Why is energy not Lorentz invariant?

Click For Summary
SUMMARY

The discussion centers on the non-invariance of energy under Lorentz transformations in the context of special relativity (SR). While energy is a scalar in classical mechanics (CM), it becomes a component of a 4-momentum vector in SR, leading to its observer-dependent nature. The distinction between observer-dependent scalars and observer-independent scalars is emphasized, with kinetic energy being highlighted as frame-dependent in both CM and SR. The conversation also touches on the necessity of using 4-vectors to maintain covariance under Lorentz transformations, reinforcing the unified treatment of energy and momentum in SR.

PREREQUISITES
  • Understanding of 4-vectors in special relativity
  • Familiarity with Lorentz transformations
  • Knowledge of classical mechanics and scalar quantities
  • Basic concepts of kinetic energy and momentum
NEXT STEPS
  • Explore the derivation of the energy-momentum 4-vector in special relativity
  • Study the implications of Poincaré transformations on physical quantities
  • Learn about observer-dependent versus observer-independent scalars in physics
  • Investigate the role of the Lorentz factor in relativistic physics
USEFUL FOR

Students and professionals in physics, particularly those studying special relativity, theoretical physicists, and anyone interested in the relationship between energy and momentum in different reference frames.

  • #31
SiennaTheGr8 said:
Yes. As someone said on the previous page, there are unfortunately two different definitions of scalar in use. Basically:

1) a number (i.e., not a vector);

2) a quantity that is invariant and whose value is just a number.

According to the first definition, total energy, kinetic energy, and rest energy are all scalars. According to the second definition, rest energy is a scalar but total energy and kinetic energy aren't.

I guess one needs to be careful then when one stipulates the transformations in which a particular quantity is a scalar with respect to.

Ok cool, I think it's becoming clearer to me now. Thanks for your help, and thanks for the previous post (#29) detailing the relativistic energy derivation.
 
  • Like
Likes   Reactions: SiennaTheGr8
Physics news on Phys.org
  • #32
Apart from technical mathematical cases (tensors) you might just consider 'scalar' to be a real number as opposed to a set of numbers. E.,g., px is a 'scalar' but it makes no sense to ask how it transforms other then in the context of being one element of a 4-vector. Energy is just the same.

Some 'energies' are defined a non-invariant way. E.g.. temperature is given by the average energy of the particles making up a block of stuff. It is defined only in the rest from of the stuff. It would not make sense to say that a object heats up when you run pass it even though the energy of the particles making up your stuff would be higher, this average energy would not be useful in thermo dynamics where the average energy in the rest frame of the stuff is the relevant quantity.

If you were computing the scattering of one blick of stuff with others than it would be relevant to treat the energy contributed by to the total by the 'internal' motion of the particles to the four vector describing the motion of he block. This is, typically, negligible even for very hot objects.
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 32 ·
2
Replies
32
Views
4K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 33 ·
2
Replies
33
Views
2K
Replies
8
Views
721