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Finshed Bivector Theory Of Gravity


Dubbelosix

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I took it upon myself to write a new post since my last one has been spammed. It's hard to follow when you have a poster, posting things with no relevance to the post.

 

This formulation is much better than the one I chose, which involved replacing a metric term in the Einstein equation with a bivector, instead, we retrieve the Einstein equations in a natural way and forms a more acceptable approach.

 

https://bivector.quora.com/Bivector-Gravity

 

The main equation we derived in this work is;

 

[math]\mathbf{G}_{\mu \nu} = \frac{8 \pi G}{c^4}\mathbf{T}_{\mu \nu} = \partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

To see how we arrive at this equation, follow the link above.

Edited by Dubbelosix
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  Wiki does a better description of bivectors than in your paper https://en.wikipedia.org/wiki/Bivector 

 

You have a conclusion at last:) which can be discussed at a higher level   :sherlock: (Mordred) :) . I hope my prods (unwelcome comments (talking(taking) piss)) did not hurt too much  :innocent:

 

Is there anything you would like to discuss ???

 

I'm always constructing the theories I present for further conversation, for instance, I'll be discussing why from the equations how the four dimensional curl of the Einstein tensor will reveal physics that are pretty much identical to the conservation of the 4-current - and then I'll be discussing further why this model implements torsion in a natural way, and unique in a sense, from the mathematical description usually presented through the Einstein-Cartan model.

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So let's start that discussion. The four dimensional wave equation acting on the Einstein tensor reveals:

 

[math]\Box G_{\mu \nu} = \partial^{\mu} \partial_{\mu} \cdot T_{\mu \nu} = \partial^{\mu}\partial_{\mu} (\partial_{\mu} \cdot \mathbf{D}_{\nu}) + i \sigma \partial^{\mu}\partial_{\mu} (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

Because the d'Alembertian (wave operator) is squared in its derivatives, the total dimensions yields [math]1/length^4[/math] and when we define the gravitational 4-current which is conserved:

 

[math]\nabla^{\mu} \nabla^{\nu} \phi_{\mu \nu} = \nabla^{\mu} \partial_{\mu} \cdot \nabla^{\nu} \mathbf{D}_{\nu} + i \sigma (\nabla^{\mu} \Gamma_{\mu} \times \nabla^{\nu} \mathbf{D}_{\nu}) = \frac{4 \pi G}{c^2}\nabla^{\mu \nu}\mathbf{J}_{\mu \nu} = -\mathbf{R}^{\mu \nu} \phi_{\mu \nu}[/math]

 

This means maybe the continuity relationship holds (?):

 

[math]\Box G_{\mu \nu} = \partial^{\mu}\partial_{\mu} \phi_{\mu \nu} = 0[/math]

 

The torsion naturally arises from the second term in the main equation from the geometric algebra:

 

[math]i \sigma \partial^{\mu}\partial_{\mu} (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

Where torsion arises from the cross product term

 

[math]-\Gamma_{\mu} \times \mathbf{D}_{\nu} = \frac{\partial \Omega}{\partial t}[/math]

 

Making it satisfy the full Poincare group.

Edited by Dubbelosix
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So let's start that discussion. The four dimensional wave equation acting on the Einstein tensor reveals:

 

[math]\Box G_{\mu \nu} = \partial^{\mu} \partial_{\mu} \cdot T_{\mu \nu} = \partial^{\mu}\partial_{\mu} (\partial_{\mu} \cdot \mathbf{D}_{\nu}) + i \sigma \partial^{\mu}\partial_{\mu} (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

Because the d'Alembertian (wave operator) is squared in its derivatives, the total dimensions yields [math]1/length^4[/math] and when we define the gravitational 4-current which is conserved:

 

[math]\nabla^{\mu} \nabla^{\nu} \phi_{\mu \nu} = \nabla^{\mu} \partial_{\mu} \cdot \nabla^{\nu} \mathbf{D}_{\nu} + i \sigma (\nabla^{\mu} \Gamma_{\mu} \times \nabla^{\nu} \mathbf{D}_{\nu}) = \frac{4 \pi G}{c^2}\nabla^{\mu \nu}\mathbf{J}_{\mu \nu} = -\mathbf{R}^{\mu \nu} \phi_{\mu \nu}[/math]

 

This means maybe the continuity relationship holds (?):

 

[math]\Box G_{\mu \nu} = \partial^{\mu}\partial_{\mu} \phi_{\mu \nu} = 0[/math]

 

The torsion naturally arises from the second term in the main equation from the geometric algebra:

 

[math]i \sigma \partial^{\mu}\partial_{\mu} (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

Where torsion arises from the cross product term

 

[math]-\Gamma_{\mu} \times \mathbf{D}_{\nu} = \frac{\partial \Omega}{\partial t}[/math]

 

Making it satisfy the full Poincare group.

 

 

As I normally do, I look for different variations from the theory, here we distribute a derivative through the equation and we change the order of the cross product

 

 

[math]\partial \mathbf{T}_{\nu} = \partial^{\mu} \mathbf{T}_{\mu \nu} =  \partial^{\mu} [\partial_{\mu} \cdot \mathbf{D}_{\nu} - i \sigma g_{\mu \nu}  \frac{\partial \Omega}{\partial t}][/math]

 

 

 

[math] =  \Box \cdot \mathbf{D}_{\nu} - i \sigma g_{\mu \nu} \partial^{\mu}  \frac{\partial \Omega}{\partial t}[/math]

 

 

(note to self, investigate a matter-density as the field varies four dimensionally:

 

[math]\Box \phi = \rho[/math]

 

only this time treat the derivative: [math]D[/math] as a scalar instead)

Edited by Dubbelosix
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[math]\mathbf{G}_{\mu \nu} = \frac{8 \pi G}{c^4}\mathbf{T}_{\mu \nu} = \partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma_{\mu} \times \mathbf{D}_{\nu})[/math]

 

A nice equation can be obtained from the equation above: Working in natural units of [math]8 \pi G = c = 1[/math] and identifying [math]\mathbf{A}^{\mu \nu}[/math] as the inverse of the Einstein tensor, we have a description for the force related to the symmetric gravitational theory and the skew symmetric theory involving the torsion:

 

[math]\mathbf{F} = \mathbf{A}^{\mu \nu} \mathbf{T}_{\mu \nu} =  \mathbf{A}^{\mu \nu}[\partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma_{\mu} \times \mathbf{D}_{\nu})][/math]

 

What makes this slightly different is that [math]\mathbf{A}^{\mu \nu} \mathbf{T}_{\mu \nu}[/math] can be interpreted as the spacetime tension, which then relates the tension to the spacetime torsion additionally.

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[math]\Box = \partial^{\mu}\partial_{\mu}[/math]

[math]\Box  = \partial^{\mu} \partial_{\mu} + i (\sigma \partial^{\mu} \Gamma_{\mu})[/math]

 

[math]\Box \phi  = \partial^{\mu} \partial_{\mu}\phi + i (\sigma \partial^{\mu} \Gamma_{\mu} \phi) = \rho[/math]

 

Nordstrom derived a simpler version, but he argued the equation says matter depends on the gravitational field - but it is also inversely true that the gravitational field (curved spacetime) depends on the density of matter. So the relationship can be interpreted a few different ways.

 

[math]\mathbf{G}_{\mu \nu} = \frac{8 \pi G}{c^4} \mathbf{T}_{\mu \nu} = \partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma^{\mu} \times \mathbf{D}_{\nu})[/math]

 

[math]\mathbf{F} = \mathbf{A}^{\mu \nu} \mathbf{T}_{\mu \nu} =  \mathbf{A}^{\mu \nu}[\partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma_{\mu} \times \mathbf{D}_{\nu})][/math]

 

because

 

[math]\Box \phi = \frac{Gm}{r^3}[/math]

 

being edited:

Edited by Dubbelosix
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hey dubbelosix: may I ask a question:

 

why don't you try to publish at acceptable journals (especially reputable ones or at least indexed ones)

 

if you achieve that, I am almost sure that most of people including scientists will respect your ideas. 

 

but otherwise,you will likely continue to see insulting words everywhere ...

 

this is my honest advice.

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Why is force variable? Because [math]G[/math] is variable!

 

The Gravitational Aether and Diffraction of Gravity In A Dynamic Medium

 

If [math]G[/math] had not been variable in the coefficient (Planck force) then it would imply a tension constant; if the tension of spacetime requires dynamic components, this may not be an absolute truth within Einstein's equations - a dynamic tension should exist for a dynamic vacuum.

 

There are so many aether theories that fail, in my mind, this is the only one that makes sense. It is an extract from my essay, but before I post it, I want to quote Einstein, ''General Relativity is unthinkable without an aether.''

 

A Gravitational Aether

 

Excellent arguments exist now for the existence of the gravitational permittivity and permeability with the discovery of gravitational waves. The constancy of the speed of light only holds in a vacuum - but the density of gravitation varies between celestial objects and therefore the speed of light does technically vary.

 

In fact, authors Masanori Sato and Hiroki Sato in their paper ‘’Gravitational wave derived from fluid mechanics applied on the permittivity and the permeability of free space’’ suggests that gravitational waves are simply fluctuations of the medium, which appears as the product of the permittivity of free space and the permeability of free space. That is, the gravitational wave is an acoustic wave in the medium - the proposal shows how the phase velocity of the fluctuation relates to the speed of light [math]c = \frac{1}{\sqrt{\epsilon_G \mu_G}}[/math].

 

The model has some interesting consequences, first being that permittivity and permeability are allowed to vary. A second is that the speed of light is variable in gravitational fields. Another interesting property is that while both Newtonian mechanics and Einstein’s relativity theories predict the confinement of light by gravity, neither theory defines the escape velocity or the Schwarzschild radius; in fact, the actual speed of light can only approach zero but never reach it - so in effect light is allowed to escape from a black hole.

 

Let’s be clear about something - I do not believe that the thickness of space (the medium) is an aether made from any particle. In fact there cannot be any motion associated to this aether because it would violate the first principles of relativity. In fact you can argue as I have already done, that any true quantization of gravity would be at odds concerning how we actually think about the roles of pseudo forces. But then physics tends to throw uncertainties into the mix, what if it was possible to violate the third law? We will investigate this in the next part, but first an anomaly…

 

Many experiments have been performed to measure the value of the Newtonian G but has come up with varied results and up until this year another measurement has cast a shadow over settling why we keep measuring different values for the constant. Since in this aether theory I have chosen, both permittivity and permeability will depend on G ~

 

[math]\frac{1}{\epsilon_G} = 4 \pi G[/math]

 

[math]\frac{1}{\mu_G} = \frac{c^2}{4 \pi G}[/math]

 

This leaves open a question of whether the deviations in the value of G has something to do with variations spacetime permittivity and permeability. This particular theory of the aether, as a dynamical ''thickness'' of space due to varying gravitational density, the refractive index for radiation is proportional to [math]\sqrt{\epsilon_G \mu_G}[/math] (permittivity and permeaility) and is represented as:

 

[math]n = \sqrt{\frac{\epsilon_G \mu_G}{\epsilon_0 \mu_0}}[/math]

 

A high refractive index for the equation [math]\frac{1}{\sqrt{\epsilon_G \mu_G}}[/math] causes a low speed of light (such as found round strong gravitational fields of black holes). It has been argued in literature that the refractive index is more intuitive than curvature; this suggestion is probably quite true, since curvature is the presence of a dynamic metric but we know not what causes this ''dynamic feature'' other through the presence of matter - which is well-known to tell spacetime how to curve, but still doesn't explain why the dynamic phenomenon exists. In a sense, the gravitational explanation for a refractive index supposes a type of mechanical explanation to curvature.

 

I proposed that the Von Klitzing constant may be subject fundamentally to the permittivity and permeability of space:

 

[math]\frac{\mathbf{J}}{e^2} = \sqrt{\epsilon_G \mu_G}[/math]

 

How to make any sense from this hypothesis so far as shown to be difficult.

Edited by Dubbelosix
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[math]\Box = \partial^{\mu}\partial_{\mu}[/math]

 

[math]\Box  = \partial^{\mu} \partial_{\mu} + i (\sigma \partial^{\mu} \Gamma_{\mu})[/math]

 

[math]\Box \phi  = \partial^{\mu} \partial_{\mu}\phi + i (\sigma \partial^{\mu} \Gamma_{\mu} \phi) = \rho[/math]

 

Nordstrom derived a simpler version, but he argued the equation says matter depends on the gravitational field - but it is also inversely true that the gravitational field (curved spacetime) depends on the density of matter. So the relationship can be interpreted a few different ways.

 

[math]\mathbf{G}_{\mu \nu} = \frac{8 \pi G}{c^4} \mathbf{T}_{\mu \nu} = \partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma^{\mu} \times \mathbf{D}_{\nu})[/math]

 

[math]\mathbf{F} = \mathbf{A}^{\mu \nu} \mathbf{T}_{\mu \nu} =  \mathbf{A}^{\mu \nu}[\partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma_{\mu} \times \mathbf{D}_{\nu})][/math]

 

because

 

[math]\Box \phi = \frac{Gm}{r^3}[/math]

 

being edited:

 

There is also an identity from the main equation that can be obtained, known as the shear stress: A shear stress is when a fluid possesses a motion. In classical physics, this motion is often attributed to the particles which make up the fluid. Aside from zero point energy, there cannot be any particle associated to the vacuum fundamentally - in other words, unification attempts to describe say an aether made of particles, should be forbidden by principles of relativity. It is easy to argue from relativity that thiings like gravitons should probably not exist, due to gravity being strictly a pseudo force. It's not so easy to throw away the idea though that there is some ''particular aether'' associated to quantum mechanics, especially in light of field theory which involves the creation and annihilation of particles in the quantum realm. To say motion is forbidden from relativity, may be a harsh statement, so perhaps we can state:

 

1. There is no [detectable] motion can be associated to the aether field

 

That is 

 

2. Until we find evidence of particle creation and annihilation on scales much smaller than an atom. 

 

There is a lot of energy out there in the vacuum, in fact physics predicts the energy scale as  [math]10^{120}[/math] which is how many orders of magnitude in which exists the discrepancy: We do not measure this massive amount of energy, so where is it? Zero point energy is not observable, at least not yet - they are known as off shell particles, and in theory are treated in such a way that they are not described by Hermitian operators (which is the way to create ''observables'' in quantum theory) - off shell particles [are] virtual particles. Might it be there is no such discrepancy and dark energy is really off-shell zero point fluctuations? Why can we not measure this energy? The answer may be surprisingly simple - zero point fluctuations do not generally live long enough to interact with real matter in the vacuum so the presence of this energy is completely shielded from our experimental prowess. 

 

​In the case of shear stress of a vacuum and the idea of a spacetime tension, have to be gravitational features and analogues of quantum mechanical types. Viewing space like a fluid makes wonderful predicts, as our own cosmological physics is based primarily from derivations involving the ideal fluid solution which also gives rise to the continuity equation (time evolution) within the Friedmann model, something which general relativity ironically enough lacks. Some physicists have considered whether spacetime itself is a type of superfluid! When we say spacetime tension and shear stress have to be gravitational features, has a strong connection with the gravitational aether theory, in which not only is spacetime not nothing, but it predicts that the speed of light and the gravitational constant is variable. It even provides logical reasons out of the information paradox. 

 

The speed of light being variable, could very well be true, but we mean this variability in a different sense to thinking it varies without reason. Phenomenon like the Shapiro effect suggests that frame dragging makes light move a longer distance when traveling in the opposite direction of earths spin. In a similar stance, [we know] light does not always move at light speed in a general theory of relativity, in fact it strictly states in relativity, that light moves at c in an empty vacuum (ie when gravity is sufficiently weak) so it remains to be only a special case. However, gravity can affect the speed in which a photon moves, due to the thickness of space cause by a gravitational field - this is why light has to travel that extra bit more when coupling to the curvature of some source of gravity. Now... does a photon then still move at light speed? Of course, it probably does, but relative to someone outside the system watching this happen, would suggest spacetime is the medium and the speed of light varies proportional to the field strength. In gravitational aether theory, the speed of light can only approach zero speeds, therefore light cannot be bent in such a way that there is a point of no return, concerning black holes. It might take a photon billions of years to travel from inside the system and back out again, similar to how a combination of nuclear events and gravity prevents a photon from leaving the inner core of the sun and will take roughly 40,000 years to make its escape!

 

As for variability in Newton's so-called ''constant'' [math]G[/math] surely this is all just pseudoscience I hear you say perhaps? Well no, the implications of a varying [math]G[/math] have been speculated upon for a while, even back to Dirac's large number hypothesis. Historical attempts to measure the value of [math]G[/math] to current day has shown remarkable discrepancies, that vary on either spectrum. 

 

It has been argued that a black hole cannot contain a surface tension because it is ''not a thing,'' - that the area boundary of a black hole is not special in the sense it should have a tension, but this depends on the way you might view this. Certainly in analogy, you could theoretically place something on the boundary - and even though this is not about inter-molecular bonds in the way of Van der Waals forces, this does have something to do with the dynamic feature of spacetime itself. Just like placing an object with some surface on water taking extra force to remove it due to the waters surface tension, there is also a force pulling on the system that has touched the event horizon - and so additional force theoretically would be needed to ''pull it out,'' if such a thing could even be possible. I see this as an analogue to a type of spacetime tension. All we need to do, is think of spacetime, not only as a fluid, but a special fluid that varies around massive bodies, like planets, stars and black holes due to the presence of gravity.

 

Back to shear stress - as a I stated, shear stress arises from fluids that are in motion - the Ricci flow is the heat equation for a Riemannian manifold. It is a simple proposition, that curvature itself can flow and this remarkable feature allows a spacetime to take on fluid like features from nevertheless, a heat equation written in a form which uses gravitational physics with a usual diffusion constant. The Ricci flow of curvature should be the missing piece to explain the motion of a spacetime as if it were acting like a perfect fluid in motion. So how do we get the shear stress from the modified EFE? 

 

[math]\mathbf{G}_{\mu \nu} = \frac{8 \pi G}{c^4} \mathbf{T}_{\mu \nu} = \partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma^{\mu} \times \mathbf{D}_{\nu})[/math]

 

Well what we will find out is the shear stress must be related to the stress energy tensor as:

 

[math]\tau_{\mu \nu} = \frac{c^4}{8 \pi G} \mathbf{G}_{\mu \nu} =  \mathbf{T}_{\mu \nu} = \frac{c^4}{8 \pi G}[\partial_{\mu} \cdot \mathbf{D}_{\nu} + i \sigma \cdot (\Gamma^{\mu} \times \mathbf{D}_{\nu})][/math]

 

This has dimensions of force over area, which is the same dimensions for the shear stress. The relationship of sheer stress to the stress energy tensor has been well-known for a while, whether in this form or not, the stress energy tensor does contain off-diagonal elements which describes the sheer stress of a system from the momentum density tensor. 

 
The flux of relativistic mass across a surface is equivalent to the density of the i'th component of linear momentum,
 
[math]T^{0i} = T^{i0}[/math]
 
and the components
 
[math]T^{ik}[/math]
 
represents the flux of linear momentum and the remaining component after [math]T^{ii}[/math] which represents the pressure, then
 
[math]T^{ik}[/math]
 
represents the shear stress. Knowing this we can write it under standard convention:

 

[math]g_{ik} \tau = \frac{c^4}{8 \pi G} \mathbf{G}_{i k} =  \mathbf{T}_{i k} = \frac{c^4}{8 \pi G}[\partial_{i} \cdot \mathbf{D}_{k} + i \sigma \cdot (\Gamma_{i} \times \mathbf{D}_{k})][/math]

Edited by Dubbelosix
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Just a couple of things, I am sure you are aware of Lorentz ether theory, which gives all the same answers as SR. LET never failed, it just became more fashionable to SR because the maths was easier. 

 

Ref the speed of light being variable in free space, I do not believe any experiment has ever shown this to be true. Gravity curves and changes its direction but it is always c. Do you happen to have any measurements proving c is variable in free space?

 

ref the aether concept and space, gravity particles etc. I am sure you are aware space is a conductor of fields and all things are fluctuations in the field of space(aether). In the scheme of things it is logical to think space came first, along with quantum fluctuations, with caused time to emerge. At absolute zero these fluctuations might behave differently to how they might at above 2.7K for example. 

 

I am curious to know where you are going with the third law of thermodynamics :)

 

 

i disregard all aether theories, except for the main one, the gravitational aether, which Einstein first proposed and said, that his general theory would be unthinkable without it. 

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I am curious to know where you are going with the third law of thermodynamics :) Are you toying with the idea particle creation, forming clouds of very cold nebulae, which might be primordial matter, a bit like the Boomerang Nebulae for example.

Another lazy person link 3rd law https://en.wikipedia.org/wiki/Third_law_of_thermodynamics

 

A gravitational field bends the photon field around in ever decreasing circles until it disapears up its own photon field. for  example an electron field orbiting a nucleus of an atom, can absorb a photon field raising the electon to a higher energy level. This is exactly the same for a black hole singularity. The similarity between black holes and fundamental particles I find intriguing. 

 

 

I've used the third law a few times, first to predict that stable black hole particles cannot exist. I used the third law to predict a cold big bang opposed to a hot big bang, which is at odds with how we understand entropy. In this case, I speak of the zero point field (as off shell energy) meaning it is hidden from plain sight and doesn't normally couple to real matter due to their short life span.

Edited by Dubbelosix
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You misunderstand, free space means there is no gravity, everything is absent that could hinder the speed of light. This is why we say, the speed of light travels only at the speed in free space/vacuum with absence of significant gravity. This is why the speed of light varies around celestial objects, because gravity is like a ''thickness'' of space and to some observer, appears as though light slows down in gravitational fields.

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I am well aware of what the conventional model states, such as, I am well aware we have been led to believe that the speed of light cannot change. Yet I give you an example in which the extreme current model of gravitational physics predicts light can completely slow down around a black hole. Is it now moving at the speed of light?

 

Also, light does not possess a frame of reference, which means, to which observer is the photon moving at the speed of light constantly? To an observer sitting outside a gravitational system, we can feel quite comfortable to say that the speed of light technically varies in a [general sense] while the speed of light is constant in absence of gravitational field (which is by no other name), [special relativity]. We don't destroy anything fundamental within relativity by stating these things, in fact, the notion of a gravitational aether (and later models that predicted that light can escape black holes) solves many problems. For instance, light does not come to a standstill around a black hole, you will eventually see a test pilot pass the event horizon. Information additionally is allowed to escape, which is an on-going mystery.

 

As I said, nothing in relativity breaks down, but under gravitational aether theory, we not only understand why curvature should exist, but we come to understand solutions to other very important questions that surround the theoretical black hole and other various gravitational studies. I have plenty references, for instance, supporting the gravitational aether. Perhaps tomorrow I will go to my blog and chase a few up for you.

 

My last words for now would be, be careful just accepting that the speed of light cannot vary, when experimentally speaking, we know light slows down in gravitational fields. If light could not slow down, we wouldn't have ridiculous notions of observers sitting outside an event horizon in which they never see their test pilot pass the boundary because the light never reaches them. But if light can only approach zero, then we avoid these kinds of paradoxes. Variable Newton's constant, also required in this theory, is [at least] backed with some hard evidence and anomalies suggested it is not a constant.

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First of all, there are no singularities in the universe. Ininities do not exist in the real world, and no such object can copy itself indefinitely. The singularity is an artifact of the earliest black hole models. Both Hawking and Penrose later changed their minds on their singularity theorems, believing that singularities do not in fact form. In fact, singularity-free models have become very popular and I was hinting at this before it became as popular as it is. Secondly, when we speak about light slowing down, we are not talking about the interior of the black hole, we refer to a famous thought experiment in which an astronaut falls past the horizon, classical theory predicts the light cannot escape and so an observer sitting outside would seem to see the astronaut take [forever] to pass the boundary. The fact is, the speed of light is a relative term and the statement it only moves at the speed of light in a vacuum, can only be good within the special theory of relativity, not a general case.

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My reference to singularity was sloppy wording, thanks for picking me up on that. The ER = EPR conjecture is a key part of the Holographic universe principle. Pinpricks in the fabric of 3D space, might have been better wording. 

 

I used the black hole particle model references only because the idea has been around for a few years. However black holes assume mass at their centre causes the curvature of space time. This is wrong, based on both emergent gravity and the holographic principle which both rely on entanglement ie an EPR or ER bridge.

 

A quantum wormhole (pinprick) may cause quantum fluctuations to fall towards said wormhole creating a particle. Which when many such particles are added together form a black hole. I wonder if quantum fluctuations falling in towards a quantum wormhole would ever pass the event horizon :) ???.

 

As for singularities I agree they are most likely a case of the maths being pushed past breaking point. 

 

 

 

As far what happens inside a blackhole, I do not buy the various graviton ideas. They have never been detected, are assumed to be very low energy, and not even high energy gamma rays escape a blackhole, so how is a graviton going to get out. 

 

The laws of thermodynamics must apply inside a Black hole, anything that is compressed is going to get hot, and will turn into a plasma, then most likely into some form of high energy photons which might actually be self supporting and not be compressed. If Hawking Radiation slowly evaporates a Blackhole, it might intermittently release huge gamma ray bursts, from it core, until the central mass is reduced enough, for a supernovae type big bang as in QLG.

 

What goes on inside a BH is speculation theories like QLG might be part way to solving what goes on.

 

It was a bit of surprise for me to learn how well a condensate model for a black hole really is - the larger the condensate will minimize the free energy of the system (so that larger black holes gives off less radiation than smaller black holes) which is at least similar to how we think of thermodynamics applied to black holes. I think you are right and that not only thermodynamics is important to understand internal dynamics, but we should also concentrate on the idea that quantum mechanics does not vanish either, for instance, a particle cannot be confined to a region smaller than its wavelength, preventing singularities.

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