What is the gamma factor in a particle's rest frame?

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Discussion Overview

The discussion revolves around the concept of the gamma factor in special relativity (SR), particularly in relation to a particle's rest frame and its implications for 4-momentum. Participants explore the definitions and applications of the gamma factor, addressing its role in different inertial reference frames (IRFs) and the confusion surrounding its use when a particle is at rest.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that in the rest frame of a particle, the 4-momentum is given by (m, 0, 0, 0) and that the gamma factor γ(v) equals 1 when v = 0.
  • Others clarify that the gamma factor is a function that can be evaluated for any velocity v in its domain, and that it is not limited to the relative velocity between two IRFs.
  • Some participants propose that there are multiple gamma factors: one for the relative velocity between two IRFs (γ_v) and others for the particle's velocity in each frame (γ and γ').
  • A later reply questions whether the second frame can be considered as the rest frame of the particle, and if the particle must be at the origin of that frame.
  • Participants discuss the potential confusion arising from the use of the gamma factor in different contexts, emphasizing that it is simply a function that appears in various formulas in special relativity.
  • One participant notes that the relative velocity between two inertial frames can indeed be zero, leading to γ = 1.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and confusion regarding the gamma factor's application in different contexts. There is no consensus on the best way to conceptualize the gamma factor in relation to the rest frame of a particle, and multiple competing views remain on its interpretation.

Contextual Notes

Participants highlight that the gamma factor can arise in multiple contexts and is not solely associated with Lorentz transformations. The discussion reveals a need for clarity regarding the definitions and applications of the gamma factor in special relativity.

dyn
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Hi.
If the 4-momentum in SR is given by p = m γ(v) ( 1 , v ) then in the rest frame of a particle the 4-momentum is ( m , 0 , 0 , 0 ) using c=1 units. This uses the fact that because v = 0 then γ(v) = 1.
I'm confused about this last sentence. The gamma factor is used for the relative velocity between 2 inertial frames but in the rest frame the particle is at rest relative to every other inertial frame so how can we specify a gamma factor ?
 
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v is velocity of a body in your IFR. v=0 means the body is at rest in your IFR.
 
dyn said:
Hi.
If the 4-momentum in SR is given by p = m γ(v) ( 1 , v ) then in the rest frame of a particle the 4-momentum is ( m , 0 , 0 , 0 ) using c=1 units. This uses the fact that because v = 0 then γ(v) = 1.
I'm confused about this last sentence. The gamma factor is used for the relative velocity between 2 inertial frames but in the rest frame the particle is at rest relative to every other inertial frame so how can we specify a gamma factor ?

I think you may be confusing the gamma factor that connects two IRF's with the gamma factor of a particle. In fact, if you have a particle and two IRF's then there are three gamma factors.

Suppose the frames are ##S## and ##S'## and the relative velocity between them is ##v##. Then we have a gamma factor ##\gamma_v## that determines the Lorentz Transformation between the frames.

If we then have a particle moving with velocity ##u## in frame ##S## and velocity ##u'## in frame ##S'##, then the particle has a different gamma factor in each frame and the energy-momentum of that particle in those frames is given by:

##p^\mu = m \gamma (1, \vec{u}) \ ## and ##p'^\mu = m \gamma' (1, \vec{u'})##

Where ##\gamma## is the gamma factor of the particle in frame ##S## and ##\gamma'## is the gamma factor of the particle in frame ##S'##.

There is a useful relationship between these gamma factors, which is:

##\gamma' = \gamma_v \gamma (1 - vu_x)##

(Assuming, as usual, that ##S'## is moving with velocity ##v## in the +ve x-direction in frame ##S##.)

It's a good exercise to derive that formula.
 
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dyn said:
This uses the fact that because v = 0 then γ(v) = 1.
I'm confused about this last sentence.
I am not sure how this can be confusing.
##\gamma(v)=1/\sqrt{1-v^2/c^2}## so clearly ##\gamma(0)=1##

##\gamma(v)## is just a function. It does show up in the Lorentz transform, but it is still just a function which can be evaluated for any v in its domain.
 
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dyn said:
Hi.
If the 4-momentum in SR is given by p = m γ(v) ( 1 , v ) then in the rest frame of a particle the 4-momentum is ( m , 0 , 0 , 0 ) using c=1 units. This uses the fact that because v = 0 then γ(v) = 1.
I'm confused about this last sentence. The gamma factor is used for the relative velocity between 2 inertial frames but in the rest frame the particle is at rest relative to every other inertial frame so how can we specify a gamma factor ?
I think what confuses you is that when considering the speed v between frames, at least TWO observers MUST be considered. But when considering the gamma factor of a particle in your frame, at least ONE observer must be considered. If you are at rest and the particle moves at speed u, it’s gamma factor FOR YOUR FRAME is γu. (Of course you can combine the two situations, like in your original example).Useful information:

https://courses.lumenlearning.com/physics/chapter/28-5-relativistic-momentum/

As PeroK pointed out, in your example there are THREE gamma factors: a gamma factor relating the two reference frames (γv), but there are also gamma factors for the particles themselves in each frame (γu and γu’).The gamma factor of the particle in your rest frame is 1, as you said.
 
Sorcerer said:
I think what confuses you is that when considering the speed v between frames, at least TWO observers MUST be considered. But when considering the gamma factor of a particle in your frame, at least ONE observer must be considered. If you are at rest and the particle moves at speed u, it’s gamma factor FOR YOUR FRAME is γu. (Of course you can combine the two situations, like in your original example)
.
Yes this is what is confusing me. For questions involving 4-momentum , the gamma factor uses the velocity of the particle in my frame but that is the only frame being used and I am the only observer. Can the second frame be considered as the rest frame of the particle with the particle at its origin ? Does it have to be at the origin ? In which case the velocity of the particle in my frame is the relative velocity between these 2 frames .
 
dyn said:
Yes this is what is confusing me. For questions involving 4-momentum , the gamma factor uses the velocity of the particle in my frame but that is the only frame being used and I am the only observer.
Again, that is one context in which the gamma factor arises, but it is just a function that can arise in other contexts. In this context v is just the velocity of the particle in a given frame.
 
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dyn said:
Yes this is what is confusing me. For questions involving 4-momentum , the gamma factor uses the velocity of the particle in my frame but that is the only frame being used and I am the only observer. Can the second frame be considered as the rest frame of the particle with the particle at its origin ? Does it have to be at the origin ? In which case the velocity of the particle in my frame is the relative velocity between these 2 frames .
Let me ask you a question: if we always wrote the Lorentz transforms as$$\begin{eqnarray*}
t'&=&\frac{t-vx/c^2}{\sqrt{1-v^2/c^2}}\\
x'&=&\frac{x-vt}{\sqrt{1-v^2/c^2}}
\end{eqnarray*}$$and always wrote the particle momentum as$$p=\frac{mv}{\sqrt{1-v^2/c^2}}$$then would the appearance of that same square root term in both bother you? You'd just use the appropriate ##v## and carry on. But since we've given it its own symbol you seem to be getting confused. Don't. ##\gamma## is simply an expression that comes up often enough that we got fed up of writing out that square root every time.

Another thing to ask yourself - ##v## appears in the Lorentz transforms and in the expression for momentum. Why aren't you worried about ##v## in the same way you are worried about ##\gamma##?

Basically, you are confusing yourself, I think. There is no mystery - ##\gamma## isn't solely associated with Lorentz transforms. It appears in many formulae in special relativity. Generally it's obvious which velocity you should use because there's only one physically relevant velocity which, in the case of a particle's momentum, is the velocity of the particle. What else could matter?
 
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dyn said:
The gamma factor is used for the relative velocity between 2 inertial frames but in the rest frame the particle is at rest relative to every other inertial frame so how can we specify a gamma factor ?

The relative velocity between two inertial frames can be zero! In that case ##\gamma=1##.
 
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