"relativistic mass" still a no-no?

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Discussion Overview

The discussion revolves around the concept of "relativistic mass" in the context of special relativity, particularly in relation to how mass is measured and defined when objects are in relative motion. Participants explore the implications of using the term "relativistic mass" versus sticking to "rest mass" and "relativistic momentum," as well as the historical context of these terms in physics education and practice.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Historical

Main Points Raised

  • Some participants reference a Wikipedia article suggesting to avoid the term "relativistic mass" and instead use "relativistic momentum" to clarify measurements made by observers in different inertial frames.
  • One participant emphasizes the need to specify the type of mass being measured (gravitational, inertial, or mass-energy) when discussing measurements in relativity.
  • Another participant argues that the historical context of the term "relativistic mass" reflects outdated concepts from early relativity, advocating for the use of modern four-dimensional tensor formalism instead.
  • There is a contention about whether to refer to the mass as ##\gamma m## or simply ##m##, with some participants arguing that the distinction complicates understanding without resolving the underlying issues.
  • Some participants assert that the mass ##m## used in Newtonian physics is not the same as the relativistic concepts, highlighting the differences in definitions and implications in relativistic physics.
  • References are made to Lev Okun's article, with differing interpretations of his stance on the nature of mass in modern relativity.

Areas of Agreement / Disagreement

Participants express differing views on the appropriateness of the term "relativistic mass," with no consensus reached on whether it should be used or replaced with other terminology. The discussion reflects a variety of perspectives on the definitions and implications of mass in both Newtonian and relativistic contexts.

Contextual Notes

Participants highlight the historical evolution of the concept of mass and its definitions, indicating that the understanding of mass in relativity is nuanced and context-dependent. There are unresolved questions regarding the implications of using different terms and the relationship between various types of mass.

  • #91
I am closing the thread for moderation.
 
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  • #92
A number of off topic posts have been deleted and the thread is reopened.
 
  • #93
The whole thing could have been avoided had the old way of calling rest mass m0 and the relativistic mass m = γm0. Then E=mc2 would have survived, also centripetal force mv2/r. Like Regietheater opera, dumbing-down prevailed however. I was happy to see that even in the new millennial edition of Dr. Feynman's Lectures on Physics the editors decided to stick with what did not need fixin' 'cause it wasn't broke.
 
  • #94
rude man said:
The whole thing could have been avoided had the old way of calling rest mass m0 and the relativistic mass m = γm0. Then E=mc2 would have survived, also centripetal force mv2/r.

You cannot make the Newtonian expression ##\frac{mv^2}{r}## valid by replacing ##m## with the relativistic mass.

Like Regietheater opera, dumbing-down prevailed however. I was happy to see that even in the new millennial edition of Dr. Feynman's Lectures on Physics the editors decided to stick with what did not need fixin' 'cause it wasn't broke.

Feynman states that you can replace ##m## in the expressions of Newtonian physics with the relativistic mass and create relations that are valid. It's been discussed in the literature that such a notion is in general wrong. There are a few important and often-used relations where that can be done, but in the general case it's not valid.

In other words, it's an oversimplification.

The fact is, high energy physicists have never changed the practice of referring to only one kind of mass in their work and in their professional publications. Some of them, when authoring books and articles for the public, have used the concept of relativistic mass.

I'll leave it to you to decide which arrangement is a "dumbing down".

The main argument for doing away with it was indeed that it allowed survival of ##E=mc^2##. To people trying to learn physics it was obscuring the true meaning of Einstein's mass-energy relation. A misconception that often persisted into the professional phase of a physicist's life.
 
  • #95
rude man said:
The whole thing could have been avoided had the old way of calling rest mass m0 and the relativistic mass m = γm0. Then E=mc2 would have survived, also centripetal force mv2/r. Like Regietheater opera, dumbing-down prevailed however. I was happy to see that even in the new millennial edition of Dr. Feynman's Lectures on Physics the editors decided to stick with what did not need fixin' 'cause it wasn't broke.

The whole thing could have been avoided if Einstein and his contemporaries had stuck with either "mass" or "energy" for all mass/energy terms. Instead they adopted a confusing mishmash of various ##m##'s and ##E##'s.

There's nothing that ##m## quantifies that ##E## doesn't. They're the same quantity in different units.

There's nothing that ##m_0## quantifies that ##E_0## doesn't. They're the same quantity in different units.

Why we've ended up with ##E## and ##m_0## (now usually just called ##m##) is beyond me. I use ##E## and ##E_0##. If an answer is needed in mass units, I convert.
 
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  • #96
Mister T said:
You cannot make the Newtonian expression ##\frac{mv^2}{r}## valid by replacing ##m## with the relativistic mass.

You can. It's one of the special cases where it works. If you should it's another question.
 

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