What Are Non-Astrophysical Examples of Experimental Evidence for E=MC^2?

AI Thread Summary
Experimental evidence for Einstein's E=mc^2 outside of astrophysics includes nuclear fission and fusion, particularly from bomb detonations, which demonstrate the conversion of mass into energy. Particle accelerators also provide significant evidence by showing how energy contributes to mass and vice versa. While fission is often associated with stellar processes, it can be observed in controlled experiments on Earth. Additionally, alpha decay experiments illustrate the mass-energy equivalence through the transformation of "missing" mass into gamma rays. Overall, these examples highlight the practical applications of E=mc^2 beyond astrophysical contexts.
Brewer
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I have a question that asks for experimental evidence for Einsteins famous E=MC^2 equation that isn't from an astrophysics, but the only evidence I can think of is nuclear fission, but I'm sure this occurs in stars in some way. Would this count as evidence that isn't from astrophysics or would you suggest another type of evidence to satisfy the question?

Any hints as to what the other evidence might be?
 
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Fission isn't normally done in stars. Particle accelerators also provide evidence both of conversion of matter to energy and the other side of the coin: the inertia gained with energy.
 
No I realized that after a further read through my textbook. Its fusion in stars!

Thanks though
 
Brewer said:
I have a question that asks for experimental evidence for Einsteins famous E=MC^2 equation that isn't from an astrophysics, but the only evidence I can think of is nuclear fission, but I'm sure this occurs in stars in some way. Would this count as evidence that isn't from astrophysics or would you suggest another type of evidence to satisfy the question?
Any hints as to what the other evidence might be?
The fission and fussion bombs that have been detonated in this world are pretty good examples of the relationship E = mc2 holding true.

Pete

Note: There are instances of when E = mc2 does not hold, e.g. when a body is under stress.
 
in experiments with alpha decay, the "missing" mass from the remaining particle is transformed into gamma rays via E=mc^2
 
simon009988 said:
in experiments with alpha decay, the "missing" mass from the remaining particle is transformed into gamma rays via E=mc^2
..which is an example of fission (although some people don't like to define the term "fission" in that way - but I do).

It should be noted that mass is conserved in these examples (i.e. "relativistic mass" is conserved)

Pete
 
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