# Singularity Mechanics? Blackhole Spin

1. Jun 29, 2013

### TWest

Singularity Spin Mechanics

Okay I within the last week too a look at a article about black hole spin and in this article it was said by a scientist that black hole's spin near the speed of light that are supermassive blazars I was thinking if a object is spinning wouldn't that make this massive object subject to angular momentum laws and found I think a equation that accurately explains this phenomena if this is the case. what happens is simple The black hole spins and opens a hole in event horizon allowing matter to escape where the spin counteracts the gravitational pull which I call a "Void zone or spot where the jet escapes" which makes a coordinate system. dx'∇ = dx(1-(∇Δv^2/C^2))^(1/2) which shows external spin pressure is making the singularity expand in a direction. Δv^2 = (Vg-Vs)^2 , Vg^2 = 2MbG / Rs, Vs^2 = Es/Mb

Final Equation

∇'(x',y',z') = ∇(1-(((2MbG / Rs) - (Es/Mb))^2/C^2))^(1/2)
Blazar means the number is Less than C at a point or more, and Supermassive black hole means all equal to C.
Does this seem possible to you guys?

Tory Cortland Weston 6/29/2013

Proof

Coords = http://www.wolframalpha.com/input/?i=dx'∇+=+dx(1-(∇Δv^2/C^2))^(1/2)+

Part I = http://www.wolframalpha.com/input/?i=2*M*G+/+R

part II = http://www.wolframalpha.com/input/?i=E/M

Article = http://www.gizmag.com/supermassive-black-hole-spin-nustar-newton/26543/

Last edited: Jun 29, 2013
2. Jun 29, 2013

### Simon Bridge

Yep - see how angular momentum works in GR.

... the spin creates a coordinate system.

AFAICT this sentence has no meaning.

I think you need to clean up the math.

3. Jun 29, 2013

### TWest

Final Equation

∇'(x',y',z') = ∇(1-(((2MbG / Rs) - (Es/Mb))^2/C^2))^(1/2)

Not Quite it would be like this wouldn't it

∇'(x',y',z') = ∇(1-(((2MbG / Rs) - (Isws^2/2Mb))^2/C^2))^(1/2)

4. Jun 29, 2013

### Simon Bridge

∇'(x',y',z') = ∇(1-(((2MbG / Rs) - (Isws^2/2Mb))^2/C^2))^(1/2)

Well... while we are at it - more like:

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{I_s\omega_s^2}{2M_b} \right )^2 \right ]^{1/2}$$

... ??

5. Jun 30, 2013

### TWest

I guess?

6. Jun 30, 2013

### TWest

$$i\hbar \frac{\partial}{\partial t}\Psi(\mathbf{r},\,t)=-\frac{\hbar^2}{2m}\nabla^2\Psi(\mathbf{r},\,t) + V(\mathbf{r})\Psi(\mathbf{r},\,t).$$
which makes Quantum Relativity for a blackhole

$$i\hbar \frac{\partial}{\partial t}\Psi(\mathbf{r},\,t')=-\frac{\hbar^2}{2m}\nabla'^2 (x',y',z')\Psi(\mathbf{r},\,t) + V(\mathbf{r})\Psi(\mathbf{r},\,t).$$

????

7. Jun 30, 2013

### TWest

Or more Correctly

$$i\hbar \frac{\partial}{\partial t'}\Psi(\mathbf{r},\,t')=-\frac{\hbar^2}{2m}\nabla'^2 (x',y',z')\Psi(\mathbf{r},\,t) + V(\mathbf{r})\Psi(\mathbf{r},\,t).$$

8. Jun 30, 2013

### TWest

9. Jun 30, 2013

### TWest

Which makes time the spin of the universe and a black hole's Quantum tunneling events just like photons leaving a Quantum Field, time is non reversible, fractal until the moment happens, and there are others .

Last edited: Jun 30, 2013
10. Jun 30, 2013

### Simon Bridge

I think that's unlikely - I don't see how you've done anything other than put stuff arbitrarily into formulas without reference to what they describe.

Have you done any GR at all?

11. Jun 30, 2013

### TWest

Well, I am just thinking aloud, It could be could not I would have to solve it to find out if I was right but the visual translation looks promising.

Last edited: Jun 30, 2013
12. Jun 30, 2013

### TWest

Lets See first I subbed in the Schwarzschild radius Singularity Equation that explains the event horizon of a singularity then I took it against the angular momentum of the black hole pushing outward then tossed that into Lorentz Contraction and made it three dimensional with the Laplacian then subbed in the relativistic Laplacian for the standard in 3-D Schrödinger equation.

why wouldn't this work?

I think I have http://www.physics.fsu.edu/courses/spring98/ast3033/Relativity/GeneralRelativity.htm [Broken]

Last edited by a moderator: May 6, 2017
13. Jul 1, 2013

### TWest

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{I_s\omega_s^2}{2M_b} \right )^2 \right ]^{1/2}$$

Which Makes a mass field in a direction
$$I_s = ∑i m_i r_i = m_1 r_1 + m_2 r_2 + ..... + m_nr_n$$

which is the expansion rate of time
$$ω_s^2 = C^2$$

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_uG}{R_u} - \frac{(∑im_i r_i = m_1 r_1 + m_2 r_2 + ..... + m_nr_n) C^2}{2M_u} \right )^2 \right ]^{1/2}$$

or i have i just taken this way to far?

14. Jul 1, 2013

### TWest

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{(∑im_i r_i = m_1 r_1 + m_2 r_2 + ..... + m_ur_s) C^2}{2M_b} \right )^2 \right ]^{1/2}$$

making the limit of the series Schwarzschild Radius

15. Jul 1, 2013

### TWest

Which makes them all $$M_G$$ or Mass Graviton I think

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{(∑im_G r_i = m_G r_1 + m_G r_2 + ..... + m_Gr_s) C^2}{2M_b} \right )^2 \right ]^{1/2}$$

16. Jul 1, 2013

### TWest

Lets take a step back

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{(∑im_G r_i = m_G r_1 + m_G r_2 + ..... + m_Gr_s) ω^2}{2M_b} \right )^2 \right ]^{1/2}$$
$$ω = √(k/m)$$

Then

$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{(∑im_G r_i = m_G r_1 + m_G r_2 + ..... + m_Gr_s) (k/m)}{2M_b} \right )^2 \right ]^{1/2}$$

17. Jul 1, 2013

### TWest

Which shows the Construction of a black hole........Boson.

18. Jul 1, 2013

### TWest

which finishes to
$$\nabla'(x',y',z') = \nabla \left [ 1-\frac{1}{C^2}\left ( \frac{2M_bG}{R_s} - \frac{(∑im_G r_s = m_G r_1 + m_G r_2 + ..... + m_Gr_s) k}{2M_b^2} \right )^2 \right ]^{1/2}$$

making
$$k = 1/(1-ε^2)^{1/2}$$

19. Jul 1, 2013

### TWest

$$ε ^2 = Δt_u^2$$

20. Jul 1, 2013

### TWest

$$Δt_u ^2= 0$$
maybe?