Atkisnon's derivation of \gamma factor.

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In summary, the conversation discusses a confusion about the concept of gamma in special theory of relativity, which is a function of velocity. The person is puzzled about why gamma cannot be an even function of velocity, such as v^4. However, it is pointed out that every even function of velocity is actually a function of velocity squared. Thus, the person realizes their mistake and thanks the other person for their clarification.
  • #1
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So I am rereading David Atkinson's QFT book:
http://books.google.co.il/books/about/Quantum_Field_Theory.html?id=vbAnQAAACAAJ&redir_esc=y

And I am puzzled by what is written in pages 5-6 section 1.3 Special Theory of Relativity.

He writes down the transformation between two inertial frames, one moving at speed v compared to the other.

[tex] x'=\gamma (x-vt) \ y'=y \ z'=z[/tex]

Now he writes on page 6:
What is gamma?
From the uniformity of space, we see that \gamma may not depend on the coordinates (...).
In the absence of gravity, \gamma is independent of t,x,y,z but it may depend on v.
...
Rotational invariance therefore means that \gamma must be independent of the sign of v, i.e, it's a function only of v^2.

My problem is with the last conclusion, why can't we have \gamma to be any even function of v, like v^4 and so forth?
 
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  • #2
any even function of v is a function of v^2.

v^4 = (v^2)^2
 
  • #3
Feel so stupid now... :-D

Thanks.
 
  • #4
don't feel bad. everybody misses stuff like that at times.

in fact you could come back and ask. really? every even function
of v is a function of v^2? those are two different things in principle,
even functions f(v) = f(-v) and f(v) = h(v^2) for some h.

it's not that hard to prove either.
 
  • #5


I would respond by saying that Atkinson's derivation of the \gamma factor is based on the principles of special relativity, which state that the laws of physics should be the same in all inertial frames of reference. This leads to the conclusion that \gamma cannot depend on the coordinates, as it would violate the principle of uniformity of space. Additionally, rotational invariance requires \gamma to be independent of the sign of v, which means it can only be a function of v^2.

It is possible that other even functions of v, such as v^4, could satisfy these requirements, but they would not be consistent with the principles of special relativity. Atkinson's derivation is based on these principles and has been extensively tested and verified through experiments, making it a valid and reliable explanation of the \gamma factor.
 

1. What is Atkinsnon's derivation of \gamma factor?

Atkinsnon's derivation of \gamma factor is a mathematical equation that calculates the relative velocity between two objects in terms of their masses, distances, and time. It is a key component of Einstein's theory of special relativity.

2. How is Atkinsnon's derivation of \gamma factor used in science?

Atkinsnon's derivation of \gamma factor is used in many fields of science, including astronomy, physics, and engineering. It is particularly useful in calculating the effects of time dilation and length contraction at high speeds.

3. What is the significance of Atkinsnon's derivation of \gamma factor in Einstein's theory of special relativity?

Atkinsnon's derivation of \gamma factor is a crucial part of Einstein's theory of special relativity. It helps to explain the observed effects of time dilation and length contraction, which occur at high speeds and are fundamental to our understanding of the universe.

4. Can Atkinsnon's derivation of \gamma factor be applied to objects moving at any speed?

No, Atkinsnon's derivation of \gamma factor is specifically designed for objects moving at speeds close to the speed of light. It does not accurately calculate the relative velocity of objects at lower speeds.

5. What are the limitations of Atkinsnon's derivation of \gamma factor?

Atkinsnon's derivation of \gamma factor is only accurate for objects moving at constant speeds in a straight line. It does not account for acceleration or changes in direction, and it does not apply to objects with massless particles.

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