holes.

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