Equivalence without relativity

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    Equivalence Relativity
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Discussion Overview

The discussion revolves around the derivation of the equation E=mc² without relying on the principles of special relativity (SR). Participants explore various interpretations and historical contexts of the equation, including references to earlier works and assumptions made in the derivations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Historical

Main Points Raised

  • Some participants reference Andrew Gould's paper, suggesting it offers a derivation of E=mc² that does not assume a constant speed of light (c).
  • Others point out that Gould's derivation may still rely on assumptions inherent to special relativity, such as the constancy of c in any reference frame.
  • One participant notes that Gould's approach aims to derive the principle of equivalence using only tools available in 1884, avoiding modern assumptions.
  • There is mention of earlier derivations of E=mc², including those by Fritz Rohrlich and references to Einstein's 1906 paper.
  • Some participants discuss the implications of Maxwell's equations and the historical context of the aether theories, suggesting that the constancy of c was interpreted differently before relativity.
  • There is a suggestion that multiple individuals, including Heaviside, may have independently derived E=mc² prior to the formal establishment of relativity, though the validity of these derivations is questioned.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions made in Gould's derivation and the historical context of E=mc², indicating that multiple competing interpretations and models remain unresolved.

Contextual Notes

Some participants highlight that assumptions about the constancy of c and the interpretation of Maxwell's equations are critical to the discussion, but these assumptions are not universally agreed upon.

Chronos
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Here is a very interesting read on SR. Were Gould not the author, I probably would have glossed and flossed this paper.
http://www.arxiv.org/abs/astro-ph/0504486
E = mc^2 Without Relativity
Authors: Andrew Gould
 
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Chronos,

Get out your floss!

Maybe I'm missing something, but in the introductory book "Special Relativity" by Anthony French, there's a derivation of E=mc2 that doesn't assume constant c. A 1906 paper by Einstein (Ann. Phys., 20, 627-633) is cited. Gould's derivation seems along the same lines (momentum of EM radiation) although he takes longer to get to the result than Einstein did.

But, like I said, maybe I'm missing something!
 
Interesting tutorial - the second part (3.1) is bootstrap however - since it assumes c constant in any reference frame, it recovers the relativistic mass (eq 10), but that assumption is part of SR, which is what the author seeks to prove.
 
The more interesting point that Gould raises is how one could have derived the principle of equivalence using only the tools available in 1884. He takes the long way around because he deliberately avoids using any assumptions that were not accessible at that time.
 
yogi said:
Interesting tutorial - the second part (3.1) is bootstrap however - since it assumes c constant in any reference frame, it recovers the relativistic mass (eq 10), but that assumption is part of SR, which is what the author seeks to prove.

Care to elaborate? It looks to me like he explicitly avoids doing that.
 
Chronos said:
Here is a very interesting read on SR. Were Gould not the author, I probably would have glossed and flossed this paper.
http://www.arxiv.org/abs/astro-ph/0504486
E = mc^2 Without Relativity
Authors: Andrew Gould
A buddy of mine told me about this paper today. It turns out that the author referenced an article I (ref 2 - "Brown, P.M.") wrote last year. Please note that my article is in the physics archive and not in the astro-ph archive. The author of this article is not the first to derive E = mc^2 by the method he uses. Fritz Rorhlich did this several years ago. It appears in the American Journal of Physics.

jdavel - The author does not use the Lorentz transformation nor does he use time dilatation. He approximates red shift using the classical relation rather than the relativistic one (which assumes c = invariant).

Pete
 
Last edited:
Space Tiger - top of page 5 ..."but c is constant in anyone frame" One way isotropy is a premise of SR.
 
yogi said:
Space Tiger - top of page 5 ..."but c is constant in anyone frame" One way isotropy is a premise of SR.

Ok, I thought you were saying that he was assuming its constantcy across reference frames. Although single-frame constancy is an assumption which is implicit to SR, it seems like that assumption was also implicit to Maxwell's equations, work done prior to relativity.
 
SpaceTiger said:
Ok, I thought you were saying that he was assuming its constantcy across reference frames. Although single-frame constancy is an assumption which is implicit to SR, it seems like that assumption was also implicit to Maxwell's equations, work done prior to relativity.
I think the interpretation of Maxwell´s equation was that c is constant only in one special frame (the aether).
further, if I were a scientist back then and would know nothing about photons, I would rather believe that my calculation was oversimplyfied than announce that E=mc².
 
  • #10
Ich said:
I think the interpretation of Maxwell´s equation was that c is constant only in one special frame (the aether).

From what I understand about the aether theories, they were claiming that c was simply a different constant, depending on your motion with respect to the aether. This would make sense because they were looking to preserve Galilean relativity. When you apply this to Maxwell's equations, you will simply find that c is a different constant, but constant nonetheless.
 
  • #11
SpaceTiger said:
From what I understand about the aether theories, they were claiming that c was simply a different constant, depending on your motion with respect to the aether. This would make sense because they were looking to preserve Galilean relativity. When you apply this to Maxwell's equations, you will simply find that c is a different constant, but constant nonetheless.
Michelson and Morley expected to find different c in different directions, just like you would expect for sound.
 
  • #12
I the impression that the E=mc^2 equation was independently derived more than once before the advent of relativity?

Heaviside is a name that rings a bell in this context.
 
  • #13
PeteSF said:
I the impression that the E=mc^2 equation was independently derived more than once before the advent of relativity?

Heaviside is a name that rings a bell in this context.
There were some people who wrote down the equation, but in each case they either meant for it only to apply to some very specific physical situation rather than being a general relation, or their derivation was wrong, or both. http://users.net.yu/~mrp/chapter23.html from another forum.
 
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