Conservation laws and relativistic dynamics

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Discussion Overview

The discussion revolves around the role of conservation laws of momentum and energy in the derivation of fundamental equations of relativistic dynamics. Participants explore whether these conservation laws are essential or merely suggestive in formulating relativistic dynamics, with references to both special and general relativity.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue that conservation laws are compulsory for deriving fundamental equations of relativistic dynamics, suggesting that without them, one is discussing a new theory.
  • Others contend that conservation laws arise from symmetries and are not strictly necessary for defining relativistic dynamical quantities or formulating equations.
  • A participant notes that in general relativity, the conservation law pertains to energy-momentum rather than energy, highlighting the frame-dependent nature of energy.
  • One participant emphasizes that the fundamental equations of dynamics are derived from the action principle, which incorporates conservation laws.
  • Concerns are raised regarding the clarity and pedagogical effectiveness of deriving transformation equations from collisions, with a request for alternative derivations that do not rely on conservation laws.
  • Another participant proposes defining 4-velocity and 4-momentum to derive transformation laws, while also noting the potential confusion this may cause for students unfamiliar with these concepts.
  • There is a discussion about the importance of understanding the geometry of Minkowski space to grasp the implications of special relativity before delving into the mathematics.
  • Some participants express differing views on the effectiveness of traditional versus alternative teaching methods in conveying the concepts of relativistic dynamics.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the necessity of conservation laws in relativistic dynamics, and the discussion remains unresolved with no consensus reached.

Contextual Notes

Some participants highlight limitations in teaching methods and the potential for confusion among students regarding advanced concepts like 4-velocity and 4-momentum, as well as the implications of Minkowski space geometry.

bernhard.rothenstein
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do you consider that conservation laws of momentum and energy are compulsory in the derivation of the fundamental equations of relativistic dynamics
 
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In my opinion,... no, they are not compulsory.

Conservation laws arise from symmetries in the situation and may suggest interesting dynamical quantities. However, the lack of such symmetries shouldn't preclude the definition of relativistic dynamical quantities and the formulation of equations involving them.
 
bernhard.rothenstein said:
do you consider that conservation laws of momentum and energy are compulsory in the derivation of the fundamental equations of relativistic dynamics
Yes. If not, you are talking about a new theory.
 
But note in GR the conservation law is that of the conservation of energy-momentum, not in general energy, as energy is a frame dependent quantity and energy-momentum is frame independent.

Garth
 
Garth said:
But note in GR the conservation law is that of the conservation of energy-momentum, not in general energy, as energy is a frame dependent quantity and energy-momentum is frame independent.

Garth
i have in mind only the special relativity case
 
bernhard.rothenstein said:
do you consider that conservation laws of momentum and energy are compulsory in the derivation of the fundamental equations of relativistic dynamics

The fundamental equations of dynamics(equations of motion) contain (within them) the laws of conservation. We derive those equations of motion from ACTION PRINCIPLE.


regards

sam
 
OK Bernhard, I had a look at your paper (arxiv physics/0505025).
I am afraid, I saw no dynamical equation in it. The transformation equations of some dynamical quantities are not the "fundamental" equations of dynamics. It is the "equation of motion" like Newton's, Dirac's, Maxwell's, Schrödinger's and other's equation that represents the fundamental equations of dynamics.

In your paper, you seem to have derived (though I did not check the accuracy) the relativistic transformation of energy and momentum from strange combination of a result from SR (adding velocities) with some sort of "thought" experiment. But why bother yourself with this when the two postulates of SR can do all your work plus more without any thought (or otherwise) experiment?

regards

sam
 
samalkhaiat said:
OK Bernhard, I had a look at your paper (arxiv physics/0505025).
I am afraid, I saw no dynamical equation in it. The transformation equations of some dynamical quantities are not the "fundamental" equations of dynamics. It is the "equation of motion" like Newton's, Dirac's, Maxwell's, Schrödinger's and other's equation that represents the fundamental equations of dynamics.

In your paper, you seem to have derived (though I did not check the accuracy) the relativistic transformation of energy and momentum from strange combination of a result from SR (adding velocities) with some sort of "thought" experiment. But why bother yourself with this when the two postulates of SR can do all your work plus more without any thought (or otherwise) experiment?

regards

sam
thank you. all the textbooks i know, derive the transformation equations for mass, momentm and energy (i have considered that they are the fundamental equations of relativistic dynamics) from collisions, less or more complicated, not very easy to teach without mnemonic aids using conservation of momentum, mass, energy or of the center of mass. do you know a derivation of them without conservation laws?
sine ira et studio
 
bernhard.rothenstein said:
thank you. all the textbooks i know, derive the transformation equations for mass, momentm and energy (i have considered that they are the fundamental equations of relativistic dynamics) from collisions, less or more complicated, not very easy to teach without mnemonic aids using conservation of momentum, mass, energy or of the center of mass. do you know a derivation of them without conservation laws?
sine ira et studio
All you have to do is to define the 4-velocity as U^\mu=dx^\mu/d\tau, and the 4-momentum as p=mU, where m is a scalar. Then the transformation laws of mass, momentum, and energy follow immediately.

Jackson just confuses this by an irrelevant 8 page discussion of collisions.
PMB wants to confuse it by giving mass an awkward velocity dependence.
 
  • #10
Meir Achuz said:
All you have to do is to define the 4-velocity as U^\mu=dx^\mu/d\tau, and the 4-momentum as p=mU, where m is a scalar. Then the transformation laws of mass, momentum, and energy follow immediately.

Jackson just confuses this by an irrelevant 8 page discussion of collisions.
PMB wants to confuse it by giving mass an awkward velocity dependence.

IMO, the problem with doing the development in this way is that the student generally has no idea as to what the 4-velocity really is, why it is that the derivative must be taken with respect to proper time, or how the 4-momentum differs from regular momentum, aside from the fact that it now has an extra component. In order to get a real conceptual understanding of the framework of SR I believe it is important to get a solid grasp of the geometry of Minkowski space and the implied consequences this has on previously well defined quantities such as spatial and temporal intervals and simultenaity before the mathematics are introduced.

The main problem with the method I've proposed is that it typically takes much longer than the more traditional method, however the advantage is that the students get a much better understanding of the underlying theory and are more able to apply it to situations which are new to them.
 
  • #11
dicerandom said:
IMO, the problem with doing the development in this way is that the student generally has no idea as to what the 4-velocity really is, why it is that the derivative must be taken with respect to proper time, or how the 4-momentum differs from regular momentum, aside from the fact that it now has an extra component..
"the student generally has no idea" only if the teacher and textbook don't explain this.
 
  • #12
dicerandom said:
In order to get a real conceptual understanding of the framework of SR I believe it is important to get a solid grasp of the geometry of Minkowski space and the implied consequences this has on previously well defined quantities such as spatial and temporal intervals and simultenaity before the mathematics are introduced.
The math of Minkowski space is so simple and straightforward (with a good teacher and textbook) that I find students get a better understanding using math rather than handwaving grasps. I agree with Sam on this.
 
  • #13
dicerandom said:
IMO,
The main problem with the method I've proposed is that it typically takes much longer than the more traditional method, however the advantage is that the students get a much better understanding of the underlying theory and are more able to apply it to situations which are new to them.
Where do you propose your method?
Also, what is IMO?
 

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