B How Did Einstein's E=mc² Transform Our Understanding of Inertia and Gravity?

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Einstein's equation E=mc² is a specific case of the more general equation E²=(m₀c²)²+(pc)², which accounts for momentum (p) and invariant mass (m₀). While E=mc² applies when momentum is zero, the general equation is valid for all objects, including massless particles like photons. The discussion emphasizes that relativistic mass varies with velocity, while invariant mass remains constant across reference frames. Misinterpretations of E=mc² can lead to incorrect conclusions about the rest mass of particles with energy. Understanding these distinctions is crucial for accurately applying relativistic physics.
  • #31
vanhees71 said:
"relativistic mass" is out of fashion since 1907.
Oh, that is a very specific date. What happened in 1907?
 
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  • #33
Dale said:
Oh, that is a very specific date. What happened in 1907?
Einstein learnt about the consistent description of classical point-particle mechanics within SRT from Planck.
 
  • #34
Dale said:
Oh, that is a very specific date. What happened in 1907?
It may be unralated, but at that time he was asked to write a review article about relativity. Then he decided that gravity needs to be treated relativistically and it is a problem that can be worked on. May be he also realized that relativistic mass is more confusing than usefull.
 
  • #35
vanhees71 said:
One should also once more state that the use of "relativistic mass" is out of fashion since 1907.
vanhees71 said:
Einstein learnt about the consistent description of classical point-particle mechanics within SRT from Planck.

The statement 'the use of "relativistic mass" is out of fashion since 1907' is true, if you focus on Einstein. However, other physicists used "relativistic mass" after 1907:
Wikipedia said:
Planck (1906a) defined the relativistic momentum and gave the correct values for the longitudinal and transverse mass by correcting a slight mistake of the expression given by Einstein in 1905. Planck's expressions were in principle equivalent to those used by Lorentz in 1899.[80] Based on the work of Planck, the concept of relativistic mass was developed by Gilbert Newton Lewis and Richard C. Tolman (1908, 1909) by defining mass as the ratio of momentum to velocity. So the older definition of longitudinal and transverse mass, in which mass was defined as the ratio of force to acceleration, became superfluous. Finally, Tolman (1912) interpreted relativistic mass simply as the mass of the body.[81] However, many modern textbooks on relativity do not use the concept of relativistic mass anymore, and mass in special relativity is considered as an invariant quantity.
Source:
https://en.wikipedia.org/wiki/History_of_special_relativity#Relativistic_momentum_and_mass
 
  • #36
Indeed, people where confused about the relativistic redefinition of quantities till much later. Particularly thermodynamics and statistical physics was a mess until the late 1960ies, when people realized how to define the phase-space-distribution function as a scalar and following from that the thermodynamic potentials and other quantities like temperature and chemical potential in a consistent relativistic way as scalars. This was particularly due to the raised interest in General Relativity at this time, where you cannot in any way deal with complicated non-covariant quantities like "relativistic mass" or frame-dependent temperatures. All this is far from trivial!
 
  • #37
As I wrote in the Insight (FAQ at the time), one has to be very conscious about what one means with ”mass”. In relativity, ”mass” is related to the invariant norm of the 4-momentum. The term ”relativistic mass” is misapplied in many senses as it is neither related to the classical gravitational mass nor to the actual inertia (which is not a scalar!). To me, the great insight of ##E=mc^2## is that the inertia of an object in its rest frame (which is well defined and can be directly connected to the concept of mass in classical mechanics) is its rest energy.
 
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  • #38
Ibix said:
Relativity still says that ##E=mc^2## is a special case of ##E^2=m^2c^4+p^2c^2##

Nugatory said:
Long before then we are using ##E^2=(m_0c^2)+(pc)^2##
I don't think anyone has noticed, or at least commented on, but there's a typo in the first term on the right side. There's a missing exponent that should appear outside of the right parenthesis, as in ##(m_0c^2)^2##.
 
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  • #39
Mark44 said:
there's a typo
So there is - thx. Fixed
 
  • #40
vanhees71 said:
"relativistic mass" is out of fashion since 1907
Just out of curiosity, why 1907? I though Minkowski was in 1908.

And if there was any doubt that relativistic mass produced nothing but confusion, this thread should remove it.
 
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  • #41
I think in the famous review article of 1907, Einstein used ##E/c^2## as a measure of inertia and also argued that it is the "source of the gravitational interaction". It may be that he still called this quantity "relativistic mass", but there was no hint anymore to so confusing concepts as also direction-dependent "relativistic masses". I interpret this as a reaction to the discovery of the correct equations of motion by Planck (1906) and the first development towards a relativistic theory of gravitation, which finally ended up famously with GR in 1915, and it's not only energy but the energy-momentum-stress tensor of all fields except the gravitational field that is the source of the gravitational field.
 
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