Is There a Non-QED Derivation of E=pc?

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In summary: I do not know if it has a solution, this is why I asked.Shankar derives it by quantizing the electromagnetic field, but it's not really fully-fledged QED, in my opinion. See Shankar's text on QM, chapter 18, pg. 516 (2nd ed.), equation 18.5.69.
  • #1
clj4
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Can anybody point out if there is a NON-QED derivation of E=pc ?
I would need a reference if such a derivation existed. Thank you in advance.

PS: I am not looking for the definition of 4 vector invariants that leads to [tex]E^2 = (pc)^2 + (mc^2)^2[/tex].
In the same vein, I am not looking for setting m=0 in the above equation because it brings up the question of deriving [tex]E^2 = (pc)^2 + (mc^2)^2[/tex] from first principles without resorting to QED.
 
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  • #2
Derived from which principles?
 
  • #3
E=pc can be derived from special relativity. The general relationship between energy and momentum is:

[tex]E^2 = (pc)^2 + (mc^2)^2[/tex]

For a photon with rest mass m=0, the result follows.

p=hf is incorrect. The correct de Broglie wavelength formula is [itex]p=h/\lambda[/itex].

This can be derived from the formula E=pc for a photon, by using the photon energy E=hf.
 
  • #4
masudr said:
Derived from which principles?

From base principles, in the style of Einstein's derivation of [tex]E=mc^2[/tex] (not from a definition and nor from the trivial exercise of setting m=0 in [tex]E^2=(pc)^2+(mc^2)^2[/tex]. The latter derivation is of no use.
This appears to be a tough problem, I do not know if it has a solution, this is why I asked.
 
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  • #5
James R said:
E=pc can be derived from special relativity. The general relationship between energy and momentum is:

[tex]E^2 = (pc)^2 + (mc^2)^2[/tex]

For a photon with rest mass m=0, the result follows.

p=hf is incorrect. The correct de Broglie wavelength formula is [itex]p=h/\lambda[/itex].

This can be derived from the formula E=pc for a photon, by using the photon energy E=hf.

Thank you, I appreciate the effort. I should have mentioned that I am not looking for setting m=0 in
[tex]E^2 = (pc)^2 + (mc^2)^2[/tex]
either, since that brings about deriving this from first principles.
Since I am on this subject, I am not looking for the definition of 4 vector invariants that leads to [tex]E^2 = (pc)^2 + (mc^2)^2[/tex]
 
  • #6
It most likely follows from stat mech, if you *assume* the various distributions are true apriori and run it in reverse, though I have never seen it done before.

The field theory proof is sort of the nontrivial one that kinda jumps out at you, but I guess that doesn't interest you.
 
  • #7
clj4 said:
Can anybody point out if there is a NON-QED derivation of E=pc ?
I would need a reference if such a derivation existed. Thank you in advance.

I imagine you could find the energy and momentum of a plane wave, and point out that they are related by E=pc? (At least in a vacuum).

I suppose you'd also need a proof that the far field can always be written as a sum of plane waves. (I think this is true, but actually I'm not 100% sure).
 
  • #8
pervect said:
I imagine you could find the energy and momentum of a plane wave, and point out that they are related by E=pc? (At least in a vacuum)..

I tried that , didn't manage. I tried with a spherical wave , for some reason I thought it would be easier due to symmetry. Thiis is why I a asking for a reference :-)
 
  • #9
masudr asked "from which principles" and dj4's answer was "Yes"?

You have said you wanted to know a "non-QED" method to derive E=pc (which is peculiar in itself since E= pc doesn't involve QED to begin with) and you don't want to use "one method" and you don't want to use "another method". Exactly what do you want? Your question is very unclear.
 
  • #10
Shankar derives it by quantizing the electromagnetic field, but it's not really fully-fledged QED, in my opinion. See Shankar's text on QM, chapter 18, pg. 516 (2nd ed.), equation 18.5.69.
 
  • #11
HallsofIvy said:
masudr asked "from which principles" and dj4's answer was "Yes"?

You have said you wanted to know a "non-QED" method to derive E=pc (which is peculiar in itself since E= pc doesn't involve QED to begin with) and you don't want to use "one method" and you don't want to use "another method". Exactly what do you want? Your question is very unclear.
From base principles, in the style of Einstein's derivation of [tex]E=mc^2[/tex] (not from a definition and nor from the trivial exercise of setting m=0 in [tex]E^2=(pc)^2+(mc^2)^2[/tex]. The latter derivation is of no use.
This appears to be a tough problem, I do not know if it has a solution, this is why I asked.
 
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  • #12
masudr said:
Shankar derives it by quantizing the electromagnetic field, but it's not really fully-fledged QED, in my opinion. See Shankar's text on QM, chapter 18, pg. 516 (2nd ed.), equation 18.5.69.

Thank you, I will have a look though I would want to avoid QM as well as QED.I am looking for a derivation in the style of Einstein's derivation of [tex]E=mc^2[/tex] (not from a definition and nor from the trivial exercise of setting m=0 in [tex]E^2=(pc)^2+(mc^2)^2[/tex]. The latter derivation is of no use.
This appears to be a tough problem, I do not know if it has a solution, this is why I asked.
 
  • #13
clj4 said:
Thank you, I will have a look though I would want to avoid QM as well as QED.

Well, the photon, which is the notion of a massless boson which are the excitations of the EM field, can only reasonably be described by QED, since it is in this framework that it arises.

And from that, one can show that E = pc must be satisfied by those particles. It's kind of unfair asking to derive a property of photons without using the model/theory that predicts its existence, don't you think?
 
  • #14
masudr said:
Well, the photon, which is the notion of a massless boson which are the excitations of the EM field, can only reasonably be described by QED, since it is in this framework that it arises.

And from that, one can show that E = pc must be satisfied by those particles. It's kind of unfair asking to derive a property of photons without using the model/theory that predicts its existence, don't you think?

I don't know . The whole idea is to avoid the quantization (the notion of photon) altogether and to use wave theory only. After all , Einstein did this in deriving radiation pressure. In general, it is much more difficult to prove that something cannot be done. In effect, I am interested in how Einstein would have established E=pc with what he had at hand in 1905. Is it possible? has it been done? can we prove that it is impossible?One of the posters informed me that the issue might be covered in:

A.P.French, Special Relativity Nelson Chapter 1

I do not have the book, anyone can help with scanning the text and posting it ?
Thank you
 
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  • #15
Sorry to go on about it, but am I right in thinking that what you want is to show that the momentum of a classical EM wave is equal to it's energy divided by c?
 
  • #16
masudr said:
Sorry to go on about it, but am I right in thinking that what you want is to show that the momentum of a classical EM wave is equal to it's energy divided by c?

Yes, this is correct.
 
  • #17
I did a quick search and found http://www.tphys.physik.uni-tuebingen.de/faessler/Physik3/optik4_2.pdf" (in German).
Eq. 4.43-4.46, figure 4.4
The Lorentz Force always pushes a charged particle in the same direction. By comparing work and force you get E=pc.
 
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  • #18
Ich said:
I did a quick search and found http://www.tphys.physik.uni-tuebingen.de/faessler/Physik3/optik4_2.pdf" (in German).
Eq. 4.43-4.46, figure 4.4
The Lorentz Force always pushes a charged particle in the same direction. By comparing work and force you get E=pc.

Thank you!

Following the same search principle I found another derivation:

http://www.mathpages.com/home/kmath601/kmath601.htm
 
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  • #19
E=pv

You can refer to http://www.geocentricity.com/ba1/no82/byl.html
dU=Fx=(dp/dt)x=dp(x/dt)=dpv, after integral, you can get E=pv
 
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Related to Is There a Non-QED Derivation of E=pc?

1. How is the equation E=pc derived without using QED?

The equation E=pc can be derived using the principles of classical mechanics and special relativity. It involves the conservation of energy and momentum, along with the relationship between energy, mass, and velocity.

2. Can the NON-QED derivation of E=pc be applied to all particles?

Yes, the NON-QED derivation of E=pc can be applied to all particles, including massive particles like electrons and photons.

3. What are the limitations of the NON-QED derivation of E=pc?

The NON-QED derivation of E=pc does not take into account the effects of quantum mechanics and electrodynamics. It is only applicable to macroscopic objects and cannot fully explain the behavior of subatomic particles.

4. How does the NON-QED derivation of E=pc differ from the QED derivation?

The NON-QED derivation of E=pc is based on classical mechanics and special relativity, while the QED derivation takes into account quantum mechanics and electrodynamics. The QED derivation is more accurate and can fully explain the behavior of particles at the subatomic level.

5. Is the NON-QED derivation of E=pc widely accepted by the scientific community?

Yes, the NON-QED derivation of E=pc is widely accepted by the scientific community as it is based on well-established principles and has been experimentally verified. However, it is not the most accurate explanation for the behavior of particles at the subatomic level.

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