What Is the Correct Interpretation of 4-Vector Momentum Squared?

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Homework Help Overview

The discussion revolves around the interpretation of the squared 4-momentum in the context of special relativity, specifically the equation P^2=P_{\mu}P^\mu=m^2. Participants are examining the relationship between energy, momentum, and mass, particularly under the condition where the speed of light c is set to 1.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are questioning the validity of assuming E=mc^2 in the context of total energy and are exploring the implications of using relativistic momentum. There is also discussion about the correct interpretation of the terms in the equations and the conditions under which certain formulas apply.

Discussion Status

Some participants have provided clarifications regarding the definitions of energy and momentum in relativistic contexts, suggesting that the original poster's assumptions may be incorrect. There is ongoing exploration of the relationships between the variables involved, with no explicit consensus reached yet.

Contextual Notes

Participants note that the commonly referenced equation E=mc^2 is often misapplied and that the context of its use is critical. The discussion highlights the need for careful consideration of the conditions under which different energy-momentum relationships hold true.

Ene Dene
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I'm having a problem understanding this:

[tex]P^2=P_{\mu}P^\mu=m^2[/tex]

If we take c=1.

Here is what bothers me:

[tex]P(E, \vec{p})=E^2-(\vec{p})^2[/tex]

Now, I assume that E=mc^2, and for c=1, E^2=m^2? Is that correct?

And I don't know what p^2 is, I look at it as:

[tex](\vec{p})^2=m^2(\vec{v})^2[/tex]

What am I doing wrong?
 
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Ene Dene said:
I'm having a problem understanding this:

[tex]P^2=P_{\mu}P^\mu=m^2[/tex]

If we take c=1.

Here is what bothers me:

[tex]P(E, \vec{p})=E^2-(\vec{p})^2[/tex]

Now, I assume that E=mc^2, and for c=1, E^2=m^2? Is that correct?

And I don't know what p^2 is, I look at it as:

[tex](\vec{p})^2=m^2(\vec{v})^2[/tex]

What am I doing wrong?

I am not exactly sure what bothers you but one point: [tex]E = \gamma m c^2[/tex], not mc^2 (which is valid only in the rest frame of the particle). Also the momentum is the relativistic three-momentum so it's [itex]\gamma m \vec{v}[/itex]
 
Your first equation shows m^2=E^2-p^2.
Your assumption E=m is wrong.
 
Ene Dene said:
I'm having a problem understanding this:

[tex]P^2=P_{\mu}P^\mu=m^2[/tex]

If we take c=1.

Here is what bothers me:

[tex]P(E, \vec{p})=E^2-(\vec{p})^2[/tex]

Now, I assume that E=mc^2, and for c=1, E^2=m^2? Is that correct?[/tex]

The symbol 'E' in this equation is the total energy of the particle. The popularly-known equation E = mc^2 refers to the "rest mass-energy of the particle" and is really an incorrect use of the symbol.

'p' here is just the regular ol' 3-momentum, mass times the 3-dimensional velocity vector for the particle. The so-called "4-momentum" [tex]P^{\mu}[/tex] is a 4-dimensional vector whose components are

( iE, p_x, p_y, p_z ) [or flip signs depending on whose notational convention you use].

Your original relation then,

[tex]P^2=P_{\mu}P^{\mu}[/tex]

is then just taking the "dot product" of P with itself to get the square of the magnitude,

[tex]P^2 = E^2 - p^2 = (mc^2)^2[/tex] , again with appropriate adjustments for local notational practice.
 
Last edited:
As already said, the popular formula E = mc^2 -- mostly misquoted -- is a) not generally applicable and b) not even a main result of special relativity, it's more like a small remark buried somewhere deep inside the text.

To stick with Ene Dene's approach: if you plug in the correct formula
[tex]E = \sqrt{ (\gamma m c^2)^2 + (m p^2)^2 }[/tex]
you will get a consistent result.
In units where c = 1, it'd be
[tex]E^2 = \gamma m^2 + p^4[/tex]
and
[tex]p = \gamma m v[/tex].
Also note that you can deduce where E = mc^2 is applicable; the general formula reduces to it in the rest frame (p = 0) at non-relativistic speeds ([itex]\gamma \approx 1[/itex]).
 

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