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A tweek to Einsteins theory Does this work out? Rate Topic: ***-- 2 Votes

#1 morgsboi 


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S=Speed
C=3 x 108 ms-1 (speed of light)
If S>C then E=M(C+(S-C)^2

This post has been edited by morgsboi: 6 November 2011 - 05:35 PM

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#2 User is online  timo 


Primate
Obviously, in this form the number of opening and closing parentheses in your relation between the letters E, M, C, and S does not match, which makes it very dubious. But the more fundamental issue here is: what is your point?
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#3 User is online  swansont 


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Can you derive this equation from some underlying principles?
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#4 morgsboi 


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View Postswansont, on 6 November 2011 - 03:42 PM, said:

Can you derive this equation from some underlying principles?


It's only something I've just though of while thinking about the Opera (Oscillation Project with Emulsion-tRacking Apparatus) experiment, which broke the speed of light and how the amount of energy would be measured but would breaking the speed of light change the mass of the particles?
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#5 User is online  swansont 


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View Postmorgsboi, on 6 November 2011 - 04:05 PM, said:

It's only something I've just though of while thinking about the Opera (Oscillation Project with Emulsion-tRacking Apparatus) experiment, which broke the speed of light


Well, that's not yet been confirmed. But science abhors ad-hoc-ery. You need to justify the equation.
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#6 morgsboi 


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View Postswansont, on 6 November 2011 - 04:57 PM, said:

Well, that's not yet been confirmed. But science abhors ad-hoc-ery. You need to justify the equation.


Yes, I know it's not confirmed but if light speed was broken (doesn't matter what experiment) then would this work? And I don't understand how it could be justified as it's in it's simplest form.

View Postmorgsboi, on 6 November 2011 - 05:27 PM, said:

Yes, I know it's not confirmed but if light speed was broken (doesn't matter what experiment) then would this work? And I don't understand how it could be justified as it's in it's simplest form.


Actually I've noticed a flaw, sorry. The equation should be if S=>C then E=M(C+(S-C)^2 which I will change in the forum. And as a word equation it would simply be: If the speed is greater than the speed of light then Energy is equal to the speed of light plus the sum of the speed minus the speed of light.
Make sense??
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#7 insane_alien 


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by justify i'm fairly sure swansont meant: why should that be the equation used? how did you come to that equation?

equations don't just pop out of nowhere.

also, as this is most definitely considering motion why have you used E=mc^2 (the simplification for zero momentum) rather than the full equation?
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#8 User is online  swansont 


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View Postmorgsboi, on 6 November 2011 - 05:34 PM, said:

Yes, I know it's not confirmed but if light speed was broken (doesn't matter what experiment) then would this work? And I don't understand how it could be justified as it's in it's simplest form.


How was it derived, or otherwise arrived at?
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#9 morgsboi 


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View Postswansont, on 6 November 2011 - 06:49 PM, said:

How was it derived, or otherwise arrived at?


As I said, I was thinking about if something went faster than the speed of light then what would happen to Einstein's theory, so I developed a simple and quick tweak.

View Postinsane_alien, on 6 November 2011 - 06:15 PM, said:

by justify i'm fairly sure swansont meant: why should that be the equation used? how did you come to that equation?

equations don't just pop out of nowhere.

also, as this is most definitely considering motion why have you used E=mc^2 (the simplification for zero momentum) rather than the full equation?


I've explained it a couple of posts below and also I am only 14 and I come on here to learn more about my thoughts and theories that I have so I'm not a big expert in science but I am hoping to be.
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#10 Cap'n Refsmmat 


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The full form of the equation for particles in motion is E^2 = m^2 c^4 + p^2 c^2, where p is momentum. Your equation will need to reduce to this when v<c.
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#11 DrRocket 


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View PostCap, on 6 November 2011 - 07:25 PM, said:

The full form of the equation for particles in motion is E^2 = m^2 c^4 + p^2 c^2, where p is momentum. Your equation will need to reduce to this when v<c.



That is somewhat a matter of taste and definitions (in particular what is meant by "mass").

E^2 = m^2 c^4 + p^2 c^2,

applies with m being rest mass (m_0), which is currently in fashion.


E = m c^2 ,

applies if m is taken to be relativistic mass ( \gamma m_0) and if the rest mass is non-zero. It is equivalent to E^2 = m_0^2 c^4 + p^2 c^2 in that case.

So for massive neutrinos E = m c^2 is fully accurate if properly interpreted

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#12 Cap'n Refsmmat 


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I suppose so; I must've been taught by fashionable physicists.

There's still the issue of units. If the equation is E=m(c+(s-c)^2), then there are two parts:

E=mc + m(s-c)^2

The left term does not have units of energy, while the right term does, so the equation doesn't work out.

One could interpret the missing parenthesis differently, as E=m(c+(s-c))^2, but that's just algebraically equivalent to E=m(s)^2.

morgsboi, which version of the equation did you mean?
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#13 morgsboi 


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View PostCap, on 6 November 2011 - 07:25 PM, said:

The full form of the equation for particles in motion is E^2 = m^2 c^4 + p^2 c^2, where p is momentum. Your equation will need to reduce to this when v<c.


Okay, thanks. So what is V?

View PostCap, on 6 November 2011 - 08:20 PM, said:

I suppose so; I must've been taught by fashionable physicists.

There's still the issue of units. If the equation is E=m(c+(s-c)^2), then there are two parts:

E=mc + m(s-c)^2

The left term does not have units of energy, while the right term does, so the equation doesn't work out.

One could interpret the missing parenthesis differently, as E=m(c+(s-c))^2, but that's just algebraically equivalent to E=m(s)^2.

morgsboi, which version of the equation did you mean?

Yes, the right hand version is a lot better.
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#14 Fuzzwood 


Formerly known as Fswd
velocity.
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#15 DrRocket 


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View Postmorgsboi, on 6 November 2011 - 09:32 PM, said:

Okay, thanks. So what is V?


Yes, the right hand version is a lot better.


But E=ms^2 would imply that E \rightarrow 0 as s \rightarrow 0 which we know is grossly wrong (or nuclear weapons and nuclear power plants would not work). This also flies in the face of Einstein's recognition of the equivalence of mass and energy, so it is a long way from a mere tweak -- it is just plain wrong.

And THAT is why swansont's challenge to you to derive your equation from some set of basic principles is important. You don't revise a theory that is supported by a mountain of empirical data and developed logically from simple principles by simply pulling an equation out of ................ the air perhaps.

You can know the name of a bird in all the languages of the world, but when you're finished, you'll know absolutely nothing whatever about the bird... -- Richard P. Feynman
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#16 morgsboi 


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View PostDrRocket, on 6 November 2011 - 09:49 PM, said:

But E=ms^2 would imply that E \rightarrow 0 as s \rightarrow 0 which we know is grossly wrong (or nuclear weapons and nuclear power plants would not work). This also flies in the face of Einstein's recognition of the equivalence of mass and energy, so it is a long way from a mere tweak -- it is just plain wrong.

And THAT is why swansont's challenge to you to derive your equation from some set of basic principles is important. You don't revise a theory that is supported by a mountain of empirical data and developed logically from simple principles by simply pulling an equation out of ................ the air perhaps.


Yes, it was "out of the air" and I put it on here to get help with it.
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#17 Mystery111 


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View PostDrRocket, on 6 November 2011 - 07:58 PM, said:

That is somewhat a matter of taste and definitions (in particular what is meant by "mass").

E^2 = m^2 c^4 + p^2 c^2,

applies with m being rest mass (m_0), which is currently in fashion.


E = m c^2 ,

applies if m is taken to be relativistic mass ( \gamma m_0) and if the rest mass is non-zero. It is equivalent to E^2 = m_0^2 c^4 + p^2 c^2 in that case.

So for massive neutrinos E = m c^2 is fully accurate if properly interpreted


For a nuetrino at rest, and even at that it is missing some important details in describing neutrino's. In fact, some theories of neutrino's would not have a mass term in it under a Weyl Limit.

The mass does the same thing to coupling particles and antiparticles together as you would find from a majorana equation. Nuetrino's are spin 1/2 so they are fermions:

-i(\alpha \hat{p})c\psi + \beta M c^2 \psi = i\hbar \partial_t \psi

This can be re-written as:

i\hbar \frac{\partial \phi}{\partial t} = -ic\hbar \vec{\sigma} \cdot \nabla_{\phi} + M c^2 \phi'

i\hbar \frac{\partial \chi}{\partial t} = -ic\hbar \vec{\sigma} \cdot \nabla_{\chi} + M c^2 \chi'

as two component equations, when this equation is under a Weyl representation

i\hbar \frac{\partial \eta}{\partial t} = -ic\hbar \vec{\xi} \cdot \nabla \eta + M c^2 \xi

and

i\hbar \frac{\partial \xi}{\partial t} = -ic\hbar \vec{\eta} \cdot \nabla \xi - M c^2 \eta

\eta and \xi are in fact coupled to a limit where M is nonzero. Under mathematcial strutiny, the fact that the Nuetrino has such a ridiculously small mass incorporates the similar contention that the nuetrino could act more or less like a particle with no mass. So in this case, the non-relativistic case Mc^2 will not suffice.

With the limit where M=0 reduces to the Weyl equation

\frac{\partial \xi v'}{\partial} = -c\vec{\sigma} \cdot \nabla \xi v'

This only suits right solutions for antiparticles for nuetrinos v'.

\frac{\partial \xi v'}{\partial} = -c\vec{\sigma} \cdot \nabla \xi v'

I think we established that it described antineutrinos.... The second equation in your coupled set up vanish because \phi = \chi when M=0. Now this is actually related to parity (you may understand parity under CPT-symmetry.) The Weyl equation is only permitted for right handed antineutrino's since a nuetrino is only ever left handed.

For that purpose you may introduce a transformation \alpha \rightarrow -\alpha. Anticommutator relations are preserved in the Dirac Equation which would describe the neutrino. The transformation also effects \sigma \rightarrow -\sigma so the Weyl equation becomes

\frac{\partial \xi v}{\partial} = c\vec{\sigma} \cdot \nabla \xi v

For a nuetrino. Simply a neutrino must have a mass at a specific limit which allows us to make these valid transformations. The non-relativistic case of Mc^2 also fails to descrive fermions correctly. As you will surely know, the correct energy condition has both a positive and negative solution E= \pm Mc^2. So you will also deal with

\psi^1 = \begin{pmatrix} 1 \\ 0 \\ 0 \\ 0 \end{pmatrix} e^{\frac{iMc^2 t}{\hbar}}

\psi^2 = \begin{pmatrix} 0 \\ 1 \\ 0 \\ 0 \end{pmatrix} e^{\frac{iMc^2 t}{\hbar}}

Are your two positive energy solutions with opposite spin states

\psi^3 = \begin{pmatrix} 0 \\ 0 \\ 1 \\ 0 \end{pmatrix} e^{\frac{+iMc^2 t}{\hbar}}

\psi^4 = \begin{pmatrix} 0 \\ 0 \\ 0 \\ 1 \end{pmatrix} e^{\frac{+iMc^2 t}{\hbar}}

Are your two negative energy states with opposite spin

This post has been edited by Mystery111: 6 November 2011 - 10:07 PM

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#18 User is online  swansont 


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View Postmorgsboi, on 6 November 2011 - 07:12 PM, said:

As I said, I was thinking about if something went faster than the speed of light then what would happen to Einstein's theory, so I developed a simple and quick tweak.



That's not how science is done. You can get relationships by matching the pattern of some data, but mainly you start with some physical principle and derive the equation.
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#19 morgsboi 


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View Postswansont, on 6 November 2011 - 11:19 PM, said:

That's not how science is done. You can get relationships by matching the pattern of some data, but mainly you start with some physical principle and derive the equation.


Yes, but as I also said, I put it on here to get information to learn about it. I am only 14 so I haven't exactly been able to get a PHD with years of studying. But I am hoping too.
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#20 Mystery111 


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You are 14, and you want to know about neutrino's, or how they are applied in relativity? All due respect but you really are jumping in the deep end my friend first.
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