Relativistic momentum and photons

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Discussion Overview

The discussion centers on the relationship between relativistic momentum and photons, particularly addressing how photons, which have zero rest mass, can possess momentum and energy. The scope includes theoretical considerations and interpretations from both classical and quantum physics perspectives.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how photons can have momentum and energy given that the relativistic momentum formula becomes undefined when mass is zero.
  • Another participant suggests that the definition of momentum used is applicable only to particles with nonzero rest mass and proposes using quantum mechanics, where the energy of a photon is expressed as E=hf, to derive its momentum.
  • A third participant notes that in classical electrodynamics, electromagnetic waves, including photons, carry momentum proportional to their energy, aligning with the relationship E=pc.
  • One participant emphasizes the importance of understanding which formulas apply to different physical situations, indicating a broader conceptual approach to the topic.
  • A later reply introduces transformation equations for momentum and energy, suggesting how they simplify in the case of a photon moving at the speed of light.

Areas of Agreement / Disagreement

Participants generally agree on the need to consider different frameworks (classical vs. quantum) for understanding photon momentum, but there are differing views on how to reconcile the relativistic momentum equation with the properties of massless particles.

Contextual Notes

Limitations include the dependency on definitions of momentum and energy in different contexts, as well as unresolved aspects of the transformation equations presented.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of physics, particularly those interested in the nuances of relativistic mechanics and quantum theory as they relate to massless particles like photons.

FrankJ777
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I have a question about photons and relativistic momentum. According to my Physics text (Serway & Beichner), the energy of a partle with zero mass, such as a photon, can be related by E[tex]^{}2[/tex]=p[tex]^{}2[/tex]c[tex]^{}2[/tex]+(mc[tex]^{}2[/tex])[tex]^{}2[/tex]. m=0 so the expression becomes E=pc. Since relativistic momentum is p=mu/[tex]\sqrt{}1(-u2^{}[/tex]/c[tex]^{}2[/tex]) and m=0 for a photon, how is there any momentum and thus energy?
 
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That definition of momentum only works for things with nonzero rest mass, as you've noticed it becomes undefined (0/0) when you set m=0 and u=c. We can turn to quantum physics for the momentum of a photon--in QM we have E=hf where h is Planck's constant and f is the frequency, so you can substitute this value of E into E=pc to find the photon's relativistic momentum.
 
Also note that in classical electrodynamics, an electromagnetic wave carries momentum in proportion to its energy, via E = pc, same as you get from the relativistic mass-energy-momentum relationship with m = 0.
 
I agree with the posts above. A major trick in physics, that usually comes after studying different pehenomena in different situations, is "which formula(s) applies to the situation I'm working on now"...
 
Naty1 said:
I agree with the posts above. A major trick in physics, that usually comes after studying different pehenomena in different situations, is "which formula(s) applies to the situation I'm working on now"...

I would start with the transformation equations for the momentum and the energy of a particle moving with speed u' relative to I' presented as
p=gp'(1+V/u') (1)
E=gE'(1+Vu'/cc) (2)
In the case of a photon (u'=c) (1) and (2) become
p=gp'(1+V/c)
E=gE'(1+V/c)
 

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