Special Relativity: Kinetic Energy Expansion and Contradictions

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Discussion Overview

The discussion revolves around the expansion of kinetic energy in the context of special relativity, specifically examining the expressions for kinetic energy derived from different formulations. Participants explore potential contradictions in the results obtained from these expansions and the implications of using different definitions of momentum.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants present the kinetic energy expansion as T=mc²-m₀c², where m₀ is the rest mass and m is defined as m₀/sqrt(1-β²), leading to a correction term of -p⁴/8m₀³c².
  • Others propose an alternative approach using T=E-m₀c², where E=sqrt(c²p²+m₀²c⁴), resulting in a different correction term of 3p⁴/8m₀³c².
  • There is a question raised about whether these two approaches yield a contradiction.
  • Some participants emphasize the need to clarify the use of the relativistic expression for momentum (p) versus the Newtonian definition (p=m₀v).
  • Concerns are expressed regarding the application of the binomial expansion in the calculations, with some suggesting that mistakes may have been made in the first case.
  • One participant notes that if p is assumed to be small, an expansion in terms of p/c can be derived, but highlights that p includes a gamma factor, complicating direct comparisons with expansions involving v/c.
  • Another participant mentions that the first terms of the expansions yield different results, indicating that they are not equal and have different signs.
  • There is a reference to a related thread that uses different notation for mass, which may help clarify the discussion.

Areas of Agreement / Disagreement

Participants express differing views on the validity of the expansions and the definitions used for momentum, indicating that the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Limitations include potential misunderstandings in the application of the binomial expansion and the definitions of momentum, which may affect the results. The discussion also highlights the complexity of comparing different formulations in special relativity.

Das apashanka
When expanding Kinetic energy as
T=mc2-m0c2
where m0=rest mass and
m=m0/sqrt(1-β2)
the first term correction is coming out to be -p4/8m03c2
but taking T=E-m0c2
where E=sqrt(c^2p^2+m02c4) the correction is coming to be 3p^4/8m03c2
is there any contradiction?
 
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You would need to show your work. Are you using the relativistic expression for ##p##?
 
Last edited:
Das apashanka said:
When expanding Kinetic energy as
T=mc2-m0c2
where m0=rest mass and
m=m0/sqrt(1-β2)
the first term correction is coming out to be -p4/8m03c2
but taking T=E-m0c2
where E=sqrt(c^2p^2+m02c4) the correction is coming to be 3p^4/8m03c2
is there any contradiction?

Are you trying to get ##\frac12 m_0v^2##?
 
PeroK said:
Are you trying to get ##\frac12 m_0v^2##?
this term is coming from both but the second term is coming different
 
PeroK said:
Are you trying to get ##\frac12 m_0v^2##?

I think he's looking at the next term in the series.
 
Mister T said:
You would need to show your work. Are you using the relativistic expression for ##p##?
for the second case p remains as it is but for the first case I have taken p=m0v
 
Mister T said:
I think he's looking at the next term in the series.
yes
 
Das apashanka said:
this term is coming from both but the second term is coming different
You must have made a mistake with the binomial expansion in the first case.

I don't see how you can take ##p = m_0 v##.
 
Das apashanka said:
for the second case p remains as it is but for the first case I have taken p=m0v

Well, that's likely the reason for the discrepancy in your two results!

In the relation ##E=\sqrt{(pc)^2+(m_oc^2)^2}##, ##p## is the relativistic momentum given by ##\frac{m_o v}{\sqrt{1-\beta^2}}##, not the Newtonian ##m_o v##.
 
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  • #10
Mister T said:
Well, that's likely the reason for the discrepancy in your two results!

In the relation ##E=\sqrt{(pc)^2+(m_oc^2)^2}##, ##p## is the relativistic momentum given by ##\frac{m_o v}{\sqrt{1-\beta^2}}##, not the Newtonian ##m_o v##.
ok thanks, I have mislooked that thing
 
  • #11
Das apashanka said:
ok thanks, I have mislooked that thing
but that doesn't match the coefficient of -1/8 and 3/8
 
  • #12
Das apashanka said:
ok thanks, I have mislooked that thing

I'm not sure how you apply the binomial expansion to that, given that neither term need be larger than the other.
 
  • #13
PeroK said:
You must have made a mistake with the binomial expansion in the first case.

I don't see how you can take ##p = m_0 v##.
PeroK said:
You must have made a mistake with the binomial expansion in the first case.

I don't see how you can take ##p = m_0 v##.
the term is coming as
m0c2(-.5C2(-v2/c2)2)
 
  • #14
Das apashanka said:
the term is coming as
m0c2(-.5C2(-v2/c2)2)
It's a mess in any case.

If you assume ##p## is small, then you can get an expansion in terms ##p/c##. But, ##p## has a gamma factor, so you cannot compare this expansion directly with the expansion involving ##v/c##.

The first terms are ##\frac12 m_0v^2## and ##\frac{p^2}{2m_0}## respectively. But, these are not equal; and neither are the second terms, which in fact have different signs.
 
  • #15
Das apashanka said:
When expanding Kinetic energy as
T=mc2-m0c2
where m0=rest mass and
m=m0/sqrt(1-β2)

You should get ##T \approx m_oc^2\left(\frac{1}{2}\beta^2 + \frac{3}{8}\beta^4\right)##

the first term correction is coming out to be -p4/8m03c2

Mine is ##\frac{3m_ov^4}{8c^2}##.

Replace ##m_o v## with ##p## and you get ##\frac{3p^4}{8m_o^3c^2}##.

but taking T=E-m0c2
where E=sqrt(c^2p^2+m02c4) the correction is coming to be 3p^4/8m03c2
is there any contradiction?

I'm not sure how you did that, but it matches what I got above!

By the way, you may find this thread interesting:
https://www.physicsforums.com/threads/kinetic-energy-and-momentum-of-a-relativistic-particle.895897/
There the usual notation is used, where ##m## is the ordinary mass, what you are calling the rest mass.
 

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