Special Relativity: Kinetic Energy Expansion and Contradictions

The momentum is ##p##. the term is coming asm0c2(-.5C2(-v2/c2)2)I think you should write it as ##\frac{m_0c^2}{2}\left(-\frac{v^2}{c^2}\right)^2##.
  • #1
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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  • #2
You would need to show your work. Are you using the relativistic expression for ##p##?
 
Last edited:
  • #3
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##?
 
  • #4
PeroK said:
Are you trying to get ##\frac12 m_0v^2##?
this term is coming from both but the second term is coming different
 
  • #5
PeroK said:
Are you trying to get ##\frac12 m_0v^2##?

I think he's looking at the next term in the series.
 
  • #6
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
 
  • #7
Mister T said:
I think he's looking at the next term in the series.
yes
 
  • #8
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##.
 
  • #9
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.
 

1. What is special relativity?

Special relativity is a theory developed by Albert Einstein in 1905 that explains the relationship between space and time. It states that the laws of physics are the same for all observers, regardless of their relative motion.

2. What is the kinetic energy expansion in special relativity?

The kinetic energy expansion in special relativity refers to the increase in an object's kinetic energy as it approaches the speed of light. According to Einstein's famous equation E=mc², the mass of an object increases as it gains speed, resulting in an increase in its kinetic energy.

3. What are some contradictions in special relativity?

One of the most well-known contradictions in special relativity is the Twin Paradox, which involves two twins, one traveling near the speed of light and the other remaining on Earth. When the traveling twin returns, they will have aged less than the twin who stayed on Earth, despite the fact that time should have passed at the same rate for both twins according to special relativity.

4. How does special relativity affect our everyday lives?

Special relativity has a significant impact on our everyday lives, especially in the fields of technology and communication. GPS systems, for example, must account for the effects of special relativity in order to accurately calculate location and time. Additionally, special relativity has led to advancements in nuclear energy and particle accelerators.

5. Is special relativity still a valid theory?

Yes, special relativity is still considered a valid theory and has been extensively tested and proven through experiments and observations. It is widely accepted by the scientific community and is used in many areas of physics, including astrophysics and quantum mechanics.

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